(B) For an ideal gas,the adiabatic elasticity $E_{\phi}$ is given by $E_{\phi} = \gamma P$,where $\gamma$ is the adiabatic index and $P$ is the pressu

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(B) For an ideal gas,the adiabatic elasticity $E_{\phi}$ is given by $E_{\phi} = \gamma P$,where $\gamma$ is the adiabatic index and $P$ is the pressure.The isothermal elasticity $E_{\theta}$ is given by $E_{\theta} = P$.The ratio of adiabatic elasticity to isothermal elasticity is $\frac{E_{\phi}}{E_{\theta}} = \frac{\gamma P}{P} = \gamma$.Since $\gamma = \frac{C_p}{C_v}$,the ratio is $\frac{C_p}{C_v}$.

Class 11 Physics Kinetic Theory of Gases Molar Specific Heat of gas and relation between them (Mayer's formula)

Easy

The specific heat at constant pressure and at constant volume for an ideal gas are $C_p$ and $C_v$,and its adiabatic and isothermal elasticities are $E_{\phi}$ and $E_{\theta}$ respectively. The ratio of $E_{\phi}$ to $E_{\theta}$ is

A
$C_v/C_p$
B
$C_p/C_v$
C
$C_p C_v$
D
$1/(C_p C_v)$

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Kinetic Theory of Gases

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Molar Specific Heat of gas and relation between them (Mayer's formula)

Molar specific heat at constant pressure $C_p$ is related to internal energy $U$ and absolute temperature $T$ as $C_p$ is equal to

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For a gas if $\gamma = 1.4$,then atomicity,${C_p}$ and ${C_v}$ of the gas are respectively

Medium

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An ideal mono-atomic gas of given mass is heated at constant pressure. In this process,the fraction of supplied heat energy used for the increase of the internal energy of the gas is

MediumWBJEE 2013

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Obtain the value of $\frac{C_P}{C_V}$ for a non-linear triatomic gas.

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For hydrogen gas,$C_P - C_V = a$,and for oxygen gas,$C_P - C_V = b$. The relationship between $a$ and $b$ is given by: (where $C_P$ and $C_V$ are molar specific heats at constant pressure and constant volume,respectively.)

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The specific heat at constant pressure and at constant volume for an ideal gas are $C_p$ and $C_v$,and its adiabatic and isothermal elasticities are $E_{\phi}$ and $E_{\theta}$ respectively. The ratio of $E_{\phi}$ to $E_{\theta}$ is

Similar Questions

Molar specific heat at constant pressure $C_p$ is related to internal energy $U$ and absolute temperature $T$ as $C_p$ is equal to

For a gas if $\gamma = 1.4$,then atomicity,${C_p}$ and ${C_v}$ of the gas are respectively

An ideal mono-atomic gas of given mass is heated at constant pressure. In this process,the fraction of supplied heat energy used for the increase of the internal energy of the gas is

Obtain the value of $\frac{C_P}{C_V}$ for a non-linear triatomic gas.

For hydrogen gas,$C_P - C_V = a$,and for oxygen gas,$C_P - C_V = b$. The relationship between $a$ and $b$ is given by: (where $C_P$ and $C_V$ are molar specific heats at constant pressure and constant volume,respectively.)

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