The current \( I \) is related to the drift velocity \( v_d \) by the equation:
\[
I = n e A v_d
\]
where:
- \( I \) is the current,
- \( n \) is the electron density,
- \( e \) is the charge of an electron (\( e = 1.6 \times 10^{-19} \, \text{C} \)),
- \( A \) is the cross-sectional area of the conductor,
- \( v_d \) is the drift velocity.
Step 1: Rearrange the equation to solve for \( v_d \).
We can rearrange the equation to solve for \( v_d \):
\[
v_d = \frac{I}{n e A}
\]
Step 2: Substitute the given values.
Substitute the given values into the equation:
\[
v_d = \frac{16}{(5 \times 10^{23}) \times (1.6 \times 10^{-19}) \times (1 \times 10^{-7})}
\]
Step 3: Calculate the drift velocity.
Now, calculate the value of \( v_d \):
\[
v_d = \frac{16}{(5 \times 10^{23}) \times (1.6 \times 10^{-19}) \times (1 \times 10^{-7})} = \frac{16}{8 \times 10^{7}} = 2 \times 10^{-7} \, \text{m/s}
\]
Step 4: Conclusion.
The drift velocity is:
\[
\boxed{2 \times 10^{-7} \, \text{m/s}}
\]