



To determine the correct sketch that represents the group velocity \(v_g\) for the given dispersion relation, we begin by understanding the relationship and deriving the group velocity expression.
The given dispersion relation is:
\(\omega = \sqrt{k^2 + a^2}\)
Here, \(\omega\) is the angular frequency, \(k\) is the wave vector, and \(a\) is a constant. The group velocity \(v_g\) is defined as the derivative of \(\omega\) with respect to \(k\):
\(v_g = \frac{d\omega}{dk}\)
Let's differentiate \(\omega = \sqrt{k^2 + a^2}\) with respect to \(k\):
Hence, the expression for the group velocity is:
\(v_g = \frac{k}{\sqrt{k^2 + a^2}}\)
Analyzing the expression, we see:
This implies that the group velocity increases from 0 to 1 as \(k\) increases from 0 to very large values. The sketch that represents this behavior will show the group velocity starting from 0 and asymptotically approaching 1.
Comparing the options, the correct representation of the group velocity is found in the following sketch:

This option shows \(v_g\) starting from 0 and asymptotically approaching 1 with increasing \(k\), which matches our derived behavior for the group velocity.
