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Question: To an ideal trigonometric gas 800 Cal heat energy is given at constant pressure. If the vibrational ...

To an ideal trigonometric gas 800 Cal heat energy is given at constant pressure. If the vibrational mode is neglected, then energy used by gas in work done against surrounding is:
A. 200 Cal
B. 300 Cal
C. 400 Cal
D. 60 Cal

Explanation

Solution

Hint: - We must know the ideal gas equation for solving this question. Hence our ideal gas equation is PV = nRT. It can be established from the postulates of the kinetic theory of gases developed by Clerk Maxwell.

Complete answer:
According to the first law of thermodynamics,
ΔU=q+W\Delta U = q + W
W=ΔUqW = \Delta U - q ---(i)
Here ΔU is the change in the internal energy system and W is the work done by the system.
We know
W=PΔVW = P\Delta V----(ii)
From (i) & (ii)
PΔV=ΔUqP\Delta V = \Delta U - q
ΔU=q+PΔV\Delta U = q + P\Delta V---(iii)

Also, we know
ΔU=nCVΔT\Delta U = n{C_V}\Delta T
Initial internal energy of n moles of diatomic gas is
U1=n(62R)T1{U_1} = n\left( {\dfrac{6}{2}R} \right){T_1}=3nRT13nR{T_1}
Now, Internal energy of gas after heating is
U2=n(62R)T2{U_2} = n\left( {\dfrac{6}{2}R} \right){T_2}=3nRT23nR{T_2}
Therefore,
ΔU=U2U1\Delta U = U_2 - U_1
ΔU=3nRT23nRT1\Delta U = 3nR{T_2} - 3nR{T_1}
ΔU=3nR(T2T1)\Delta U = 3nR({T_2} - {T_1})
ΔU=3nRΔT\Delta U = 3nR\Delta T

We know that in ideal gas equation,
PV=nRTPV = nRT
PΔV=nRΔTP\Delta V = nR\Delta T
ΔU=3PΔV\Delta U = 3P\Delta V---(iv)

From (iii) and (iv)
3PΔV=q+PΔV3P\Delta V = q + P\Delta V
2PΔV=q2P\Delta V = q
PΔV=q2P\Delta V = \dfrac{q}{2}
W=8002W = \dfrac{{800}}{2}
W=400 Cal from (i)

Hence option C is correct i.e., work done is 400 Cal

Note: - An ideal gas is a theoretical gas composed of many randomly moving point particles that are not subjected to interparticle interactions. The ideal gas concept is useful because it obeys the ideal gas law, a simplified equation of state, and it is also amenable to analysis under statistical mechanics