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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">BG</journal-id>
<journal-title-group>
<journal-title>Biogeosciences</journal-title>
<abbrev-journal-title abbrev-type="publisher">BG</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Biogeosciences</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1726-4189</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/bg-14-3287-2017</article-id><title-group><article-title>Size-dependent response of foraminiferal calcification<?xmltex \hack{\newline}?> to seawater carbonate chemistry</article-title>
      </title-group><?xmltex \runningtitle{Size-dependent response of calcification to acidification}?><?xmltex \runningauthor{M. J. Henehan et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Henehan</surname><given-names>Michael J.</given-names></name>
          <email>michael.henehan@yale.edu</email>
        <ext-link>https://orcid.org/0000-0003-4706-1233</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Evans</surname><given-names>David</given-names></name>
          <email>de32@st-andrews.ac.uk</email>
        <ext-link>https://orcid.org/0000-0002-8685-671X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Shankle</surname><given-names>Madison</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Burke</surname><given-names>Janet E.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Foster</surname><given-names>Gavin L.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3688-9668</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Anagnostou</surname><given-names>Eleni</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7200-4794</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Chalk</surname><given-names>Thomas B.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4">
          <name><surname>Stewart</surname><given-names>Joseph A.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff5">
          <name><surname>Alt</surname><given-names>Claudia H. S.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Durrant</surname><given-names>Joseph</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Hull</surname><given-names>Pincelli M.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Geology and Geophysics, Yale University, 210 Whitney Avenue, New Haven, CT 06511, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Earth and Environmental Sciences, University of St Andrews, Irvine Building, North Street, St Andrews, Fife, KY16 9AL, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Ocean and Earth Science, University of Southampton, National Oceanography Centre Southampton, Southampton,<?xmltex \hack{\newline}?> SO14 3ZH, UK</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>National Institute of Standards and Technology, Hollings Marine Laboratory, 331 Ft. Johnson Road
Charleston,<?xmltex \hack{\newline}?> SC 29412, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Biology, College of Charleston, Charleston, SC 29424, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Michael J. Henehan (michael.henehan@yale.edu) and David Evans (de32@st-andrews.ac.uk)</corresp></author-notes><pub-date><day>10</day><month>July</month><year>2017</year></pub-date>
      
      <volume>14</volume>
      <issue>13</issue>
      <fpage>3287</fpage><lpage>3308</lpage>
      <history>
        <date date-type="received"><day>26</day><month>October</month><year>2016</year></date>
           <date date-type="rev-request"><day>8</day><month>November</month><year>2016</year></date>
           <date date-type="rev-recd"><day>16</day><month>May</month><year>2017</year></date>
           <date date-type="accepted"><day>19</day><month>May</month><year>2017</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017.html">This article is available from https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017.html</self-uri>
<self-uri xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017.pdf">The full text article is available as a PDF file from https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017.pdf</self-uri>


      <abstract>
    <p>The response of the marine carbon cycle to changes in atmospheric CO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
concentrations will be determined, in part, by the relative response of
calcifying and non-calcifying organisms to global change. Planktonic
foraminifera are responsible for a quarter or more of global carbonate
production, therefore understanding the sensitivity of calcification in these
organisms to environmental change is critical. Despite this, there remains
little consensus as to whether, or to what extent, chemical and physical
factors affect foraminiferal calcification. To address this, we directly test
the effect of multiple controls on calcification in culture experiments and
core-top measurements of <italic>Globigerinoides ruber</italic>. We find that two
factors, body size and the carbonate system, strongly influence calcification
intensity in life, but that exposure to corrosive bottom waters can overprint
this signal post mortem. Using a simple model for the addition of calcite
through ontogeny, we show that variable body size between and within datasets
could complicate studies that examine environmental controls on foraminiferal
shell weight. In addition, we suggest that size could ultimately play a role
in determining whether calcification will increase or decrease with
acidification. Our models highlight that knowledge of the specific
morphological and physiological mechanisms driving ontogenetic change in
calcification in different species will be critical in predicting the
response of foraminiferal calcification to future change in atmospheric
<inline-formula><mml:math id="M2" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>CO<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Calcium carbonate (CaCO<inline-formula><mml:math id="M4" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>) production and transport to the deep ocean (the
so-called “carbonate pump”) is one of the most important sinks of carbon,
acting across a range of geological timescales
<xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx15" id="paren.1"/>. In the Cenozoic (0–66 Ma),
biogenic CaCO<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> production by foraminifera, coccolithophores and coral reef
ecosystems comprises the vast majority of marine carbonate production
<xref ref-type="bibr" rid="bib1.bibx62" id="paren.2"/>. The strength of this carbonate pump can be altered
in three principal ways: (1) by changing the efficiency of inorganic and/or
organic carbon export and burial, (2) by changing the absolute or relative
abundance of calcifying and non-calcifying taxa, and (3) by changes in the
calcification efficiency of marine calcifiers. All three factors are thought
to be sensitive to environmental conditions
<xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx5" id="paren.3"><named-content content-type="pre">e.g.</named-content></xref>, although the exact
nature of this environmental sensitivity remains unclear. Here we use a
series of culturing experiments to specifically address how pH change can
influence the extent to which foraminifera calcify their tests (i.e. their
“calcification intensity”).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Description of important terms used in this paper and the relevant
literature.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="199.169291pt"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="128.037402pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Term</oasis:entry>  
         <oasis:entry colname="col2">Shorthand</oasis:entry>  
         <oasis:entry colname="col3">Meaning</oasis:entry>  
         <oasis:entry colname="col4">Further reading</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Size-normalised weight</oasis:entry>  
         <oasis:entry colname="col2">SNW</oasis:entry>  
         <oasis:entry colname="col3">A general term for the mass of foraminiferal tests divided by some metric of test size. The term describes how “heavily calcified” foraminiferal shells are, but importantly, it does not discern between changes in the degree of calcification during life vs. post mortem thinning and dissolution. Many methods exist in the literature for normalising test mass to size, each with merits and pitfalls.</oasis:entry>  
         <oasis:entry colname="col4">e.g. <xref ref-type="bibr" rid="bib1.bibx1" id="text.4"/>,<?xmltex \hack{\hfill\break}?> <xref ref-type="bibr" rid="bib1.bibx11" id="text.5"/></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Calcification intensity</oasis:entry>  
         <oasis:entry colname="col2">CI</oasis:entry>  
         <oasis:entry colname="col3">A more specific term under the umbrella of SNW that refers to how thickly foraminifera calcified in life. For our culture experiments, this is defined more specifically by Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>).</oasis:entry>  
         <oasis:entry colname="col4">This study, Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Area density</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3">A specific metric of size-normalised weight that normalises test mass to cross-sectional area. Since it has been increasingly used in recent studies, we discuss some implications for this particular metric.</oasis:entry>  
         <oasis:entry colname="col4">e.g. <xref ref-type="bibr" rid="bib1.bibx51" id="text.6"/>,<?xmltex \hack{\hfill\break}?> <xref ref-type="bibr" rid="bib1.bibx86" id="text.7"/></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>Metrics of calcification in planktonic foraminifera have already been the
subject of much scientific attention because of both the importance of
foraminifera to the global carbonate burial flux <xref ref-type="bibr" rid="bib1.bibx68" id="paren.8"><named-content content-type="pre">32–80 % of the
total deep marine calcite budget; </named-content></xref> and the potential of
these metrics to act as proxies for changes in marine carbonate chemistry. In
this paper we will refer to several types of related (but distinct) metrics
that have been used to describe calcification in foraminifera, and so for
clarity these are summarised in Table <xref ref-type="table" rid="Ch1.T1"/>. Foraminiferal
size-normalised weight (SNW) has variously been used as either a tracer of
the carbonate saturation state of bottom waters <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx18" id="paren.9"><named-content content-type="pre">reflecting dissolution
of carbonate shells after death, e.g.</named-content></xref>, or
as a proxy for the surface ocean carbonate system <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx16 bib1.bibx56 bib1.bibx51" id="paren.10"><named-content content-type="pre">reflecting the
environmental conditions experienced by foraminifera over the course of their lifetime,
e.g.</named-content></xref>. In
the first case, studies implicitly assume that the environmental controls on
shell weight during life have a relatively minor effect on SNW, or can be
accounted for by other means <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx5" id="paren.11"><named-content content-type="pre">as discussed by</named-content></xref>. In the second, conversely, studies may assume a
relatively minor influence of post-depositional dissolution after death. This
issue aside, although culture and field studies support a surface carbonate
system control on foraminiferal calcification
<xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx5 bib1.bibx67 bib1.bibx49 bib1.bibx51" id="paren.12"/>,
others have observed secondary environmental controls on SNW such as nutrient
availability or temperature
<xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx86" id="paren.13"><named-content content-type="pre">e.g.</named-content></xref>. Furthermore, other studies
have observed an inverse response of SNW to carbonate system change in some
species <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx33" id="paren.14"/> – that is, a greater test
thickness at lower pH and/or [<inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>].</p>
      <p>It is possible that at least some of the discrepancies described above may
stem from methodological differences, since foraminiferal SNW has been
quantified in a number of different ways <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx1 bib1.bibx51" id="paren.15"><named-content content-type="pre">see</named-content><named-content content-type="post">for further
discussion</named-content></xref>. Many
early studies used sieve-based weight measurements, where SNW is calculated
as the measured mass of pooled individuals within a set sieve-size fraction
divided by the number of individual tests
<xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx18" id="paren.16"><named-content content-type="pre">e.g.</named-content></xref>. However, shell size can vary
within a studied sieve range <xref ref-type="bibr" rid="bib1.bibx11" id="paren.17"/>. Many later studies
circumvented this issue by directly measuring the major axis length
<xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx1 bib1.bibx11" id="paren.18"/> or
cross-sectional area
<xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx51 bib1.bibx52 bib1.bibx58 bib1.bibx85 bib1.bibx86" id="paren.19"/> of each individual within a sampled
population. However, as discussed by <xref ref-type="bibr" rid="bib1.bibx86" id="text.20"/>, an assumption
common to most shell-weight studies is that SNW metrics themselves do not
vary as a function of size – which is unlikely to be true. The predominant
model of foraminiferal biomineralisation posits that every time a new chamber
is added, foraminifera thicken the calcite of their previous chambers
<xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx27 bib1.bibx66" id="paren.21"><named-content content-type="pre">e.g.</named-content></xref>, so that a given chamber will appear
increasingly heavily calcified over the course of an individual
foraminifera's life. It is therefore possible that size may contribute to
variability in calcification responses recorded between and within studies.
Furthermore, whilst SNW is often assumed to reflect changes in the average
thickness of the shell walls, it is theoretically possible that it is also
driven by other factors which could vary as a function of size. Porosity, for
example, has been suggested as having a considerable influence on shell
weight in <italic>O. universa</italic> <xref ref-type="bibr" rid="bib1.bibx9" id="paren.22"/>. A change in porosity in
<italic>G. ruber</italic> through ontogeny could result in a different SNW between
two otherwise identical foraminifera. However, variability in porosity in
<italic>G. ruber</italic> is not as pronounced as in <italic>O. universa</italic>, and
observations indicate that porosity varies to a lesser degree than wall
thickness <xref ref-type="bibr" rid="bib1.bibx23" id="paren.23"/>. Nonetheless, investigations into how
porosity changes with ontogeny in <italic>G. ruber</italic> would be valuable.</p>
      <p>Attempts to reconcile various
experimental and open-ocean SNW
data with each other and with foraminiferal biomineralisation models
<xref ref-type="bibr" rid="bib1.bibx24" id="paren.24"><named-content content-type="post">and references within</named-content></xref> are still broadly lacking.
To address this shortfall, we show here how a simple model of wall thickness
and calcification can be used to provide a theoretical framework for SNW
metrics. We then present new observations from core-top measurements and
culture experiments with the
shallow-dwelling symbiont-bearing species <italic>Globigerinoides ruber</italic>
<xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx29 bib1.bibx30" id="paren.25"/>, in light of this new
model framework. We discuss the
implications of our modelling and empirical observations both for explaining
the often conflicting results in previous studies, and for predicting the
response of planktonic foraminifera to future global change.</p>
</sec>
<sec id="Ch1.S2">
  <title>Methods</title>
<sec id="Ch1.S2.SS1">
  <title>Culturing</title>
      <p>Data from <italic>Globigerinoides ruber</italic> (white) used in this study are
collated from numerous experiments across a range of temperature, pH and
major ion seawater chemistries, cultured at the Interuniversity Institute of
Eilat between January 2010 and November 2013. These cultures include both
sensu stricto and sensu lato morphotypes <xref ref-type="bibr" rid="bib1.bibx84" id="paren.26"/>. A detailed
description of culturing methods is provided elsewhere
<xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx29 bib1.bibx30" id="paren.27"/>. Briefly, for all
experiments, foraminifera were towed from the Gulf of Aqaba (Eilat) (depth
<inline-formula><mml:math id="M8" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 20 m, temperature 22–24 <inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, salinity <inline-formula><mml:math id="M10" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 40.4 psu), and
cultured in individual 120 mL airtight flasks within temperature-controlled
water baths. Illumination was provided by a metal halide lamp (420 W) with an intensity of
<inline-formula><mml:math id="M11" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 200 <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>mol photons m<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (13 h
light : 11 h dark), equivalent to irradiance at 15–20 m depth in the
open waters of the northern Gulf of Aqaba <xref ref-type="bibr" rid="bib1.bibx71" id="paren.28"/>. Every
1–2 days, individuals were transferred to a Petri dish, measured using an
optical micrometer under a Zeiss inverted light microscope, and fed a
juvenile brine shrimp. After gametogenesis, foraminifera were rinsed in
deionised water, dried and stored for subsequent analysis.</p>
      <p>Here we consider changes in calcification intensity in foraminifera that were
originally cultured to investigate two different geochemical proxy systems:
boron isotopes and Mg <inline-formula><mml:math id="M15" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca
<xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx29 bib1.bibx30" id="paren.29"/>. The experimental
design varies slightly between these two cases, so we discuss any such
differences where they arise. In all experiments, culture solution pH was
determined using an electrode calibrated against NBS buffers. The same
electrode was also used to measure the pH of a range of prepared seawater
solutions which were subsequently analysed for dissolved inorganic carbon
(DIC) concentrations and total alkalinity (TAlk), allowing us to
cross-calibrate our electrode-derived pH values against calculated pH on the
total scale using CO2sys.m <xref ref-type="bibr" rid="bib1.bibx83" id="paren.30"/>, the constants of
<xref ref-type="bibr" rid="bib1.bibx26" id="text.31"/>, <xref ref-type="bibr" rid="bib1.bibx50" id="text.32"/>, and boron concentrations from
<xref ref-type="bibr" rid="bib1.bibx47" id="text.33"/>. Because pH control for boron isotope experiments was
paramount, in these experiments each individual flask pH was measured every
2–3 days, and flasks that experienced pH drift had culture seawater solution
replaced from a stock solution stored throughout the experiment in airtight
bottles without headspace. Uncertainty on pH is therefore calculated as two
standard errors on the mean of each culture flask pHs during cultures. For
those experiments intended to test Mg incorporation
<xref ref-type="bibr" rid="bib1.bibx29" id="paren.34"/>, pH monitoring during culture was less frequent,
and this is reflected in a more conservative approximation of pH uncertainty
in these cultures. In total, we collate calcification intensity data from 11
separate culture experiments, with temperatures ranging from 22.8 to
27.8 <inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, seawater Mg <inline-formula><mml:math id="M17" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca ratios ranging from 2.17 to
6.25 mol mol<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and pH (total scale) ranging from 7.54 to 8.20. Some
estimates of future anthropogenic ocean acidification suggest a pH drop of
0.5 units by 2100 <xref ref-type="bibr" rid="bib1.bibx21" id="paren.35"/>, and so this wide pH range allows us
to investigate the possible changes in calcification over the next century.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Deriving weights from cultures</title>
      <p>Dried cultured foraminifera were imaged and major and perpendicular axes
measured using Macnification software (Orbicule Inc., v2.0). They were then
weighed individually on microbalances at Royal Holloway University of London (Exps. DE3 &amp; DE4), Yale
University (Exp. MH2), and the University of Bristol (Exp. MH1). Mean
uncertainty assessed by 2 standard deviations of triplicate measurements of
individual foraminifera was <inline-formula><mml:math id="M19" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M20" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>1 <inline-formula><mml:math id="M21" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g. While these
foraminifera were not ashed to remove any remnant organic matter prior to
weighing, previous comparisons of non-ashed sample weights with mass of
CaCO<inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> determined by inductively coupled plasma mass spectrometry showed no
significant difference <xref ref-type="bibr" rid="bib1.bibx40" id="paren.36"/>.</p>
      <p>Since it is unfeasible to take direct shell weight measurements from live
pre-culture foraminifera without harming the organism, we estimate
pre-culture shell mass from test size (major and perpendicular axes measured
via ocular micrometer) at the beginning of culture, using a locally defined
size–weight relationship for <italic>G. ruber</italic>, as in previous studies
<xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx49 bib1.bibx40" id="paren.37"><named-content content-type="pre">e.g.</named-content></xref>. Here we
expand on our previous size–weight calibration dataset, combining a total of
205 measurements from individuals of <italic>G. ruber</italic> (mixed morphotypes,
ranging in size from 141 to 517 <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) towed from the Gulf of Aqaba
(Eilat). The equation of this line (<inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.61</mml:mn></mml:mrow></mml:math></inline-formula>) is
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M25" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9.1}{9.1}\selectfont$\displaystyle}?><mml:mtext mathvariant="normal">shell mass</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mtext>in</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">µ</mml:mi><mml:mtext>g</mml:mtext><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">217</mml:mn><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:msup><mml:mtext>product
of axes, in mm</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">1.43</mml:mn></mml:msup><mml:mo>.</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula></p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Defining a calcification metric for cultured foraminifera</title>
      <p>Existing metrics for calcification (as discussed  in Sect. <xref ref-type="sec" rid="Ch1.S1"/>),
cannot be applied directly to laboratory cultures of planktonic species, as
many chambers are precipitated prior to collection. Previous studies
therefore used mean test weight of cultured foraminifera from a given size
range <xref ref-type="bibr" rid="bib1.bibx16" id="paren.38"><named-content content-type="pre">e.g.</named-content></xref>, or made corrections for pre-culture mass
and time spent in culture <xref ref-type="bibr" rid="bib1.bibx49" id="paren.39"/> to describe how
calcification responded to culture conditions. Here, we have  developed a new
metric, calcification intensity (CI; Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>), that accounts for
both the size/mass of foraminifera upon collection, as well as the (often
differential) amount of mass added between culture experiments:
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M26" display="block"><mml:mrow><mml:mi mathvariant="normal">CI</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">mass</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">area</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>mass is the difference in mass between the start and end of the
culture (expressed in <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g) and <inline-formula><mml:math id="M29" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>area is the difference in
product of the major and minor axes (in mm<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) between the start and end of
the culture. We quantify calcification in cultured foraminifera in this
simple way because it allows for more complete consideration of mass grown
outside of culture, and relies only on pre- and post-culture dimensions and
mass that are routinely measured. We note that for our experiments,
pre-culture mass was estimated from a relationship of size to mass
(Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>) constructed from foraminifera towed from in the
Gulf of Aqaba (Eilat) at the same time as our culture experiments. pH
measured at the time of sampling these tows was 8.10 <inline-formula><mml:math id="M31" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.05 (2 SE),
approximately at the middle of our range of experimental pH. Thus while the
size–mass calibration presented here is suitable for our investigations, we
suggest that future culture studies considering CI should characterise this
relationship in the populations from which their cultured individuals were
sampled. We note also that since this metric uses cross-sectional area as a
measure of size, direct comparison of CI values across different
foraminiferal species is not advisable without considering the effect of
species-specific chamber morphologies (i.e. flattened vs. spheroidal
chambers).</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>Ontogenetic modelling of calcification intensity</title>
      <p>Planktonic foraminifera are single-celled eukaryotes with calcium carbonate
tests that show distinct morphological changes throughout ontogeny
<xref ref-type="bibr" rid="bib1.bibx70 bib1.bibx20" id="paren.40"/>. Planktonic foraminifera grow by
sequentially adding calcium carbonate chambers along a primary coiling axis,
and it is thought that they lay down an extra layer of calcite (“secondary
calcite”) over existing chambers when a new chamber is formed
<xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx8 bib1.bibx39" id="paren.41"/>. Over ontogeny coiling behaviour
often changes, as do the relative size, shape, abundance of perforations
(i.e. “porosity”) and wall thickness of the calcium carbonate chambers
<xref ref-type="bibr" rid="bib1.bibx70" id="paren.42"><named-content content-type="pre">e.g.</named-content></xref>. Finally, immediately before foraminifera
reproduce and die, many species <xref ref-type="bibr" rid="bib1.bibx22" id="paren.43"><named-content content-type="pre">although not <italic>G. ruber</italic>;</named-content></xref> precipitate a thick final layer of carbonate known as
gametogenic calcite. Other species appear to secondarily thicken their tests
following precipitation of their final chamber and some may form a crust
<xref ref-type="bibr" rid="bib1.bibx75 bib1.bibx74 bib1.bibx31" id="paren.44"><named-content content-type="pre">e.g.</named-content></xref>,
although this has not yet been observed in <italic>G. ruber</italic>. Studies of
calcification in foraminifera must therefore disentangle the effects of
environmental factors from these known ontogenetic phenomena. In open-ocean
studies (e.g. sediment trap, core top), SNW measurements are commonly taken
from within narrow size ranges to minimise the effect of size-dependent
variation in calcification <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx86" id="paren.45"><named-content content-type="pre">as discussed
in</named-content></xref>. However, normalisation for size
effectively assumes that there is no ontogenetic variation in calcification
or that all individuals come from the same ontogenetic stage, which is
unlikely, particularly when comparing results across different studies. In
laboratory cultures, there are additional difficulties in
assessing CI as it is generally not
possible to select a narrow starting size range (given specimen limitation),
and the number of chambers added by each individual over the course of
culture experiments is highly variable. Therefore, to provide a quantitative
framework for exploring the relationship between CI and ontogeny, and to
explore how existing calcification metrics may be biased by the use of large
or variable size fractions, we developed an ontogenetic model of CI using
empirical observations from <italic>G. ruber</italic>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><caption><p>Observational constraints on
<italic>G. ruber</italic> morphology used to construct the model.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="99.584646pt"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="156.490157pt"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="76.822441pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1">Parameter</oasis:entry>  
         <oasis:entry colname="col2">Variable name<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3">Value</oasis:entry>  
         <oasis:entry colname="col4">Definition/notes</oasis:entry>  
         <oasis:entry colname="col5">Source</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">Foraminifer aspect ratio</oasis:entry>  
         <oasis:entry colname="col2">forAspRat</oasis:entry>  
         <oasis:entry colname="col3">1.16</oasis:entry>  
         <oasis:entry colname="col4">Test aspect ratio (major <inline-formula><mml:math id="M34" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> minor axis)</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Foraminifer test growth rate</oasis:entry>  
         <oasis:entry colname="col2">forAxIn</oasis:entry>  
         <oasis:entry colname="col3">1.19</oasis:entry>  
         <oasis:entry colname="col4">Fraction increase in test major axis<?xmltex \hack{\hfill\break}?>per chamber addition</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Number of chambers</oasis:entry>  
         <oasis:entry colname="col2">noCh</oasis:entry>  
         <oasis:entry colname="col3">16</oasis:entry>  
         <oasis:entry colname="col4">To better assess model behaviour 18<?xmltex \hack{\hfill\break}?>chambers were modelled, but only 16 were utilised in calculations and plots</oasis:entry>  
         <oasis:entry colname="col5">
                      <xref ref-type="bibr" rid="bib1.bibx59" id="text.46"/>
                    </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Chamber aspect ratio</oasis:entry>  
         <oasis:entry colname="col2">chAspRat</oasis:entry>  
         <oasis:entry colname="col3">1.66</oasis:entry>  
         <oasis:entry colname="col4">Chamber aspect ratio (major <inline-formula><mml:math id="M35" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> minor axis)</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Chamber growth rate</oasis:entry>  
         <oasis:entry colname="col2">axInOb</oasis:entry>  
         <oasis:entry colname="col3">1.15</oasis:entry>  
         <oasis:entry colname="col4">Fraction increase in chamber major axis per chamber addition</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Chamber overlap with<?xmltex \hack{\hfill\break}?>previous</oasis:entry>  
         <oasis:entry colname="col2">chCut</oasis:entry>  
         <oasis:entry colname="col3">45 %</oasis:entry>  
         <oasis:entry colname="col4">Proportion of spheroid chamber</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Initial chamber minor axis</oasis:entry>  
         <oasis:entry colname="col2">inchAx2</oasis:entry>  
         <oasis:entry colname="col3">5 <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m</oasis:entry>  
         <oasis:entry colname="col4">Proloculus semi axis based on <italic>T. sacculifer</italic></oasis:entry>  
         <oasis:entry colname="col5">
                      <xref ref-type="bibr" rid="bib1.bibx70" id="text.47"/>
                    </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Porosity</oasis:entry>  
         <oasis:entry colname="col2">forPor</oasis:entry>  
         <oasis:entry colname="col3">4.2 %</oasis:entry>  
         <oasis:entry colname="col4">Percentage chamber wall that is pore space</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Maximum primary<?xmltex \hack{\hfill\break}?>wall thickness</oasis:entry>  
         <oasis:entry colname="col2">maxInWall</oasis:entry>  
         <oasis:entry colname="col3"/>  
         <oasis:entry colname="col4">Saturation point of wall thickness<?xmltex \hack{\hfill\break}?>with ontogeny:</oasis:entry>  
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">10.5–19.5 <inline-formula><mml:math id="M37" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m</oasis:entry>  
         <oasis:entry colname="col4">Model 2</oasis:entry>  
         <oasis:entry colname="col5">
                      <xref ref-type="bibr" rid="bib1.bibx23" id="text.48"/>
                    </oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2"/>  
         <oasis:entry colname="col3">18–22 <inline-formula><mml:math id="M38" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m</oasis:entry>  
         <oasis:entry colname="col4">Models 1 and 3</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">Secondary calcite<?xmltex \hack{\hfill\break}?>layer thickness</oasis:entry>  
         <oasis:entry colname="col2">secChAd</oasis:entry>  
         <oasis:entry colname="col3">67 %</oasis:entry>  
         <oasis:entry colname="col4">Secondary calcite added per chamber<?xmltex \hack{\hfill\break}?>addition, calculated as a proportion of<?xmltex \hack{\hfill\break}?>the mass of all previous chambers</oasis:entry>  
         <oasis:entry colname="col5">This study</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p><inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> Variable names are those used to construct the MATLAB code,
available in the Supplement.</p></table-wrap-foot></table-wrap>

<sec id="Ch1.S2.SS4.SSS1">
  <title>Model parameter constraints</title>
      <p>To ground the model in empirical observations, morphological measurements of
39 specimens were taken from a natural <italic>G. ruber</italic> population from a
Woods Hole Oceanographic Institution core-top sample (sample KC78) from the
equatorial Atlantic <xref ref-type="bibr" rid="bib1.bibx76" id="paren.49"><named-content content-type="pre">5.267<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N by 44.133<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W; 3273 m
water depth;</named-content></xref>. Selected specimens range in size from
250 to 600 <inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m (150 to 250 <inline-formula><mml:math id="M42" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m (<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">11</mml:mn></mml:mrow></mml:math></inline-formula>), 250 to 300 <inline-formula><mml:math id="M44" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m
(<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">11</mml:mn></mml:mrow></mml:math></inline-formula>), 300 to 425 <inline-formula><mml:math id="M46" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m (<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula>), and 425 to 600 <inline-formula><mml:math id="M48" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m (<inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>)).
Foraminifera were first mounted and imaged using a light microscope and
ImageJ (<uri>www.imagej.net</uri>), so that major and minor axis measurements
could be taken from as many chambers as possible, as well as from the whole
test. Individual chambers were subsequently broken and removed so that
chamber wall cross sections could be imaged and measured. Wall thickness
measurements were made away from sutures and chamber apertures, as wall
thickness often varies in these regions of the test <xref ref-type="bibr" rid="bib1.bibx7" id="paren.50"/>. All
reported values are the mean of three replicate measurements, and are given
in Table S1 in the Supplement.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS2">
  <title>Model description</title>
      <p>Building upon the measurements described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS4.SSS1"/> and
other published data (listed in Table <xref ref-type="table" rid="Ch1.T2"/>), we designed a simple
calcification intensity model in MATLAB that tracks the cumulative calcium
carbonate in an idealised individual of <italic>G. ruber</italic> throughout its life
cycle. For a full description of the model, see Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/> (note the
MATLAB code also accompanies this paper). In short, this model simulates the
addition of CaCO<inline-formula><mml:math id="M50" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> mass with growth, as scaled to numerous morphological
and wall-thickness parameters. Morphological parameters used to determine
carbonate content include chamber size, chamber shape, and chamber overlap.
Wall thickness parameters include the thickness of the initial chamber wall
prior to any subsequent thickening (the “primary wall”), wall porosity, and
the thickness of secondary layers added to preceding chambers. There is no a
priori knowledge of which (if any) morphological parameter(s) we should
expect to vary in response to environmental conditions. To address this, we
allowed each parameter to vary randomly within set tolerances and ran the
model 10<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula> times. With a set of model runs this large, we could identify
which factors were systematically linked to change in CI irrespective of
concomitant random changes in others. This is an important advantage of this
computationally inexpensive model over more complex and sophisticated
foraminiferal growth models <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx73" id="paren.51"><named-content content-type="pre">e.g.</named-content></xref>.
Another critical aspect of our model is that it captures the non-linear
behaviour of calcification with ontogenetic growth. Three variant forms of
the model (each ran 10<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula> times) are presented here, with wall thickness
parameterised either as a function of size (models 1 and 2) or of chamber
number (model 3). All model variants are built upon open-ocean measurements,
and are screened against open-ocean populations to ensure they are
representative (see Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/> for a more detailed
explanation).</p>
      <p>We use the CI models for two primary ends. First, we explore the effect of
ontogeny on CI given size-dependent and chamber-dependent variation in
primary wall thickness. Second, we use the ontogenetic predictions to correct
for variable chamber addition in culture, given the importance of secondary
calcification on shell weight <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx27" id="paren.52"><named-content content-type="pre">e.g.</named-content></xref>. For
instance, a foraminifera possessing eight chambers that is of similar overall
test size to a seven-chambered individual will have layered their previous
chambers with calcite to a greater extent,
leading to higher CI at the same body size. Control for variable chamber
addition in culture was achieved by simulating the change in CI with each
chamber addition (<inline-formula><mml:math id="M53" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>CI) for a foraminifera growing from a set starting
size (a maximum axis of 100 <inline-formula><mml:math id="M54" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) using all feasible shell growth
models.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS5">
  <title>Core-top sampling</title>
      <p>To supplement modelling and culturing, and to examine the extent to which the
physiological controls observed in culture are preserved in fossil
assemblages, we also examined SNW in core-top <italic>G. ruber</italic>. Core-top
sites and locations are given in the Supplement, and span a range of bottom
water calcite saturation state (<inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Ω</mml:mi><mml:mtext>calcite</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) from 0.78 to 4.06.
Pre-industrial surface ocean carbonate system conditions for each site were
estimated using modern alkalinity relationships <xref ref-type="bibr" rid="bib1.bibx46" id="paren.53"><named-content content-type="pre">from</named-content></xref>,
air–sea <inline-formula><mml:math id="M56" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>CO<inline-formula><mml:math id="M57" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> disequilibrium <xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx35" id="paren.54"><named-content content-type="pre">from</named-content></xref> and local hydrography <xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx34" id="paren.55"><named-content content-type="pre">from</named-content></xref> following <xref ref-type="bibr" rid="bib1.bibx40" id="text.56"/>. Deep-ocean carbonate
chemistry and calcite saturation state were calculated from DIC and TAlk
estimates at depth from <xref ref-type="bibr" rid="bib1.bibx36" id="text.57"/>. Carbonate system calculations
were carried out as in Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/> above, with pressure
corrections from <xref ref-type="bibr" rid="bib1.bibx54" id="text.58"/> according to each core site's
bathymetry.</p>
      <p>For size-normalisation of shell weight measurements, we follow the “area
density” (<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) approach of <xref ref-type="bibr" rid="bib1.bibx51" id="text.59"/>, as used
elsewhere <xref ref-type="bibr" rid="bib1.bibx85 bib1.bibx86 bib1.bibx52 bib1.bibx58" id="paren.60"/>. From each core-top sample, individual specimens (<inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>–26) of <italic>G. ruber</italic> sensu stricto and sensu lato
were picked from discrete sieve size fractions, imaged (umbilical side up),
and weighed, and their cross-sectional or silhouette area determined using
Macnification (Orbicule Inc., v2.0). <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was calculated as mass
(in <inline-formula><mml:math id="M61" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g) over silhouette area (in mm<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>). As in
<xref ref-type="bibr" rid="bib1.bibx51" id="text.61"/> and <xref ref-type="bibr" rid="bib1.bibx58" id="text.62"/>, the mean
<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and silhouette area in each core-top sample was then used
in multivariate statistical analysis.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F1" specific-use="star"><caption><p>Model output for the three model scenarios described in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS4.SSS2"/>. <bold>(a)</bold> Measured size–mass relationship for
<italic>G. ruber</italic> based on towed specimens from the Gulf of Eilat that were
not cultured. The residual sum of squares between these data defines which
model runs (individual blue lines) are taken as representative of this
natural population. <bold>(b)</bold> CI data of cultured specimens
(Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>), shown in the context of that predicted from the same
set of models for the scenario where two chambers were precipitated in
culture. All models predict that CI is dependent on body size on collection,
which is also our empirical observation. <bold>(c)</bold> Model CI dependence on
the amount of chambers added in culture. Broadly, the more chambers
precipitated, the higher the resultant measured CI. Because of this finding,
we use the model relationship between CI and the number of chambers added in
culture to normalise the culture CI data
shown in panel <bold>(b)</bold>. Panels <bold>(d–i)</bold> show equivalent results
when the model is set up in two alternative ways (see Sect. 2.4.2 and
Appendix A1).</p></caption>
          <?xmltex \igopts{width=349.968898pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f01.pdf"/>

        </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2" specific-use="star"><caption><p><bold>(a)</bold> Measured CI as a function of the product of major and
minor axes at the start of culture for all experiments. <bold>(b)</bold> CI data
can normalised for the number of chambers added in culture, according to the
median CI increase of 17 <inline-formula><mml:math id="M64" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M65" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g/<inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>mm<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> per chamber
added from Fig. <xref ref-type="fig" rid="Ch1.F1"/>c, f, i. In this case, data were normalised
to two chambers added during culture, which was the mode for our culture
experiments.</p></caption>
          <?xmltex \igopts{width=298.753937pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f02.pdf"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <?xmltex \opttitle{Modelling ontogenetic trends and intrinsic drivers of CI and $\rho _{\mathrm{A}}$}?><title>Modelling ontogenetic trends and intrinsic drivers of CI and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></title>
      <p>Model parameter combinations within the prescribed tolerances of the
size–weight ratios seen in non-cultured populations of <italic>G. ruber</italic>
(white, mixed morphotype) are displayed in Fig. <xref ref-type="fig" rid="Ch1.F1"/>a, d, g.
Using the validated subsets of each model, we calculated CI as it evolved
through the ontogenetic growth of each individual modelled foraminifera
(Fig. <xref ref-type="fig" rid="Ch1.F1"/>b, e, h). All models suggest that CI should increase
rapidly with test size up to size of <inline-formula><mml:math id="M69" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.05 mm<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> (equating to a
major axis of approximately 210 <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m). Beyond this size there is
considerably more scope for inter-individual (i.e. inter-model run)
variability, but most model runs continue to show increasing CI with size
throughout the remainder of their ontogeny.</p>
      <p>From the perspective of foraminiferal cultures, these models predict a strong
dependency of CI on foraminifer size on collection, and also the number of
chambers precipitated in culture. For instance, cultures in which foraminifer
added three chambers on average are expected to have a higher CI than
cultures in which most foraminifera added two chambers. Panels (c), (f) and
(i) of Fig. <xref ref-type="fig" rid="Ch1.F1"/> explore this effect of chamber addition on CI.
For each model, frequency distributions of modelled change in CI (<inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>CI)
after two and three chamber additions are shown, relative to a baseline
addition of one chamber and a starting size of 100 <inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m maximum axis
diameter. The median increase of calculated CI with each chamber addition is
17 <inline-formula><mml:math id="M74" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g mm<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and was largely insensitive to the base model – a
similar dependency of chamber addition on CI was observed in models 1–3
(Fig. <xref ref-type="fig" rid="Ch1.F1"/>c, f, i). Because the mean number of chambers added per
individual varied between culture experiments, we therefore normalise our
culture CI data for the mean number of chambers precipitated in culture
(detailed in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>).</p>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T3" orientation="landscape"><caption><p>Culture experiment details, raw calcification intensity (CI), and
residual CI calculated following correction for the observed and modelled
relationship between CI and axes product. Note that for experiments beginning
“DE”, carbonate ion concentrations are calculated with carbonate system
constants adjusted for Mg <inline-formula><mml:math id="M76" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula> using the MyAMI model
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.63"/>. For MH2-Exp1, carbonate system calculations were
adjusted for artificially enhanced seawater boron concentrations. DIC
concentrations from experiments beginning “DE” are from measured composite
seawater solutions, and for experiments beginning “MH” are derived from
total alkalinity measured in composite seawater solutions.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="11">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:colspec colnum="11" colname="col11" align="right"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Experiment</oasis:entry>  
         <oasis:entry colname="col2">Temperature</oasis:entry>  
         <oasis:entry colname="col3">Mg <inline-formula><mml:math id="M78" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M79" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4">pH</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math id="M80" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6">DIC</oasis:entry>  
         <oasis:entry colname="col7">[CO<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>]</oasis:entry>  
         <oasis:entry colname="col8">CI <inline-formula><mml:math id="M82" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> SE</oasis:entry>  
         <oasis:entry colname="col9">Initial product</oasis:entry>  
         <oasis:entry colname="col10">Mean chamber</oasis:entry>  
         <oasis:entry colname="col11">Residual CI</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">  
         <oasis:entry colname="col1"/>  
         <oasis:entry colname="col2">(<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>  
         <oasis:entry colname="col3">(mol mol<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col4">(total)</oasis:entry>  
         <oasis:entry colname="col5"/>  
         <oasis:entry colname="col6">(<inline-formula><mml:math id="M85" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>M)</oasis:entry>  
         <oasis:entry colname="col7">(<inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>M)</oasis:entry>  
         <oasis:entry colname="col8">(<inline-formula><mml:math id="M87" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M88" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g/<inline-formula><mml:math id="M89" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>mm<inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col9">of axes (mm<inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>  
         <oasis:entry colname="col10">addition</oasis:entry>  
         <oasis:entry colname="col11">(<inline-formula><mml:math id="M92" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M93" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g/<inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>mm<inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">DE3-2-26</oasis:entry>  
         <oasis:entry colname="col2">26.3</oasis:entry>  
         <oasis:entry colname="col3">2.17</oasis:entry>  
         <oasis:entry colname="col4">8.0</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2194</oasis:entry>  
         <oasis:entry colname="col7">228</oasis:entry>  
         <oasis:entry colname="col8">194 <inline-formula><mml:math id="M96" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 32</oasis:entry>  
         <oasis:entry colname="col9">0.096</oasis:entry>  
         <oasis:entry colname="col10">1.4</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M97" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>48</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE3-3-26</oasis:entry>  
         <oasis:entry colname="col2">26.3</oasis:entry>  
         <oasis:entry colname="col3">3.25</oasis:entry>  
         <oasis:entry colname="col4">8.0</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2067</oasis:entry>  
         <oasis:entry colname="col7">216</oasis:entry>  
         <oasis:entry colname="col8">126 <inline-formula><mml:math id="M98" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 26</oasis:entry>  
         <oasis:entry colname="col9">0.043</oasis:entry>  
         <oasis:entry colname="col10">2.5</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M99" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>11</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE3-4-26</oasis:entry>  
         <oasis:entry colname="col2">26.3</oasis:entry>  
         <oasis:entry colname="col3">4.15</oasis:entry>  
         <oasis:entry colname="col4">8.0</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2057</oasis:entry>  
         <oasis:entry colname="col7">209</oasis:entry>  
         <oasis:entry colname="col8">127 <inline-formula><mml:math id="M100" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 42</oasis:entry>  
         <oasis:entry colname="col9">0.043</oasis:entry>  
         <oasis:entry colname="col10">2.0</oasis:entry>  
         <oasis:entry colname="col11">1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE3-6-26</oasis:entry>  
         <oasis:entry colname="col2">26.3</oasis:entry>  
         <oasis:entry colname="col3">6.25</oasis:entry>  
         <oasis:entry colname="col4">8.0</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2042</oasis:entry>  
         <oasis:entry colname="col7">201</oasis:entry>  
         <oasis:entry colname="col8">202 <inline-formula><mml:math id="M101" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 29</oasis:entry>  
         <oasis:entry colname="col9">0.083</oasis:entry>  
         <oasis:entry colname="col10">1.8</oasis:entry>  
         <oasis:entry colname="col11">14</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE4-3-22.5</oasis:entry>  
         <oasis:entry colname="col2">22.8</oasis:entry>  
         <oasis:entry colname="col3">3.40</oasis:entry>  
         <oasis:entry colname="col4">8.2</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2024</oasis:entry>  
         <oasis:entry colname="col7">281</oasis:entry>  
         <oasis:entry colname="col8">142 <inline-formula><mml:math id="M102" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 30</oasis:entry>  
         <oasis:entry colname="col9">0.048</oasis:entry>  
         <oasis:entry colname="col10">1.2</oasis:entry>  
         <oasis:entry colname="col11">22</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE4-3-25</oasis:entry>  
         <oasis:entry colname="col2">25.3</oasis:entry>  
         <oasis:entry colname="col3">3.40</oasis:entry>  
         <oasis:entry colname="col4">8.2</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">1997</oasis:entry>  
         <oasis:entry colname="col7">300</oasis:entry>  
         <oasis:entry colname="col8">209 <inline-formula><mml:math id="M103" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 28</oasis:entry>  
         <oasis:entry colname="col9">0.034</oasis:entry>  
         <oasis:entry colname="col10">3.8</oasis:entry>  
         <oasis:entry colname="col11">88</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">DE4-3-27.5</oasis:entry>  
         <oasis:entry colname="col2">27.8</oasis:entry>  
         <oasis:entry colname="col3">3.40</oasis:entry>  
         <oasis:entry colname="col4">8.2</oasis:entry>  
         <oasis:entry colname="col5">0.1</oasis:entry>  
         <oasis:entry colname="col6">2072</oasis:entry>  
         <oasis:entry colname="col7">336</oasis:entry>  
         <oasis:entry colname="col8">163 <inline-formula><mml:math id="M104" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 42</oasis:entry>  
         <oasis:entry colname="col9">0.059</oasis:entry>  
         <oasis:entry colname="col10">1.3</oasis:entry>  
         <oasis:entry colname="col11">6</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">MH1-HighpH</oasis:entry>  
         <oasis:entry colname="col2">26.0</oasis:entry>  
         <oasis:entry colname="col3">5.18</oasis:entry>  
         <oasis:entry colname="col4">8.182</oasis:entry>  
         <oasis:entry colname="col5">0.007</oasis:entry>  
         <oasis:entry colname="col6">1959</oasis:entry>  
         <oasis:entry colname="col7">297</oasis:entry>  
         <oasis:entry colname="col8">120 <inline-formula><mml:math id="M105" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 5</oasis:entry>  
         <oasis:entry colname="col9">0.034</oasis:entry>  
         <oasis:entry colname="col10">3.5</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M106" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">MH1-MedpH</oasis:entry>  
         <oasis:entry colname="col2">26.0</oasis:entry>  
         <oasis:entry colname="col3">5.18</oasis:entry>  
         <oasis:entry colname="col4">7.893</oasis:entry>  
         <oasis:entry colname="col5">0.013</oasis:entry>  
         <oasis:entry colname="col6">1955</oasis:entry>  
         <oasis:entry colname="col7">164</oasis:entry>  
         <oasis:entry colname="col8">91 <inline-formula><mml:math id="M107" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 4</oasis:entry>  
         <oasis:entry colname="col9">0.027</oasis:entry>  
         <oasis:entry colname="col10">4.2</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M108" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>13</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">MH1-LowpH</oasis:entry>  
         <oasis:entry colname="col2">26.0</oasis:entry>  
         <oasis:entry colname="col3">5.18</oasis:entry>  
         <oasis:entry colname="col4">7.564</oasis:entry>  
         <oasis:entry colname="col5">0.008</oasis:entry>  
         <oasis:entry colname="col6">1942</oasis:entry>  
         <oasis:entry colname="col7">79</oasis:entry>  
         <oasis:entry colname="col8">72 <inline-formula><mml:math id="M109" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 10</oasis:entry>  
         <oasis:entry colname="col9">0.033</oasis:entry>  
         <oasis:entry colname="col10">3.0</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M110" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>37</oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">MH2-Exp1</oasis:entry>  
         <oasis:entry colname="col2">26.0</oasis:entry>  
         <oasis:entry colname="col3">5.18</oasis:entry>  
         <oasis:entry colname="col4">7.617</oasis:entry>  
         <oasis:entry colname="col5">0.01</oasis:entry>  
         <oasis:entry colname="col6">2064</oasis:entry>  
         <oasis:entry colname="col7">94</oasis:entry>  
         <oasis:entry colname="col8">97 <inline-formula><mml:math id="M111" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 47</oasis:entry>  
         <oasis:entry colname="col9">0.050</oasis:entry>  
         <oasis:entry colname="col10">2.2</oasis:entry>  
         <oasis:entry colname="col11"><inline-formula><mml:math id="M112" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>47</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p>In addition to discerning ontogenetic trends in CI, these models also help to
constrain which morphological parameters exert the most coherent control on
CI. For almost any given model parameter, the full range of CI observed in
culture can be produced given the right combination of other morphological
parameters. For example, CIs of between 120 and 250 <inline-formula><mml:math id="M113" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g mm<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> can
be produced irrespective of the chamber aspect ratio. In other words, whilst
a change in chamber aspect ratio can affect CI, any such change can also be
offset by a compensatory change in other model parameters. The only
exceptions to this in our model are the variation in the coefficients <inline-formula><mml:math id="M115" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and
<inline-formula><mml:math id="M116" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in Eq. (<xref ref-type="disp-formula" rid="App1.Ch1.E2"/>) – the parameters that determine the non-linear
growth function of wall thickness. Specifically, very low CIs in adult-sized
foraminifera were only observed with <inline-formula><mml:math id="M117" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M118" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> at their lowermost and
uppermost limit respectively (Fig. <xref ref-type="fig" rid="App1.Ch1.F2"/>). In contrast to all
other parameters, CI change as forced by the shape of the regression between
wall thickness and chamber size/number cannot be compensated for by other
prescribed ontogenetic parameters.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Culture results</title>
      <p>Consistent with the modelling results
and chamber addition. A logarithmic regression of individuals' CI versus
their size at the beginning of culture experiments (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a)
yields an <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.37. Once normalised according to the mean number of
chambers added during each culture experiment (see Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/> and
Fig. <xref ref-type="fig" rid="Ch1.F1"/>c), the coherence of this relationship with size becomes
stronger, with an <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.59 (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b). We chose
logarithmic regression fits because in most of our models for <italic>G. ruber</italic> CI change through ontogeny approximates to a logarithmic relationship
within the range in test size of our cultured specimens (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>b).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p>Ambient environmental response of chamber-addition corrected
residual CI (change in mass/change in area compared to the logarithmic
regression through all experiments shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>; see text
for justification). <bold>(a)</bold> Mg <inline-formula><mml:math id="M121" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula>,
<bold>(b)</bold> temperature, <bold>(c)</bold> pH. Shaded regions are 1<inline-formula><mml:math id="M123" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> and
2<inline-formula><mml:math id="M124" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> bounds of uncertainty, as calculated via combined wild bootstrap
and Monte Carlo analysis, accounting for error in <inline-formula><mml:math id="M125" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M126" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula> variables,
following <xref ref-type="bibr" rid="bib1.bibx41" id="text.64"/>. Dashed lines indicate non-significant
relationships, solid regression lines are significant to <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>.
Shaded regions of uncertainty are 1 and 2 SD of 1000 Monte Carlo linear
regression models through randomly simulated datasets sampled within the
given 2<inline-formula><mml:math id="M128" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M129" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>- and <inline-formula><mml:math id="M130" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula>-error margins for each sample.
Mg <inline-formula><mml:math id="M131" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M132" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula> analytical uncertainty is <inline-formula><mml:math id="M133" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>3 %
<xref ref-type="bibr" rid="bib1.bibx28" id="paren.65"/>, smaller than symbol size in <bold>(a)</bold>.</p></caption>
          <?xmltex \igopts{width=378.421654pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f03.pdf"/>

        </fig>

      <p>To investigate the effect of culture conditions on CI, the residuals from the
logarithmic regression fit in Fig. <xref ref-type="fig" rid="Ch1.F2"/>b (given in
Table <xref ref-type="table" rid="Ch1.T3"/>) are compared to environmental parameters
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>). No significant variation with
Mg <inline-formula><mml:math id="M134" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M135" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula> was observed (Fig. <xref ref-type="fig" rid="Ch1.F3"/>), consistent
with previous observations that varying seawater [Mg] does not change growth
rates in foraminifera <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx29" id="paren.66"/>. Similarly, no
effect of temperature on CI was observed (Fig. <xref ref-type="fig" rid="Ch1.F3"/>b).
However, a statistically significant
correlation with pH was found (<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.47</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>;
Fig. <xref ref-type="fig" rid="Ch1.F3"/>c). Other studies often parameterise carbonate system
changes in terms of carbonate ion concentration, [CO<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>]
<xref ref-type="bibr" rid="bib1.bibx51" id="paren.67"><named-content content-type="pre">e.g.</named-content></xref>, or [DIC] <inline-formula><mml:math id="M139" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> [H<inline-formula><mml:math id="M140" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>]
<xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx4" id="paren.68"/>. We also tested residual CI against these
parameters, using carbonate speciation constants adjusted for changing
Mg <inline-formula><mml:math id="M141" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M142" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">sw</mml:mi></mml:msub></mml:math></inline-formula> according to <xref ref-type="bibr" rid="bib1.bibx38" id="text.69"/>. There was little
difference in correlation coefficient in the case of [DIC] <inline-formula><mml:math id="M143" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> [H<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>]
(<inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.47</mml:mn></mml:mrow></mml:math></inline-formula> for [DIC] <inline-formula><mml:math id="M146" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> [H<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>] and pH), but in the case of
[CO<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>] correlation was weaker (<inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.40</mml:mn></mml:mrow></mml:math></inline-formula>). We opt to primarily
focus on pH in figures and discussions here as a less abstracted parameter,
but we cannot rule out [DIC] <inline-formula><mml:math id="M150" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> [H<inline-formula><mml:math id="M151" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>] as being the primary driver, as
suggested by <xref ref-type="bibr" rid="bib1.bibx4" id="text.70"/>. Finally, while <xref ref-type="bibr" rid="bib1.bibx80" id="text.71"/>
suggest [DIC] may be the most important carbonate parameter
affecting calcification, we see no
significant correlation between [DIC] and residual CI (<inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.553</mml:mn></mml:mrow></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p>Drivers of <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in core-top <italic>G. ruber</italic> (white).
In <bold>(a)</bold>, the relative importance of environmental (surface and deep
ocean pH) and physiological (size and species) factors in predicting
<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are shown. A multiple linear regression model containing
bottom water pH (i.e. pH at the site of deposition), test size (i.e. mean
silhouette area in the core-top sample), and morphospecies (i.e. <italic>G. ruber</italic> (white) sensu stricto vs. sensu lato) can describe 86 % of the
variance in <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, with all predictors significant to <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>
except surface ocean pH, which is not a significant contributor to the model
but is shown here for illustrative purposes only (see also Table S3). Of
these variables, bottom water pH is the strongest correlate, as determined by
the R package <italic>relaimpo</italic> <xref ref-type="bibr" rid="bib1.bibx37" id="paren.72"/>. Uncertainty bounds on
the relative contribution of each variable are determined via bootstrapping.
Univariate regression lines of <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> vs. bottom-water pH and vs.
mean test size are shown in <bold>(b, c)</bold> respectively. Error
bars on <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are 2SD of variation within
core-tops <bold>(b, c)</bold>. Error bars on mean silhouette area <bold>(c)</bold>
are 2 standard deviations of silhouette area within a core-top sieve size
fraction. In each case, <italic>G. ruber</italic> sensu stricto are plotted in
orange, and sensu lato in red. Generally heavier values of <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
are observed in <italic>G. ruber</italic> sensu lato <bold>(b, c)</bold>, constituting
the third most important control on <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> within our core-top
dataset <bold>(a)</bold>. Multiple linear regression statistics are given in
Table S3. Residual variation in <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> around the relationship
with bottom water pH is significantly correlated with test silhouette area
(<inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.35</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>; see Fig. S5). Note that other deep-ocean carbonate
system parameters (<inline-formula><mml:math id="M165" display="inline"><mml:mi mathvariant="normal">Ω</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>[CO<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>]) were also trialled in
multiple regression models, but the strongest correlation was observed with
pH at each core-top site, and so that variable is preferred here.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f04.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <title>Core-top results</title>
      <p>Core-top results are given in Table S2. Multiple linear regression analysis
demonstrates that deep-ocean carbonate system conditions at the core-top
site, test size, and morphospecies identity were all statistically
significant controls on <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> within the set of core-top samples
measured here. Together, these three factors could explain 86 % of the
variance in <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> seen in our core-top assemblages (for
regression statistics, see Table S3). We used the <italic>relaimpo</italic> R package <xref ref-type="bibr" rid="bib1.bibx37" id="paren.73"/> to determine
relative importance of these factors, and found bottom water pH at the site
of deposition to be the strongest determinant of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (as shown
in Fig. <xref ref-type="fig" rid="Ch1.F4"/> a and b, and Table S3). Shell size (as
parameterised by shell silhouette area; Fig. <xref ref-type="fig" rid="Ch1.F4"/>c), and
species type within the broader <italic>G. ruber</italic> plexus
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>b, c) were found to be secondary, but nevertheless
significant factors. Where both <italic>G. ruber</italic> sensu stricto and sensu
lato (encompassing both <italic>G. elongatus</italic> and <italic>G. pyramidalis</italic>;
<xref ref-type="bibr" rid="bib1.bibx3" id="altparen.74"/>) were measured at the same site, <italic>G. ruber</italic>
sensu stricto displayed significantly lower values of <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
(paired <inline-formula><mml:math id="M172" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>-test; <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>). Despite the observations from our culture
experiments, estimated surface-ocean pH was not found to be a significant
control on <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in the core-top samples, and would be excluded
from the model by stepwise parameter reduction according to its Akaike
information criterion (AIC). We include it here for illustrative purposes
only given the focus of our study (Fig. <xref ref-type="fig" rid="Ch1.F4"/>), since it has
little effect on the overall model fit (<inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.86</mml:mn></mml:mrow></mml:math></inline-formula> in both cases), or the
relative importance of other factors in the regression. We note also that we
tested other deep and surface water carbonate system parameters in lieu of pH
(<inline-formula><mml:math id="M176" display="inline"><mml:mi mathvariant="normal">Ω</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M177" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>[CO<inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>], etc.), but in all cases pH produced stronger model fits.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <title>Towards understanding the differential response of foraminifera to acidification</title>
      <p>While some progress has been made in explaining differential responses of
groups of marine calcifiers to acidification
<xref ref-type="bibr" rid="bib1.bibx65 bib1.bibx64" id="paren.75"><named-content content-type="pre">e.g.</named-content></xref>, highly divergent responses within the
major groups of calcifiers continue to pose a challenge to our understanding.
For example, coccolithophores were more heavily calcified during geological
epochs characterised by higher CO<inline-formula><mml:math id="M179" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and lower pH
<xref ref-type="bibr" rid="bib1.bibx17" id="paren.76"><named-content content-type="pre">e.g.</named-content></xref>, even if this result has not always been
reproduced in culture <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx45" id="paren.77"/>. Additionally,
despite observations of decreasing pH and [CO<inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>] negatively impacting
calcification in most planktonic and reef-dwelling foraminifera
<xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx51 bib1.bibx44" id="paren.78"><named-content content-type="pre">e.g.</named-content></xref> in
agreement with results from our cultures (Fig. <xref ref-type="fig" rid="Ch1.F2"/>), benthic
foraminifera became more heavily calcified or exhibited little response over
the Palaeocene–Eocene Thermal Maximum (PETM) and ETM2 <xref ref-type="bibr" rid="bib1.bibx33" id="paren.79"/>.
Examining this finding in the context of our model allows us to investigate
the morphological responses to pH change that could produce these patterns,
and so begin to form a unifying hypothesis to explain these various
apparently contradictory observations. To do this, we must first consider how
foraminiferal morphology itself might affect calcification.</p>
      <p>Our model predicts that calcification intensity – a metric for how heavily
calcified cultured foraminifera are – is dependent on foraminifera size on
collection as well as the number of chambers precipitated in culture, as we
observe (Figs. <xref ref-type="fig" rid="Ch1.F1"/>, <xref ref-type="fig" rid="Ch1.F2"/>). But beyond this, varying
permutations of model parameters (as laid out in Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>) reveals
that CI is most strongly dependent on covariation of the coefficients that
describe the increase in wall thickness with ontogeny (<inline-formula><mml:math id="M181" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M182" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in
Eq. <xref ref-type="disp-formula" rid="App1.Ch1.E2"/>). It appears that the overall shape of this regression,
rather than either of its constituent coefficients alone, is most important
in controlling CI. Furthermore, the size–wall thickness coefficients drive CI
in models 1 and 3, but varying maximum wall thickness in isolation has no
systematic effect (model 2). These observations lead us to hypothesise that
it is not simply that large adult foraminifera lay down less calcite in their
walls in response to acidification, but rather that the slope of the
regression between wall thickness and chamber diameter is shallower. This
mechanism, if correct, would produce two physiological responses: (1) lower
pH will result in a thinning of shell walls when the foraminifer is larger,
and (2) smaller foraminifera will exhibit ambiguous, or even positive,
responses to acidification. These hypothesised responses are represented in
Fig. <xref ref-type="fig" rid="Ch1.F5"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p>Schematic response of the chamber wall thickness-chamber size slope
with carbonate chemistry, based on our observations that (1) CI is controlled
by pH in culture, and (2) modelled CI responds principally to the slope of
this relationship, where shallower slopes are characterised by lower CI.
These findings potentially reconcile the differential response of small and
large foraminifera to acidification. For example, <italic>G. ruber</italic> in
culture (this study) and the Arabian Sea <xref ref-type="bibr" rid="bib1.bibx23" id="paren.80"/> respond
negatively to reduced pH (blue line). Conversely, if benthic foraminiferal
calcification can be considered analogous to planktonic, the positive
calcification response small benthic species exhibit to acidification over
the PETM and ETM2 <xref ref-type="bibr" rid="bib1.bibx33" id="paren.81"/> could support our hypothesised
size-dependent calcification response. Images of <italic>G. ruber</italic> from
<xref ref-type="bibr" rid="bib1.bibx23" id="text.82"/> reproduced under CC3.0 licence.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f05.pdf"/>

        </fig>

      <p>Although it is perhaps counter-intuitive to envisage such contrasting
calcification responses to acidification with size, such a hypothesis may
have a mechanistic foundation in the physiology of biomineralisation, when
one considers two important observations of calcite precipitation in
foraminifera. Firstly, based on test oxygen isotope ratios, it seems that
foraminifera precipitate calcite from a species-specific combination of
HCO<inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and CO<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx87 bib1.bibx82" id="paren.83"/>. Secondly,
small foraminifera may not have large internal calcium and/or carbon pools
<xref ref-type="bibr" rid="bib1.bibx57" id="paren.84"/>, whereas large foraminifera do
<xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx78 bib1.bibx79" id="paren.85"/>. This is because smaller
foraminifera build chambers that require far less material volumetrically,
and so they can potentially source the ions required for calcification on the
same timescales as chamber precipitation. In this way, lower pH could have
less of an effect on their wall thickness, or even favour more heavily
calcified chambers, if associated with a rise in [DIC]. Increased
availability of carbon for calcification could promote calcification,
decreasing the volume of seawater needing to be cycled to produce a given
amount of calcite for chamber formation. Once planktonic and benthic
foraminifera reach a certain size, however, the large amounts of CaCO<inline-formula><mml:math id="M185" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
required to build a new chamber may necessitate prior storage of carbon
internally <xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx78 bib1.bibx79" id="paren.86"><named-content content-type="pre">as shown by</named-content></xref>.
Importantly, the efficiency of this internal storage mechanism is thought to
be related to the ability of the organisms to raise the pH of vacuolised
seawater <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx25" id="paren.87"/>. Therefore, lower seawater
pH acts against the efficiency of this carbon concentrating mechanism,
meaning that chamber formation is more difficult. Alternatively, it has been
suggested that foraminifera acquire the carbon needed for calcification
through proton pumping into their microenvironment in order to promote
diffusion of CO<inline-formula><mml:math id="M186" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mtext>(aq)</mml:mtext></mml:mrow></mml:msub></mml:math></inline-formula> into the cytoplasm <xref ref-type="bibr" rid="bib1.bibx80" id="paren.88"/>.
This model is also consistent with our findings, as larger foraminifera
generally have a lower surface area <inline-formula><mml:math id="M187" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> volume ratio, and therefore the
efficiency of this mechanism may be reduced in larger individuals. Our data
does not allow us to differentiate between these biomineralisation models
(which may not be mutually exclusive) but provides a framework within either
to understand the response of calcification to the carbonate system.</p>
      <p>Besides our observed response of planktonic foraminiferal wall thickness to
changes in seawater carbonate chemistry (Fig. <xref ref-type="fig" rid="Ch1.F2"/>), there is
other empirical evidence to support our size-dependent model (see
Fig. <xref ref-type="fig" rid="Ch1.F5"/>). Field studies indicate that large
shallow-water species of planktonic foraminifera respond to decreased pH by
producing thinner walls <xref ref-type="bibr" rid="bib1.bibx23" id="paren.89"/>. Among benthic foraminifera,
culture experiments in <italic>Elphidium</italic> also revealed reduced calcification
at low pH <xref ref-type="bibr" rid="bib1.bibx2" id="paren.90"/>. While there are as yet few data from
smaller species of planktonic foraminifera and early ontogenetic stage
individuals of larger planktonic foraminiferal species, there are some lines
of evidence from small benthic foraminifera that could support the inverse
calcification response that we propose. <xref ref-type="bibr" rid="bib1.bibx33" id="text.91"/> found that
small benthic foraminifera became more heavily calcified during the
PETM, when ocean pH was lower
<xref ref-type="bibr" rid="bib1.bibx60" id="paren.92"/>. By contrast, during the high pH “carbonate
overshoot”
in the aftermath of the event <xref ref-type="bibr" rid="bib1.bibx61" id="paren.93"/>, these foraminifera
displayed thinner walls <xref ref-type="bibr" rid="bib1.bibx33" id="paren.94"/>. Diverse small benthic
foraminifera assemblages have also been found living in highly undersaturated
oligohaline conditions <xref ref-type="bibr" rid="bib1.bibx32" id="paren.95"/>. Indeed, while biomineralisation
pathways clearly differ, recent work favours a similarly positive response of
calcification to increased aqueous <inline-formula><mml:math id="M188" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>CO<inline-formula><mml:math id="M189" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> with lower pH in the much
smaller coccolithophores <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx53" id="paren.96"/>.</p>
      <p>Size-dependent calcification could yet provide a common mechanism to unify
the often variable responses observed in foraminifera to date. However, we
note that there may be different ecophysiological factors driving
calcification in benthic and planktonic foraminifera, and that it remains
untested as to what extent calcification mechanisms in juvenile individuals
of large foraminiferal species may be comparable to adult individuals of
smaller species. We suggest therefore that this hypothesis requires further
investigation. At present, there are insufficient measurements of changes in
calcification and morphology through ontogeny to robustly test this model, or
indeed to re-interpret existing SNW data with confidence. Comparative CT
scans of foraminifera, including examination of individuals grown under
different pH conditions, could provide such a test by constraining
ontogenetic variation in calcite <xref ref-type="bibr" rid="bib1.bibx70" id="paren.97"><named-content content-type="pre">as in</named-content></xref>, while
further multi-species culture experiments would no doubt be beneficial.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p>Modelled dependency of area density (<inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) on
foraminiferal diameter <bold>(a)</bold>, for comparison with the wide range of
size fractions used in studies of size-normalised weight <bold>(b)</bold>. Note
that we model area density in <bold>(a)</bold>, and so those studies that also
use this exact metric are shaded separately in blue in <bold>(b)</bold>. Species
numbers are (1) <italic>Globigerina bulloides</italic>, (2) <italic>Truncorotalia truncatulinoides</italic>, (3) <italic>Neogloboquadrina pachyderma</italic>,
(4) <italic>Globoconella inflata</italic>, (5) <italic>Globigerinoides ruber</italic>
(white), (6) <italic>Orbulina universa</italic>, (7) <italic>Trilobatus sacculifer</italic>,
(8) <italic>Globigerinoides ruber</italic> (pink), (9) <italic>Neogloboquadrina dutertrei</italic>, (10) <italic>Pulleniatina obliquiloculata</italic>,
(11) <italic>Globorotalia scitula</italic>, (12) <italic>Globigerinoides elongatus</italic>.
<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> Since <italic>O. universa</italic> is spherical, we stress that test size exerts
a negligible control on <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, in contrast to other species.
<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="italic">‡</mml:mi></mml:msup></mml:math></inline-formula> We note that this study uses cross-sectional area in calculating a
size-normalised weight, but their approach to normalisation to a set size is
different to the <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> method outlined in
<xref ref-type="bibr" rid="bib1.bibx51" id="text.98"/>.</p></caption>
          <?xmltex \igopts{width=298.753937pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <title>Implications for size-normalised weight (SNW) in foraminifera as a proxy</title>
      <p>Published investigations using SNW as an environmental proxy commonly assume
that the SNW metrics themselves are independent of size or ontogeny. Our
modelling approach shows that there is in fact a strong effect of test size
on SNW. Modelled area density <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx52 bib1.bibx58 bib1.bibx85 bib1.bibx86" id="paren.99"><named-content content-type="pre"><inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, a commonly used SNW
metric</named-content></xref> is shown in Fig. <xref ref-type="fig" rid="Ch1.F6"/>a as a
function of test diameter. Virtually all model runs predict a positive
relationship between <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and test size, although the exact
nature of this relationship varies
with model parameterisation. This suggests that at least some of the
variability between and within published studies could derive from the widely
divergent shell sizes and sieve size ranges used (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b).
Our models similarly reveal a strong size dependency in volume-normalised
approaches, such as that used by <xref ref-type="bibr" rid="bib1.bibx33" id="text.100"/> across the PETM. All
model runs predict that the foraminiferal calcite volume <inline-formula><mml:math id="M197" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> total volume
ratio exhibits a strong dependence on test size (Fig. S2 in the Supplement).</p>
      <p>It has been suggested, given that some size–mass (or volume–mass) relationships in
planktonic foraminifera appear approximately linear <xref ref-type="bibr" rid="bib1.bibx86" id="paren.101"/>,
that the use of area- and volume-normalised weight to estimate SNW is not
complicated by spatial or temporal variations in mean body size. In fact, a
linear relationship between mass and area or between mass and volume directly
implies that area density <italic>is</italic> size-dependent, given
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M198" display="block"><mml:mrow><mml:mi mathvariant="normal">mass</mml:mi><mml:mo>=</mml:mo><mml:mi>k</mml:mi><mml:mo>×</mml:mo><mml:msup><mml:mi mathvariant="normal">mm</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M199" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> is a constant equal to the slope. If volume is approximated from
area by raising to the power of <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx86" id="paren.102"/>, then

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M201" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">mass</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>≈</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>k</mml:mi><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>≈</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi>k</mml:mi><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            which predicts a linear dependence of <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> on body size (given
aspect ratio in Table <xref ref-type="table" rid="Ch1.T2"/>), such that
            <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M203" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub><mml:mo>≈</mml:mo><mml:mi>k</mml:mi><mml:mo>×</mml:mo><mml:msqrt><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow><mml:mn mathvariant="normal">1.16</mml:mn></mml:mfrac></mml:mstyle></mml:msqrt><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>≈</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>k</mml:mi><mml:msqrt><mml:mn mathvariant="normal">1.16</mml:mn></mml:msqrt></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          For <italic>G. ruber</italic>, the slope of this relationship between size and
<inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> approximates to <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.6</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. This means that a
100 <inline-formula><mml:math id="M206" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m increase in test major axis would lead to an
<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> increase of <inline-formula><mml:math id="M208" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 38 <inline-formula><mml:math id="M209" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>g mm<inline-formula><mml:math id="M210" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> due to the
change in body size alone, demonstrating consistency between these simple calculations and our model (Fig. 6a). This
response is of the same magnitude as the area density response to carbonate
system changes reported in other studies <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx58" id="paren.103"><named-content content-type="pre">e.g.</named-content></xref>. Higher overall <inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> observed by
<xref ref-type="bibr" rid="bib1.bibx51" id="text.104"/> for <italic>T. sacculifer</italic> in larger size fractions
may constitute further evidence of a positive size effect on
<inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Similarly, we also find that cross-sectional area is a
significant predictor of <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in our core-top foraminifera
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>).</p>
      <p>We thus provide theoretical, model, and empirical evidence for a strong test
size control on size-normalised weight metrics. This size dependence applies
equally to other SNW metrics, as well as the specific metrics directly
discussed here. That said, size dependence of SNW metrics may be variably
manifest, and variably problematic, in real-world datasets. One implication
of this finding is that datasets from different studies using different
foraminiferal size fractions are not directly comparable. Given the range of
size fractions used in SNW studies (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b), size and
ontogenetic stage may explain some of the discrepancies between findings,
particularly for those studies using a wide sieve size fraction (e.g. several
hundred <inline-formula><mml:math id="M214" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m). The magnitude of increase in SNW (here quantified as
<inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, Fig. <xref ref-type="fig" rid="Ch1.F6"/>a) with size is likely strongest at
smaller body sizes (<inline-formula><mml:math id="M216" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M217" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 350 <inline-formula><mml:math id="M218" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m) – encompassing size
fractions commonly used in both modern calibration and down-core studies
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>b). With these findings in mind, here we make
recommendations of best practice for future studies. Firstly, in death
assemblages, where post-gametogenic foraminifera will likely have added a
similar number of chambers within a full life cycle, the influence of
ontogeny and body size on SNW can be minimised by using the narrowest
possible size fraction of only post-gametogenic individuals, and reporting
mean test size. This may of course be challenging over transient climatic
events associated with a shift in body size, such as the PETM – in that
case, models of calcification with size and ontogeny are needed. Living
assemblages may present other difficulties, as individuals of the same size
may have more or fewer chambers, and hence differing amounts of secondary
calcification. For pre-gametogenic individuals, then, some estimate of
chamber number and overall test size is needed. These additional measurements
are necessary because the SNW metrics are inherently dependent on foraminifer
size, and because changes in the carbonate system may have a differential
effect through ontogeny <xref ref-type="bibr" rid="bib1.bibx1" id="paren.105"><named-content content-type="pre">as previously suggested
by</named-content></xref>.</p>
      <p>Besides the influence of size on SNW, our study highlights other fundamental
caveats about the applicability of SNW as a surface-water proxy. Although our
culture data support a primary carbonate system control on calcification, in
agreement with other studies <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx51 bib1.bibx58" id="paren.106"><named-content content-type="pre">e.g.</named-content></xref>, our core-top samples demonstrate that
this may be overwhelmed by dissolution processes at the site of deposition
(see Fig. <xref ref-type="fig" rid="Ch1.F4"/>). Indeed, while size and morphospecies are
preserved as significant controls on SNW (quantified in this case as
<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; Fig. <xref ref-type="fig" rid="Ch1.F4"/>), any primary signal of surface
carbonate chemistry (for a range in pH of 8.09–8.21) in our core-top sample
set has been entirely lost to dissolution. We therefore urge caution before
attributing open-ocean SNW patterns exclusively to either primary or
secondary processes. In sites where carbonate saturation at the site of
deposition is high, it is probably reasonable to attribute SNW changes to
surface conditions <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx51 bib1.bibx85 bib1.bibx58" id="paren.107"><named-content content-type="pre">as in</named-content><named-content content-type="post">etc.</named-content></xref>. At depths approaching
the lysocline, our data support the earlier uses of SNW as a proxy for the
deep sea carbonate system <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx18" id="paren.108"><named-content content-type="pre">e.g.</named-content></xref>. In
between these end-member scenarios, it may be difficult to untangle competing
effects <xref ref-type="bibr" rid="bib1.bibx16" id="paren.109"/>, and so combining shallow-water and deep-water
cores is advisable, following <xref ref-type="bibr" rid="bib1.bibx6" id="text.110"/>.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <title>Significance for global biogeochemical cycling</title>
      <p>Previous investigations into the controls on foraminiferal shell weight have
often struggled to determine conclusively which environmental controls, if
any, impact foraminiferal calcification, as temperature and [CO<inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>] are
often correlated in hydrographic datasets
<xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx51" id="paren.111"/>. In our cultures where both
temperature and carbonate system parameters were varied, we show that the
carbonate system is the most likely  driver of CI in <italic>G. ruber</italic>
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>). Given the significance of planktonic foraminiferal
tests to the global pelagic CaCO<inline-formula><mml:math id="M221" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> budget <xref ref-type="bibr" rid="bib1.bibx68" id="paren.112"/>, this
finding could therefore have important implications for global carbonate
alkalinity fluxes, and projections of the response of biogeochemical cycling
to anthropogenic ocean acidification. Within the pelagic realm, foraminiferal
calcification reduces TAlk and DIC in a 2 : 1 ratio, releasing CO<inline-formula><mml:math id="M222" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and
thereby lowering surface ocean pH <xref ref-type="bibr" rid="bib1.bibx88" id="paren.113"><named-content content-type="pre">e.g.</named-content></xref>.
Therefore, it is possible that reduced alkalinity uptake in surface waters
may constitute a weak negative feedback on surface ocean acidification.
Scaling this in terms of fluxes, considering changes in other calcifying
groups like coccolithophorids, and accounting for body size and population
size, is beyond the scope of this study. We also note that if the response to
acidification is size-related, there may be some role for other environmental
parameters that influence body size in foraminifera <xref ref-type="bibr" rid="bib1.bibx69 bib1.bibx49" id="paren.114"><named-content content-type="pre">e.g. temperature,
light; </named-content></xref> in determining their response to
anthropogenic ocean acidification. We suggest that modelling of the pelagic
ecosystem should include the physiological costs to calcification in each
group of marine calcifiers. Such considerations may be critical in addressing
current shortfalls in prediction of future biogeochemical changes
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.115"/>.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p>In this study we approach the question of environmental controls on changing
foraminiferal calcification intensity from multiple perspectives,
incorporating observations from culturing and the open ocean with models of
ontogenetic growth. Our models for shell growth suggest that calcification
intensity (i.e. mass increase per unit size increase) changes as a function
of ontogeny and body size in <italic>G. ruber</italic>. This finding provides a
theoretical framework for interpreting results from culture experiments.
After controlling for size and chamber addition, our culture experiments
suggest that neither temperature nor seawater Mg / Ca ratios affect calcification
intensity, but that acidification significantly reduces calcification in
adult-stage foraminifera, supporting previous open-ocean observations
<xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx51" id="paren.116"><named-content content-type="pre">e.g.</named-content></xref>. Based on our
modelling work, we hypothesise that carbonate chemistry may affect different
sized foraminifera differently, with acidification leading to reduced
calcification in bigger foraminifera, but conversely exerting little control
(or even favouring calcification) in small individuals. While further work is
required to test this differential response in larger and smaller
individuals, these model results could help to explain a number of published
observations, and serve to stress the importance of considering size and
ontogeny when studying foraminiferal SNW. Additionally, our core-top results
also highlight the central importance of post mortem dissolution, followed by
body size and species ID, in driving SNW in fossil assemblages. While the
effects of lower ocean pH upon ecosystem-level biogeochemical fluxes are not
yet fully constrained, our findings suggest that production of CaCO<inline-formula><mml:math id="M223" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> by
large planktonic foraminifera in the pelagic realm will likely be reduced by
future anthropogenic ocean acidification.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p>All data related to this study are given in the
Supplementary data files that accompany this paper. This includes core-top
<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> measurements, size-weight measurements in Gulf of Aqaba
tows, and morphological measurements used to ground the model.</p>
  </notes><?xmltex \hack{\clearpage}?><app-group>

<app id="App1.Ch1.S1">
  <title>Model description and discussion</title>
<sec id="App1.Ch1.S1.SS1">
  <title>Model introduction</title>
      <p>A number of excellent models already exist that describe chamber addition and
three-dimensional coiling in foraminifera <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx73 bib1.bibx81" id="paren.117"><named-content content-type="pre">e.g.</named-content></xref>. The models we present here, by contrast, are more
directly focused on addressing questions of foraminiferal size-normalised
shell weight, which can be difficult to address with these more complex types
of models. The annotated source MATLAB code for the model accompanies this
paper. With simplicity in mind, our models track the mass of calcium
carbonate in a particular chamber, as the foraminifera grows. With each
chamber addition, the amount of the total calcium carbonate in the shell is
summed up, before the content of the subsequent chamber is calculated. These
data can then be normalised to overall test size to calculate metrics of
size-normalised weight currently used in palaeoceanographic studies.</p>
      <p>The mass of calcium carbonate in a particular chamber is determined from a
number of prescribed morphological and wall-thickness parameters, which are
derived from empirical observations. Morphological parameters used to
determine a chamber's carbonate content include chamber size relative to
preceding chambers, chamber aspect ratio (i.e. relative round or ovoid), and
relative overlap with previous chambers (effectively hiding part of test).
Wall thickness parameters include the thickness of the initial chamber wall
(i.e. before subsequent thickening – the “primary wall”), wall porosity, and
the thickness of secondary layers added to preceding chambers. Wall thickness
was then scaled with ontogeny either as a function of size or of chamber
number (see below), up to a parameterised maximum primary wall thickness that
was constrained from observations of <italic>G. ruber</italic> (see
Tables <xref ref-type="table" rid="Ch1.T2"/>, S1, and Fig. S1).</p>
      <p>Three distinct models were explored to assess the importance of the choice of
growth model (illustrated schematically in Fig. <xref ref-type="fig" rid="App1.Ch1.F1"/>):
<list list-type="bullet"><list-item>
      <p>Model 1. Ontogenetic changes in calcification were modelled as a function
of body size, with calcification changes controlled by the shape of the
relationship between wall thickness and increasing chamber size.</p></list-item><list-item>
      <p>Model 2. As model 1, except that calcification changes through ontogeny
were mainly driven by varying the maximum primary wall thickness attainable
in later chambers.</p></list-item><list-item>
      <p>Model 3. As model 1, except that ontogenetic changes in wall thickness
were varied as a function of chamber number rather than increasing chamber
size.</p></list-item></list></p>

      <?xmltex \floatpos{t}?><fig id="App1.Ch1.F1" specific-use="star"><caption><p>Scaling of wall thickness with chamber size in the calcification
models, showing the principal difference between the models described in
Sect. <xref ref-type="sec" rid="Ch1.S2.SS4.SSS2"/>. <bold>(a)</bold> Model 1 was designed to test the effect
of varying the slope (parameterised by constants <inline-formula><mml:math id="M225" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M226" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>) of this
relationship. <bold>(b)</bold> Model 2 was designed to test the effect of varying
the maximum primary chamber wall thickness, while keeping <inline-formula><mml:math id="M227" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M228" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> roughly
constant. <bold>(c)</bold> Model 3 parameterises wall thickness as a function of
chamber number instead of body size. The two lines in each model show the
maximum extent by which this regression was allowed to randomly vary, and
therefore delineate model extremes. See Eq. (<xref ref-type="disp-formula" rid="App1.Ch1.E2"/>) for the
definition of this relationship.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f07.pdf"/>

        </fig>

      <p>The differences between models appear subtle, but are important. In models 1
and 2, two post-gametogenic foraminifera of different sizes would have a
different calcite thickness on their final chamber – the larger individual
would have thicker final chamber calcite. By contrast in model 3, two
post-gametogenic foraminifera of different sizes, but the <italic>same total chamber number</italic>, would have the same calcite thickness on their final
chamber. In a scenario where calcification is limited by availability of the
necessary ions rather than energetic cost, model 1 foraminifera might
accommodate unfavourable conditions by maintaining chamber dimensions at the
expense of wall thickness, whereas model 3 foraminifera would maintain
chamber wall thickness at the expense of chamber size and/or shape.
Similarly, the difference between models 1 and 2 is subtle but important.
Both models explore the role that the relationship between foraminifer size
and wall thickness exert on calcification intensity. However, model 1
achieves this mainly through varying the test size at which wall thickness
increases begin to rapidly ramp up, whereas model 2 instead varies the
maximum primary wall thicknesses attained in later chambers (although we
stress that some flexibility was maintained in all parameters). Together,
these models cover a range of possible scenarios for parameterising
ontogenetic and environmental calcification change, and hence provide a solid
framework for understanding the size dependence of inferred CI and the
apparent conflict in previous studies.</p>
</sec>
<sec id="App1.Ch1.S1.SS2">
  <title>Model construction</title>
      <p>Each model was constructed on the basis of sequential addition of spheroid
chambers of a set porosity. Chamber addition is initialised relative to a
specified first chamber (i.e. proloculus) with an average diameter of
10 <inline-formula><mml:math id="M229" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m as based on empirical measurements (Table <xref ref-type="table" rid="Ch1.T2"/>).
Approximate volume of subsequent chambers was
calculated by modelling chambers as spheroids:
            <disp-formula id="App1.Ch1.E1" content-type="numbered"><mml:math id="M230" display="block"><mml:mrow><mml:mi mathvariant="normal">chamber</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">volume</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mo>×</mml:mo><mml:mi mathvariant="normal">semi</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>×</mml:mo><mml:mi mathvariant="normal">semi</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msubsup><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mi mathvariant="normal">semi</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is half the Feret diameter of the spheroid
chamber, and is equal to <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mi mathvariant="normal">semi</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi mathvariant="normal">axis</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> multiplied by the prescribed
chamber aspect ratio (Table <xref ref-type="table" rid="Ch1.T2"/>). Chamber addition continued in
steps until all chambers were added. <italic>G. ruber</italic> typically adds between
15 and 17 chambers <xref ref-type="bibr" rid="bib1.bibx59" id="paren.118"/>, so a terminal chamber count of 16 was
used in all models (Table <xref ref-type="table" rid="Ch1.T2"/>).</p>
      <p>Specific morphometric measurements from which the ontogenetic model was
constructed are given in Table S1 and Fig. S1. These are based on core-top
<italic>G. ruber</italic> from the equatorial Atlantic; see main text Sect. 2.4.1 for
full description. Because we observe no significant trend in any of these
parameters as a function of size (Fig. S1), we use the mean of all
measurements to derive the numbers stated in Table <xref ref-type="table" rid="Ch1.T2"/>. Porosity
measurements were on foraminifera spanning a smaller size range than those
from which the other measurements were taken (250–425 <inline-formula><mml:math id="M233" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m), so we
cannot constrain possible ontogenetic changes in porosity based on this
dataset. Since it has been suggested that porosity could have a significant
effect on SNW <xref ref-type="bibr" rid="bib1.bibx9" id="paren.119"/>, this may be an important avenue for future
research. With this in mind, work is ongoing at Yale to examine the
environmental and ontogenetic controls on foraminiferal porosity.</p>
      <p>The three important features of the model are (1) ontogenetic growth and
parameterisation with random variation, (2) independent variation of test
size and chamber size, and (3) the inclusion and effect of non-linear
ontogenetic changes. Firstly, with each step in ontogeny (i.e. each chamber
addition) the amount of calcium carbonate added is determined as a function
of body size in the preceding step (size models, models 1 and 2) or chamber
number (chamber model, model 3) based on the empirical <italic>G. ruber</italic>
measurements in Tables <xref ref-type="table" rid="Ch1.T2"/> and S1. Specifically, on average,
each new chamber had a major axis length 15 % greater than the preceding
one, a chamber aspect ratio of 1.66 (major <inline-formula><mml:math id="M234" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> minor chamber axis length), an
overlap of 45 % with previous chambers, and a wall porosity of 4.2 %.
With each chamber addition, the total mass of carbonate in the foraminifera
was determined as a function of the size, shape, and porosity of the newly
added chamber (parameters described above), the thickness of calcite wall of
the new chamber (which varied ontogenetically according to the three models
listed above, described in detail below), and the addition of secondary
calcite to the pre-existing test (on average parameterised as 67 % of the
cumulative carbonate content).</p>
      <p>For a given model run, each parameter (i.e. model input) was varied randomly
from the mean parameter listed in Table <xref ref-type="table" rid="Ch1.T2"/> by <inline-formula><mml:math id="M235" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>10 %. This
allowed us to explore parameter space and account for uncertainty in each
biometric input. Whilst individual foraminifera may deviate by more than
10 % from the population mean for any given parameter (see morphological
measurements of <italic>G. ruber</italic> in Table S1 and Fig. S1), we assume that
the population mean (the parameter primarily of interest in calcification
intensity studies) does not vary beyond this range.</p>
      <p>Secondly, to calculate a size-normalised weight as in culture and field
studies, the model requires a measure of total foraminiferal size
(approximated as the sum of the maximum and perpendicular axes). We modelled
this independently as a cumulative function, based on the observed increase
in foraminifer diameter per chamber addition from our measurements. The test
maximum axis (i.e. maximum Feret diameter) was increased by 19 % on
average per chamber addition, with an average test major <inline-formula><mml:math id="M236" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> minor axis
ratio of 1.16. In this way, the foraminiferal test area was not derived
directly from the size of the modelled chambers. Instead, chamber size and
foraminifer size were allowed to vary independently from each other. A
benefit of this approach (besides computational efficiency) is that
foraminiferal morphology varies in the third dimension (height), so by
modelling chamber size and foraminiferal size independently we effectively
are capturing this three-dimensional variation. A limitation of this model
structure is that it can produce morphologically impossible scenarios, for
example foraminifer with a maximum test Feret diameter less than that of
the final chamber. We therefore used natural population measurements of
<italic>G. ruber</italic> to filter model parameter combinations. Specifically,
randomly generated model combinations were discarded if they (a) produced
impossible morphological scenarios, like that described above or (b) produced
area–mass ratios far outside of that observed in natural <italic>G. ruber</italic>
populations in the Gulf of Aqaba (Eilat). In the second case, models falling
outside of root mean square error of 3.12 of the best-fit regression line of the
Gulf of Aqaba populations were discarded. In practical terms, this allows for
up to a factor of two change in the size–mass relationship given in
Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>). This range in successful models constitutes
<inline-formula><mml:math id="M237" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 8 % of the total runs for each model type.</p>
      <p>A third key feature of this model is the inclusion of non-linear ontogenetic
changes in calcification. Many aspects of foraminiferal morphology, including
chamber dimensions and coiling, primary wall thickness, and porosity are
known to change non-linearly over ontogeny.
<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx20" id="text.120"/> noted distinct phases in
foraminiferal morphology correlated with chamber count, a finding supported
by new results from <xref ref-type="bibr" rid="bib1.bibx70" id="text.121"/>. For <italic>G. ruber</italic>, we lacked
the in-depth ontogenetic measurements available for other modern species
<xref ref-type="bibr" rid="bib1.bibx70" id="paren.122"/>, and so we parameterise all non-linear growth
functions as non-linear primary wall thickness functions (described below;
note that, for clarity, we define primary wall thickness as the thickness of a
given chamber wall after precipitation but prior to any secondary
calcification during later chamber additions). We recognise that similar
transitions likely occur in other aspects of morphology in step with changes
in wall thickness, but since wall thickness is likely volumetrically to be by
far the most important (rather than, for example, differential porosity in early
chambers), it seems reasonable to essentially treat primary wall thickness as
a proxy for all such conflated transitions. Our empirical measurements of
<italic>G. ruber</italic> wall thickness (Tables <xref ref-type="table" rid="Ch1.T2"/>, S1) reveal that
there is no relationship between wall thickness and test diameter above a
diameter of <inline-formula><mml:math id="M238" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 250 <inline-formula><mml:math id="M239" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m, with wall thickness remaining roughly
constant at <inline-formula><mml:math id="M240" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 20 <inline-formula><mml:math id="M241" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m. We therefore define three logistic
relationships to describe the co-variation of primary chamber wall thickness
with foraminifer size (shown schematically above in
Fig. <xref ref-type="fig" rid="App1.Ch1.F1"/>), such that

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M242" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">primary</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">chamber</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">thickness</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="App1.Ch1.E2"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mspace linebreak="nobreak" width="1em"/><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">maximum</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="normal">primary</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">thickness</mml:mi></mml:mrow><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>exp⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>a</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:mi>b</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M243" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M244" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> are constants, and <inline-formula><mml:math id="M245" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> is a measure of test size – either
the previous chamber's major axis (models 1 and 2) or chamber number (model
3). The coefficients that define how wall thickness increases over ontogeny
describe the shape of a non-linear relationship. The first coefficient (<inline-formula><mml:math id="M246" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula>)
controls how tightly curved the regression is; models with more negative
values of <inline-formula><mml:math id="M247" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> have thinner chambers during earlier stages of growth, but then
more quickly transition to growing chambers with maximum primary wall
thickness. The second coefficient (<inline-formula><mml:math id="M248" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>) defines the size at which the
foraminifera begin to build thicker chambers, i.e. models with lower values
of <inline-formula><mml:math id="M249" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> reach maximum primary wall thickness at a lower chamber diameter (Fig. S2).</p>
      <p>Maximum primary wall thickness in models 1 and 3 is fixed at 20 <inline-formula><mml:math id="M250" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m
(<inline-formula><mml:math id="M251" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>10 %) on the basis of our core-top measurements of <italic>G. ruber</italic>. In model 2, to test the influence of this parameter, <inline-formula><mml:math id="M252" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M253" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> were
constrained to within 10 %, but maximum test wall was allowed to vary
more widely, between 10 and 20 <inline-formula><mml:math id="M254" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m. In models 1 and 3, the shape of
the logistic regression (as described by <inline-formula><mml:math id="M255" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M256" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in Eq. <xref ref-type="disp-formula" rid="App1.Ch1.E2"/>
above, and illustrated in Fig. A1) was allowed to vary considerably as, to
our knowledge, it is unconstrained by observation. Limits were set only by
the post hoc screening of models that fell outside of the possible range of
natural populations (for example, those in which proloculus wall thickness is
greater than the chamber diameter).</p>
      <p>Because this simple model can be run quickly, we could allow model parameters
to vary randomly (within tolerances) and independently of each other, so as
to interrogate the parameters driving CI. As stated in the main text, any
individual parameter can drive calcification intensity if varied in isolation
and unconstrained by the requirement of an ontogenetic model to approximate
size–mass relationships seen in the open-ocean samples. However, when we
examine only the subset (<inline-formula><mml:math id="M257" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 8 %) of model permutations that produce
realistic size–weight relationships, no significant relationship between CI
and any one parameter listed in Table <xref ref-type="table" rid="Ch1.T2"/> is observed. This is
demonstrated in Fig. S3 by plotting the relationship between modelled CI
against all input parameters (at a body size of <inline-formula><mml:math id="M258" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.1 mm<inline-formula><mml:math id="M259" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, for the
case of two chamber additions). None of these parameters alone drives CI,
which as we discuss in the main text, has the implication that a change in
one may be offset by a change in another (that shifts CI in the opposite
direction) in order to produce foraminifera that conform – within tolerances
– to the observed size–weight relationship for this species. In contrast,
the parameterisation (<inline-formula><mml:math id="M260" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M261" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>) of the relationship between wall thickness
and body size or chamber number unavoidably drive CI irrespective of
simultaneous changes in the other parameters. This is the case whether primary wall
thickness is defined as a function of chamber diameter (model 1) or chamber
number (model 3) (Fig. <xref ref-type="fig" rid="App1.Ch1.F2"/>; see also Sect. 2.4.2). However,
changing the maximum wall thickness that is reached at maturity while keeping
<inline-formula><mml:math id="M262" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M263" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> fixed to within <inline-formula><mml:math id="M264" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>10 % (model 2) has no significant effect
on CI. The dependence of CI on coefficients <inline-formula><mml:math id="M265" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M266" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in isolation is also
far less strong than when both vary in tandem (Fig. <xref ref-type="fig" rid="App1.Ch1.F2"/>,
right-hand panels). This suggests it is the overall shape of the regression
between wall thickness and ontogeny, rather than just one of its constituent
coefficients, which is important in controlling CI – thereby leading us to
our hypothesis of size-dependent calcification responses.</p>

      <?xmltex \floatpos{t}?><fig id="App1.Ch1.F2" specific-use="star"><caption><p>Modelled dependence of CI on morphological parameters within the
three model groups for foraminifera of <inline-formula><mml:math id="M267" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.1 mm<inline-formula><mml:math id="M268" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. No parameter
exerts a systematic control on CI in foraminifera of this size with the
exception of the coefficients <inline-formula><mml:math id="M269" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M270" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> that parameterise the relationship
between body size and primary wall thickness (see Eq. <xref ref-type="disp-formula" rid="App1.Ch1.E2"/>). In
model 1 (top row), these coefficients are varied, but the maximum primary
wall thickness (i.e. before secondary thickening) is kept at
20 <inline-formula><mml:math id="M271" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 <inline-formula><mml:math id="M272" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m. In model 2, conversely, <inline-formula><mml:math id="M273" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M274" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> are
constrained, with maximum chamber thickness allowed to vary. In model 3, wall
thickness is scaled with at chamber addition step, rather than chamber size.
Regardless of base model, varying <inline-formula><mml:math id="M275" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M276" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> will drive CI changes (bottom
and top row, central pairs). Varying maximum wall thickness does not drive
such a relationship (middle row left). When changed together, the <inline-formula><mml:math id="M277" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M278" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>
explain <inline-formula><mml:math id="M279" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 50 % of the variance in CI, as illustrated by the
coloured plots (models 1 and 3, top- and bottom-right panels).</p></caption>
          <?xmltex \igopts{width=321.516142pt}?><graphic xlink:href="https://bg.copernicus.org/articles/14/3287/2017/bg-14-3287-2017-f08.pdf"/>

        </fig>

</sec>
<sec id="App1.Ch1.S1.SS3">
  <title>Model caveats</title>
      <p>An inherent limitation in our models is that parameter
combinations are not utilised if they do not
produce realistic mass–size curves matching the natural mass–axes product
relationship of <italic>G. ruber</italic> in the
Red Sea. However, a substantial relaxation of this tolerance does not
significantly change our results. Moreover, relaxing this tolerance too far
would result in mass–size relationships that can no longer be reasonably
assumed to represent the species <italic>G. ruber</italic>. Although we note that the
tolerances permitted for matching the natural populations are quite large
(they allow for change in the size–mass relationship by a factor of 2), this
natural population itself was sampled from within a narrow range in ambient
pH. As a result, we cannot unequivocally rule out the possibility that some pH-induced change in another input parameter (other than the chamber wall coefficients a and b) could change C. That said, to our
knowledge there is little empirical support for factors such as chamber
aspect ratio or porosity to respond drastically to acidification. In
addition, in the open ocean, trade-offs in allocation of calcification
resources likely operate that make it difficult for one morphological
parameter alone to drive CI. For example, a decrease in the thickness of
secondary calcite layering might be compensated for by building smaller
chambers so as to ensure structural integrity is maintained. Similarly, the
need for cellular defence would preclude an increase in porosity of the
magnitude that would be required to effect large changes in CI. Thus we
suggest that allowing all parameters to vary randomly and then screening
models may be more realistic in reproducing morphological variability in
natural populations.</p>
      <p>Another potential limitation of this model may stem from our parameterisation
of shell thickening as occurring as a series of discrete additions concurrent
with each chamber formation <xref ref-type="bibr" rid="bib1.bibx27" id="paren.123"><named-content content-type="pre">sensu</named-content></xref>. Emerging
findings from species such as <italic>Neogloboquadrina dutertrei</italic>
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.124"><named-content content-type="pre">e.g.</named-content></xref> suggest that at least some foraminifera
may first add chambers until they reach a final test size, and then
subsequently thicken all chambers continually over some days prior to
gametogenesis. Note that this is distinct from concepts such gametogenic
calcite addition or encrustation, and refers specifically to ontogenetic
thickening. It has been argued that the same continual thickening processes
are observed in <italic>Orbulina universa</italic> <xref ref-type="bibr" rid="bib1.bibx74" id="paren.125"/>. However, to
date, there has been no investigation confirming the existence of such a
thickening mechanism in <italic>G. ruber</italic>. Thus, while future work could yet
reveal some secondary thickening process at work, at present we lack the
observational constraints required to incorporate such a mechanism in our
models. In a practical sense, however, we suspect the conceptualisation of
shell thickening chosen is not likely to greatly impact our conclusions, for
two reasons. Firstly, even with observed end-stage thickening in <italic>N. dutertrei</italic>, older chambers are often more heavily thickened than later
chambers <xref ref-type="bibr" rid="bib1.bibx31" id="paren.126"/>, which could in a post hoc sense result
in similarly thickened older chambers as in the models we use here, even if
the ontogenetic pathway to achieving this differs. Secondly, and perhaps more
crucially, our model ontogenies are screened against size–weight
relationships in towed foraminifera, and so by necessity our modelled
ontogenetic trends must approximate true physiology. Nonetheless, should
secondary thickening be observed in <italic>G. ruber</italic> in future, these sorts
of modelling exercises should be revisited.</p><?xmltex \hack{\clearpage}?><supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/bg-14-3287-2017-supplement" xlink:title="zip">https://doi.org/10.5194/bg-14-3287-2017-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
</sec>
</app>
  </app-group><notes notes-type="authorcontribution">

      <p>MJH and DE cultured, weighed, and measured foraminifera,
co-drafted the paper, and processed data. DE devised and constructed
foraminiferal calcification models. MJH directed core-top investigations. PMH
directed the study, co-designed models and co-drafted the paper. MS collected
and collated shell weight data and aided in data processing. JEB collected
foraminifera shell morphology measurements to ground models. GLF funded and
co-directed foraminiferal culturing expeditions and co-supervised core-top
investigations. EA, TBC, JAS and CHSA cultured foraminifera. JD collected
core-top shell weight data. All co-authors contributed to refining and
editing the manuscript.</p>
  </notes><notes notes-type="competinginterests">

      <p>The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p>We are grateful for the hard work of James Rae and Katy Prentice when
culturing experiment “MH1” presented here. Jonathan Erez is thanked for
hosting the culturing work at his lab, and in providing intellectual
guidance. Shai Oron, and the staff and students at the IUI in Eilat are
thanked for their assistance throughout culturing work. Michal Kucera,
Helen Bostock and Bruce Corliss are thanked for the provision of core-top
sample materials. We thank the other members of the Hull lab at Yale for
helpful input and discussion, and Ralf Schiebel, Lennart de Nooijer and one
anonymous reviewer for their constructive comments. Michael J. Henehan
acknowledges financial support from the Yale Peabody Museum.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: Lennart de Nooijer<?xmltex \hack{\newline}?> Reviewed by:
Ralf Schiebel and one anonymous referee</p></ack><ref-list>
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