The acceleration of a block descending a frictionless inclined plane is determined by:
\[
a = g \sin \theta
\]
In this equation:
- \( a \) represents the block's acceleration.
- \( g \) denotes the acceleration due to gravity.
- \( \theta \) signifies the angle of the plane's inclination.
Given that the block's acceleration is \( \frac{g}{8} \), we have:
\[
\frac{g}{8} = g \sin \theta
\]
Dividing both sides by \( g \):
\[
\frac{1}{8} = \sin \theta
\]
Consequently, the angle \( \theta \) is:
\[
\theta = \sin^{-1} \left( \frac{1}{8} \right)
\]
Therefore, the angle of inclination \( \theta \) is equivalent to \( \tan^{-1} \left( \frac{1}{8} \right) \), corresponding to option (a).