Kuhn length

The Kuhn length is a theoretical treatment, developed by Werner Kuhn, in which a real polymer chain is considered as a collection of $N$ Kuhn segments each with a Kuhn length $b$ . Each Kuhn segment can be thought of as if they are freely jointed with each other.^[1]^[2]^[3]^[4] Each segment in a freely jointed chain can randomly orient in any direction without the influence of any forces, independent of the directions taken by other segments. Instead of considering a real chain consisting of $n$ bonds and with fixed bond angles, torsion angles, and bond lengths, Kuhn considered an equivalent ideal chain with $N$ connected segments, now called Kuhn segments, that can orient in any random direction.

The length of a fully stretched chain is $L=Nb$ for the Kuhn segment chain.^[5] In the simplest treatment, such a chain follows the random walk model, where each step taken in a random direction is independent of the directions taken in the previous steps, forming a random coil. The average end-to-end distance for a chain satisfying the random walk model is $\langle R^{2}\rangle =Nb^{2}$ .

Since the space occupied by a segment in the polymer chain cannot be taken by another segment, a self-avoiding random walk model can also be used. The Kuhn segment construction is useful in that it allows complicated polymers to be treated with simplified models as either a random walk or a self-avoiding walk, which can simplify the treatment considerably.

For an actual homopolymer chain (consists of the same repeat units) with bond length $l$ and bond angle θ with a dihedral angle energy potential,^{[clarification needed]} the average end-to-end distance can be obtained as

\langle R^{2}\rangle =nl^{2}{\frac {1+\cos(\theta )}{1-\cos(\theta )}}\cdot {\frac {1+\langle \cos(\textstyle \phi \,\!)\rangle }{1-\langle \cos(\textstyle \phi \,\!)\rangle }}

,

where

\langle \cos(\textstyle \phi \,\!)\rangle

is the average cosine of the dihedral angle.

The fully stretched length $L=nl\,\cos(\theta /2)$ . By equating the two expressions for $\langle R^{2}\rangle$ and the two expressions for $L$ from the actual chain and the equivalent chain with Kuhn segments, the number of Kuhn segments $N$ and the Kuhn segment length $b$ can be obtained.

For worm-like chain, Kuhn length equals two times the persistence length.^[6]

References

^ Flory, P.J. (1953) Principles of Polymer Chemistry, Cornell Univ. Press, ISBN 0-8014-0134-8
^ Flory, P.J. (1969) Statistical Mechanics of Chain Molecules, Wiley, ISBN 0-470-26495-0; reissued 1989, ISBN 1-56990-019-1
^ Rubinstein, M., Colby, R. H. (2003)Polymer Physics, Oxford University Press, ISBN 0-19-852059-X
^ Doi, M.; Edwards, S. F. (1988). The Theory of Polymer Dynamics. Volume 73 of International series of monographs on physics. Oxford science publications. p. 391. ISBN 0198520336.
^ Michael Cross (October 2006), Physics 127a: Class Notes; Lecture 8: Polymers (PDF), California Institute of Technology, retrieved 2013-02-20
^ Gert R. Strobl (2007) The physics of polymers: concepts for understanding their structures and behavior, Springer, ISBN 3-540-25278-9

[1] Flory, P.J. (1953) Principles of Polymer Chemistry, Cornell Univ. Press, ISBN 0-8014-0134-8

[2] Flory, P.J. (1969) Statistical Mechanics of Chain Molecules, Wiley, ISBN 0-470-26495-0; reissued 1989, ISBN 1-56990-019-1

[3] Rubinstein, M., Colby, R. H. (2003)Polymer Physics, Oxford University Press, ISBN 0-19-852059-X

[4] Doi, M.; Edwards, S. F. (1988). The Theory of Polymer Dynamics. Volume 73 of International series of monographs on physics. Oxford science publications. p. 391. ISBN 0198520336.

[5] Michael Cross (October 2006), Physics 127a: Class Notes; Lecture 8: Polymers (PDF), California Institute of Technology, retrieved 2013-02-20

[6] Gert R. Strobl (2007) The physics of polymers: concepts for understanding their structures and behavior, Springer, ISBN 3-540-25278-9

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