LECTURE  1

 

INTRODUCTION

 

THERMODYNAMICS

 

Thermodynamics is the science that deals with heat and work and those properties of substance that bear a relation to heat and work.

Thermodynamics is the study of the patterns of energy change. Most of this course will be concerned with understanding the patterns of energy change.

More specifically, thermodynamics deals with (a) energy conversion and (b) the direction of change.

Basis of thermodynamics is experimental observation. In that sense it is an empirical science. The principles of thermodynamics are summarized in the form of four laws known as zeroth, first, second, and the third laws of thermodynamics.

 

The zeroth law of thermodynamics deals with thermal equilibrium and provides a means of measuring temperature.

 

The first law of thermodynamics deals with the conservation of energy and introduces the concept of internal energy.

 

 

The second law of thermodynamics dictates the limits on the conversion of heat into work and provides the yard stick to measure the performance of various processes. It also tells whether a particular process is feasible or not and specifies the direction in which a process will proceed. As a consequence it also introduces the concept of entropy.

 

The third law defines the absolute zero of entropy.

 

 

 

 

 

Macroscopic and Microscopic Approaches:

 

Microscopic approach uses the statistical considerations and probability theory, where we deal with “average” for all particles under consideration. This is the approach used in the disciplines known as kinetic theory and statistical mechanics.

 

In the macroscopic point of view, of classical thermodynamics, one is concerned with the time-averaged influence of many molecules that can be perceived by the senses and measured by the instruments.

The pressure exerted by a gas is an example of this. It results from the change in momentum of the molecules, as they collide with the wall. Here we are not concerned with the actions of individual molecules but with the time-averaged force on a given area that can be measured by a pressure gage.

 

From the macroscopic point of view, we are always concerned with volumes that are very large compared to molecular dimensions, and therefore a system (to be defined next) contains many molecules, and this is called continuum.

 

 

The concept of continuum loses validity when the mean free path of molecules approaches the order of typical system dimensions.

 

 

 

 

 

 

 

Marks distribution

(Out of 200)

 

 

 

1st Mid semester exam:     35

2nd Mid semester exam:    35

End semester exam:        90

Quizzes:                  30

Tutors:                        10

 

 

 

 

All tutorial problems will be from “An introduction to thermodynamics” by Y.V.C. Rao.