Correct answer Carries: 4.
Wrong Answer Carries: -1.
Which condition ensures that the total mechanical energy in an SHM system remains conserved during the motion?
Total mechanical energy (kinetic + potential) is conserved in SHM when no external dissipative forces (e.g., friction) act, allowing energy to transform without loss.
A particle in SHM has \( x = 4 \cos (2t + \frac{\pi}{3}) \) (in m). What is its speed at \( t = 0.5 \, \text{s} \)? (Take \( \sin 60^\circ = \frac{\sqrt{3}}{2} \))
Velocity: \( v = -\omega A \sin (\omega t + \phi) \).
\( A = 4 \, \text{m}, \omega = 2 \, \text{s}^{-1}, \phi = \frac{\pi}{3} \).
At \( t = 0.5 \): \( 2 \times 0.5 + \frac{\pi}{3} = 1 + \frac{\pi}{3} \approx 2.047 \, \text{rad} \approx 117^\circ \).
\( v = -2 \times 4 \sin 117^\circ \approx -8 \sin (180^\circ - 63^\circ) \approx -8 \times 0.838 \approx -6.7 \, \text{m/s} \).
A pendulum has \( L = 0.6 \, \text{m}, g = 9.8 \, \text{m/s}^2 \). What is its angular frequency?
\( \omega = \sqrt{\frac{g}{L}} = \sqrt{\frac{9.8}{0.6}} \approx \sqrt{16.33} \approx 4.04 \, \text{rad/s} \).
A pendulum of length \( 0.36 \, \text{m} \) oscillates with \( g = 9.8 \, \text{m/s}^2 \). What is its frequency?
Period: \( T = 2\pi \sqrt{\frac{L}{g}} = 2\pi \sqrt{\frac{0.36}{9.8}} \approx 2 \times 3.14 \sqrt{0.0367} \approx 1.2 \, \text{s} \).
Frequency: \( v = \frac{1}{T} = \frac{1}{1.2} \approx 0.833 \, \text{Hz} \).
What underlies the periodic nature of SHM when expressed as a superposition of sine and cosine functions?
The periodicity arises from the repeating nature of sine and cosine functions, which have a fixed period (\( 2\pi/\omega \)), ensuring the motion repeats consistently.
A pendulum has \( L = 1.4 \, \text{m}, g = 9.8 \, \text{m/s}^2 \). What is its angular frequency?
\( \omega = \sqrt{\frac{g}{L}} = \sqrt{\frac{9.8}{1.4}} \approx \sqrt{7} \approx 2.65 \, \text{rad/s} \).
Which of the following periodic motions cannot be classified as oscillatory due to the absence of a fixed equilibrium point?
Rotational motion of a ceiling fan is periodic but not oscillatory, as it lacks a fixed equilibrium point about which it moves to-and-fro, unlike SHM examples.
A particle in SHM has \( a = -36 x \) (in SI units). What is its frequency?
For SHM, \( a = -\omega^2 x \). Given \( a = -36 x \), \( \omega^2 = 36 \Rightarrow \omega = 6 \, \text{rad/s} \).
Frequency: \( v = \frac{\omega}{2\pi} = \frac{6}{2 \times 3.14} \approx 0.955 \, \text{Hz} \).
A particle’s motion is \( x = 4 \sin (3t - \frac{\pi}{3}) \) (in m). What is its velocity at \( t = \frac{\pi}{6} \, \text{s} \)? (Take \( \cos 30^\circ = \frac{\sqrt{3}}{2} \))
Velocity: \( v = \omega A \cos (\omega t + \phi) \).
\( A = 4 \, \text{m}, \omega = 3 \, \text{s}^{-1}, \phi = -\frac{\pi}{3} \).
At \( t = \frac{\pi}{6} \): \( 3 \times \frac{\pi}{6} - \frac{\pi}{3} = \frac{\pi}{2} - \frac{\pi}{3} = \frac{\pi}{6} \).
\( v = 3 \times 4 \cos \frac{\pi}{6} = 12 \times \frac{\sqrt{3}}{2} = 6\sqrt{3} \approx 10.39 \, \text{m/s} \).
What is the significance of the phase constant in the displacement equation of SHM?
The phase constant (\( \phi \) in \( x = A \cos (\omega t + \phi) \)) determines the initial position and velocity, setting the starting point of the oscillation cycle.
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