148297 An ideal gas at pressure $p$ is adiabatically compressed so that its density becomes $n$ times the initial value. The final pressure of the gas will be $\left(\gamma=\frac{C_{p}}{C_{v}}\right)$

148298 At constant temperature on increasing the pressure of a gas by $10 \%$, its volume will decrease by-

148299 Certain amount of an ideal gas of molecular mass $M$ is contained in a closed vessel. If the vessel is moving with a constant velocity $v$, then the rise in temperature of the gas when the vessel is suddenly stopped will be
$\left(\right.$ Take $\left.\gamma=\frac{\mathbf{C}_{\mathbf{P}}}{\mathbf{C}_{\mathrm{V}}}\right)$

148300 At $27^{\circ} \mathrm{C}$ a gas suddenly compressed such that its pressure becomes 1/8th of original pressure, The temperature of the gas will be $(\gamma=5 / 3)$

148297 An ideal gas at pressure $p$ is adiabatically compressed so that its density becomes $n$ times the initial value. The final pressure of the gas will be $\left(\gamma=\frac{C_{p}}{C_{v}}\right)$

148298 At constant temperature on increasing the pressure of a gas by $10 \%$, its volume will decrease by-

148299 Certain amount of an ideal gas of molecular mass $M$ is contained in a closed vessel. If the vessel is moving with a constant velocity $v$, then the rise in temperature of the gas when the vessel is suddenly stopped will be
$\left(\right.$ Take $\left.\gamma=\frac{\mathbf{C}_{\mathbf{P}}}{\mathbf{C}_{\mathrm{V}}}\right)$

148300 At $27^{\circ} \mathrm{C}$ a gas suddenly compressed such that its pressure becomes 1/8th of original pressure, The temperature of the gas will be $(\gamma=5 / 3)$

148297 An ideal gas at pressure $p$ is adiabatically compressed so that its density becomes $n$ times the initial value. The final pressure of the gas will be $\left(\gamma=\frac{C_{p}}{C_{v}}\right)$

148298 At constant temperature on increasing the pressure of a gas by $10 \%$, its volume will decrease by-

148299 Certain amount of an ideal gas of molecular mass $M$ is contained in a closed vessel. If the vessel is moving with a constant velocity $v$, then the rise in temperature of the gas when the vessel is suddenly stopped will be
$\left(\right.$ Take $\left.\gamma=\frac{\mathbf{C}_{\mathbf{P}}}{\mathbf{C}_{\mathrm{V}}}\right)$

148300 At $27^{\circ} \mathrm{C}$ a gas suddenly compressed such that its pressure becomes 1/8th of original pressure, The temperature of the gas will be $(\gamma=5 / 3)$

148297 An ideal gas at pressure $p$ is adiabatically compressed so that its density becomes $n$ times the initial value. The final pressure of the gas will be $\left(\gamma=\frac{C_{p}}{C_{v}}\right)$

148298 At constant temperature on increasing the pressure of a gas by $10 \%$, its volume will decrease by-

148299 Certain amount of an ideal gas of molecular mass $M$ is contained in a closed vessel. If the vessel is moving with a constant velocity $v$, then the rise in temperature of the gas when the vessel is suddenly stopped will be
$\left(\right.$ Take $\left.\gamma=\frac{\mathbf{C}_{\mathbf{P}}}{\mathbf{C}_{\mathrm{V}}}\right)$

148300 At $27^{\circ} \mathrm{C}$ a gas suddenly compressed such that its pressure becomes 1/8th of original pressure, The temperature of the gas will be $(\gamma=5 / 3)$