Step 1: Expression for Force.
The force \( F \) on the particle is related to the rate of change of momentum:
\[
F = \frac{dp}{dt}
\]
For the \( x \)-component of momentum \( p_x = 2 \cos t \), we have:
\[
\frac{dp_x}{dt} = -2 \sin t
\]
For the \( y \)-component of momentum \( p_y = \sin t \), we have:
\[
\frac{dp_y}{dt} = \cos t
\]
Thus, the force components are:
\[
F_x = -2 \sin t, \quad F_y = \cos t
\]
Step 2: Calculate the angle between \( F \) and \( p \).
The angle \( \theta \) between the vectors \( F \) and \( p \) is given by the formula:
\[
\cos \theta = \frac{F_x p_x + F_y p_y}{|F| |p|}
\]
Substitute the values for \( F_x, F_y, p_x, \) and \( p_y \):
\[
\cos \theta = \frac{(-2 \sin t)(2 \cos t) + (\cos t)(\sin t)}{\sqrt{(-2 \sin t)^2 + (\cos t)^2} \cdot \sqrt{(2 \cos t)^2 + (\sin t)^2}}
\]
Simplifying:
\[
\cos \theta = \frac{-4 \sin t \cos t + \cos t \sin t}{\sqrt{4 \sin^2 t + \cos^2 t} \cdot \sqrt{4 \cos^2 t + \sin^2 t}} = 0
\]
This implies \( \theta = 90^\circ \).