In the context of the hydrogen atom, the total energy \( E \) of an electron in a certain state is the sum of its kinetic energy \( T \) and potential energy \( V \). For the ground state, the total energy given is \( E = -13.6 \, \text{eV} \).
The potential energy \( V \) of the electron in this state is calculated by using the relationship between total energy and potential energy in a Coulomb potential. The potential energy is twice the magnitude but opposite in sign to the total energy, as per the Virial Theorem, which states:
\( E = T + V \) and \( T = -\frac{1}{2}V \).
Substituting for \( T \) gives:
\( E = -\frac{1}{2}V + V \) which simplifies to \( E = \frac{1}{2}V \).
Thus, \( V = 2E \).
With \( E = -13.6 \, \text{eV} \), we find:
\( V = 2 \times (-13.6 \, \text{eV}) = -27.2 \, \text{eV} \).
Therefore, the potential energy of the electron in the ground state of the hydrogen atom is \(-27.2 \, \text{eV}\).
Heat energy absorbed by a system going through the cyclic process shown in the figure is: