The correct option is D Pressure in compartment I is 5P3.
At equilibrium position, the net force on the partition will be zero.
Hence, the gases in both the compartments are in mechanical equilibrium i.e pressure on both sides is the same.
Hence, option (a) is correct.
Given, P,2P are the initial pressures and V,2V are the initial volumes of compartment I and II.
Also, both the compartments are at the same temperature T.
From the ideal gas equation PV=nRT, we can write that no of moles in compartment I and II are:
n1=P1V1R T1=P VR T
n2=P2 V2R T2=(2P)(2V)RT=4PVRT
⇒n2=4n1
Since the walls are closed, the number of moles remains conserved.
At mechanical equlibrium, pressure becomes equal in both parts
i.e P′1=P′2
Using P′1V′1=n1R T1
P′2V′2=n2R T2
∵P′1=P′2 & T1=T2=T
[because the partition is conducting, both sides will remain in thermal equilibrium]
We can write that, V′1V′2=n1n2=14
⇒V′2=4V′1 .....(1)
Also, V′1+V′2=3V
[total volume of container remains constant]
Using equation (1), we get
⇒V′1+4V′1=3V
⇒V′1=35V and V′2=125V
Hence, (b) and (c) are correct.
In compartment (I):
P′1V′1=n1RT1
⇒P′1(3V5)=(PVRT)R(T)
⇒P′1=5PV3V=53P
Thus, options (a), (b), (c) and (d) are correct answers.