This problem requires calculating the angular momentum of an object at its peak altitude. We will proceed with a step-by-step solution:
\(v_{0x} = v_0 \cos 45^\circ = \frac{v_0}{\sqrt{2}}\) and \(v_{0y} = v_0 \sin 45^\circ = \frac{v_0}{\sqrt{2}}\)
\(t = \frac{v_{0y}}{g} = \frac{v_0/\sqrt{2}}{g} = \frac{v_0}{\sqrt{2}g}\)
\(x = v_{0x} \cdot t = \frac{v_0}{\sqrt{2}} \cdot \frac{v_0}{\sqrt{2}g} = \frac{v_0^2}{2g}\)
\(L = \mathbf{r} \times \mathbf{p} = m(x \, v_y - y \, v_x)\)
\(L = -m \left(\frac{v_0^2}{4g}\right) \left(\frac{v_0}{\sqrt{2}}\right) = -\frac{mv_0^3}{4\sqrt{2}g}\)
Therefore, the magnitude of the object's angular momentum with respect to the origin at its maximum height is \( \frac{mv_0^3}{4\sqrt{2}g} \), and its direction is along the negative z-axis.
Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Knowing the initial position \( x_0 \) and initial momentum \( p_0 \) is enough to determine the position and momentum at any time \( t \) for a simple harmonic motion with a given angular frequency \( \omega \).
Reason (R): The amplitude and phase can be expressed in terms of \( x_0 \) and \( p_0 \).
In the light of the above statements, choose the correct answer from the options given below: