148249 Two identical containers $A$ and $B$ with frictionless pistons contain the same ideal gas at the same temperature and the same volume $V$. The mass of the gas in $A$ is $M_{A}$ and that in $B$ is $M_{B}$. The gas in each container is now allowed to expand isothermally to the same final volume $2 \mathrm{~V}$. The changes in the pressure in $A$ and $B$ are to be found $\Delta p$ and $1.5 \Delta p$ respectively, then relation for masses will be
148249 Two identical containers $A$ and $B$ with frictionless pistons contain the same ideal gas at the same temperature and the same volume $V$. The mass of the gas in $A$ is $M_{A}$ and that in $B$ is $M_{B}$. The gas in each container is now allowed to expand isothermally to the same final volume $2 \mathrm{~V}$. The changes in the pressure in $A$ and $B$ are to be found $\Delta p$ and $1.5 \Delta p$ respectively, then relation for masses will be
148249 Two identical containers $A$ and $B$ with frictionless pistons contain the same ideal gas at the same temperature and the same volume $V$. The mass of the gas in $A$ is $M_{A}$ and that in $B$ is $M_{B}$. The gas in each container is now allowed to expand isothermally to the same final volume $2 \mathrm{~V}$. The changes in the pressure in $A$ and $B$ are to be found $\Delta p$ and $1.5 \Delta p$ respectively, then relation for masses will be
148249 Two identical containers $A$ and $B$ with frictionless pistons contain the same ideal gas at the same temperature and the same volume $V$. The mass of the gas in $A$ is $M_{A}$ and that in $B$ is $M_{B}$. The gas in each container is now allowed to expand isothermally to the same final volume $2 \mathrm{~V}$. The changes in the pressure in $A$ and $B$ are to be found $\Delta p$ and $1.5 \Delta p$ respectively, then relation for masses will be