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T HERMODYNAMICS · Part 3

Chapter 11: THERMODYNAMICS · PHYSICS

motion of the bullet, not to the motion of the bullet as a whole. . THERMAL EQUILIBRIUM Equilibrium in mechanics means that the net external force and torque on a system are zero. The term ‘equilibrium’ in thermodynamics appears in a different context : we say the state of a system is an equilibrium state if the macroscopic variables that characterise the system do not change in time.

For example, a gas inside a closed rigid container, completely insulated from its surroundings, with fixed values of pressure, volume, temperature, mass and composition that do not change with time, is in a state of thermodynamic equilibrium. Fig. . (a) Systems A and B (two gases) separated by an adiabatic wall – an insulating wall that does not allow flow of heat.

(b) The same systems A and B separated by a diathermic wall – a conducting wall that allows heat to flow from one to another. In this case, thermal equilibrium is attained in due course . In general, whether or not a system is in a state of equilibrium depends on the surroundings and the nature of the wall that separates the system from the surroundings. Consider two gases A and B occupying two different containers.

We know experimentally that pressure and volume of a given mass of gas can be chosen to be its two independent variables. Let the pressure and volume of the gases be ( P A , V A ) and ( P B , V B ) respectively. Suppose first that the two systems are put in proximity but are separated by an (a) (b) * Thermodynamics may also involve other variables that are not so obvious to our senses e.g. entropy, enthalpy, etc., and they are all macroscopic variables.

However, a thermodynamic state is specified by five state variables viz., pressure, volume, temperature, internal energy and entropy. Entropy is a measure of disorderness in the system. Enthalpy is a measure of total heat content of the system. adiabatic wall – an insulating wall (can be movable) that does not allow flow of energy

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