148508 During an experiment, an ideal gas is found to obey an additional law $V^{2}=$ constant. The gas is initially at temperature $T$ and volume. $V$. The temperature of the gas will be following, when it expands to a volume $2 \mathrm{~V}$ ?

148509 Two containers of equal volume contain the same gas at pressure $P_{1}$ and $P_{2}$ and absolute temperature $T_{1}$ and $T_{2}$ respectively. On joining the vessels the gas reaches a common pressure $P$ and common temperature $T$. The ratio $P / T$ is equal to

148510 2 moles of an ideal mono-atomic gas is carried from a state $\left(\mathrm{P}_{0}, \mathrm{~V}_{0}\right)$ to state $\left(2 \mathrm{P}_{0}, 2 \mathrm{~V}_{0}\right)$ along a straight line path in a $P-V$ diagram. The amount of heat absorbed by the gas in the process is given by

148512 If the coefficient of superficial expansion is $x$ times the coefficient of cubical expansion, then the value of $x$ is

148513 ' $m$ ' grams of a gas of molecular weight $M$ is flowing in an isolated tube velocity $v$. If the gas flow is suddenly stopped the rise in the temperature is : $(\gamma=$ ratio of specific heats, $\mathbf{R}=$ universal gas constant, $J=$ mechanical equivalent of heat).

148508 During an experiment, an ideal gas is found to obey an additional law $V^{2}=$ constant. The gas is initially at temperature $T$ and volume. $V$. The temperature of the gas will be following, when it expands to a volume $2 \mathrm{~V}$ ?

148509 Two containers of equal volume contain the same gas at pressure $P_{1}$ and $P_{2}$ and absolute temperature $T_{1}$ and $T_{2}$ respectively. On joining the vessels the gas reaches a common pressure $P$ and common temperature $T$. The ratio $P / T$ is equal to

148510 2 moles of an ideal mono-atomic gas is carried from a state $\left(\mathrm{P}_{0}, \mathrm{~V}_{0}\right)$ to state $\left(2 \mathrm{P}_{0}, 2 \mathrm{~V}_{0}\right)$ along a straight line path in a $P-V$ diagram. The amount of heat absorbed by the gas in the process is given by

148512 If the coefficient of superficial expansion is $x$ times the coefficient of cubical expansion, then the value of $x$ is

148513 ' $m$ ' grams of a gas of molecular weight $M$ is flowing in an isolated tube velocity $v$. If the gas flow is suddenly stopped the rise in the temperature is : $(\gamma=$ ratio of specific heats, $\mathbf{R}=$ universal gas constant, $J=$ mechanical equivalent of heat).

148508 During an experiment, an ideal gas is found to obey an additional law $V^{2}=$ constant. The gas is initially at temperature $T$ and volume. $V$. The temperature of the gas will be following, when it expands to a volume $2 \mathrm{~V}$ ?

148509 Two containers of equal volume contain the same gas at pressure $P_{1}$ and $P_{2}$ and absolute temperature $T_{1}$ and $T_{2}$ respectively. On joining the vessels the gas reaches a common pressure $P$ and common temperature $T$. The ratio $P / T$ is equal to

148510 2 moles of an ideal mono-atomic gas is carried from a state $\left(\mathrm{P}_{0}, \mathrm{~V}_{0}\right)$ to state $\left(2 \mathrm{P}_{0}, 2 \mathrm{~V}_{0}\right)$ along a straight line path in a $P-V$ diagram. The amount of heat absorbed by the gas in the process is given by

148512 If the coefficient of superficial expansion is $x$ times the coefficient of cubical expansion, then the value of $x$ is

148513 ' $m$ ' grams of a gas of molecular weight $M$ is flowing in an isolated tube velocity $v$. If the gas flow is suddenly stopped the rise in the temperature is : $(\gamma=$ ratio of specific heats, $\mathbf{R}=$ universal gas constant, $J=$ mechanical equivalent of heat).

148508 During an experiment, an ideal gas is found to obey an additional law $V^{2}=$ constant. The gas is initially at temperature $T$ and volume. $V$. The temperature of the gas will be following, when it expands to a volume $2 \mathrm{~V}$ ?

148509 Two containers of equal volume contain the same gas at pressure $P_{1}$ and $P_{2}$ and absolute temperature $T_{1}$ and $T_{2}$ respectively. On joining the vessels the gas reaches a common pressure $P$ and common temperature $T$. The ratio $P / T$ is equal to

148510 2 moles of an ideal mono-atomic gas is carried from a state $\left(\mathrm{P}_{0}, \mathrm{~V}_{0}\right)$ to state $\left(2 \mathrm{P}_{0}, 2 \mathrm{~V}_{0}\right)$ along a straight line path in a $P-V$ diagram. The amount of heat absorbed by the gas in the process is given by

148512 If the coefficient of superficial expansion is $x$ times the coefficient of cubical expansion, then the value of $x$ is

148513 ' $m$ ' grams of a gas of molecular weight $M$ is flowing in an isolated tube velocity $v$. If the gas flow is suddenly stopped the rise in the temperature is : $(\gamma=$ ratio of specific heats, $\mathbf{R}=$ universal gas constant, $J=$ mechanical equivalent of heat).

148508 During an experiment, an ideal gas is found to obey an additional law $V^{2}=$ constant. The gas is initially at temperature $T$ and volume. $V$. The temperature of the gas will be following, when it expands to a volume $2 \mathrm{~V}$ ?

148509 Two containers of equal volume contain the same gas at pressure $P_{1}$ and $P_{2}$ and absolute temperature $T_{1}$ and $T_{2}$ respectively. On joining the vessels the gas reaches a common pressure $P$ and common temperature $T$. The ratio $P / T$ is equal to

148510 2 moles of an ideal mono-atomic gas is carried from a state $\left(\mathrm{P}_{0}, \mathrm{~V}_{0}\right)$ to state $\left(2 \mathrm{P}_{0}, 2 \mathrm{~V}_{0}\right)$ along a straight line path in a $P-V$ diagram. The amount of heat absorbed by the gas in the process is given by

148512 If the coefficient of superficial expansion is $x$ times the coefficient of cubical expansion, then the value of $x$ is

148513 ' $m$ ' grams of a gas of molecular weight $M$ is flowing in an isolated tube velocity $v$. If the gas flow is suddenly stopped the rise in the temperature is : $(\gamma=$ ratio of specific heats, $\mathbf{R}=$ universal gas constant, $J=$ mechanical equivalent of heat).