Chapter 9: Problem 27
Which of the following represents a standing wave? (A) \(y=A \sin (\omega t-k x)\) (B) \(y=A \sin k x \sin (\omega t-\theta)\) (C) \(y=A e^{-b x} \sin (\omega t-k x+\alpha)\) (D) \(y=(a x+b) \sin (\omega t-k x)\)
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Chapter 9: Problem 27
Which of the following represents a standing wave? (A) \(y=A \sin (\omega t-k x)\) (B) \(y=A \sin k x \sin (\omega t-\theta)\) (C) \(y=A e^{-b x} \sin (\omega t-k x+\alpha)\) (D) \(y=(a x+b) \sin (\omega t-k x)\)
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A particle moves along the \(x\)-axis as per the equation \(x=4+3 \sin (2 \pi t)\). Here \(x\) is in \(\mathrm{cm}\) and \(t\) in seconds. Select the correct alternative(s) (A) The motion of the particle is simple harmonic with mean position at \(x=0\). (B) The motion of the particle is simple harmonic with mean position at \(x=4 \mathrm{~cm}\). (C) The motion of the particle is simple harmonic with mean position at \(x=-4 \mathrm{~cm}\). (D) Amplitude of oscillation is \(3 \mathrm{~cm}\).
Which of the following statements are true for wave motion? (A) Mechanical transverse waves can propagate through all mediums. (B) Longitudinal waves can propagate through solids only. (C) Mechanical transverse waves can propagate through solids only. (D) Longitudinal waves can propagate through vacuum.
The displacement of a particle varies according to the relation. \(x=4(\cos \pi t+\sin \pi t)\) The amplitude of the particle is (A) \(-4\) (B) 4 (C) \(4 \sqrt{2}\) (D) 8
A train is moving on a straight track with speed \(20 \mathrm{~ms}^{-1}\). It is blowing its whistle at the frequency of \(1000 \mathrm{~Hz}\). The percentage change in the frequency heard by a person standing near the track as the train passes him is (speed of sound \(=320 \mathrm{~ms}^{-1}\) ) close to (A) \(12 \%\) (B) \(18 \%\) (C) \(24 \%\) (D) \(6 \%\)
A particle starts SHM at time \(t=0 .\) Its amplitude is \(A\) and angular frequency is \(\omega .\) At time \(t=0\), its kinetic energy is \(\frac{E}{4}\), where \(E\) is total energy. Assuming potential energy to be zero at mean position, the displacement-time equation of the particle can be written as (A) \(x=A \cos \left(\omega t+\frac{\pi}{6}\right)\) (B) \(x=A \sin \left(\omega t+\frac{\pi}{3}\right)\) (C) \(x=A \sin \left(\omega t-\frac{2 \pi}{3}\right)\) (D) \(x=A \cos \left(\omega t-\frac{\pi}{6}\right)\)
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