QUESTION IMAGE
Question
section a - multiple choice (40 marks)
- a simple pendulum is oscillating in a lift. if the lift starts moving upwards with a uniform acceleration, then the period will
a. remain the same
b. be shorter
c. be longer
d. may be shorter or longer, depending on the magnitude of acceleration
- the bob of a simple pendulum of period t is given a negative charge. if it is allowed to oscillate above a positively charged plate, the new time period will be
a. equal to t
b. more than t
c. less than t
d. infinite
- a body of mass 5 g is executing s.h.m. with amplitude 10 cm. its maximum velocity is 100 cm/s. its velocity will be 50 cm/s at a displacement from the mean position equal to
a. 5 cm
b. 5√3 cm
c. 10 cm
d. 10√3 cm
- a simple harmonic oscillator has a period of 0.01 s, and an amplitude of 0.2 m. the magnitude of the velocity in m/s at the center of oscillation is
a. 20π
b. 40π
c. 60π
d. 80π
- a loaded spring vibrates with a period t. the spring is divided into four equal parts and the same load is suspended from one of these parts. the new time period is
a. t/4
b. t/2
c. 2t
d. 4t
- the length of a seconds pendulum on the surface of the moon, where g is 1/6th of the value of the surface of the earth, is
a. 1/36 m
b. 1/6 m
c. 6 m
d. 36 m
- a particle of mass 0.5 kg executes s.h.m. its energy is 0.04 j. if its time period is π sec amplitude is
a. 10 cm
b. 15 cm
c. 20 cm
d. 40 cm
Step1: Recall the formula for the period of a simple pendulum
The formula for the period of a simple pendulum is \(T = 2\pi\sqrt{\frac{l}{g_{eff}}}\). When the lift moves upwards with uniform acceleration \(a\), the effective acceleration \(g_{eff}=g + a\). Since \(g_{eff}\) increases, and \(T\propto\frac{1}{\sqrt{g_{eff}}}\), the period \(T\) will be shorter.
Step2: Analyze the effect of charge on the period of a simple pendulum
The period of a simple pendulum \(T = 2\pi\sqrt{\frac{l}{g}}\) is independent of the mass and charge of the bob. So, when the bob is given a charge and oscillates above a charged plate, the new time period will be equal to \(T\).
Step3: Use the formula for velocity in SHM
The formula for velocity in SHM is \(v=\omega\sqrt{A^{2}-x^{2}}\), and also \(v_{max}=\omega A\). Given \(v_{max} = 100\space cm/s\), \(A = 10\space cm\), so \(\omega=\frac{v_{max}}{A}=10\space s^{-1}\). Given \(v = 50\space cm/s\), then \(50=10\sqrt{10^{2}-x^{2}}\). Squaring both sides: \(2500 = 100(100 - x^{2})\), \(25=100 - x^{2}\), \(x^{2}=75\), \(x = 5\sqrt{3}\space cm\).
Step4: Use the formula for maximum velocity in SHM
The formula for maximum velocity in SHM is \(v_{max}=\omega A\), and \(\omega=\frac{2\pi}{T}\). Given \(T = 0.01\space s\), \(A=0.2\space m\), then \(\omega=\frac{2\pi}{0.01}=200\pi\space rad/s\), \(v_{max}=200\pi\times0.2 = 40\pi\space m/s\).
Step5: Recall the formula for the period of a spring - mass system
The formula for the period of a spring - mass system is \(T = 2\pi\sqrt{\frac{m}{k}}\). When a spring is divided into \(n\) equal parts, the spring constant of each part \(k_{new}=nk\). Here \(n = 4\), so \(k_{new}=4k\). The new period \(T_{new}=2\pi\sqrt{\frac{m}{4k}}=\frac{T}{2}\).
Step6: Use the formula for the period of a second's pendulum
A second's pendulum has \(T = 2s\) on earth. The formula \(T = 2\pi\sqrt{\frac{l}{g}}\). On earth \(T_{e}=2\pi\sqrt{\frac{l_{e}}{g_{e}}}=2s\). On the moon \(T_{m}=2\pi\sqrt{\frac{l_{m}}{g_{m}}}\), and \(g_{m}=\frac{g_{e}}{6}\). If we assume the period on the moon is also considered for a pendulum with the same time - keeping concept (assuming \(T_{m}\) is related to the same kind of'second' - like measurement in terms of formula), and if we consider the ratio \(\frac{T_{e}}{T_{m}}=\sqrt{\frac{l_{e}g_{m}}{l_{m}g_{e}}}\). But if we consider the formula \(l=\frac{gT^{2}}{4\pi^{2}}\), for a second's pendulum \(T = 2s\). On earth \(l_{e}=\frac{g_{e}\times4}{4\pi^{2}}\), on the moon \(l_{m}=\frac{g_{m}\times4}{4\pi^{2}}\), and since \(g_{m}=\frac{g_{e}}{6}\), \(l_{m}=\frac{l_{e}}{6}\).
Step7: Use the formula for the energy of a SHM system
The energy of a SHM system is \(E=\frac{1}{2}m\omega^{2}A^{2}\), and \(\omega=\frac{2\pi}{T}\). Given \(m = 0.5\space kg\), \(E = 0.04\space J\), \(T=\pi\space s\), \(\omega=\frac{2\pi}{\pi}=2\space rad/s\). Then \(0.04=\frac{1}{2}\times0.5\times4\times A^{2}\), \(0.04 = A^{2}\), \(A = 0.2\space m=20\space cm\).
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