Statistical mechanics of chain molecules

By P. Flory, E. Dimarzio. 1970

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Citations in the corpus

lDDT: a local superposition-free score for comparing protein structures and models using distance difference tests (2013, methodology): “The web server has been implemented using the Python Django and JavaScript jQuery frameworks; it supports all the major browsers.”
Monte Carlo Simulation of Long Chain Polymer Melts: Crossover from Rouse to Reptation Dynamics (2000, background): “ N→∞ R2e/[(N−1)l2]) is the characteristic ratio which measures the swelling of a chain due to its intrinsic stiﬀness compared to a pure random walk. Using C∞ ≃ 1.56 (see Fig. 1) and l p = l(C∞ + 1)/2 [41], the persistence length, l p, of the model is given by l p ≃ 3.38. The shape of a polymer is no”
Solution spraying of poly(methyl methacrylate) blends to fabricate microtextured, superoleophobic surfaces (2011, unknown): “54 10 l m    [48].”
Proton multiple-quantum NMR for the study of chain dynamics and structural constraints in polymeric soft materials (2007, methodology): “Second, under the assumption of Gaussian statistics, Sb yields the number of statistical segments N, which in turn can be converted into Mc using the known characteristic ratio C1 [81].”
An Average-Stretch Full-Network Model for Rubber Elasticity (2003, background): “statistical theory, the distribution P( r) being a rough measure of the range of variation among the very many possible configurations of a chain [ 1 ].”
Static and Dynamical Properties of Single Poly(Ethylene Glycol) Molecules Investigated by Force Spectroscopy (2000, background): “Since the Kuhn length in the FJC model is two times the persistence length in the WLC model [ 32 ], this value is in fair agreement with our value.”