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Question: The work of \[146\,{\text{kJ}}\] is performed in order to compress one kilo mole of a gas adiabatica...

The work of 146kJ146\,{\text{kJ}} is performed in order to compress one kilo mole of a gas adiabatically and in this process the temperature of the gas increases by 7C7^\circ {\text{C}}. The gas is (R=8.3Jmol1K1)\left( {R = 8.3\,{\text{Jmo}}{{\text{l}}^{ - 1}}{{\text{K}}^{ - 1}}} \right) :
(A) Diatomic
(B) Triatomic
(C) A mixture of monoatomic and diatomic
(D) Monoatomic

Explanation

Solution

First of all, we will find an expression for energy in an adiabatic process which also contains a ratio of specific heats. We will substitute the required values and manipulate accordingly.

Complete step by step answer:
In the given, question we are supplied with the following data:
The total work done is 146kJ146\,{\text{kJ}} .
Number of moles (n)\left( n \right) is one kilo moles.
The increase in temperature is 7C7^\circ {\text{C}} .
Gas constant is given as R=8.3Jmol1K1R = 8.3\,{\text{Jmo}}{{\text{l}}^{ - 1}}{{\text{K}}^{ - 1}} .
We know,
1kJ=1000J1\,{\text{kJ}} = 1000\,{\text{J}}
So,
146kJ =146×103J =146000J 146\,{\text{kJ}} \\\ = {\text{146}} \times {\text{1}}{{\text{0}}^{\text{3}}}\,{\text{J}} \\\ = 146000\,{\text{J}} \\\
The temperature change can also be written as:
ΔT=7C\Delta T = 7^\circ {\text{C}}
We are asked to find out what is the nature of the gas. For this we need to find the ratio of the specific heats which is represented by a Greek symbol (γ)\left( \gamma \right). If the ratio of the specific heats comes out to be 1.61.6, then the gas is ideal monatomic and if the ratio of the specific heats comes out to be 1.41.4, then the gas is a diatomic one.
We have a formula which gives the work done in adiabatic process, as follows:
W=nR(T2T1)γ1W = \dfrac{{nR\left( {{T_2} - {T_1}} \right)}}{{\gamma - 1}} …… (1)
Where,
WW indicates the work done on the gas.
nn indicates the number of moles.
RR indicates gas constant.
T2{T_2} indicates final temperature.
T1{T_1} indicates initial temperature.
γ\gamma indicates ratio of specific heats.
Now, we substitute the required values in the equation (1) and we get:
W = \dfrac{{nR\Delta T}}{{\gamma - 1}} \\\
146000 = \dfrac{{1000 \times 8.3 \times 7}}{{\gamma - 1}} \\\
\gamma - 1 = \dfrac{{1000 \times 8.3 \times 7}}{{146000}} \\\
\gamma - 1 = 0.398 \\\
We now further simplify:
\Rightarrow \gamma - 1 = 0.398 \\\
\Rightarrow \gamma = 1 + 0.398 \\\
\Rightarrow \gamma = 1.398 \\\
\Rightarrow \gamma \sim 1.4 \\\
Since, the value of ratio of specific heats comes out to be 1.41.4, so the gas is a diatomic.
The correct option is (A).

Note: In the given problem, we need to take care of the units. It always needs to be in S.I units. To correctly answer this question, we need to remember the value of the ratio of the specific heats for different types of gases whether it be monatomic or diatomic. In an adiabatic system there is no transfer of heat or mass between the system and the surrounding.