By Robert J. Hardy

This textbook brings jointly the basics of the macroscopic and microscopic elements of thermal physics via proposing thermodynamics and statistical mechanics as complementary theories in response to small numbers of postulates. The e-book is designed to provide the trainer flexibility in structuring classes for complicated undergraduates and/or starting graduate scholars and is written at the precept sturdy textual content must also be a very good reference.

The presentation of thermodynamics follows the good judgment of Clausius and Kelvin whereas referring to the options concerned to general phenomena and the fashionable student's wisdom of the atomic nature of subject. one other precise point of the booklet is the therapy of the math concerned. the fundamental mathematical thoughts are in brief reviewed sooner than utilizing them, and the similarity of the math to that hired in different fields of physics is emphasized.

The textual content supplies extensive remedies of low density gases, harmonic solids, magnetic and dielectric fabrics, part transitions, and the concept that of entropy. The microcanonical, canonical, and grand canonical ensembles of statistical mechanics are derived and used because the start line for the research of fluctuations, blackbody radiation, the Maxwell distribution, Fermi-Dirac data, Bose-Einstein condensation, and the statistical foundation of computing device simulations.

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**Additional resources for Thermodynamics and Statistical Mechanics: An Integrated Approach**

**Example text**

Tex V3 - 03/14/2014 Properties and Partial Derivatives 37 Using the chain rule to differentiate both sides of this with respect to y with z fixed gives ( )( ) ????y(x, z) ????x(y, z) ????y ????x =1 or = 1. 43) ????x ????y ????x z ????y z This relationship is easily visualized. Choose a value of z and hold it fixed. Plot y(x, z) as a line on a graph with the y-axis pointing up and the x-axis pointing to the right. Rotate the graph 90∘ counter-clockwise, so the x-axis points up and the y-axis points to the left.

Since the value of x is x, it follows that x = x(y, z(x, y)). M. M. 43), we find that ( )( )( ) ????y ????x ????z = −1. 50) The minus sign may be unexpected. The symbols ????x, ????y, and ????z can sometimes be treated as small displacements that can be cancelled between numerator and denominator. Such cancellations are not justified here, because the symbol in the numerator refers to a different displacement than the corresponding symbol in the denominator. The notation specifies that the ????y in the numerator represents a displacement in the x direction, while the ????y in the denominator represents a displacement with x fixed.

The actual source of energy that caused the temperature to increase was the work done by the external force. Notice that, as the frictional force on the stationary block is equal in magnitude but opposite in direction to the frictional force on the stationary block, the work done on the stationary block (μND) is the negative of the work done on the moving block (−μND). Before leaving the subject of dissipative forces, it should be pointed out that processes that involve dissipative forces are always irreversible.