Physics Objective Questions and Answers: Oscillations
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Multiple Choice Questions
(a) \( \pi/6 \)
(b) \( \pi/3 \)
(c) \( 5\pi/6 \)
(d) \( 2\pi/3 \)
Show Answer & Explanation
Answer: (b) \( \pi/3 \)
Explanation:
1. Let \( x=A\sin\phi \). Then \( \sin\phi=\sqrt3/2 \), so \( \phi=\pi/3 \) (moving towards +A) or \( 2\pi/3 \) (moving back).
2. Phase difference = \( 2\pi/3-\pi/3=\pi/3 \).
Teacher's Note:
1. Two phases give the same displacement, one on the way out and one on the way back. Their difference is twice the angle measured from the extreme position.
(a) \( T/12 \)
(b) \( T/6 \)
(c) \( 5T/12 \)
(d) \( 7T/12 \)
Show Answer & Explanation
Answer: (d) \( 7T/12 \)
Explanation:
1. Path in one oscillation = 4A, so the required path = \( \tfrac58\times4A=2.5A \).
2. 2A (mean to extreme and back to the mean) takes T/2. The remaining 0.5A from the mean takes \( T/12 \) (since \( \sin30^\circ=\tfrac12 \)).
3. Total time = \( T/2+T/12=7T/12 \).
Teacher's Note:
1. Break the path into whole half-oscillations plus a part. Moving from the mean position to A/2 takes one twelfth of the period.
(a) \( \dfrac{2\pi}{5\sqrt3}\ \text{s} \)
(b) \( \dfrac{\pi}{3\sqrt2}\ \text{s} \)
(c) \( \dfrac{\pi}{2\sqrt5}\ \text{s} \)
(d) \( \dfrac{2\pi}{\sqrt3}\ \text{s} \)
Show Answer & Explanation
Answer: (c) \( \dfrac{\pi}{2\sqrt5}\ \text{s} \)
Explanation:
1. Divide by 4: \( \ddot x+80x=0 \), so \( \omega^2=80 \), \( \omega=4\sqrt5 \).
2. \( T=\dfrac{2\pi}{\omega}=\dfrac{2\pi}{4\sqrt5}=\dfrac{\pi}{2\sqrt5}\ \text{s} \).
Teacher's Note:
1. Write the equation in the standard form x double dot plus omega squared x equals zero. Do not forget to divide by the coefficient of the second derivative.
(a) \( \pi/2\ \text{s} \)
(b) \( \pi\ \text{s} \)
(c) \( 2\pi\ \text{s} \)
(d) \( 3\pi\ \text{s} \)
Show Answer & Explanation
Answer: (a) \( \pi/2\ \text{s} \)
Explanation:
1. Amplitude A = 10 cm and maximum speed \( v_{max}=A\omega=40 \) cm/s, so \( \omega=4\ \text{s}^{-1} \).
2. \( T=2\pi/\omega=\pi/2\ \text{s} \).
Teacher's Note:
1. The intercepts of the v-x ellipse give amplitude and maximum speed. Their ratio is the angular frequency.
(a) \( 2\sin\left(\dfrac{2\pi}{5}t+\dfrac{\pi}{6}\right) \)
(b) \( 4\sin\left(\dfrac{\pi}{5}t+\dfrac{\pi}{6}\right) \)
(c) \( 4\sin\left(\dfrac{\pi}{6}t+\dfrac{\pi}{3}\right) \)
(d) \( 4\sin\left(\dfrac{\pi}{6}t+\dfrac{\pi}{6}\right) \)
Show Answer & Explanation
Answer: (d) \( 4\sin\left(\dfrac{\pi}{6}t+\dfrac{\pi}{6}\right) \)
Explanation:
1. Successive zero crossings are half a period apart, so \( T/2=11-5=6 \) s, \( T=12 \) s and \( \omega=\pi/6 \).
2. Amplitude is 4 cm. At t = 0, \( 2=4\sin\phi\Rightarrow\phi=\pi/6 \).
3. Check: at t = 5, \( \tfrac{5\pi}{6}+\tfrac\pi6=\pi \), which is a downward crossing.
Teacher's Note:
1. Use the zero crossings for the period and the starting value for the phase. A quick check of a crossing time confirms the phase.
(a) 24.7 cm/s
(b) 20.5 cm/s
(c) 28.3 cm/s
(d) 31.4 cm/s
Show Answer & Explanation
Answer: (d) 31.4 cm/s
Explanation:
1. \( v=\dfrac{dx}{dt}=-20\pi\sin\left(2\pi t+\dfrac\pi2\right)=-20\pi\cos2\pi t \).
2. At t = 1/6: \( \cos60^\circ=0.5 \), so \( |v|=10\pi=31.4 \) cm/s.
Teacher's Note:
1. Differentiate, then substitute the time. Keep the phase inside the trigonometric function.
(a) \( 2\pi\sqrt{\dfrac{2\beta}{m}} \)
(b) \( 2\pi\sqrt{\dfrac{m}{2\beta}} \)
(c) \( \pi\sqrt{\dfrac m\beta} \)
(d) \( \pi\sqrt{\dfrac\beta m} \)
Show Answer & Explanation
Answer: (c) \( \pi\sqrt{\dfrac m\beta} \)
Explanation:
1. \( F=-\dfrac{dU}{dx}=-4\beta x \), so the force constant is \( k=4\beta \).
2. \( T=2\pi\sqrt{m/k}=2\pi\sqrt{\dfrac{m}{4\beta}}=\pi\sqrt{\dfrac m\beta} \).
Teacher's Note:
1. The constant alpha does not affect the force. Compare U with one half k x squared to read off k.
(a) 1 s, 0.628 m/s, 4 m/s²
(b) 1 s, 0.314 m/s, 2 m/s²
(c) 2 s, 0.628 m/s, 4 m/s²
(d) 0.5 s, 1.256 m/s, 8 m/s²
Show Answer & Explanation
Answer: (a) 1 s, 0.628 m/s, 4 m/s²
Explanation:
1. \( T=2\pi/\omega=1\ \text{s} \).
2. \( v_{max}=A\omega=0.1\times6.28=0.628\ \text{m/s} \).
3. \( a_{max}=\omega^2A=(6.28)^2(0.1)\approx4\ \text{m/s}^2 \).
Teacher's Note:
1. Maximum speed is amplitude times omega and maximum acceleration is amplitude times omega squared. Convert 10 cm to metres.
(a) 50.2 cm/s
(b) 62.8 cm/s
(c) 37.7 cm/s
(d) 80.0 cm/s
Show Answer & Explanation
Answer: (a) 50.2 cm/s
Explanation:
1. \( v=\omega\sqrt{A^2-x^2}=6.28\sqrt{100-36} \).
2. \( =6.28\times8=50.2\ \text{cm/s} \).
Teacher's Note:
1. The 6-8-10 triangle makes the root exact. Speed falls from maximum at the mean position to zero at the extreme.
(a) -54.4 cm/s
(b) -31.4 cm/s
(c) -62.8 cm/s
(d) -36.2 cm/s
Show Answer & Explanation
Answer: (a) -54.4 cm/s
Explanation:
1. Starting from the extreme: \( x=A\cos\omega t \), so \( v=-A\omega\sin\omega t \).
2. At t = 1/6 s, \( \omega t=2\pi/6=60^\circ \): \( v=-62.8\times\sin60^\circ=-54.4\ \text{cm/s} \).
Teacher's Note:
1. Choose cosine when the motion starts at the extreme. The negative sign shows the particle is moving towards the mean position.
(a) \( \theta=\dfrac\pi{10}\cos40\pi t \)
(b) \( \theta=\dfrac\pi{10}\sin40\pi t \)
(c) \( \theta=\dfrac\pi{10}\cos20\pi t \)
(d) \( \theta=\dfrac\pi{20}\cos40\pi t \)
Show Answer & Explanation
Answer: (a) \( \theta=\dfrac\pi{10}\cos40\pi t \)
Explanation:
1. \( \omega=2\pi/0.05=40\pi\ \text{rad/s} \).
2. At t = 0 the displacement equals the amplitude, so the cosine form is used: \( \theta=\dfrac\pi{10}\cos40\pi t \).
Teacher's Note:
1. The same equations hold for angular SHM. Starting at the extreme means cosine with zero phase.
(a) 2 m/s and 4 m/s²
(b) 4 m/s and 2 m/s²
(c) 2 m/s and 2 m/s²
(d) 1 m/s and 4 m/s²
Show Answer & Explanation
Answer: (a) 2 m/s and 4 m/s²
Explanation:
1. \( \omega^2=4\Rightarrow\omega=2\ \text{rad/s} \); amplitude A = 1 m.
2. \( v_{max}=A\omega=2\ \text{m/s} \), \( a_{max}=\omega^2A=4\ \text{m/s}^2 \).
Teacher's Note:
1. Read omega squared as the coefficient in the acceleration equation. Use amplitude to get the maxima.
(a) 195°
(b) 15°
(c) 165°
(d) 105°
Show Answer & Explanation
Answer: (a) 195°
Explanation:
1. Phase of \( Y_1 \) at 0.5 s = \( 5\pi+\pi/3 \); phase of \( Y_2 \) = \( 4\pi+\pi/4 \).
2. Difference = \( \pi+\pi/3-\pi/4=\pi+\pi/12=195^\circ \).
Teacher's Note:
1. Phase is the whole argument of the sine, not only the constant term. Subtract the two arguments at the given time.
(a) \( a/8 \)
(b) \( a/(2\sqrt2) \)
(c) \( a/2 \)
(d) \( a/\sqrt2 \)
Show Answer & Explanation
Answer: (d) \( a/\sqrt2 \)
Explanation:
1. \( y=a\sin\omega t=a\sin\left(\dfrac{2\pi}{T}\cdot\dfrac T8\right)=a\sin45^\circ=\dfrac a{\sqrt2} \).
Teacher's Note:
1. Time measured from the mean position uses the sine form. One eighth of a period is 45 degrees of phase.
(a) 0
(b) \( \pi/2 \)
(c) \( \pi \)
(d) \( 2\pi \)
Show Answer & Explanation
Answer: (c) \( \pi \)
Explanation:
1. Acceleration \( a=-\omega^2x \) is always opposite to displacement, so they are out of phase by \( \pi \).
Teacher's Note:
1. Velocity leads displacement by pi by two and acceleration leads velocity by another pi by two. Together that is pi.
(a) periodic, oscillatory but not SHM
(b) periodic but not oscillatory
(c) oscillatory but not periodic
(d) simple harmonic
Show Answer & Explanation
Answer: (d) simple harmonic
Explanation:
1. Write \( a=-100(x-0.5) \): the acceleration is proportional to the displacement from x = 0.5 m and directed towards it.
2. This is the condition for SHM, with the equilibrium shifted to x = 0.5 m.
Teacher's Note:
1. A constant term only shifts the centre of oscillation. The restoring nature is unchanged.
(a) 2.0 m
(b) 8.4 m
(c) 16.8 m
(d) 17.64 m
Show Answer & Explanation
Answer: (a) 2.0 m
Explanation:
1. The maximum acceleration is \( \omega^2A=35.28 \) with \( \omega=4.2 \).
2. \( A=\dfrac{35.28}{(4.2)^2}=\dfrac{35.28}{17.64}=2.0\ \text{m} \).
Teacher's Note:
1. The coefficient of the cosine is the maximum acceleration, not the amplitude. Divide by omega squared.
(a) Zero
(b) T/2
(c) 2T
(d) Infinite
Show Answer & Explanation
Answer: (d) Infinite
Explanation:
1. The total mechanical energy of an ideal oscillator is constant.
2. A constant does not oscillate, so its period is infinite.
Teacher's Note:
1. Kinetic and potential energy each oscillate with half the period, T/2. Their sum does not change.
(a) \( \dfrac{2\pi}{25}\ \text{s} \)
(b) \( \dfrac{\pi\sqrt2}{5}\ \text{s} \)
(c) \( \dfrac{4\pi}{5}\ \text{s} \)
(d) \( \dfrac{2\pi\sqrt2}{5}\ \text{s} \)
Show Answer & Explanation
Answer: (d) \( \dfrac{2\pi\sqrt2}{5}\ \text{s} \)
Explanation:
1. \( U=\tfrac12kx^2\Rightarrow k=\dfrac{2(1.0)}{(0.2)^2}=50\ \text{N/m} \).
2. \( T=2\pi\sqrt{m/k}=2\pi\sqrt{4/50}=2\pi\sqrt{\dfrac{2}{25}}=\dfrac{2\pi\sqrt2}{5}\ \text{s} \).
Teacher's Note:
1. Read the force constant from the potential energy curve. Then use T equals two pi root m by k.
(a) 3.5 kg
(b) 8.2 kg
(c) 4.7 kg
(d) 2.6 kg
Show Answer & Explanation
Answer: (a) 3.5 kg
Explanation:
1. \( T\propto\sqrt m \): \( \dfrac{5^2}{4^2}=\dfrac{m+2}{m} \).
2. \( 25m=16m+32\Rightarrow m=\dfrac{32}{9}\approx3.5\ \text{kg} \).
Teacher's Note:
1. Take the ratio of the periods to eliminate k. Square before cross-multiplying.
(a) \( \dfrac\pi2\ \text{kg} \)
(b) \( \dfrac{160}{\pi^2}\ \text{kg} \)
(c) \( 8\times10^{-3}\ \text{kg} \)
(d) \( \dfrac{16}{\pi^2}\ \text{kg} \)
Show Answer & Explanation
Answer: (b) \( \dfrac{160}{\pi^2}\ \text{kg} \)
Explanation:
1. Force constant \( k=10/1=10\ \text{N/m} \); angular frequency \( \omega=2\pi/8=\pi/4 \).
2. \( m=\dfrac{k}{\omega^2}=\dfrac{10}{\pi^2/16}=\dfrac{160}{\pi^2}\ \text{kg} \).
Teacher's Note:
1. Slope of the F-x line gives k and the x-t graph gives omega. Mass follows from omega squared equals k by m.
(a) \( \dfrac\pi2\ \text{J} \)
(b) \( \dfrac{160}{\pi^2}\ \text{J} \)
(c) \( 8.0\times10^{-3}\ \text{J} \)
(d) \( 4\times10^{-3}\ \text{J} \)
Show Answer & Explanation
Answer: (c) \( 8.0\times10^{-3}\ \text{J} \)
Explanation:
1. \( K_{max}=\tfrac12kA^2=\tfrac12(10)(0.04)^2=8\times10^{-3}\ \text{J} \).
Teacher's Note:
1. Maximum kinetic energy equals the total energy, half k A squared. Convert the amplitude to metres.
(a) 160 J
(b) 100 J
(c) 60 J
(d) 260 J
Show Answer & Explanation
Answer: (b) 100 J
Explanation:
1. Energy exchanged in the oscillation = \( \tfrac12kA^2=\tfrac12(2\times10^6)(10^{-4})=100\ \text{J} \).
2. The total of 160 J includes a constant potential energy of 60 J at the mean position, so the maximum kinetic energy is 160 - 60 = 100 J.
Teacher's Note:
1. Total energy depends on where potential energy is taken to be zero. The kinetic energy swing is always half k A squared.
(a) 5 m
(b) 3 m
(c) 7 m
(d) 8 m
Show Answer & Explanation
Answer: (c) 7 m
Explanation:
1. \( F=-dU/dx=20-10x=0\Rightarrow x_0=2\ \text{m} \) (equilibrium).
2. Amplitude = 2 - (-3) = 5 m, so the maximum x = 2 + 5 = 7 m.
Teacher's Note:
1. Find the equilibrium position first. The particle swings equally far on both sides of it.
(a) 5 s
(b) 10 s
(c) 15 s
(d) 20 s
Show Answer & Explanation
Answer: (d) 20 s
Explanation:
1. Potential energy is maximum at an extreme position and minimum (zero) at the mean position.
2. That takes a quarter of the period: \( T/4=5 \) s, so T = 20 s.
Teacher's Note:
1. Extreme to mean is a quarter period. Do not use half the period here.
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