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arXiv 1206.6007cond-mat.soft
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“加热冷却”--展示纵向specific heat的重要性

"Cooling by heating" - demonstrating the significance of the longitudinal specific heat

Jon J. Papini, Jeppe C. Dyre, Tage Christensen

摘要:

在表面加热固体球体会在球体内部产生机械应力。如果提供有限的热量,随着温度在整个球体上变得均匀,应力逐渐消失。我们表明,在此之前发生,有一个暂时的压力和密度在球体内部的降低,诱导一个短暂的温度降低。对于普通固体,这种影响很小,因为c_p几乎等于c_V。对于流动液体,这种影响可以忽略,因为它们的动态剪切模量为零。然而,对于处于玻璃化转变的液体,这种影响通常比固体大得多。本文给出了相应的耦合热粘弹性方程的解析解。通常,在恒压下测得的等压比热c_p和纵向比热c_l之间存在差异,这与限制相关膨胀为纵向的机械边界条件有关。在热传播的精确处理的热扩散常数包含C_L,而不是C_P。我们表明,控制的“冷却加热”效应的大小的关键参数是这两个比热之间的相对差异。对于典型的玻璃形成液体,当表面温度增加1 K时,如果在玻璃化转变下进行实验,则预期球心温度降低5 mK级。通过在玻璃化转变时对直径为19 mm的葡萄糖球进行测量,证实了加热冷却效应。

英文摘要:

Heating a solid sphere at the surface induces mechanical stresses inside the sphere. If a finite amount of heat is supplied, the stresses gradually disappear as temperature becomes homogeneous throughout the sphere. We show that before this happens, there is a temporary lowering of pressure and density in the interior of the sphere, inducing a transient lowering of the temperature here. For ordinary solids this effect is small because c_p is almost equal to c_V. For fluent liquids the effect is negligible because their dynamic shear modulus vanishes. For a liquid at its glass transition, however, the effect is generally considerably larger than in solids. This paper presents analytical solutions of the relevant coupled thermoviscoelastic equations. In general, there is a difference between the isobaric specific heat, c_p, measured at constant isotropic pressure and the longitudinal specific heat, c_l, pertaining to mechanical boundary conditions that confine the associated expansion to be longitudinal. In the exact treatment of heat propagation the heat diffusion constant contains c_l rather than c_p. We show that the key parameter controlling the magnitude of the "cooling-by-heating" effect is the relative difference between these two specific heats. For a typical glass-forming liquid, when temperature at the surface is increased by 1 K, a lowering of the temperature in the sphere center of order 5 mK is expected if the experiment is performed at the glass transition. The cooling-by-heating effect is confirmed by measurements on a 19 mm diameter glucose sphere at the glass transition.

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