The electrical conductivity \( \sigma \) of an intrinsic semiconductor is given by the relation:
\[
\sigma = A \cdot e^{-\frac{E_g}{2k_B T}}
\]
where:
- \( E_g \) is the band gap energy,
- \( k_B \) is the Boltzmann constant,
- \( T \) is the temperature,
- \( A \) is a constant that depends on the material (and cancels out in the ratio).
We are given the conductivity at two different temperatures, 300 K and 500 K. To find the band gap \( E_g \), we use the ratio of conductivities at two temperatures:
\[
\frac{\sigma_2}{\sigma_1} = \frac{e^{-\frac{E_g}{2k_B T_2}}}{e^{-\frac{E_g}{2k_B T_1}}}
\]
Substituting the given values, we have:
\[
\frac{300}{100} = \frac{e^{-\frac{E_g}{2 \times 8.6 \times 10^{-5} \times 500}}}{e^{-\frac{E_g}{2 \times 8.6 \times 10^{-5} \times 300}}}
\]
Simplifying the expression:
\[
3 = e^{\frac{E_g}{2 \times 8.6 \times 10^{-5}} \left(\frac{1}{300} - \frac{1}{500}\right)}
\]
After solving for \( E_g \), we find:
\[
E_g \approx 0.14 \, {eV}
\]
Thus, the band gap is between 0.13 eV and 0.15 eV.
Answer: 0.13 to 0.15 eV.