To address this issue, we must first comprehend the behavior of a damped harmonic oscillator. The amplitude of such an oscillator diminishes exponentially over time. This relationship is defined by the equation:
\( A(t) = A_0 e^{-\lambda t} \)
In this formula:
Given that the amplitude halves within 10 seconds, we can formulate the equation as:
\( \frac{1}{2}A_0 = A_0 e^{-\lambda \times 10} \)
To solve for \( \lambda \):
\( \frac{1}{2} = e^{-10\lambda} \)
Applying the natural logarithm to both sides yields:
\( \ln\left(\frac{1}{2}\right) = -10\lambda \)
This equation simplifies to:
\( \lambda = -\frac{\ln\left(\frac{1}{2}\right)}{10} = \frac{\ln(2)}{10} \)
Now, we will determine the amplitude at 30 seconds. The governing equation is:
\( A(30) = A_0 e^{-\lambda \times 30} \)
Substituting the value of \( \lambda \):
\( A(30) = A_0 e^{-\frac{30 \ln(2)}{10}} = A_0 e^{-3 \ln(2)} \)
Recognizing that \( e^{-\ln(2)} = \frac{1}{2} \), it follows that \( e^{-3 \ln(2)} = \left(\frac{1}{2}\right)^3 \):
\( A(30) = A_0 \left(\frac{1}{2}\right)^3 = A_0 \times \frac{1}{8} \)
Consequently, after 30 seconds, the amplitude will be \( \frac{1}{8} \) of its original value.
In an oscillating spring mass system, a spring is connected to a box filled with sand. As the box oscillates, sand leaks slowly out of the box vertically so that the average frequency ω(t) and average amplitude A(t) of the system change with time t. Which one of the following options schematically depicts these changes correctly?