Step 1: Find the Fermi wave vector first.
Instead of jumping straight to the energy formula, first find the radius of the Fermi sphere in k-space, $k_F$, which is fixed by how many electron states must fit inside it:
\[ k_F = (3\pi^2 n)^{1/3} \]
Step 2: Evaluate k_F numerically.
With $n = 8.3\times 10^{28}$ m$^{-3}$:
\[ 3\pi^2 n = 2.458\times 10^{30}\ \text{m}^{-3} \]
\[ k_F = (2.458\times 10^{30})^{1/3} = 1.350\times 10^{10}\ \text{m}^{-1} \]
Step 3: Get the Fermi energy from k_F.
A free electron with wave vector $k_F$ has energy $E_F = \hbar^2 k_F^2/(2m_e)$, treating the electron like a free particle carrying momentum $\hbar k_F$.
\[ E_F = \frac{(1.06\times 10^{-34})^2 \times (1.350\times 10^{10})^2}{2\times 9.10\times 10^{-31}} \]
\[ E_F = \frac{1.1236\times 10^{-68}\times 1.822\times 10^{20}}{1.82\times 10^{-30}} = 1.125\times 10^{-18}\ \text{J} \]
Step 4: Convert to electron volts.
$1$ eV $= 1.60\times 10^{-19}$ J, so:
\[ E_F = \frac{1.125\times 10^{-18}}{1.60\times 10^{-19}} = 7.03\ \text{eV} \]
Final Answer:
Rounded to one decimal place, the Fermi energy of copper is 7.0 eV.
\[ \boxed{E_F = 7.0\text{ eV}} \]