139081 An ideal gas at $27^{\circ} \mathrm{C}$ is compressed adiabatically to $\frac{8}{27}$ of its original volume. The rise in temperature is $\left(\gamma=\frac{5}{3}\right)$

139082 The pressure $p$ for a gas is plotted against its absolute temperatures $T$ for two different volumes $V_{1}$ and $V_{2}$ where $V_{1}>V_{2}$.If $p$ is plotted on $\mathrm{y}$-axis and $\mathrm{T}$ on $\mathrm{x}$-axis, then

139083 An ideal gas is initially at temperature $T$ and volume $V$. Its volume is increased by $\Delta V$, due to an increase in temperature $\Delta T$, pressure remaining constant. The physical quantity $\delta=\frac{\Delta V}{V \Delta T}$ varies with temperature as

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139084 If the pressure of an ideal gas contained in a closed vessel is increased by $0.5 \%$ the increase in temperature is $2^{0} \mathrm{C}$. the initial temperature of the gas is:

139081 An ideal gas at $27^{\circ} \mathrm{C}$ is compressed adiabatically to $\frac{8}{27}$ of its original volume. The rise in temperature is $\left(\gamma=\frac{5}{3}\right)$

139082 The pressure $p$ for a gas is plotted against its absolute temperatures $T$ for two different volumes $V_{1}$ and $V_{2}$ where $V_{1}>V_{2}$.If $p$ is plotted on $\mathrm{y}$-axis and $\mathrm{T}$ on $\mathrm{x}$-axis, then

139083 An ideal gas is initially at temperature $T$ and volume $V$. Its volume is increased by $\Delta V$, due to an increase in temperature $\Delta T$, pressure remaining constant. The physical quantity $\delta=\frac{\Delta V}{V \Delta T}$ varies with temperature as

1

2

3

4

139084 If the pressure of an ideal gas contained in a closed vessel is increased by $0.5 \%$ the increase in temperature is $2^{0} \mathrm{C}$. the initial temperature of the gas is:

139081 An ideal gas at $27^{\circ} \mathrm{C}$ is compressed adiabatically to $\frac{8}{27}$ of its original volume. The rise in temperature is $\left(\gamma=\frac{5}{3}\right)$

139082 The pressure $p$ for a gas is plotted against its absolute temperatures $T$ for two different volumes $V_{1}$ and $V_{2}$ where $V_{1}>V_{2}$.If $p$ is plotted on $\mathrm{y}$-axis and $\mathrm{T}$ on $\mathrm{x}$-axis, then

139083 An ideal gas is initially at temperature $T$ and volume $V$. Its volume is increased by $\Delta V$, due to an increase in temperature $\Delta T$, pressure remaining constant. The physical quantity $\delta=\frac{\Delta V}{V \Delta T}$ varies with temperature as

1

2

3

4

139084 If the pressure of an ideal gas contained in a closed vessel is increased by $0.5 \%$ the increase in temperature is $2^{0} \mathrm{C}$. the initial temperature of the gas is:

139081 An ideal gas at $27^{\circ} \mathrm{C}$ is compressed adiabatically to $\frac{8}{27}$ of its original volume. The rise in temperature is $\left(\gamma=\frac{5}{3}\right)$

139082 The pressure $p$ for a gas is plotted against its absolute temperatures $T$ for two different volumes $V_{1}$ and $V_{2}$ where $V_{1}>V_{2}$.If $p$ is plotted on $\mathrm{y}$-axis and $\mathrm{T}$ on $\mathrm{x}$-axis, then

139083 An ideal gas is initially at temperature $T$ and volume $V$. Its volume is increased by $\Delta V$, due to an increase in temperature $\Delta T$, pressure remaining constant. The physical quantity $\delta=\frac{\Delta V}{V \Delta T}$ varies with temperature as

1

2

3

4

139084 If the pressure of an ideal gas contained in a closed vessel is increased by $0.5 \%$ the increase in temperature is $2^{0} \mathrm{C}$. the initial temperature of the gas is: