Step 1: Use the time-slope/angle relation.
For a planar reflector, the zero-offset time slope is \[ \frac{\partial t}{\partial x}= \frac{2\sin\theta}{v}, \] where \(\theta\) is the reflector dip (equal to the incidence angle at the reflection point) and \(v\) is the migration velocity.
Step 2: Solve for \(\theta\).
Given \(\partial t/\partial x=0.5\ \text{s/km}\) and \(v=2\ \text{km/s}\), \[ \sin\theta=\frac{v}{2}\,\frac{\partial t}{\partial x} =\frac{2}{2}\times 0.5=0.5. \] Hence, \[ \theta=\sin^{-1}(0.5)=30^\circ. \] \[ \boxed{30.0^\circ} \]