<?xml version="1.0" encoding="UTF-8"?>
<term>
  <id>12265</id>
  <title>Flory–Fox equation</title>
  <longtitle>IUPAC Gold Book - Flory–Fox equation</longtitle>
  <doi>10.1351/goldbook.12265</doi>
  <code>12265</code>
  <status>current</status>
  <definitions>
    <item>
      <id>1</id>
      <text>Equation relating intrinsic viscosity, \(\eta\), and molar mass, \(M\), to the mean-square radius of gyration, with \[[\eta]M = \mathit{\Phi}^{\prime}\!\lt\!s^{2}\!\gt^{3/2}\] where \(\mathit{\Phi}^{\prime}\) is a parameter the value of which depends on the molar-mass distribution, macromolecular constitution, and chain expansion.</text>
      <notes>
        <item>\([\eta]M/N_{\rm{A}}\), where \(N_{\rm{A}}\) is the Avogadro constant, is the equivalent hydrodynamic volume in viscous flow, \(V_{\eta}\), with \(V_{\eta} = 4\uppi r_{\eta}^{3}/3\), Hence, the Flory–Fox equation is consistent with the Kirkwood–Riseman theory and the Flory–Fox assumption. (See Notes to Kirkwood–Riseman theory and Flory–Fox assumption.)</item>
        <item>For a solution in the theta state, \(\mathit{\Phi}^{\prime}\) is denoted \(\mathit{\Phi}_{\uptheta}^{\prime}\) and its value is given by the Kirkwood–Riseman theory, with \(\mathit{\Phi}_{\uptheta}^{\prime} = \pu{4.22E22 mol-1}\).</item>
        <item>The Flory–Fox equation is sometimes written in terms of \(\lt\!r^{2}\!\gt\), the mean-square end-to-end distance, instead of \(\lt\!s^{2}\!\gt\), with \[[\eta]M = \mathit{\Phi} \lt\!r^{2}\!\gt^{3/2}\] where \(\mathit{\Phi} = \mathit{\Phi}^{\prime}/6^{3/2}\). The latter equality assumes that \(\lt\!r^{2}\!\gt = 6\!\lt\!s^{2}\!\gt\), which is only exactly true in the theta state. In this case, \[[\eta]M = \mathit{\Phi}_{\theta}\!\lt\!r^{2}\!\gt^{3/2}\] where \(\mathit{\Phi}_{\theta} = \mathit{\Phi}_{\theta}/6^{3/2} = \pu{2.87E21 mol-1}\).</item>
        <item>\(\mathit{\Phi}\) is known as the viscosity function or the Flory function.</item>
      </notes>
      <links>
        <item>
          <term>Flory–Fox assumption</term>
          <url>https://goldbook.iupac.org//terms/view/12264</url>
        </item>
        <item>
          <term>Kirkwood–Riseman theory</term>
          <url>https://goldbook.iupac.org//terms/view/12263</url>
        </item>
        <item>
          <term>equivalent hydrodynamic volume</term>
          <url>https://goldbook.iupac.org//terms/view/12257</url>
        </item>
        <item>
          <term>mean-square end-to-end distance</term>
          <url>https://goldbook.iupac.org//terms/view/12197</url>
        </item>
        <item>
          <term>mean-square radius of gyration</term>
          <url>https://goldbook.iupac.org//terms/view/12192</url>
        </item>
      </links>
      <sources>
        <item>PAC, 2015, 87, 71. 'Definitions of terms relating to individual macromolecules, macromolecular assemblies, polymer solutions, and amorphous bulk polymers (IUPAC Recommendations 2014)' on page 104 (https://doi.org/10.1515/pac-2013-0201)</item>
      </sources>
    </item>
  </definitions>
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    <html>https://goldbook.iupac.org/terms/view/12265/html</html>
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  <citation>Citation: 'Flory–Fox equation' in IUPAC Compendium of Chemical Terminology, 5th ed. International Union of Pure and Applied Chemistry; 2025. Online version 5.0.0, 2025. 10.1351/goldbook.12265</citation>
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  <accessed>2026-04-18T08:21:35+00:00</accessed>
</term>
