\(\frac{Mv^2}{7R}\)
\( \frac{Mv^2}{5R} \)
\(\frac{2Mv^2}{7R}\)
\(\frac{7Mv^2}{5R}\)
To solve this problem, let's analyze the situation step by step. We are given an ideal gas in a thermally insulated vessel, meaning no heat is exchanged with the environment. The vessel was moving with a speed \(\nu\) and is suddenly brought to rest. As a result, the kinetic energy of the vessel gets converted into the internal energy of the gas, leading to a rise in its temperature. Let's find the increase in temperature of the gas.
Given:
Firstly, the kinetic energy of the vessel before it stops is given by: \(\frac{1}{2}Mv^2\)
This kinetic energy is converted entirely into the internal energy of the gas due to the insulation of the vessel.
The change in internal energy, \(\Delta U\), for an ideal gas due to a temperature change \(\Delta T\) is given by: \(\Delta U = nC_V\Delta T\)
Where:
For a monoatomic gas, using \(C_V\), we have the relation: \(C_V = \frac{R}{\gamma - 1}\)
\(C_V\) for our gas will be: \(\frac{R}{1.4 - 1} = \frac{R}{0.4} = \frac{5R}{2}\)
Now, equating the kinetic energy to the change in internal energy: \(\frac{1}{2}Mv^2 = nC_V\Delta T\)
Since number of moles \(n\) can be represented as mass \(m\) divided by molar mass \(M\), i.e., \(n = \frac{m}{M}\), the equation becomes: \(\frac{1}{2}Mv^2 = \frac{m}{M} \cdot \frac{5R}{2} \cdot \Delta T\)
Thus, solving for \(\Delta T\): \(\Delta T = \frac{Mv^2}{5R}\)
So the temperature increase of the gas is given by \(\frac{Mv^2}{5R}\).
Therefore, the correct answer is: \(\frac{Mv^2}{5R}\), which matches option \(B\).