Abstract
A basic prototype for polymer chains can be represented as where R is the monomer unit. The configuration shown above is only one of the enormous number which can be assumed by the chain, since the molecule can perform internal rotations around each of the R - R bonds. Because of its flexibility a polymer chain fluctuates constantly, acquiring various configurations within very short time invervals. Therefore, at any given moment different chains belonging to the same ensemble can be found in states having different configurations. Consequently, a polymer described by an ideal chemical formula is, generally speaking, a mixture of a multiplicity of different configurations. Thus the problem of the geometry of polymer chains acquires a statistical character. The chain can be described therefore only by its averaged parameters. The size and shape of a polymer chain are of great interest to the polymer scientist, since physical properties such as light scattering, diffusion, and viscosity can only be understood if they are discussed in the light of configurational properties.
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Bruns, W. (1981). Polymer Configuration. In: Monte Carlo Applications in Polymer Science. Lecture Notes in Chemistry, vol 27. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-93195-6_3
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