Step 1: Understanding the Concept
In a small time \(\Delta t\), the radius vector sweeps a thin triangle of area \(\Delta A=\dfrac{1}{2}r\,(v\,\Delta t)\sin\theta\).
Step 2: Calculation
\(\dfrac{\Delta A}{\Delta t}=\dfrac{1}{2}rv\sin\theta\). Angular momentum \(L=mrv\sin\theta\), so \(rv\sin\theta=\dfrac{L}{m}\).
Step 3: Result
\(\dfrac{\Delta A}{\Delta t}=\dfrac{L}{2m}\). It is constant because gravity exerts no torque about the sun, so \(L\) is conserved.
Final Answer:
The areal velocity equals L divided by 2m.
\[ \boxed{\text{(D) }\dfrac{L}{2m}} \]