Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/18/84; site oddjob.UUCP Path: utzoo!watmath!clyde!burl!ulysses!mhuxr!mhuxt!houxm!ihnp4!gargoyle!oddjob!sra From: sra@oddjob.UUCP (Scott R. Anderson) Newsgroups: net.physics Subject: Real Physics -- Specific Heat of Glasses Message-ID: <713@oddjob.UUCP> Date: Sat, 11-May-85 02:42:52 EDT Article-I.D.: oddjob.713 Posted: Sat May 11 02:42:52 1985 Date-Received: Sun, 12-May-85 04:56:54 EDT References: <1397@mtx5b.UUCP> <> Reply-To: sra@oddjob.UUCP (Scott R. Anderson) Organization: University of Chicago, Department of Physics Lines: 39 Summary: In article <1397@mtx5b.UUCP> mat@mtx5b.UUCP (Mark Terribile) writes: >The specific heat of metals is very low ... approximately one fifth to >one tenth that of water. Ceramics and glassy materials have specific >heats that are approximately the specific heat of water, give or take >a factor of one part in three. > Is the specific heat of more reminiscent of the >specific heat of the metallic phase of the material, or is it reminiscent >of the specific heat of glass? In article <> chas@gtss.UUCP (Charles Cleveland) writes: >If you examine specific heats in some reasonable units (such as calories >per degree kelvin per atom) you will find that there is no systematic >variation is specific heats as one moves between materials belonging >to the classes you consider...The variations do not particularly have >to do with crystalline vs. amorphous or insulator vs. conductor. These >are about room temperature considerations (specific heat dominated by >'lattice vibrations'. It should be pointed out that there is more than one kind of specific heat: Cv, the specific heat measured at constant volume, and Cp, the specific heat measured at constant pressure. What Charles refers to is Cv, which is relatively constant amongst solids at room temperature. However, it is much easier to measure Cp, so that is usually what is reported in handbooks of materials. I believe this is what Mark refers to. The difference between the two is an equation of thermodynamics which involves the adiabatic and isothermal compressibilities of the material. Cp for water is 1 cal/g-K (this is the definition of the calorie) or 18 cal/mol-K, while most metals are about 5 cal/mol-K. "Ordinary" glasses are indeed around 20 cal/mol-K, but this is about half of the specific heat of the corresponding liquid phase; the specific heat of the glass phase is only slightly higher than that of the crystalline phase. The latter is also true of metallic glasses; i.e., the answer to Mark's question is 'yes' (:-). Scott Anderson ihnp4!oddjob!kaos!sra