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<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Cell Dev. Biol.</journal-id>
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<journal-title>Frontiers in Cell and Developmental Biology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Cell Dev. Biol.</abbrev-journal-title>
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<issn pub-type="epub">2296-634X</issn>
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<publisher-name>Frontiers Media S.A.</publisher-name>
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<article-id pub-id-type="publisher-id">1728827</article-id>
<article-id pub-id-type="doi">10.3389/fcell.2026.1728827</article-id>
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<subj-group subj-group-type="heading">
<subject>Original Research</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>A novel culture flask for clinostat-based simulation of extraterrestrial gravities</article-title>
<alt-title alt-title-type="left-running-head">Perra et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fcell.2026.1728827">10.3389/fcell.2026.1728827</ext-link>
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<name>
<surname>Perra</surname>
<given-names>Giovanni</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
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<xref ref-type="aff" rid="aff2">
<sup>2</sup>
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<sup>&#x2020;</sup>
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<name>
<surname>Fais</surname>
<given-names>Giacomo</given-names>
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<sup>1</sup>
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<sup>2</sup>
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<sup>&#x2020;</sup>
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<name>
<surname>Dess&#xec;</surname>
<given-names>Debora</given-names>
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<sup>3</sup>
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<name>
<surname>Concas</surname>
<given-names>Alessandro</given-names>
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<sup>1</sup>
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<name>
<surname>Follesa</surname>
<given-names>Paolo</given-names>
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<sup>2</sup>
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<sup>3</sup>
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<surname>Cao</surname>
<given-names>Giacomo</given-names>
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<surname>Lai</surname>
<given-names>Nicola</given-names>
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<sup>1</sup>
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<aff id="aff1">
<label>1</label>
<institution>Department of Mechanical, Chemical and Materials Engineering, University of Cagliari</institution>, <city>Cagliari</city>, <country country="IT">Italy</country>
</aff>
<aff id="aff2">
<label>2</label>
<institution>Interdepartmental Centre of Environmental Science and Engineering (CINSA), University of Cagliari</institution>, <city>Cagliari</city>, <country country="IT">Italy</country>
</aff>
<aff id="aff3">
<label>3</label>
<institution>Department of Life and Environmental Sciences, University of Cagliari</institution>, <city>Cagliari</city>, <country country="IT">Italy</country>
</aff>
<author-notes>
<corresp id="c001">
<label>&#x2a;</label>Correspondence: Nicola Lai, <email xlink:href="mailto:nicola.lai@unica.it">nicola.lai@unica.it</email>
</corresp>
<fn fn-type="equal" id="fn001">
<label>&#x2020;</label>
<p>These authors have contributed equally to this work</p>
</fn>
</author-notes>
<pub-date publication-format="electronic" date-type="pub" iso-8601-date="2026-02-16">
<day>16</day>
<month>02</month>
<year>2026</year>
</pub-date>
<pub-date publication-format="electronic" date-type="collection">
<year>2026</year>
</pub-date>
<volume>14</volume>
<elocation-id>1728827</elocation-id>
<history>
<date date-type="received">
<day>20</day>
<month>10</month>
<year>2025</year>
</date>
<date date-type="rev-recd">
<day>27</day>
<month>12</month>
<year>2025</year>
</date>
<date date-type="accepted">
<day>22</day>
<month>01</month>
<year>2026</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2026 Perra, Fais, Dess&#xec;, Concas, Follesa, Cao and Lai.</copyright-statement>
<copyright-year>2026</copyright-year>
<copyright-holder>Perra, Fais, Dess&#xec;, Concas, Follesa, Cao and Lai</copyright-holder>
<license>
<ali:license_ref start_date="2026-02-16">https://creativecommons.org/licenses/by/4.0/</ali:license_ref>
<license-p>This is an open-access article distributed under the terms of the <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution License (CC BY)</ext-link>. The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</license-p>
</license>
</permissions>
<abstract>
<sec>
<title>Introduction</title>
<p>Conventional T-flasks (T-25) filled to capacity are frequently employed to minimize shear stress arising from fluid motion during ground-based microgravity simulations using a clinostat or random positioning machine (RPM). However, this approach can introduce confounding factors, such as hypoxia and CO<sub>2</sub> accumulation that affect cell metabolism and function. Therefore, <italic>in vitro</italic> platform simulating microgravity is crucial to distinguish true gravity-dependent responses from culture artifacts. Here, we proposed an innovative engineered culture system (F-25) with a growth area of 25 cm<sup>2</sup> primarily designed for full-filled and clinostat experiments.</p>
</sec>
<sec>
<title>Methods</title>
<p>We assessed the effects of static and rotational (i.e., microgravity) full-filled cultures including conventional T-25 and eighteen customized F-25 with different medium depths, gas exchange areas and membrane types on mitochondrial function of intact C<sub>2</sub>C<sub>12</sub> myoblasts by high resolution respirometry.</p>
</sec>
<sec>
<title>Results</title>
<p>After 24 h, conventional T-25 flasks, full-filled to height of H<sub>0</sub> (2.25 cm) and with a hydrophobic-type gas exchange area of A<sub>0</sub> (0.2 cm<sup>2</sup>) showed intact cellular respiration (ICR) and maximal uncoupled respiration (ET) rates that were more than twice those measured in partially-filled controls, whose values (40 &#x00B1; 3 for ICR and 60 &#x00B1; 4 for ET pmol O<sub>2</sub> s<sup>&#x2212;1</sup> 10<sup>&#x2212;6</sup> cells<sup>&#x2212;1</sup>) remained unchanged between time zero and 24 h. At each medium depth (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub>) increasing the gas exchange area from (6A<sub>0</sub>, 12A<sub>0</sub>, and 18A<sub>0</sub>) led to a progressive decrease in ICR and ET rates reaching control values. The best optimized F-25 flask configuration, combining reduced medium depth (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>) with an enhanced hydrophilic gas exchange membrane of 18A<sub>0</sub>, maintained ICR and ET rates similar to partially-filled controls. The F-25 flask was further tested to assess mitochondrial function under simulated Mars, Moon, and space gravity conditions following 24 h of exposure. Under different extraterrestrial gravity conditions, ICR and ET rates were again twice than those of partially-filled controls but remained unchanged in optimized F-25 flask.</p>
</sec>
<sec>
<title>Discussion</title>
<p>The latter one provides a reproducible and relevant baseline, avoiding confounding factors related to O<sub>2</sub> delivery for clinostat-based simulations. The F-25 flask setup, which allows controlled oxygenation and minimized hydrostatic artifacts, offers a versatile platform not only for space biology, but also for hypoxia studies, 3D culture systems, and tissue engineering applications requiring a defined O<sub>2</sub> microenvironment.</p>
</sec>
</abstract>
<abstract abstract-type="graphical">
<title>Graphical Abstract</title>
<p>
<fig>
<graphic xlink:href="FCELL_fcell-2026-1728827_wc_abs.tif" position="anchor">
<alt-text content-type="machine-generated">Scientific infographic compares a conventional T-25 flask and a customized F-25 flask for cell culture under clinostat-based simulated gravities, highlighting improvements in oxygenation, reduced hypoxia, and experimental controls for Earth, Mars, Moon, and microgravity levels, supported by respiration and artifact data charts.</alt-text>
</graphic>
</fig>
</p>
</abstract>
<kwd-group>
<kwd>bioengineered culture flasks</kwd>
<kwd>clinostat high-resolution respirometry</kwd>
<kwd>mitochondrial respiration</kwd>
<kwd>random positioning machine (RPM)</kwd>
<kwd>rotational culture systems</kwd>
<kwd>simulated microgravity</kwd>
<kwd>space exploration biotechnology</kwd>
</kwd-group>
<funding-group>
<funding-statement>The author(s) declared that financial support was received for this work and/or its publication. GP performed his activity in the framework of the PhD in &#x201c;Innovation Sciences and Technologies&#x201d; at the University of Cagliari, Italy. This work has been developed within the framework of the project eINS-Ecosystem of Innovation for Next Generation Sardinia (cod. ECS 00000038) funded by the Italian Ministry for Research and Education (MUR) under the National Recovery and Resilience Plan (PNRR) - Mission 4, Component 2, &#x201c;From research to business&#x201d; INVESTMENT 1.5, &#x201c;Creation and strengthening of Ecosystems of innovation&#x201d; and construction of &#x201c;Territorial R&#x26;D Leaders&#x201d;.</funding-statement>
</funding-group>
<counts>
<fig-count count="9"/>
<table-count count="0"/>
<equation-count count="1"/>
<ref-count count="82"/>
<page-count count="17"/>
</counts>
<custom-meta-group>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Cellular Biochemistry</meta-value>
</custom-meta>
</custom-meta-group>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<label>1</label>
<title>Introduction</title>
<p>As humanity advances toward sustained exploration beyond Low Earth Orbit (LEO), developing systems capable of supporting long-duration missions has become a strategic priority. The main hazards of human spaceflight identified by NASA for long-duration missions: Radiation, Isolation/Confinement, Distance from Earth, Gravity, and Hostile Environment (RIDGE), provide a unifying framework to classify and prioritize research efforts aimed at mitigating spaceflight risks with altered gravity remaining one of the most pervasive and least understood factors (<xref ref-type="bibr" rid="B2">Afshinnekoo et al., 2020</xref>; <xref ref-type="bibr" rid="B48">Mcphee and Charles, 2009</xref>). Ensuring astronaut health, maintaining reliable life support, and developing biotechnological applications in extraterrestrial environments are critical priorities with adaptation to reduce gravity a fundamental Frontier of research (<xref ref-type="bibr" rid="B20">Demontis et al., 2017</xref>). Microgravity profoundly affects diverse processes, including musculoskeletal integrity, immune response, and cellular metabolism (<xref ref-type="bibr" rid="B17">Chakraborty et al., 2018</xref>; <xref ref-type="bibr" rid="B19">da Silveira et al., 2020</xref>; <xref ref-type="bibr" rid="B27">Feger et al., 2016</xref>; <xref ref-type="bibr" rid="B32">Garrett-Bakelman et al., 2019</xref>).</p>
<p>To study the biological effects of reduced gravity, researchers can employ orbital and suborbital platforms as the gold standard for achieving microgravity, and terrestrial analogues to simulate it (<xref ref-type="bibr" rid="B28">Ferranti et al., 2021</xref>). While experiments on the International Space Station (ISS) provide authentic conditions, their high cost, limited access, and logistical complexity restrict experimental throughput. Ground-based simulators of microgravity such as 2D and 3D clinostats and Random Positioning Machines (RPMs) offer practical alternatives, continuously re-orienting biological samples to average out the gravity vector at a certain level (<xref ref-type="bibr" rid="B36">Herranz et al., 2013</xref>).</p>
<p>The growing role of simulated microgravity in both basic biology and space life support research is highlighted by an almost two-fold increase in publications over the past decade (<xref ref-type="bibr" rid="B63">Ruby et al., 2022</xref>). Yet, despite this progress, several studies continue to rely on conventional clinostat protocols that introduce well-known artifacts, including uncontrolled fluid dynamics, gas exchange inefficiency, and mechanical stress (<xref ref-type="bibr" rid="B79">Wuest et al., 2015</xref>; <xref ref-type="bibr" rid="B80">2017</xref>). Their persistence largely reflects the lack of standardized protocols and cultureware designed to minimize the effect of the confounding factors, highlighting the need for improved experimental systems. Conventional tissue flasks are typically used in a partially-filled configuration, however, when these flasks are employed in rotating culture systems to investigate the effects of microgravity, they are completely filled with medium to eliminate air bubbles and minimize fluid motion during rotation (<xref ref-type="bibr" rid="B11">Braveboy-Wagner and Lelkes, 2022</xref>; <xref ref-type="bibr" rid="B13">Calcagno et al., 2023</xref>; <xref ref-type="bibr" rid="B21">Dietrichs et al., 2022</xref>; <xref ref-type="bibr" rid="B22">Dittrich et al., 2018</xref>; <xref ref-type="bibr" rid="B47">Mann et al., 2019</xref>; <xref ref-type="bibr" rid="B49">Melnik et al., 2023</xref>; <xref ref-type="bibr" rid="B64">Sahana et al., 2023</xref>; <xref ref-type="bibr" rid="B71">Tolle et al., 2025</xref>; <xref ref-type="bibr" rid="B81">Yuzawa et al., 2022</xref>). This full-filled configuration, widely regarded as the &#x201c;gold standard&#x201d;, while effective at reducing shear and bubble formation introduces secondary challenges such as reduced oxygen delivery and the development of hydrostatic pressure gradient to the cells and medium acidification (<xref ref-type="bibr" rid="B3">Al-Ani et al., 2018</xref>; <xref ref-type="bibr" rid="B29">Fleischaker and Sinskey, 1981</xref>; <xref ref-type="bibr" rid="B73">Tse et al., 2021</xref>; <xref ref-type="bibr" rid="B80">Wuest et al., 2017</xref>).</p>
<p>Cell culture is considered to have oxygen (O<sub>2</sub>) concentration within normoxic ranges however, the nominal values reported for the incubator atmosphere often do not reflect the actual microenvironment to which cells are exposed (i.e., pericellular oxygen level). O<sub>2</sub> transfer in culture systems is governed by diffusion across the gas-liquid interface and subsequent transport through the culture medium affected by media depth. Increased medium depth imposes a longer diffusion path length and can create gradients that reduce pericellular O<sub>2</sub> availability (<xref ref-type="bibr" rid="B59">Place et al., 2017</xref>), despite normoxic incubator conditions. Consequently, cells can experience a substantially hypoxic milieu relative to the bulk medium O<sub>2</sub> content affecting cellular metabolism, signaling, and experimental reproducibility (<xref ref-type="bibr" rid="B70">Tan et al., 2024</xref>). Under such culture conditions, in addition to O<sub>2</sub> depletion, CO<sub>2</sub> can rapidly accumulate, particularly in metabolically active or dense cell populations, creating a microenvironment prone to acidification. Also, in 3D or high density cultures, increased medium depth exacerbates O<sub>2</sub> gradients toward the cell layer, impairing viability, an issue that gas-permeable systems effectively mitigate (<xref ref-type="bibr" rid="B73">Tse et al., 2021</xref>). The absence of standardized gas exchange systems and inconsistent reporting of medium volume or oxygenation strategies further undermines reproducibility, confounding the distinction between true gravity-driven responses and culture-induced artifacts.</p>
<p>To address these limitations, we developed a customized full-filled culture system for clinostat-based research, currently under patent application (Italian Application No. 102025000020278, filed on 1 August 2025). This system allows direct comparison of static and rotational full-filled cultures under identical fluidic constraints. By standardizing medium depth, gas exchange surface, and membrane type, it ensures relevant oxygenation while minimizing hydrostatic and hydrodynamic stresses, providing a reliable platform for high fidelity microgravity simulation.</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<label>2</label>
<title>Materials and methods</title>
<p>To develop the customized full-filled culture system for clinostat-based settings, C2C12 myoblasts, a widely adopted model in space biology due to their relevance to microgravity-induced musculoskeletal atrophy (<xref ref-type="bibr" rid="B5">Aventaggiato et al., 2023</xref>; <xref ref-type="bibr" rid="B6">Baek et al., 2019</xref>; <xref ref-type="bibr" rid="B12">Byerly et al., 2006</xref>; <xref ref-type="bibr" rid="B14">Calzia et al., 2020</xref>; <xref ref-type="bibr" rid="B15">Cazzaniga et al., 2020</xref>; <xref ref-type="bibr" rid="B72">Torgan et al., 2000</xref>; <xref ref-type="bibr" rid="B81">Yuzawa et al., 2022</xref>), were used. Cells were cultured under static or dynamic (rotating motion) full-filled conditions and their metabolic function was assessed by high resolution respirometry (<xref ref-type="fig" rid="F1">Figure 1</xref>), a gold standard technique for evaluating oxidative phosphorylation (OXPHOS) (<xref ref-type="bibr" rid="B43">Lai et al., 2017</xref>; <xref ref-type="bibr" rid="B44">2019</xref>; <xref ref-type="bibr" rid="B57">Pesta and Gnaiger, 2012</xref>). The assessment of mitochondrial function that was chosen as mitochondrial activity represents one of the earliest and most sensitive indicators of cellular stress (<xref ref-type="bibr" rid="B10">Brand and Nicholls, 2011</xref>; <xref ref-type="bibr" rid="B54">Nunnari and Suomalainen, 2012</xref>; <xref ref-type="bibr" rid="B82">Zorov et al., 2014</xref>). Perturbations in mitochondrial respiration, membrane potential, or reactive oxygen species (ROS) generation often preceded overt phenotypic changes, thereby providing an early and integrative measure of cellular homeostasis under altered culture conditions (<xref ref-type="bibr" rid="B18">Chen et al., 2025</xref>; <xref ref-type="bibr" rid="B53">Nguyen et al., 2021</xref>; <xref ref-type="bibr" rid="B66">Shi et al., 2025</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Experimental workflow for full-filled culture flask optimization and clinorotation. Cell culture: C2C12 myoblasts maintained at 37&#xa0;&#xb0;C and 5% CO<sub>2</sub> in conventional T-25 or customized F-25 flasks. High resolution respirometry: 2&#xa0;mL chambers (37&#xa0;&#xb0;C, 750&#xa0;rpm) of O2k high resolution respirometer (OROBOROS Instruments) with MiR05 medium. Clinorotation: Random Positioning Machine (RPM 2.0, Yuri Gravity) used to simulate altered gravity conditions. Experimental workflow: (1) optimization of F-25 configuration: medium depth (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub>), gas exchange area (6A<sub>0</sub>, 12A<sub>0</sub>, and 18A<sub>0</sub>) and membrane type (hydrophobic PTFE &#x201c;PHB&#x201d; or hydrophilic cellulose acetate &#x201c;PHL&#x201d;) effects on metabolic function and (2) evaluation of simulated extraterrestrial gravity effects on metabolic function: Earth (s-Earth, &#x223c;1<italic>g</italic>), Mars (s-Mars, &#x223c;0.38<italic>g</italic>), Moon (s-Moon, &#x223c;0.17<italic>g</italic>), and microgravity (s-&#x3bc;g, &#x223c;0.001<italic>g</italic>).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g001.tif">
<alt-text content-type="machine-generated">Infographic displaying a cell culture experimental workflow with C2C12 myoblasts, including incubator and flask types, respirometry setup with O2k respirometer, and a clinorotation machine for simulated gravity. Workflow shows flask optimization and metabolic function testing under varied gravity, with steps for cell seeding, flask filling, clinorotation, and respiratory assay. Diagrams detail flask characteristics and simulated gravity conditions: Earth, Mars, Moon, and microgravity.</alt-text>
</graphic>
</fig>
<sec id="s2-1">
<label>2.1</label>
<title>Buffers and reagents</title>
<p>The reagents used for cell culturing and respirometry were all purchased from Sigma-Aldrich (St. Louis, MI, USA). The mitochondrial respiration medium (MiR05) used for respirometry assay was prepared adding together ethylene glycol-bis(2-aminoethylether)-N,N,N&#x2032;,N&#x2032;-tetraacetic acid (EGTA, 0.5&#xa0;mM), magnesium chloride hexahydrate (MgCl<sub>2</sub>&#x2219;6H<sub>2</sub>O, 3&#xa0;mM), lactobionic acid (K-lactobionate, 60&#xa0;mM), taurine (20&#xa0;mM), potassium dihydrogen phosphate (KH<sub>2</sub>PO<sub>4</sub>, 10&#xa0;mM), HEPES (20&#xa0;mM), D-sucrose (110&#xa0;mM), and bovine serum albumin (BSA, 1&#xa0;g/L, essentially fatty acid free) (<xref ref-type="bibr" rid="B33">Gnaiger et al., 2000</xref>). The pH of MiR05 was then adjusted to 7.1 with KOH at 30&#xa0;&#xb0;C.</p>
</sec>
<sec id="s2-2">
<label>2.2</label>
<title>Development of customized flask</title>
<p>A customized culture flask (F-25) was developed (Italian Application No. 102025000020278, filed on August 1, 2025) for clinostat-based experiments requiring full-filled cultures. The designation F-25 indicates a flask with a 25&#xa0;cm<sup>2</sup> growth surface area specifically engineered for full-filled configurations. The F-25 body consisted of a cylindrical enclosure made by combining standard Petri dishes (for H<sub>0</sub> flasks) or covers (for <sup>2</sup>/<sub>3</sub>H<sub>0</sub> and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> flasks), with a wall thickness of 0.05&#x2013;0.1&#xa0;cm and a diameter of 5.7 cm, providing an approximate 25&#xa0;cm<sup>2</sup> growth area equivalent to that of a standard T-25 flask. Petri dish or cover pairs were fitted together to customize the <sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub> flask sizes. Gas exchange was facilitated by inserting gas-permeable filters with a membrane area of 1.13&#xa0;cm<sup>2</sup> and a pore size of 0.22&#xa0;&#xb5;m into one to three manually drilled symmetrical lateral holes (0.4&#xa0;cm diameter). To prevent medium leaks, the pairs were assembled using lab-grade tape and parafilm. The surface material (virgin polystyrene) and treatment were matched to those of standard T-25 flasks, ensuring equivalent cell adhesion properties. <xref ref-type="fig" rid="F2">Figure 2</xref> illustrates the comparison between the conventional T-25 and the customized F-25 flasks characteristics. The F-25 was customized with different configurations to evaluate the effect of medium depth, gas exchange areas and membrane types (<xref ref-type="fig" rid="F2">Figure 2</xref>): hydrophobic polytetrafluoroethylene (PHB) and hydrophilic cellulose acetate (PHL).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Image and schematic representation of the conventional (T-25, panel <bold>(A)</bold> and customized (F-25, panel <bold>(B)</bold> culture systems illustrating their respective geometric characteristics. <bold>(A)</bold> T-25 is a polystyrene-made parallelepiped enclosure with adhesion surface of 25&#xa0;cm<sup>2</sup>, medium depth of 2.25&#xa0;cm (H<sub>0</sub>), and PTFE-made hydrophobic gas exchange membrane of 0.2&#xa0;cm<sup>2</sup> total area (A<sub>0</sub>). In this culture system, the partially filled condition (<sup>1</sup>/<sub>5</sub>H<sub>0</sub>) was used as control, and the full-filled condition (H<sub>0</sub>) was tested. <bold>(B)</bold> The F-25 is a cylindrical enclosure made of polystyrene with adhesion surface of &#x223c;25&#xa0;cm<sup>2</sup> developed in different configurations varying in medium depth (0.75, 1.75, and 2.25&#xa0;cm corresponding to <sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub>, respectively), and equipped with either hydrophobic (PHB) or hydrophilic (PHL) gas exchange membrane with variable area (1.2, 2.4, and 3.6&#xa0;cm<sup>2</sup> corresponding to 6, 12 and 18A<sub>0</sub>, respectively).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g002.tif">
<alt-text content-type="machine-generated">Comparison of two flask types for cell culture: panel A shows a conventional T-25 flask with a side label highlighting its features, including a 25 square centimeter adhesion surface, height of 2.25 centimeters, and a small hydrophobic PTFE gas exchange membrane; panel B displays a customized F-25 flask with side ports for larger gas exchange areas, different membrane materials, and variable medium depths, with specifications provided below each panel.</alt-text>
</graphic>
</fig>
<p>For each height flask, the gas exchange surface area of the F-25 flask was varied between 1.2 and 3.6&#xa0;cm<sup>2</sup>. This corresponds to approximately 6- to 18-fold larger area compared to a conventional T-25 flask (A<sub>0</sub>, 0.2&#xa0;cm<sup>2</sup>). The gas exchange area was increased by symmetrically drilling lateral holes (0.4&#xa0;cm diameter), each fitted with a gas-permeable filter (membrane area: 1.13 cm<sup>2</sup>; pore size: 0.22&#xa0;&#xb5;m). Three such holes provided a total exchange area equivalent to 3.6&#xa0;cm<sup>2</sup>. Prior to use, all flasks were sterilized with 70% ethanol and UV light. Each configuration was tested with gas exchange areas of 6-, 12-, and 18-fold the T-25 reference (A<sub>0</sub>), using either hydrophobic (PHB) or hydrophilic (PHL) membranes. The chosen ranges allowed systematic assessment of oxygenation efficiency and medium depth. The varying volume-to-area ratios (0.75, 1.50, and 2.25&#xa0;cm) across different medium heights allowed for the examination of how changes in the volume-to-area ratio influence cell behavior, independent of differences in the adhesion surface area. In total, eighteen F-25 variants were tested (3 heights, 3 gas exchange areas, 2 membrane types). A standard T-25 flask (CTRL T-25 <sup>1</sup>/<sub>5</sub>H<sub>0</sub> A<sub>0,PHB</sub>) under partially-filled static conditions served as the control condition. All flasks were subsequently seeded with C2C12 myoblasts, as described in the following section.</p>
</sec>
<sec id="s2-3">
<label>2.3</label>
<title>Cell culture</title>
<p>C2C12 myoblasts (ECACC 91031101) were cultured in high glucose Dulbecco&#x2019;s Modified Eagle Medium (DMEM with L-glutamine and sodium carbonate, without sodium pyruvate), supplemented with 10% fetal bovine serum (FBS) and 1% penicillin-streptomycin (P/S). Cultures were maintained at 37&#xa0;&#xb0;C in a humidified incubator with 5% CO<sub>2</sub> and harvested at 70% confluence using 0.25% trypsin-EDTA. Cell viability and number were determined via Trypan Blue exclusion assay using a Neubauer chamber. Cells were then seeded at a density of 20,000 cells&#xa0;cm<sup>-2</sup> into either conventional T-25 flasks or customized F-25 flasks (with variable medium depth, gas exchange area, and membrane type, as described above). After seeding, flasks were incubated under static conditions with minimal medium volume to allow cell attachment. Following overnight incubation, T-25 and F-25 flasks were filled with medium at defined depths: partially-filled (<sup>1</sup>/<sub>5</sub>H<sub>0</sub>) corresponding to the typical cell culture condition, and filled to the flask height (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub>). The flasks were maintained under static conditions for 24&#xa0;h before the respirometry analyses or clinorotation experiments (<xref ref-type="fig" rid="F1">Figures 1</xref>, <xref ref-type="fig" rid="F2">2</xref>).</p>
</sec>
<sec id="s2-4">
<label>2.4</label>
<title>High-resolution respirometry</title>
<p>After 24&#xa0;h of exposure under three distinct culture conditions, including partially-filled static, full-filled static, and full-filled clinorotated conditions, mitochondrial function was evaluated in intact C2C12 myoblast cells using high resolution respirometry (O2k-Oxygraph, OROBOROS Instruments, Innsbruck, Austria). Oxygen (O<sub>2</sub>) consumption was continuously monitored with DatLab 7.1 software (OROBOROS Instruments) and expressed as pmol O<sub>2</sub> s<sup>-1</sup> 10<sup>&#x2212;6</sup> cells<sup>-1</sup> within an O<sub>2</sub> concentration range of 75&#x2013;195&#xa0;&#x3bc;M. Throughout the experiments, the metabolic chamber was maintained at 37&#xa0;&#xb0;C with stirring at 750&#xa0;rpm.</p>
<p>Cell suspensions were adjusted to a density of 0.5&#xb7;10<sup>6</sup> viable cells mL<sup>&#x2212;1</sup> in MiR05 respiration buffer, and 2&#xa0;mL aliquots were introduced into the respirometry chamber. Mitochondrial activity was then characterized using a respiratory protocol, designed to measure specific respiratory states. The sequence included measurement of endogenous respiration in intact cells (ICR); complex V-inhibited respiration (O) in the presence of oligomycin (0.05&#x2013;0.2&#xa0;&#x3bc;M); maximum uncoupled respiration (ET), determined by titration of CCCP (0.5&#x2013;3.5&#xa0;&#x3bc;M); complex I-inhibited respiration (R) in the presence of rotenone (1.2&#xa0;&#x3bc;M); complex III-inhibited or non-mitochondrial (Ama or NM) respiration in the presence of antimycin A (0.5&#xa0;&#x3bc;M). The mitochondrial respiration (M) rate contributing to the maximum uncoupled respiration (ET) was calculated by subtracting the non-mitochondrial respiration rate (NM), measured in the presence of antimycin A, from the ET rate.</p>
</sec>
<sec id="s2-5">
<label>2.5</label>
<title>Gravity simulations by clinostat</title>
<p>The mitochondrial function was assessed in C2C12 myoblasts exposed 24&#xa0;h to altered gravity conditions. A 3D clinostat (Random Positioning Machine, RPM 2.0, Yuri Gravity) was used to simulate terrestrial (s-Earth, &#x223c;1<italic>g</italic>), Martian (s-Mars, &#x223c;0.38<italic>g</italic>), Lunar (s-Moon, &#x223c;0.17<italic>g</italic>) and microgravity (s-&#x3bc;g, &#x223c;0.001<italic>g</italic>) conditions based on the principle of gravitational vector averaging. Two independently rotating perpendicular frames continuously modify the orientation of the gravitational vector relative to the sample, effectively minimizing its influence and creating conditions analogous to microgravity (<xref ref-type="bibr" rid="B35">Herranz et al., 2012</xref>; <xref ref-type="bibr" rid="B74">van Loon, 2007</xref>; <xref ref-type="bibr" rid="B79">Wuest et al., 2015</xref>). The system was interfaced with computer-controlled software that allowed precise adjustment of rotation speed and motion patterns according to the desired simulated gravity level. The clinorotation algorithms designed by the manufacturer (Yuri Gravity) are used in the experiments and are detailed in <xref ref-type="sec" rid="s12">Supplementary Table S1</xref>.</p>
<p>After overnight incubation, to limit shear stress artifacts T-25 and F-25 flasks were full filled with a variable volume of medium that ranged from 20 to 70&#xa0;mL depending on the flask geometry (<xref ref-type="bibr" rid="B9">Borst and Van Loon, 2009</xref>; <xref ref-type="bibr" rid="B79">Wuest et al., 2015</xref>). Air bubbles were carefully removed, and cultures were maintained for 24&#xa0;h under either static or clinorotated conditions. At the end of the 24&#xa0;h of exposure, cells from static and clinorotated conditions were harvested for assessment of respiratory capacity using high resolution respirometry. To distinguish between rotation-induced effects caused by the continuous reorientation of the flask on the clinostat and reduced gravity adaptations, a simulated Earth (s-Earth) condition was included as a dynamic control to evaluate potential effects of the fluid dynamic environment inherent to clinorotation.</p>
</sec>
<sec id="s2-6">
<label>2.6</label>
<title>Non-linear regression modeling of respiration rate</title>
<p>A two-dimensional plot of the intact cell respiration (ICR) rate in C2C12 myoblasts as a function of medium depth (H) and gas exchange area (A) was generated by fitting the experimental ICR data with the following two-dimensional polynomial equation:<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi>I</mml:mi>
<mml:mi>C</mml:mi>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>H</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>A</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>I</mml:mi>
<mml:mi>C</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>H</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>A</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>3</mml:mn>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msup>
<mml:mi>H</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>4</mml:mn>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msup>
<mml:mi>A</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>5</mml:mn>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>H</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>A</mml:mi>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>where, <italic>ICR</italic>
<sub>
<italic>0</italic>
</sub>, <italic>a</italic>
<sub>
<italic>1</italic>
</sub>, <italic>a</italic>
<sub>
<italic>2</italic>
</sub>, <italic>a</italic>
<sub>
<italic>3</italic>
</sub>, <italic>a</italic>
<sub>
<italic>4</italic>
</sub>, and <italic>a</italic>
<sub>
<italic>5</italic>
</sub> are the fitting model adjustable parameters. The Levenberg-Marquardt algorithm was employed for the iterative fitting procedure (maximum iterations of 400, tolerance level of 10<sup>&#x2212;9</sup>) using OriginPro software (Version 2024b, OriginLab Corporation, Northampton, MA, USA).</p>
</sec>
<sec id="s2-7">
<label>2.7</label>
<title>Statistical analysis</title>
<p>All experiments were performed independently in quintuplicate (n &#x3d; 5) and result data are presented as mean &#xb1; standard error of the mean (SEM). Statistical analysis was performed with the GraphPad Prism software (version 10.5, Dotmatics, Boston, Massachusetts). One-way ANOVA with Bonferroni&#x2019;s correction for multiple comparisons was used to test statistical significance in differences in respiration state rates between partially-filled (control) and static/dynamic conditions after 24&#xa0;h. Specifically: (i) in the F-25 flask optimization experiments, the single factor was the gas exchange area in full-filled flask configuration; (ii) in the clinostat experiments, the single factor was simulated gravity (levels: s-Earth, s-Mars, s-Moon, and s-&#xb5;g). Two-way ANOVA with Bonferroni&#x2019;s correction for multiple comparisons was used to test statistical significance in respiration state rates between T-25 and F-25 configurations. The two factors were filling level (partially vs. fully filled) and gas exchange membrane type (hydrophobic vs. hydrophilic). The significance levels based on the <italic>p</italic>-values are indicated by different marks (&#x2a;<sup>,&#x23;,&#xa7;</sup>): no mark corresponds to a <italic>p</italic> &#x3e; 0.05, &#x2a;<sup>,&#x23;,&#xa7;</sup> to <italic>p</italic> &#x3c; 0.05, &#x2a;&#x2a;<sup>,&#x23;&#x23;,&#xa7;&#xa7;</sup> to <italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>, &#x2a;&#x2a;&#x2a;<sup>,&#x23;&#x23;&#x23;,&#xa7;&#xa7;&#xa7;</sup> to <italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>, and &#x2a;&#x2a;&#x2a;&#x2a;<sup>,&#x23;&#x23;&#x23;&#x23;,&#xa7;&#xa7;&#xa7;&#xa7;</sup> to <italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>.</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<label>3</label>
<title>Results</title>
<p>First aim was to determine how T-25 and different F-25 flask configurations affect cellular metabolism under static conditions. To evaluate whether metabolic function was preserved with the customized F-25 flasks, the oxygen (O<sub>2</sub>) consumption rate was measured in intact C2C12 myoblasts cultured for 24&#xa0;h under static conditions, using different cell culture configurations partially-filled or full-filled with medium (<xref ref-type="fig" rid="F3">Figures 3</xref>&#x2013;<xref ref-type="fig" rid="F6">6</xref>). The second aim was to determine how full-filled flask type (T-25 vs. F-25) and clinorotation (static vs. rotational) affect metabolic function (<xref ref-type="fig" rid="F7">Figures 7</xref>, <xref ref-type="fig" rid="F8">8</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Effect of medium depth and gas exchange area with hydrophobic (PHB) membrane on respiration state rates of intact C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells mL<sup>&#x2212;1</sup>) after 24&#xa0;h culture in full-filled F-25 and T-25 flasks, compared with the control group (partially-filled T-25 flask) designated with white bar. Respiration state rates obtained with T-25 (grey bar) and F-25 (color bar) flasks with a medium depth of H<sub>0</sub> <bold>(A&#x2013;C)</bold>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub> <bold>(D&#x2013;F)</bold> and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> <bold>(G&#x2013;I)</bold> and a gas exchange area from 6 to 18A<sub>0,PHB</sub>; Respiration state rates: intact cell respiration (ICR) in panel <bold>A</bold>, <bold>D</bold>, and <bold>G</bold>; maximum uncoupled respiration (ET) in panel <bold>B</bold>, <bold>E</bold>, and <bold>H</bold>; mitochondrial (M) and non-mitochondrial respiration (NM) in panel <bold>C</bold>, <bold>F</bold>, and <bold>I</bold>. Statistically different from control flask (&#x2a; within the group): &#x2a; (<italic>p</italic> &#x3c; 0.05); &#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); &#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); &#x2a;&#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>); Statistically different from control flask (<sup>&#xa7;</sup>M vs. M): <sup>&#xa7;&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); <sup>&#xa7;&#xa7;&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>); Statistically different from control flask (<sup>&#x23;</sup> NM vs. NM): <sup>&#x23;</sup> (<italic>p</italic> &#x3c; 0.05); <sup>&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); <sup>&#x23;&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); <sup>&#x23;&#x23;&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>). Data of panel <bold>A</bold>, <bold>B</bold>, <bold>D</bold>, <bold>E</bold>, <bold>G</bold>, and <bold>H</bold> are reported as mean &#xb1; SEM of percentage of respiration state rate relative to the corresponding value obtained with control flask (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>) and data of panel <bold>C</bold>, <bold>F</bold>, and <bold>I</bold> are reported as mean &#xb1; SEM of ET &#x3d; M &#x2b; NM respiration rate (<xref ref-type="sec" rid="s12">Supplementary Figure S3</xref>, n &#x3d; 5).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g003.tif">
<alt-text content-type="machine-generated">Graphic displays a comparison between conventional T-25 flasks and customized F-25 flasks with hydrophobic filters, including diagrams of flask configurations. Nine bar graphs below show mitochondrial and non-mitochondrial respiration data (percent and pmol O&#x2082;&#xB7;s&#x207B;&#xB9;&#xB7;10&#x2076; cells&#x207B;&#xB9;) for different flask types and conditions, grouped into panels A-I with red, green, blue, white, and gray color schemes representing various conditions. Statistical significance is indicated by stars, double-s and hash symbols, with a legend clarifying mitochondrial versus non-mitochondrial measurements.</alt-text>
</graphic>
</fig>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Effect of medium depth and gas exchange area with hydrophilic (PHL) membrane on respiration state rates of intact C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells&#xa0;mL<sup>&#x2212;1</sup>) after 24&#xa0;h culture in full-filled F-25 and T-25 flasks, compared with the control group (partially-filled T-25 flask) designated with white bar. Respiration state rates obtained with T-25 (grey bar) and F-25 (color bar) flasks with a medium depth of H<sub>0</sub> <bold>(A&#x2013;C)</bold>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub> <bold>(D&#x2013;F)</bold> and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> <bold>(G&#x2013;I)</bold> and a gas exchange area from 6 to 18A<sub>0,PHL</sub>; Respiration state rates: intact cell respiration (ICR) in panel <bold>A</bold>, <bold>D</bold>, and <bold>G</bold>; maximum uncoupled respiration (ET) in panel <bold>B</bold>, <bold>E</bold>, and <bold>H</bold>; mitochondrial (M) and non-mitochondrial respiration rate (NM) in panel <bold>C</bold>, <bold>F</bold>, and <bold>I</bold>. (&#x2a;) Statistically different from control flask (&#x2a; within the group): &#x2a; (<italic>p</italic> &#x3c; 0.05); &#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); &#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); &#x2a;&#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>); Statistically different from control flask (<sup>&#xa7;</sup>M vs. M): <sup>&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); <sup>&#xa7;&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2013;3</sup>); <sup>&#xa7;&#xa7;&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>); Statistically different from control flask (<sup>&#x23;</sup> NM vs. NM): <sup>&#x23;</sup> (<italic>p</italic> &#x3c; 0.05); <sup>&#x23;&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); <sup>&#x23;&#x23;&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>). Data of panel <bold>A</bold>, <bold>B</bold>, <bold>D</bold>, <bold>E</bold>, <bold>G</bold>, and <bold>H</bold> are reported as mean &#xb1; SEM of percentage of respiration state rate relative to the corresponding value obtained with control flask (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>) and data of panel <bold>C</bold>, <bold>F</bold>, and <bold>I</bold> are reported as mean &#xb1; SEM of ET &#x3d; M &#x2b; NM respiration rate (<xref ref-type="sec" rid="s12">Supplementary Figure S4</xref>, n &#x3d; 5).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g004.tif">
<alt-text content-type="machine-generated">Graphic displays a comparison between conventional T-25 flasks and customized F-25 flasks with hydrophilic filters, including diagrams of flask configurations. Nine bar graphs below show mitochondrial and non-mitochondrial respiration data (percent and pmol O2 s-1 10-6 cells-1) for different flask types and conditions, grouped into panels A-I with white, gray, orange, green, and purple color schemes representing various conditions. Statistical significance is indicated by stars, double-s and hash with a legend clarifying mitochondrial vs. non-mitochondrial contributions.</alt-text>
</graphic>
</fig>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Hydrophobic and hydrophilic gas exchange membrane performance. <bold>(A)</bold> Three-dimensional and <bold>(B)</bold> contour map comparison of the intact cell respiration (ICR) rate of C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells&#xa0;mL<sup>&#x2212;1</sup>) obtained with hydrophobic (PHB) or hydrophilic (PHL) membrane at different medium depths (H in cm) and gas exchange areas (A in cm<sup>2</sup>).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g005.tif">
<alt-text content-type="machine-generated">Three data visualizations compare experimental data and non-linear fitting for hydrophobic (PHB) and hydrophilic (PHL) membranes. Panel A shows a 3D plot of ICR oxygen consumption rate versus medium depth and gas exchange area, with red and blue points and surfaces representing PHB and PHL membranes, respectively. Panel B displays two heat maps, left in shades of red for PHB and right in shades of blue for PHL, illustrating ICR values for various medium depths and gas exchange areas. Legends indicate value ranges and color gradients.</alt-text>
</graphic>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Comparison of intact cell respiration (ICR) rate of C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells&#xa0;mL<sup>&#x2212;1</sup>) obtained with hydrophobic (PHB, red bar) or hydrophilic (PHL, blue bar) membrane at different gas exchange area (A in cm<sup>2</sup>) for a medium depth of cm (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>). Statistically different from control flask: &#x2a; (<italic>p</italic> &#x3c; 0.05); &#x2a;&#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>); Statistical difference between membrane type: <sup>&#x23;</sup> (<italic>p</italic> &#x3c; 0.05); <sup>&#x23;&#x23;&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;4</sup>). Data are reported as mean &#xb1; SEM of intact cell respiration rate (n &#x3d; 5).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g006.tif">
<alt-text content-type="machine-generated">Bar graph comparing oxygen consumption rates of cells cultured in flasks with hydrophobic (PHB, red bars) or hydrophilic (PHL, blue bars) gas exchange areas (6, 12, and 18A0). PHB group shows higher rates at 6 and 18A0 and significant differences denoted by symbols. Error bars represent standard error. Legend identifies color coding for PHB and PHL. Y-axis labeled as oxygen consumption per million cells per second.</alt-text>
</graphic>
</fig>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Effect of 24&#xa0;h simulated gravities on cellular respiration in T-25 flask. <bold>(A)</bold> Intact cell respiration (ICR), <bold>(B)</bold> maximum uncoupled respiration (ET), <bold>(C)</bold> mitochondrial (M) and non-mitochondrial (NM) respiration rates of C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells&#xa0;mL<sup>&#x2212;1</sup>) cultured in conventional T-25 flask under simulated Earth (s-Earth, &#x223c;1<italic>g</italic>), Mars (s-Mars, &#x223c;0.38<italic>g</italic>), Moon (s-Moon, &#x223c;0.17<italic>g</italic>) and Space (s-&#x3bc;g, &#x223c;0.001<italic>g</italic>) gravity conditions generated by clinorotation. Statistically different from control flask (&#x2a;): &#x2a; (<italic>p</italic> &#x3c; 0.05); &#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); &#x2a;&#x2a;&#x2a; (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); Statistically different from control flask (<sup>&#xa7;</sup>M vs. M): <sup>&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>); <sup>&#xa7;&#xa7;&#xa7;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;3</sup>); Statistically different from control flask (<sup>&#x23;</sup> NM vs. NM): <sup>&#x23;</sup> (<italic>p</italic> &#x3c; 0.05); <sup>&#x23;&#x23;</sup> (<italic>p</italic> &#x3c; 10<sup>&#x2212;2</sup>). Data of panel <bold>A</bold> and <bold>B</bold> are reported as mean &#xb1; SEM of percentage of respiration state rate relative to the corresponding value obtained with control flask (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>) and data of panel C are reported as mean &#xb1; SEM of ET &#x3d; M &#x2b; NM respiration rate (<xref ref-type="sec" rid="s12">Supplementary Figure S5</xref>, n &#x3d; 5).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g007.tif">
<alt-text content-type="machine-generated">Bar graph with three panels comparing cell respiration under various flask conditions: Panel A shows intact cell respiration, Panel B shows maximum uncoupled respiration, and Panel C separates mitochondrial and non-mitochondrial respiration. Colored bars represent partially-filled control, full-filled control, simulated Earth, Mars, Moon, and microgravity conditions. Statistical significance is indicated by stars, double-s and hash symbols. A legend defines flask types and respiration categories. Error bars represent standard error.</alt-text>
</graphic>
</fig>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Effect of 24&#xa0;h simulated gravities on cellular respiration in F-25 flask. <bold>(A)</bold> Intact cell respiration (ICR), <bold>(B)</bold> maximum uncoupled respiration (ET), (C) mitochondrial (M) and non-mitochondrial (NM) respiration rates of C2C12 myoblasts (0.5&#xb7;10<sup>6</sup> cells&#xa0;mL<sup>&#x2212;1</sup>) cultured in the optimized F-25 flask (medium depth: <sup>1</sup>/<sub>3</sub>H<sub>0</sub> and gas exchange area: 18A<sub>0,PHL</sub>) with hydrophilic (PHL) membrane under simulated Earth (s-Earth &#x223c;1<italic>g</italic>), Mars (s-Mars &#x223c;0.38<italic>g</italic>), Moon (s-Moon &#x223c;0.17<italic>g</italic>) and Space (s-&#x3bc;g &#x223c;0.001<italic>g</italic>) gravity conditions generated by clinorotation. No statistical difference between gravity levels was found. Data of panel <bold>A</bold> and <bold>B</bold> are reported as mean &#xb1; SEM of percentage of respiration state rate relative to the corresponding value obtained with control flask (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>) and data of panel C are reported as mean &#xb1; SEM of ET &#x3d; M &#x2b; NM respiration rate (<xref ref-type="sec" rid="s12">Supplementary Figure S6</xref>, n &#x3d; 5).</p>
</caption>
<graphic xlink:href="fcell-14-1728827-g008.tif">
<alt-text content-type="machine-generated">Bar graph with three panels comparing respiration under various flas conditions. Panel A shows intact cell respiration, Panel B shows maximum uncoupled respiration, and Panel C separates mitochondrial and non-mitochondrial respiration contributions. Statistical significance is indicated by stars, double-s and hash symbols. A legend defines flask types and respiration categories. Error bars represent standard error.</alt-text>
</graphic>
</fig>
<sec id="s3-1">
<label>3.1</label>
<title>Effects of medium depth, gas exchange area, and membrane type on metabolic function</title>
<p>Across flasks partially-filled and full-filled with medium under static conditions, all C2C12 cultures reached comparable confluence levels (&#x223c;70%) prior to respirometric measurements and showed no detectable differences in viability relative to partially-filled T-25 controls (<xref ref-type="sec" rid="s12">Supplementary Figure S1</xref>). Cells exhibited similar confluence across conditions, with no visible signs of detachment or loss of viability. Cultures grown in the optimized F-25 configuration, maintained intact adhesion and normal cellular appearance over 24&#xa0;h under full-filled conditions, indicating that the culture environment did not adversely affect cell integrity.</p>
<p>Under static conditions, 24&#xa0;h exposure to partially-filled (<sup>1</sup>/<sub>5</sub>H<sub>0</sub>) culture conditions in either conventional T-25 (A<sub>0,PHB</sub>) or customized F-25 flasks differing in gas exchange area (6A<sub>0</sub>, 12A<sub>0</sub>, and 18A<sub>0</sub>) and membrane type (PHB and PHL) at the same seeding density did not affect cellular respiration (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>). It should be noted that the membrane mounted on the vent cap of the commercial T-25 is hydrophobic PHB. For comparison, respiratory state rates are shown for the T-25 and for the F-25 flasks only the configuration with the largest gas exchange area of 18A<sub>0,PHL</sub>.</p>
<p>The intact cell respiration rate (ICR) obtained with T-25 and F-25 flasks was statistically similar at time zero (43 &#xb1; 3 vs. 42 &#xb1; 4&#xa0;pmol O<sub>2</sub> s<sup>&#x2212;1</sup> 10<sup>&#x2212;6</sup> cells<sup>&#x2212;1</sup>) and remained unchanged after 24&#xa0;h (40 &#xb1; 3 vs. 43 &#xb1; 4&#xa0;pmol O<sub>2</sub> s<sup>&#x2212;1</sup> 10<sup>&#x2212;6</sup> cells<sup>&#x2212;1</sup>) (<xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>). For convenience, only T-25 <sup>1</sup>/<sub>5</sub>H<sub>0</sub> A<sub>0,PHB</sub> condition at 24&#xa0;h was selected as control for all comparisons of the respiration state rates obtained for different medium depth (H) and gas exchange area (A) with flasks mounting a hydrophobic (PHB) (<xref ref-type="fig" rid="F3">Figure 3</xref>) or hydrophilic (PHL) (<xref ref-type="fig" rid="F4">Figure 4</xref>) membrane. To facilitate comparison in the figures, each flask configuration was assigned a distinct color, consistently used to represent the corresponding data in the bar plots.</p>
<p>In comparison to the control condition, the conventional T-25 (H<sub>0</sub> A<sub>0,PHB</sub>) and the customized F-25 (H<sub>0</sub> 6A<sub>0,PHB</sub>) full-filled flasks led to a significant increase in the ICR rate of 200% (<xref ref-type="fig" rid="F3">Figure 3A</xref>, red). With an increase in gas exchange area from 6 to 18 A<sub>0,PHB</sub> at the same medium depth (H<sub>0</sub>), ICR decreased progressively reaching the control condition value for a gas exchange area of 18A<sub>0,PHB</sub>. A similar gas exchange area effects on ICR were observed for a medium depth of <sup>2</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3D</xref>, green) and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3G</xref>, blue). Similarly to what was observed for ICR, maximum uncoupled respiration (ET) showed a clear dependence on flask geometry and gas exchange area (<xref ref-type="fig" rid="F3">Figures 3B,E,H</xref>). In comparison to the control condition, the conventional T-25 (H<sub>0</sub>-A<sub>0,PHB</sub>) and the customized F-25 (H<sub>0</sub> 6A<sub>0,PHB</sub>) full-filled flasks led to a significant increase in the ET rate of 250% and 180% (<xref ref-type="fig" rid="F3">Figure 3B</xref>, red), respectively. With an increase in gas exchange area from 6 to 18 A<sub>0,PHB</sub> at the same medium depth (H<sub>0</sub>), ET decreased progressively reaching the control condition. A similar pattern was observed for a medium depth of <sup>2</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3E</xref>, green) and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3H</xref>, blue). The complete comparison of all respiratory state rates was reported in <xref ref-type="sec" rid="s12">Supplementary Figure S3</xref>.</p>
<p>To evaluate the impact of flask configuration on mitochondrial (M) and non-mitochondrial (NM) respiration, the cellular oxygen consumption rate was measured after inhibition of complex III with antimycin A (Ama), as described in <xref ref-type="sec" rid="s12">Supplementary Figure S3</xref>. This rate corresponds to NM respiration, whereas M respiration rate was calculated as the difference between ET and Ama rates. Under control conditions, the contributions of mitochondrial and non-mitochondrial respiration to maximal uncoupled respiration were approximately 80% and 20%, respectively (<xref ref-type="fig" rid="F3">Figure 3C</xref>; <xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>). Non-mitochondrial and mitochondrial respiration rate followed an analogous pattern to that observed for ET (<xref ref-type="fig" rid="F3">Figures 3C,F,I</xref>). From cells cultured in conventional T-25 (H<sub>0</sub> A<sub>0,PHB</sub>) full-filled flask, NM and M respiration rates were found approximately more than 200% greater than the rate observed for the control group. Also, NM and M respiration rates measured in F-25 (H<sub>0</sub> 6A<sub>0,PHB</sub>) were higher than the corresponding NM and M rates observed for the control group. With an increase in gas exchange area, both NM and M respiration rates decreased, reaching values similar to the corresponding NM and M rates measured in the control group (<xref ref-type="fig" rid="F3">Figure 3C</xref>, red). A similar gas exchange area effect (A<sub>0,PHB</sub>) on ICR and ET was also observed for a medium depth of <sup>2</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3F</xref>, green) and <sup>1</sup>/<sub>3</sub>H<sub>0</sub> (<xref ref-type="fig" rid="F3">Figure 3I</xref>, blue).</p>
<p>The gas exchange area effect studied with hydrophobic (PHB) membrane was also investigated with hydrophilic (PHL) membrane under static conditions (<xref ref-type="fig" rid="F4">Figure 4</xref>). The complete comparison of all respiratory state rates was reported in <xref ref-type="sec" rid="s12">Supplementary Figure S4</xref>. Even for this configuration, an increase in gas exchange area allowed preservation of ICR and ET rates at values similar to those observed in the control group. Furthermore, to assess the performance of the two membrane types, the ICR rates obtained with PHB and PHL membranes were compared at different medium depths (H) and gas exchange areas (A) (<xref ref-type="fig" rid="F5">Figure 5</xref>). A nonlinear fit based on <xref ref-type="disp-formula" rid="e1">Equation 1</xref> was performed to plot ICR as a function of H and A. In general, gas exchange area had a greater effect on ICR rate, whereas medium depth had only a minor effect.</p>
<p>Thus, we further compared at the same medium depth (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>), the ICR obtained with the PHB and PHL membrane for all three gas exchange area configurations (<xref ref-type="fig" rid="F6">Figure 6</xref>). In general, the ICR rates obtained with the PHL membrane were lower than those observed with the PHB membrane, with significant differences detected at gas exchange areas of 6A<sub>0</sub> and 18A<sub>0</sub>, but not at 12A<sub>0</sub>.</p>
</sec>
<sec id="s3-2">
<label>3.2</label>
<title>Effects of simulated extraterrestrial gravities on metabolic function</title>
<p>After analyzing the effects of medium depth and gas exchange area on metabolic function under static full-filled flask conditions for 24 h, we established that the best performing customized F-25 configuration was that with medium depth of <sup>1</sup>/<sub>3</sub>H<sub>0</sub> and a gas exchange area of 18A<sub>0,PHL</sub>. This F-25 configuration, together with the conventional T-25 flask, was then used to investigate the impact of simulated Earth, Mars, Moon, and microgravity conditions (i.e., rotational full-filled) on mitochondrial function.</p>
<p>In conventional full-filled T-25 flasks, under all gravity conditions including Earth, ICR (<xref ref-type="fig" rid="F7">Figure 7A</xref>) and ET (<xref ref-type="fig" rid="F7">Figure 7B</xref>) rates were more than 220% higher than the corresponding rates measured in control flasks. The higher rates observed appear related to an increase of the mitochondrial and non-mitochondrial respiration rates (<xref ref-type="fig" rid="F7">Figure 7C</xref>). Both mitochondrial and non-mitochondrial respiration rates in simulated gravity conditions were significantly different for the corresponding control group (<xref ref-type="fig" rid="F8">Figure 8C</xref>). In contrast, in the selected F-25 flask, the ICR (<xref ref-type="fig" rid="F8">Figure 8A</xref>) and ET (<xref ref-type="fig" rid="F8">Figure 8B</xref>) rates observed under simulated Earth gravity as well as under reduced gravity conditions (i.e., clinorotation) were similar to the corresponding rates measured in control flasks. Both mitochondrial and non-mitochondrial respiration rates in simulated gravity conditions were not significantly different for the corresponding control group (<xref ref-type="fig" rid="F8">Figure 8C</xref>).</p>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<label>4</label>
<title>Discussion</title>
<p>The effect of medium depth, gas exchange area, and membrane type were evaluated in static and dynamic (clinorotation) culture conditions on C2C12 myoblast respiratory rates, including intact cellular, maximal uncoupled, mitochondrial and non-mitochondrial respiration. Under static conditions, partially-filled cultures in T-25 or F-25 flasks showed unchanged respiratory rates after 24&#xa0;h. In contrast, full-filled cultures in T-25 (H<sub>0</sub> A<sub>0</sub>) and in customized F-25 flasks with different medium depth (<sup>1</sup>/<sub>3</sub>H<sub>0</sub>, <sup>2</sup>/<sub>3</sub>H<sub>0</sub>, and H<sub>0</sub>) and gas exchange area of 6A<sub>0</sub> produced marked increases in intact (ICR) and uncoupled (ET) respiration, exceeding 200% and 180% of partially-filled control, respectively. In both T-25 and customized F-25 flasks, the observed increase of the respiratory rates was associated with both mitochondrial (M) and non-mitochondrial (NM) contributions. Increasing the gas exchange area progressively preserved cellular respiration, with hydrophilic membranes yielding to lower respiration rates than hydrophobic ones. An optimized F-25 configuration (<sup>1</sup>/<sub>3</sub>H<sub>0</sub> 18A<sub>0,PHL</sub>) that preserved cellular respiration when validated under simulated gravities, avoided the abnormally elevated respiration observed in full-filled T-25. We proposed that increasing gas exchange area is essential to prevent hypoxic conditions leading to culture-induced artifacts and ensuring that metabolic responses measured under clinorotation are not biased by flask limitations.</p>
<sec id="s4-1">
<label>4.1</label>
<title>Flask oxygenation</title>
<p>Simulators of microgravity (s-&#x3bc;g) such as 3D clinostats are essential tools, however, conventional full-filled control flasks suffer from shears stress (<xref ref-type="bibr" rid="B79">Wuest et al., 2015</xref>; <xref ref-type="bibr" rid="B80">2017</xref>), inadequate gas exchange (<xref ref-type="bibr" rid="B59">Place et al., 2017</xref>; <xref ref-type="bibr" rid="B73">Tse et al., 2021</xref>), and nutrient gradients (<xref ref-type="bibr" rid="B70">Tan et al., 2024</xref>) that can mask gravity-specific responses. Although completely filling flasks is considered a good practice sufficient to allow a proper comparison between static and rotational cultures and to eliminate stress under rotation, our results showed that full-filled controls must also be optimized to avoid confounding effects from gas exchange limitations. Our investigations demonstrate that oxygenation is the dominant factor determining the level of cellular respiration in full-filled static cultures. In the conventional T-25 with gas exchange area of A<sub>0</sub>, full-filling increased ICR of nearly 2-fold and ET of 2.5-fold compared to partially-filled control. Notably, even with a 6-fold increase in gas exchange area in the F-25 flask, a high respiration rate was still observed. An increase of gas exchange area either with hydrophobic or hydrophilic membrane preserved metabolic function (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>). These results strongly suggest that cellular metabolic responses are determined by O<sub>2</sub> availability within the culture medium.</p>
<p>Although incubators are often considered to guarantee a &#x201c;normoxic&#x201d; environment, oxygen delivery to cultured cells has been demonstrated to be a critical factor (<xref ref-type="bibr" rid="B73">Tse et al., 2021</xref>), inherently limited by diffusion across the overlying medium (<xref ref-type="bibr" rid="B59">Place et al., 2017</xref>), and substantial evidence shows that <italic>in vitro</italic> cells frequently experience hypoxia due to high cellular respiration and limited oxygen diffusion to the cell layer (<xref ref-type="bibr" rid="B3">Al-Ani et al., 2018</xref>; <xref ref-type="bibr" rid="B31">Froese, 1962</xref>; <xref ref-type="bibr" rid="B62">Randers-Eichhorn et al., 1996</xref>; <xref ref-type="bibr" rid="B65">Saltzman et al., 2003</xref>; <xref ref-type="bibr" rid="B76">Wagner et al., 2011</xref>; <xref ref-type="bibr" rid="B77">Wenger et al., 2015</xref>; <xref ref-type="bibr" rid="B78">Wild et al., 2005</xref>). Whereas diffusion distances in mammalian tissues are typically only 10&#x2013;30&#xa0;&#x3bc;m and rarely exceed 100&#x2013;200&#xa0;&#x3bc;m from a capillary (<xref ref-type="bibr" rid="B40">Kety, 1951</xref>; <xref ref-type="bibr" rid="B42">Krogh, 1919</xref>), in culture vessels oxygen must often travel several millimeters or more to reach the cell layer. Depending on the specific oxygen consumption rate and transport only &#x223c;0.5&#x2013;1&#xa0;mm<sup>3</sup> of medium volume can adequately oxygenate tissues by diffusion alone. It should be noted that small shifts in medium depth (&#x223c;1&#xa0;mm) can change tissue pO<sub>2</sub> by nearly 30&#xa0;mmHg (<xref ref-type="bibr" rid="B16">Cechin et al., 2014</xref>; <xref ref-type="bibr" rid="B30">Fraker et al., 2009</xref>; <xref ref-type="bibr" rid="B50">Millman et al., 2009</xref>; <xref ref-type="bibr" rid="B60">Powers et al., 2008</xref>; <xref ref-type="bibr" rid="B61">2010</xref>). Also, equilibration of oxygen within static medium has been shown to be slow, requiring even hours to stabilize following a change in atmospheric composition (<xref ref-type="bibr" rid="B52">Newby et al., 2005</xref>). Thus, routine medium depths such as the one used in our study for partially-filled conditions (&#x223c;<sup>1</sup>/<sub>5</sub>H<sub>0</sub>, <xref ref-type="sec" rid="s12">Supplementary Figure S2</xref>) appear to provide sufficient oxygen flux to sustain mitochondrial respiration, while concomitantly minimizing the slow diffusion and equilibration processes associated with greater medium depths.</p>
<p>The volume-to-area ratio critically influences nutrient availability, accumulation of metabolic products, and concentrations of secreted factors in cell culture systems. Increasing the volume-to-area ratio, which corresponds to a greater medium height, increase diffusion distances under static conditions. This may limit the rate of oxygen and nutrient delivery to cells attached to the bottom of the culture vessel, while simultaneously allowing greater accumulation of metabolic waste products and secreted factors in the bulk medium. These effects can generate concentration gradients and influence cellular behavior.</p>
<p>The flask oxygenation was also enhanced using hydrophilic membrane (<xref ref-type="fig" rid="F6">Figure 6</xref>) compared to hydrophobic membrane. Hydrophilic cellulose acetate membranes are widely used in biological applications due to their low protein binding, minimal interaction with biomolecules, and low levels of extractables, making them suitable for contact with aqueous culture media (<xref ref-type="bibr" rid="B1">Abu-Zurayk et al., 2023</xref>). In our study, cellulose acetate membranes did not significantly affect cellular responses within the investigated time frame, indicating adequate short-term biocompatibility. Nevertheless, despite their favorable physical properties and enhanced gas permeability, long-term stability, potential nutrient adsorption, and cytotoxic leaching under extended culture conditions remain insufficiently characterized. These factors may become relevant during prolonged exposure or under varying culture environments. Therefore, further investigations are required to evaluate these aspects to ensure long-term biological safety and optimize their application in cell culture systems.</p>
<p>The systematic increase in mitochondrial activity observed with inadequate gas exchange area (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>) could be related to hypoxia-like conditions. This finding is consistent with evidence from both <italic>in vivo</italic> and <italic>in vitro</italic> studies of short-term hypoxia exposure (<xref ref-type="bibr" rid="B37">Holland et al., 2018</xref>; <xref ref-type="bibr" rid="B41">Korski et al., 2019</xref>; <xref ref-type="bibr" rid="B55">O&#x2019;Brien et al., 2021</xref>). Specifically, <xref ref-type="bibr" rid="B37">Holland et al. (2018)</xref> reported elevated respiration in preeclamptic tissue characterized by ischemia-reperfusion injury. The increase in mitochondrial respiration was also observed in healthy placental tissue subjected to hypoxia/reoxygenation, suggesting that enhanced respiration represents an adaptive compensatory response to stress (<xref ref-type="bibr" rid="B37">Holland et al., 2018</xref>). Similarly, <xref ref-type="bibr" rid="B41">Korski et al. (2019)</xref> investigated the effects of oxygen tension on mitochondrial function in human cardiac progenitor cells (hCPCs). These cells cultured under hypoxic conditions exhibited significantly higher ICR and ET rates (2.5- and 2-fold, respectively), as well as increased mitochondrial membrane potential (1.5-fold), compared to cells maintained under normoxia.</p>
<p>The increase in cellular respiration observed with limited gas exchange area was attributable not only to mitochondrial but also to non-mitochondrial respiration (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>). The elevated non-mitochondrial respiration rate may, in part, reflect the activity of oxidases outside the mitochondrial electron transport chain (e.g., NADH oxidases), which are often stimulated by ROS imbalance and cell signaling (<xref ref-type="bibr" rid="B51">Murphy, 2009</xref>; <xref ref-type="bibr" rid="B68">Starkov, 2008</xref>). A similar increase in non-mitochondrial respiration has been reported in human cardiac progenitor cells (hCPCs) under hypoxic conditions (<xref ref-type="bibr" rid="B41">Korski et al., 2019</xref>). Moreover, non-mitochondrial oxygen-consuming enzymes function as oxygen sensors, coupling O<sub>2</sub> availability to changes in cell signaling, differentiation, and metabolism. The most prominent examples are the HIF prolyl-hydroxylases (PHDs) and Factor Inhibiting HIF (FIH), which use molecular oxygen to hydroxylate specific residues on the HIF transcription factor (proline for PHDs, asparagine for FIH), thereby regulating its stability and transcriptional activity in response to oxygen levels (<xref ref-type="bibr" rid="B58">Place and Domann, 2013</xref>).</p>
<p>Acute hypoxia can induce a range of metabolic adaptations with an enhanced mitochondrial function, whereas prolonged exposure can lead to opposite effects, particularly in mitochondrial function and pyruvate metabolism. Thus, our results do not exclude the possibility that the short-term effects of hypoxia on cell metabolism are opposite to those observed after prolonged exposure. Indeed, while acute hypoxia can transiently stimulate mitochondrial activity, chronic hypoxia typically reduces mitochondrial function due to decreased oxidative capacity of the electron transport chain and the accumulation of damaged mitochondria which leads to significant metabolic reprogramming. In addition, pyruvate dehydrogenase (PDH) activity is inhibited under hypoxia through the induction of pyruvate dehydrogenase kinase (PDK) by HIF-1&#x3b1;, further limiting pyruvate entry into the TCA cycle (<xref ref-type="bibr" rid="B7">Bao and Wong, 2021</xref>; <xref ref-type="bibr" rid="B67">Solaini et al., 2010</xref>).</p>
</sec>
<sec id="s4-2">
<label>4.2</label>
<title>Extraterrestrial gravity effects on cellular metabolism</title>
<p>A critical issue in clinostat-based experiments lies in the absence of a standardized methodology with heterogeneous control of culture conditions. The widespread use of static cultures as terrestrial controls does not account for the fluid dynamic environment of clinorotation systems and can confound gravity-specific adaptations with artifacts from oxygen limitation. To account for both fluid dynamic and reduced gravity conditions created by the rotating motion, two types of control groups were employed. The first consisted of static controls, in which cells were cultured in flasks under standard, motionless conditions. The second involved dynamic controls, where cells were cultured in flasks mounted on a clinostat operating under Earth gravity (&#x223c;1<italic>g</italic>). Together, these two control groups allowed us to distinguish cellular responses specifically associated with altered gravity from those influenced by the fluid dynamic conditions generated by clinorotation. Medium flow patterns and shear stress distribution may influence cellular behavior under clinorotation. However, because both F-25 and T-25 flasks experienced identical rotation conditions, fluid dynamic-related mechanical stimuli are expected to be comparable between systems and therefore unlikely to account for the observed differences in metabolic outcomes. Thus, within the 24&#xa0;h exposure timeframe used in this study, shear stresses generated under clinorotation are expected to be relatively low and unlikely to dominate metabolic responses.</p>
<p>In this work, we addressed this methodological issue by highlighting the importance of both static and dynamic controls (<xref ref-type="fig" rid="F7">Figure 7</xref>). The cellular responses obtained with conventional full-filled T-25 flasks were consistently elevated, regardless of whether static or dynamic conditions were applied, indicating a comparable response across groups. The difference in respiration rate observed between partially-filled and full-filled flasks under static or dynamic conditions likely reflects methodological artifacts noted in the study section focused on static cell cultures (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>). Overall, the use of conventional flasks proved unreliable, as their responses were attributable to culture-induced stresses, as previously discussed. To avoid this artifact, F-25 flasks were employed to evaluate the effects of simulated gravity on cellular function (<xref ref-type="fig" rid="F8">Figure 8</xref>), revealing that reduced gravity did not have a major impact on respiration within the 24&#xa0;h period.</p>
<p>It should be noted that a 24&#xa0;h exposure was employed to evaluate mass transport and oxygen distribution in cell culture within the F-25 and T-25 systems under clinorotation. This short exposure duration was selected to enable a controlled comparison between the two flask designs while minimizing confounding effects associated with long-term microgravity-induced metabolic adaptation. Within this defined timeframe, the F-25 system demonstrated sensitivity to oxygen-dependent metabolic perturbations under simulated microgravity, supporting its use as a proof-of-principle platform. Future studies will be required to assess long-term performance and stability under prolonged simulated microgravity conditions.</p>
<p>The few studies that have investigated the effects of microgravity on mitochondrial function reported mitochondrial dysfunction with increased oxidative stress (<xref ref-type="bibr" rid="B14">Calzia et al., 2020</xref>; <xref ref-type="bibr" rid="B46">Locatelli et al., 2020</xref>; <xref ref-type="bibr" rid="B53">Nguyen et al., 2021</xref>). Specifically, human umbilical vein endothelial cells (HUVECs) showed decreased respiration after 4 and 10 days of simulated microgravity in a rotating wall vessel (RWV), compared to static 1<italic>g</italic> controls (<xref ref-type="bibr" rid="B46">Locatelli et al., 2020</xref>). Similarly, C2C12 myotubes exhibited a progressive decline in respiration and increased oxidative stress between 24 and 72&#xa0;h of exposure in a random positioning machine (RPM), again compared to static 1<italic>g</italic> controls (<xref ref-type="bibr" rid="B14">Calzia et al., 2020</xref>). The early mitochondrial responses to reduced gravity levels observed in our work appeared to be modest, most likely due to the short exposure period of only 24&#xa0;h.</p>
<p>Beyond microgravity, the F-25 is also suited for hypoxia and oxygen dynamics studies. Unlike standard hypoxia chambers, which control only atmospheric oxygen and neglect diffusion through the medium (<xref ref-type="bibr" rid="B4">Allen et al., 2001</xref>; <xref ref-type="bibr" rid="B59">Place et al., 2017</xref>; <xref ref-type="bibr" rid="B73">Tse et al., 2021</xref>), the F-25 allows simultaneous adjustment of medium height and membrane permeability. This dual control enables precise regulation of oxygen delivery known to affect mitochondrial function and cellular metabolism (<xref ref-type="bibr" rid="B3">Al-Ani et al., 2018</xref>; <xref ref-type="bibr" rid="B25">Ereci&#x144;ska and Silver, 2001</xref>). Applications extend to cancer (<xref ref-type="bibr" rid="B8">Bertout et al., 2008</xref>; <xref ref-type="bibr" rid="B75">Vaupel and Mayer, 2007</xref>), ischemia-reperfusion (<xref ref-type="bibr" rid="B39">Kalogeris et al., 2012</xref>), and metabolic reprogramming (<xref ref-type="bibr" rid="B23">Eales et al., 2016</xref>), where oxygen sensitivity is a central determinant. The system is promising for investigation with organoids and spheroids that often suffer from hypoxia (<xref ref-type="bibr" rid="B34">Grimes et al., 2014</xref>; <xref ref-type="bibr" rid="B45">Lancaster and Knoblich, 2014</xref>; <xref ref-type="bibr" rid="B56">Palacio-Casta&#xf1;eda et al., 2022</xref>). By enhancing gas exchange at the culture interface, the F-25 supports long-term maintenance of 3D aggregates, co-cultures, and differentiation protocols, enabling more relevant tissue phenotypes for regenerative medicine, disease modeling, and patient-derived organoid drug testing (<xref ref-type="bibr" rid="B24">Edmondson et al., 2014</xref>; <xref ref-type="bibr" rid="B26">Fatehullah et al., 2016</xref>).</p>
<p>This study relies on a ground-based simulated microgravity platform which, although proven to be an essential tool for investigating the effects of microgravity on cellular behavior, still presents certain discrepancies compared with real spaceflight conditions, underscoring the need for continued refinement and validation through experimental data obtained from actual space missions (<xref ref-type="bibr" rid="B38">Huang et al., 2018</xref>; <xref ref-type="bibr" rid="B53">Nguyen et al., 2021</xref>; <xref ref-type="bibr" rid="B69">Svejgaard et al., 2015</xref>). Nevertheless, the same limitation applies to both the F-25 and T-25 culture systems. Standard T-25 flasks have historically been used as reference in spaceflight experiments, despite not being optimized for transport phenomena. The F-25 differs primarily in geometry and gas exchange capacity, and this modification is not expected to introduce additional discrepancies with respect to simulated versus real microgravity conditions. Rather, improved exchange efficiency may enhance robustness across different gravitational environments. Validation against spaceflight data therefore remains an important objective for future studies.</p>
<p>Another limitation of the study is that the cellular status was primarily evaluated through respirometry, which provides sensitive information on cellular metabolic activity under <italic>in vitro</italic> conditions. However, oxygen consumption alone does not fully capture cellular energetics or stress responses, such as changes in ATP availability, oxidative stress, or transcriptional adaptation. Therefore, our conclusions are limited to the observation that respiratory activity was maintained at levels comparable to the control condition within the investigated time window, indicating no evidence of acute metabolic impairment. Complementary endpoints, including ATP content, ROS production, and targeted gene expression or metabolic profiling, will provide more comprehensive assessment of the cellular status and support mechanistic interpretation.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="s5">
<label>5</label>
<title>Conclusion</title>
<p>This study evaluated oxygen exchange efficiency as a physical and engineering constraint in a well-characterized <italic>in vitro</italic> model for studying skeletal muscle metabolism, mitochondrial function, and oxygen-dependent bioenergetics. While different cell types exhibit distinct oxygen demands and metabolic profiles, the present study demonstrates that inadequate oxygen exchange area alone is sufficient to induce metabolic drift under static and dynamic culture conditions. The F-25 system therefore serves as a technological and conceptual proof-of-principle, highlighting oxygen exchange geometry as a critical design parameter for preserving metabolic phenotype. Extension of this approach to additional cell types will be necessary to determine how cell-specific metabolic requirements modulate sensitivity to transport limitations.</p>
<p>The optimized F-25 configuration, which combines a large gas exchange area with a hydrophilic gas-permeable membrane, effectively prevented hypoxia-induced respiratory over-activation and maintained C2C12 myoblasts in a stable bioenergetic state. By minimizing O<sub>2</sub> depletion and CO<sub>2</sub> accumulation the F-25 system establishes a controlled baseline condition for clinostat-based experiments. This ensures that mitochondrial and metabolic responses measured under simulated Earth, Lunar, Martian, or microgravity conditions can be confidently attributed to gravitational unloading rather than to artifacts of inadequate culture conditions. The novel culture system addresses a longstanding methodological gap in space biology, enabling more reproducible and relevant <italic>in vitro</italic> models for gravitational research. Its ability to standardize static controls in rotational platforms directly supports the development of robust experimental protocols, improves cross-study comparability, and enhances the interpretability of cellular adaptation studies under partial gravity environments. Beyond space research, the precise oxygen regulation provided by this customized culture system makes it equally relevant to other research areas that require strict control of O<sub>2</sub> in the cellular microenvironment.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s6">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec sec-type="author-contributions" id="s7">
<title>Author contributions</title>
<p>GP: Conceptualization, Data curation, Methodology, Writing &#x2013; original draft, Writing &#x2013; review and editing. GF: Conceptualization, Data curation, Methodology, Writing &#x2013; original draft, Writing &#x2013; review and editing. DD: Methodology, Writing &#x2013; original draft, Writing &#x2013; review and editing. AC: Writing &#x2013; original draft, Writing &#x2013; review and editing. PF: Methodology, Writing &#x2013; original draft, Writing &#x2013; review and editing. GC: Funding acquisition, Writing &#x2013; original draft, Writing &#x2013; review and editing. NL: Conceptualization, Resources, Supervision, Writing &#x2013; original draft, Writing &#x2013; review and editing.</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<title>Conflict of interest</title>
<p>The author(s) declared that this work was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
<p>The author NL declared that they were an editorial board member of Frontiers at the time of submission. This had no impact on the peer review process and the final decision.</p>
</sec>
<sec sec-type="ai-statement" id="s10">
<title>Generative AI statement</title>
<p>The author(s) declared that generative AI was not used in the creation of this manuscript.</p>
<p>Any alternative text (alt text) provided alongside figures in this article has been generated by Frontiers with the support of artificial intelligence and reasonable efforts have been made to ensure accuracy, including review by the authors wherever possible. If you identify any issues, please contact us.</p>
</sec>
<sec sec-type="disclaimer" id="s11">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec sec-type="supplementary-material" id="s12">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fcell.2026.1728827/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fcell.2026.1728827/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.docx" id="SM1" mimetype="application/docx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2900308/overview">Martina Di Rienzo</ext-link>, National Institute for Infectious Diseases Lazzaro Spallanzani (IRCCS), Italy</p>
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<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/594719/overview">Marcus Kr&#xfc;ger</ext-link>, Otto von Guericke University Magdeburg, Germany</p>
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<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/997241/overview">Xiaohua Lei</ext-link>, Chinese Academy of Sciences (CAS), China</p>
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