Step 1: Understanding the Question:
This question asks for the relationship between the amplitude of the oscillatory angular momentum of a simple pendulum and its time period.
We are given that the angular amplitude of the oscillation is fixed.
Step 2: Key Formula or Approach:
• The time period of a simple pendulum of length \(L\) is:
\[ T = 2\pi \sqrt{\frac{L}{g}} \implies L \propto T^2 \]
• The moment of inertia of the pendulum bob of mass \(m\) about the suspension point is:
\[ I = m L^2 \]
• The angular displacement is given by \(\theta(t) = \theta_0 \sin(\omega t)\), where the angular frequency is:
\[ \omega = \frac{2\pi}{T} \]
• The angular velocity is \(\dot{\theta}(t) = \theta_0 \omega \cos(\omega t)\).
• The angular momentum is:
\[ L(t) = I \dot{\theta} = I \theta_0 \omega \cos(\omega t) \]
Step 3: Detailed Explanation:
• The amplitude of the angular momentum oscillation is the maximum value of \(L(t)\), which we denote as \(A\).:
\[ A = I \theta_0 \omega \]
• Substitute the expression for the moment of inertia \(I = m L^2\).:
\[ A = (m L^2) \theta_0 \omega \]
• Since the mass \(m\) and the angular amplitude \(\theta_0\) are constant, we have:
\[ A \propto L^2 \omega \]
• From the relation for the time period, we know that \(L \propto T^2\).
• Also, the angular frequency is related to the time period as \(\omega \propto T^{-1}\).
• Substituting these proportionality relations into the expression for \(A\).:
\[ A \propto (T^2)^2 \cdot T^{-1} \]
\[ A \propto T^4 \cdot T^{-1} = T^3 \]
Step 4: Final Answer:
Therefore, the relation between \(A\) and \(T\) is \(A \propto T^3\).