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Mark–Houwink equation

Equation in polymer science

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Through Molar mass, Polymer and Solvent

[η]=KMa

From this equation the molecular weight of a polymer can be determined from data on the intrinsic viscosity and vice versa.

The equation often receives the name of its contributors Herman F. Mark, Roelof Houwink, Ichirō Sakurada, and Werner and Hans Kuhn (unrelated), who developed it in the 1940s.

Parameter values

The values of the Mark–Houwink parameters, a and K, depend on the particular polymer-solvent system as well as temperature.

a is related to the polymer's hydrodynamic volume, and thus the solvated polymer's typical geometry. If the radius of gyration, R, scales with mass as R∼Mν, then a=3ν−1. Thus:

  • a=0 implies that the polymer is a rigid sphere, such as the DNA of bacteriophage T2
  • a=0.5 corresponds to the flexible coil induced by a theta solvent
  • a=0.76 corresponds to a good solvent described by Flory-Huggins solution theory.
  • a=2.0 implies that the polymer is an absolutely rigid rod, such as tobacco mosaic virus.

Other a values generally hold for small ranges of molar masses and exhibit a nonlinear log-log plot, because they correspond to transitions between each dynamical regime. Nevertheless, flexible polymers are defined as those for which 0.5≤a≤0.8 and semi-flexible polymers those for which a≥0.8.

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