For an adiabatic expansion of an ideal gas, the fractional change in its pressure is equal to (where $\gamma$ is the ratio of specific heats):
$-\gamma \frac{ dV }{ V }$
$-\gamma \frac{ V }{ dV }$
$-\frac{1}{\gamma} \frac{ dV }{ V }$
$\frac{ d V }{ V }$
Consider a spherical shell of radius $R$ at temperature $T$. The black body radiation inside it can be considered as an ideal gas of photons with internal energy per unit volume$E=$ $\frac{U}{V} \propto {T^4}$ and pressure $P = \frac{1}{3}\left( {\frac{U}{V}} \right)$ If the shell now undergoes an adiabatic expansion the relation between $T$ and $R$ is
An ideal gas is expanded adiabatically at an initial temperature of $300 K$ so that its volume is doubled. The final temperature of the hydrogen gas is $(\gamma = 1.40)$
What is cyclic process ? Write note on it.
Two moles of an ideal monoatomic gas at ${27^o}C$ occupies a volume of $V.$ If the gas is expanded adiabatically to the volume $2V,$ then the work done by the gas will be ....... $J$ $[\gamma = 5/3,\,R = 8.31J/mol\,K]$
Match List$-I$ with List$-II$
List$-I$ | List$-II$ |
$(a)$ Isothermal | $(i)$ Pressure constant |
$(b)$ Isochoric | $(ii)$ Temperature constant |
$(c)$ Adiabatic | $(iii)$ Volume constant |
$(d)$ Isobaric | $(iv)$ Heat content is constant |
Choose the correct answer from the options given below