We discuss theoretically and numerically the intramolecular form factor $F(q)$ in dense polymer systems. Following Florys ideality hypothesis, chains in the melt adopt Gaussian configurations and their form factor is supposed to be given by Debyes formula. At striking variance to this, we obtain noticeable (up to 20%) non-monotonic deviations which can be traced back to the incompressibility of dense polymer solutions beyond a local scale. The Kratky plot ($q^2F(q)$ {it vs.} wavevector $q$) does not exhibit the plateau expected for Gaussian chains in the intermediate $q$-range. One rather finds a significant decrease according to the correction $delta(F^{-1}(q)) = q^3/32rho$ that only depends on the concentration $rho$ of the solution, but neither on the persistence length or the interaction strength.
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