To solve the given problem about the average thermal energy of a mono-atomic gas, we will use the concept of the kinetic theory of gases.
The average thermal energy for a mono-atomic ideal gas can be derived from the equipartition theorem, which states that each degree of freedom contributes \(\frac{1}{2}k_B T\) to the energy. Here, \(k_B\) is the Boltzmann constant, and \(T\) is the absolute temperature.
For a mono-atomic gas, the molecules are in three-dimensional translational motion, which means it has three degrees of freedom. Therefore, the average thermal energy \(E\) for a mono-atomic gas is calculated as follows:
The energy contribution from each degree of freedom is:
\(E = \frac{1}{2}k_B T \times \text{number of degrees of freedom}\)
Substituting for three degrees of freedom, we have:
\(E = \frac{1}{2}k_B T \times 3 = \frac{3}{2}k_B T\)
Thus, the average thermal energy for a mono-atomic gas is \(\frac{3}{2}k_BT\).
Now, we'll verify and rule out the other options:
Hence, the correct answer is \(\frac{3}{2}k_BT\), corresponding to option 2, which represents the average thermal energy for a mono-atomic gas.