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Question: A box containing N molecules of a perfect gas at temperature \(T_{1}\) and pressure \(P_{1}\). The n...

A box containing N molecules of a perfect gas at temperature T1T_{1} and pressure P1P_{1}. The number of molecules in the box is doubled keeping the total kinetic energy of the gas same as before. If the new pressure is P2P_{2} and temperature T2T_{2}, then

A

P2=P1P_{2} = P_{1}, T2=T1T_{2} = T_{1}

B

P2=P1P_{2} = P_{1}, T2=T12T_{2} = \frac{T_{1}}{2}

C

P2=2P1P_{2} = 2P_{1}, T2=T1T_{2} = T_{1}

D

P2=2P1P_{2} = 2P_{1}, T2=T12T_{2} = \frac{T_{1}}{2}

Answer

P2=P1P_{2} = P_{1}, T2=T12T_{2} = \frac{T_{1}}{2}

Explanation

Solution

Kinetic energy of N molecule of gas E=32NkTE = \frac{3}{2}NkT

Initially E1=32N1kT1E_{1} = \frac{3}{2}N_{1}kT_{1} and finally E2=32N2kT2E_{2} = \frac{3}{2}N_{2}kT_{2}

But according to problem E1=E2E_{1} = E_{2} and N2=2N1N_{2} = 2N_{1}

32N1kT1=32(2N1)kT2\frac{3}{2}N_{1}kT_{1} = \frac{3}{2}(2N_{1})kT_{2}T2=T12T_{2} = \frac{T_{1}}{2}

Since the kinetic energy constant 32N1kT1=32N2kT2\frac{3}{2}N_{1}kT_{1} = \frac{3}{2}N_{2}kT_{2}

N1T1=N2T2N_{1}T_{1} = N_{2}T_{2}NT = constant

From ideal gas equation of N molecule PV=NkTPV = NkT

P1V1=P2V2P_{1}V_{1} = P_{2}V_{2}P1=P2P_{1} = P_{2}

[As V1=V2\lbrack\text{As }V_{1} = V_{2} and NT = constant]