Condensed Matter Physics: Crystals, Liquids, Liquid by Gert R. Strobl

By Gert R. Strobl

Derived from lectures on the college of Freiburg, this textbook introduces solid-state physics in addition to the physics of beverages, liquid crystals and polymers. The 5 chapters take care of the most important features of condensed topic: constructions, susceptibilities, molecular fields, currents, and dynamics. the writer strives to provide and clarify coherently the phrases and ideas linked to the most houses and features of condensed subject, whereas minimizing recognition to extraneous info. therefore, this article offers the company and vast foundation of realizing that readers require for extra research and research.

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Additional resources for Condensed Matter Physics: Crystals, Liquids, Liquid Crystals, and Polymers

Example text

The answer is found in the power law of Eq. 80). If applied to a volume 40 1 Structures which encloses only a part of the polymer chain – say, a sphere of diameter r – we obtain for the number of structural units n which are found on average n ∝ r2 . 81) The power to which the distance is raised corresponds, by definition, to the fractal dimension. Thus, for polymer chains in a melt, the fractal dimension takes the value two. Polymer chains are objects which exist in three dimensions; however, since they only partially fill the available space, a lower dimension is found.

71) ˜ ) 1 + 2 exp(−Δ˜ utg /RT ˜ is the universal gas constant). This equation assumes that each C-C bond (R can arrange itself independent of the others. Although this is not really true, Eq. 71) does provide a reasonable estimate for wg . , in a polyethylene melt or the melt of some other polymer, all the different rotational isomeric states can be occupied. Virtually all the chains exist in forms which can be referred to as coil-like. As they are densely packed they must interpenetrate each other.

This time becomes ever longer, the lower the temperature is – since the adjustment time depends on the viscosity, which is described by the Vogel–Fulcher equation. It is clear that as the adjustment time increases, eventually a point is reached where the equilibrium conformation can no longer be achieved in the course of normal observation times. The melt then remains in the last adopted state and hardens into a glass. Experience shows that this occurs when the viscosity has reached the value of η(Tg ) = 1012 Nm−2 s .

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