(N/A) As per the assumption made in the statement,since the $He$ atom behaves like a hydrogen-like atom (where electron-electron repulsion is ignored),we can apply Bohr's atomic model to the $He$ atom.
The energy of an electron in an orbit is given by:
$E_{n} = -\frac{m Z^{2} e^{4}}{8 \epsilon_{0}^{2} n^{2} h^{2}}$
This can be simplified as:
$E_{n} = -13.6 \frac{Z^{2}}{n^{2}} \text{ eV}$
For a $He$ atom,the atomic number $Z = 2$. For the ground state,the principal quantum number $n = 1$.
Substituting these values:
$E_{1} = -13.6 \times \frac{(2)^{2}}{(1)^{2}} \text{ eV}$
$E_{1} = -13.6 \times 4 \text{ eV}$
$E_{1} = -54.4 \text{ eV}$
Since there are two electrons in the $He$ atom and we assume no repulsion between them,the total ground state energy of the $He$ atom is the sum of the energies of both electrons:
$E_{\text{total}} = 2 \times E_{1} = 2 \times (-54.4 \text{ eV}) = -108.8 \text{ eV}$.