Step 1: Understanding the Concept:
In a damped harmonic oscillation, both the amplitude and the total mechanical energy decrease exponentially with time. The key relationship is that the mechanical energy is proportional to the square of the amplitude (\(E \propto A^2\)).
Step 2: Key Formulae:
The amplitude of a damped oscillator at time \(t\) is given by:
\[ A(t) = A_0 e^{-\gamma t} \]
where \(A_0\) is the initial amplitude and \(\gamma\) is a damping constant.
The total mechanical energy of the oscillator at time \(t\) is:
\[ E(t) = \frac{1}{2} k A(t)^2 = \frac{1}{2} k (A_0 e^{-\gamma t})^2 = \left(\frac{1}{2} k A_0^2\right) e^{-2\gamma t} \]
So, we can write:
\[ E(t) = E_0 e^{-2\gamma t} \]
where \(E_0\) is the initial energy.
Step 3: Detailed Explanation:
Using the Amplitude Information:
We are given that the amplitude becomes half its initial value in 10 s. So, at \(t = 10\) s, \(A(10) = A_0/2\).
\[ \frac{A_0}{2} = A_0 e^{-\gamma(10)} \]
\[ \frac{1}{2} = e^{-10\gamma} \quad \cdots(1) \]
Finding the Time for Energy to Halve:
We need to find the time \(t'\) when the energy becomes half its initial value. So, \(E(t') = E_0/2\).
\[ \frac{E_0}{2} = E_0 e^{-2\gamma t'} \]
\[ \frac{1}{2} = e^{-2\gamma t'} \quad \cdots(2) \]
Comparing the two expressions:
From equation (1) and (2), we can see that the expressions on the right-hand side are equal. Therefore, their exponents must be equal.
\[ e^{-10\gamma} = e^{-2\gamma t'} \]
\[ -10\gamma = -2\gamma t' \]
Assuming \(\gamma \neq 0\), we can cancel \(- \gamma\) from both sides.
\[ 10 = 2t' \]
\[ t' = \frac{10}{2} = 5 \text{ s} \]
Step 4: Final Answer:
The time taken for the mechanical energy to become half of its initial value is 5 s. Therefore, option (D) is correct.