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Question: One kg of a diatomic gas is at a pressure of \[8 \times {10^4}\,{\text{N/}}{{\text{m}}^2}\]. The den...

One kg of a diatomic gas is at a pressure of 8×104N/m28 \times {10^4}\,{\text{N/}}{{\text{m}}^2}. The density of the gas is 4kg/m34\,{\text{kg/}}{{\text{m}}^3}. The energy of the gas due to its thermal motion will be
A. 3×104J3 \times {10^4}\,{\text{J}}
B. 5×104J5 \times {10^4}\,{\text{J}}
C. 6×104J6 \times {10^4}\,{\text{J}}
D. 7×104J7 \times {10^4}\,{\text{J}}

Explanation

Solution

Use the formula for the thermal energy of the diatomic gas. Also use the ideal gas equation. Determine the volume of the gas using the formula for density of the gas. Derive the relation between thermal energy of gas, volume of gas and pressure of the gas.

Formula used:
The thermal energy UU of a diatomic gas is given by
U=52nRTU = \dfrac{5}{2}nRT …… (1)
Here, nn is the number of moles of gas, RR is the gas constant and TT is the temperature of the gas.
The ideal gas law is given by
PV=nRTPV = nRT …… (2)
Here, PP is the pressure of gas, VV is the volume of the gas, nn is the number of moles of gas, RR is the gas constant and TT is the temperature of the gas.
The density ρ\rho is given by
ρ=MV\rho = \dfrac{M}{V} …… (3)
Here, MM is the mass and VV is the volume.

Complete step by step answer:
One kg of a diatomic gas is at a pressure of 8×104N/m28 \times {10^4}\,{\text{N/}}{{\text{m}}^2}. The density of the gas is 4kg/m34\,{\text{kg/}}{{\text{m}}^3}.
M=1kgM = 1\,{\text{kg}}
P=8×104N/m2P = 8 \times {10^4}\,{\text{N/}}{{\text{m}}^2}
ρ=4kg/m3\rho = 4\,{\text{kg/}}{{\text{m}}^3}
Determine the volume of the diatomic gas.
Rearrange equation (3) for volume VV of the gas.
V=MρV = \dfrac{M}{\rho }
Substitute 1kg1\,{\text{kg}} for MM and 4kg/m34\,{\text{kg/}}{{\text{m}}^3} for ρ\rho in the above equation.
V=1kg4kg/m3V = \dfrac{{1\,{\text{kg}}}}{{4\,{\text{kg/}}{{\text{m}}^3}}}
V=14m3\Rightarrow V = \dfrac{1}{4}\,{{\text{m}}^3}
Hence, the volume of the gas is 14m3\dfrac{1}{4}\,{{\text{m}}^3}.
Determine the energy of the diatomic gas.
Substitute PVPV for nRTnRT in equation (1).
U=52PVU = \dfrac{5}{2}PV
Substitute 8×104N/m28 \times {10^4}\,{\text{N/}}{{\text{m}}^2} for PP and 14m3\dfrac{1}{4}\,{{\text{m}}^3} for VV in the above equation.
U=52(8×104N/m2)(14m3)U = \dfrac{5}{2}\left( {8 \times {{10}^4}\,{\text{N/}}{{\text{m}}^2}} \right)\left( {\dfrac{1}{4}\,{{\text{m}}^3}} \right)
U=5×104J\Rightarrow U = 5 \times {10^4}\,{\text{J}}

Therefore, the energy of the gas due to its thermal motion is 5×104J5 \times {10^4}\,{\text{J}}.

So, the correct answer is “Option B”.

Note:
The thermal energy for the monatomic, diatomic, triatomic gases is not the same. These equations for thermal energy are different for different gases and depend on the number of atoms in the gas molecule. These equations vary with the number of atoms in the molecule because gases with different atoms have different degrees of freedom.