Physics > First Law of Thermodynamics > 4.0 Different thermodynamic processes
First Law of Thermodynamics
1.0 Introduction
2.0 Three important terms in first law of thermodynamics.
3.0 First law of thermodynamics
4.0 Different thermodynamic processes
4.1 Isobaric Process:
4.2 Isochoric process
4.3 Isothermal process
4.5 Adiabatic process
4.6 Polytropic process
5.0 Graphs
6.0 Efficiency of cyclic process
7.0 Heat engine
8.0 Refrigerator
4.3 Isothermal process
4.2 Isochoric process
4.3 Isothermal process
4.5 Adiabatic process
4.6 Polytropic process
An isothermal process is a constant temperature process. In an isothermal process
$T$= constant or $\Delta T$=0
$P \propto \frac{1}{V}$ or $PV$= constant .
So $P-V$ graph is a rectangular hyperbola with $${P_i}{V_i} = {P_f}{V_f}$$
As $T$= constant, hence U=constant for an ideal gas, because $U$ is a function of $T$ only.$$\Delta U = 0$$$$\therefore Q = W$$
Work done in isothermal process
$$\begin{equation} \begin{aligned} W = \int\limits_{{V_i}}^{{V_f}} {PdV} \\ = \int\limits_{{V_i}}^{{V_f}} {\left( {\frac{{nRT}}{V}} \right)} dV\left ( {as\ P = \frac{{nRT}}{V}} \right) \\ = nRT\int\limits_{{V_i}}^{{V_f}} {\frac{{dV}}{V}} \left( {as\ T = constant} \right) \\ = nRT\ln \left( {\frac{{{V_f}}}{{{V_i}}}} \right) \\ = nRT\ln \left( {\frac{{{P_i}}}{{{P_f}}}} \right)\left( {as\ {P_i}{V_i} = {P_f}{V_f}} \right) \\\end{aligned} \end{equation} $$
Note:
For a process to be isothermal, any heat flow into or out of the system must occur slowly enough, so that thermal equilibrium is maintained.
Question 13. An ideal gas expands isothermally along $AB$ and does $700 J$ of work.
(a) How much heat does the gas exchange along $AB$?
(b) The then expands adiabatically along $BC$ and does $400 J$ of work. When the gas returns to $A$ along $CA$, it exhausts $100 J$ of heat to its surroundings. How much work is done on the gas along this path?
Solution:
(a) $AB$ is an isothermal process. Hence,$$\begin{equation} \begin{aligned} \Delta {U_{AB}} = 0 \\ {Q_{AB}} = {W_{AB}} = 700\,J \\\end{aligned} \end{equation} $$
(b) BC is an adiabatic process. Hence$$\begin{equation} \begin{aligned} {Q_{BC}} = 0 \\ {W_{BC}} = 400\,J \\ \Delta {U_{BC}} = - {W_{BC}} = - 400\,J \\\end{aligned} \end{equation} $$ABC is a cyclic process and internal energy is a state function. Therefore,$${\left( {\Delta U} \right)_{whole\,\,cycle}} = 0 = \Delta {U_{AB}} + \Delta {U_{BC}} + \Delta {U_{CA}}$$and from first law of thermodynamics,$${Q_{AB}} + {Q_{BC}} + {Q_{CA}} = {W_{AB}} + {W_{BC}} + {W_{CA}}$$Substituting the values,$$\begin{equation} \begin{aligned} 700 + 0 - 100 = 700 + 400 + \Delta {W_{CA}} \\ \Delta {W_{CA}} = - 500\;J \\\end{aligned} \end{equation} $$Negative sign implies that work is done on the gas.
Table shows different values in different processes.
Process | $Q$ ($J$) | $W$ ( $J$) | $\Delta U$($J$) |
$AB$ | $700$ | $700$ | $0$ |
$BC$ | $0$ | $400$ | $-400$ |
$CA$ | $-100$ | $-500$ | $400$ |
For complete cycle | $600$ | $600$ | $0$ |