We use the diode current equation:
\[
I = I_s \left( e^{\frac{V}{nV_T}} - 1 \right),
\]
where:
- \( I_s = 10 \, \mu A \) is the reverse saturation current,
- \( V \) is the forward voltage,
- \( n \) is the ideality factor (for an ideal diode, \( n = 1 \)),
- \( V_T = \frac{k_B T}{q} \) is the thermal voltage.
For a temperature of 300 K, the thermal voltage is:
\[
V_T = \frac{1.38 \times 10^{-23} \times 300}{1.6 \times 10^{-19}} = 0.02585 \, {V}.
\]
Now, we solve for \( V \) when the forward current \( I = 100 \, {mA} \):
\[
100 \times 10^{-3} = 10 \times 10^{-6} \left( e^{\frac{V}{0.02585}} - 1 \right).
\]
Simplifying:
\[
10^{-4} = 10^{-5} \left( e^{\frac{V}{0.02585}} - 1 \right),
\]
\[
10 = e^{\frac{V}{0.02585}} - 1,
\]
\[
e^{\frac{V}{0.02585}} = 11,
\]
\[
\frac{V}{0.02585} = \ln(11),
\]
\[
V = 0.02585 \times \ln(11) \approx 0.23 \, {V}.
\]
Thus, the voltage required is 0.23 V.