dlscrib com francois sears amp gerhard
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dlscrib com francois sears amp gerhard
MUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard , Rensselaer Polytechnic InstituteThermodynamics, Kinetic Theory, and Statistical Thermodynamics THIRD EDITIONAddison-Wesley Publishing CompanyReading. MassachusettsAmsterdam • London • Manila • Singapore • Sydney • Tokyowww.pdfgrip.comWORLD STUDENT SERIES EDITIONSIXTH PRINTING 1982Copyright o 1975 dlscrib com francois sears amp gerhard by Addison-Wesley Publishing Company. Inc. Philippines copyright 1975 by Addison-Wesley Publishing Company, Inc.AU rights reserved. No part of this pudlscrib com francois sears amp gerhard
blication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, recordinMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard brary of Congress Catalog Card No. 74-2151.www.pdfgrip.comPrefaceThis text is a major revision of An Introduction to Thermodynamics, Kinetic Theory, and Statistical Mechanics by Francis w. Sears. The general approach has been unaltered and the level remains much the same, perhaps being increased som dlscrib com francois sears amp gerhard ewhat by greater coverage. The text is still considered useful for advanced undergraduate^ in physics and engineering who have some familiarity with cdlscrib com francois sears amp gerhard
alculus.The first eight chapters are devoted to a presentation of classical thermodynamics without recourse to either kinetic theory or statistical meMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard he properties of the system can be specified without knowing anything about the microscopic properties of the system. In the later chapters we show how the microscopic properties of the system can be determined by using the methods of kinetic theory and statistical mechanics to calculate the depende dlscrib com francois sears amp gerhard nce of the macroscopic properties of a system on thermodynamic variables.The presentation of many topics differs from the earlier text. Non-PFT systemdlscrib com francois sears amp gerhard
s are introduced in the second chapter and are discussed throughout the text. The first lajv is developed as a definition of the difference in the intMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard energy of the system do not change. The heat flow is then the difference between the work in any process between two equilibrium states and the work in an adiabatic process between the same states. Care is taken to explain the effects of changes in kinetic and potential energy as well. After the dis dlscrib com francois sears amp gerhard cussion of the first law, various examples are presented to show which properties of the system can be determined on the bash of this law alone.The stdlscrib com francois sears amp gerhard
atement that "in every process taking place in an isolated system the entropy of the system either increases or remains constant’’ is used as the secoMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard ic potentials are presented in greater detail than in the earlier text. A new potential F* is introduced to make consistent the thermodynamic and statistical treatments of processes in which the potential energy of a system changes. The discussion of open systems, added in Chapter 8, is necessary fo dlscrib com francois sears amp gerhard r the new derivation of statistics.■www.pdfgrip.comtv PREFACEKinetic theory of gases is treated in Chapters 9 and 10. Although the coverage appears todlscrib com francois sears amp gerhard
be reduced from the previous edition, the remaining material is discussed from the point of view of statistics in Chapter 12.The derivation of the diMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard utset. The number of microstates belonging to each macrostate is calculated in the conventional manner for Bose-Einstein, Fermi-Dirac and Maxwell-Boltzmann statistics. The entropy is shown to be proportional to the natural logarithm of the total number of microstates available to the system and not dlscrib com francois sears amp gerhard to the number of microstates in the most probable macrostate. The distribution of particles among energy levels is determined without the use of Lagradlscrib com francois sears amp gerhard
nge multiplier? and Stirling's approximation, by calculating the change in the total number ot microstates when a particle in a particular energy leveMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard unction is introduced and it is used to derive the thermodynamic properties of systems. The coverage is much the same as the earlier text except that it is based entirely on discrete levels. The chapter on fluctuations has been omitted.The number of problems at the end of each chapter has been expan dlscrib com francois sears amp gerhard ded. Some of the problems would become tedious if one did not have access to a small calculator. The International System (SI) has been adopted througdlscrib com francois sears amp gerhard
hout. Thus the units are those of the MKS system and arc written, for example, as J kilomole*1 K~l for specific heat capacity.The section on classicalMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard tatistical thermodynamics, but probably not both, unless only classical statistics are discussed, which can be done by using the development given in the sections on Bose-Einstein statistics and taking the limit that g, » Nị.Weappreciate the helpful comments of the reviewers of the manuscript, espec dlscrib com francois sears amp gerhard iallyIL. s. Lerner and c. F. Hooper, who also gave part of the manuscript a field test. One of us (GLS) wishes to thank his colleagues at Rensselaer fdlscrib com francois sears amp gerhard
or many helpful discussions. J. Aitken worked all the problems and checked the answers. Phyllis , Kallenburg patiently retyped many parts of the manusMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics, dlscrib com francois sears amp gerhard isms from teachers and students will be welcomed.Norwich, VermontF.w.s.Troy, New YorkG.L.S.27303IMUSLIM PHYSICS DEPARTMENTCADJAH MADA UNIVERSITYFrancis w. SearsProfessor Emeritus, Dartmouth CollegeGerhard L. SalingerAssociate Professor of Physics,Gọi ngay
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