Step 1: Understanding the Concept:
Velocity is \(v = \dfrac{ds}{dt}\) and acceleration is \(a = \dfrac{dv}{dt}\). We are told \(s\) is proportional to \(v^2\).
Step 2: Key Formula or Approach:
Write \(s = c\,v^2\) for a constant \(c\), then differentiate both sides with respect to time.
Step 3: Detailed Explanation:
\[ \frac{ds}{dt} = 2c\,v\,\frac{dv}{dt} \]
Replace \(\dfrac{ds}{dt}\) by \(v\) and \(\dfrac{dv}{dt}\) by \(a\):
\[ v = 2c\,v\,a \]
For a moving particle \(v \neq 0\), so we may cancel \(v\):
\[ a = \frac{1}{2c} \]
This is a constant, since \(c\) is a constant. So the acceleration does not change with time or with displacement.
This matches uniformly accelerated motion, where \(v^2 = 2as\). Options (A), (B) and (C) say that \(a\) depends on \(s\), which would not be the case here.
Final Answer:
The acceleration is a constant, option (D).
\[ \boxed{\text{a constant (D)}} \]