Two simple harmonic motions are represented by the equations
$y _1=10\sin \left(3\pi t+\dfrac{\pi}{4}\right)$
and $y _2=5(3\sin 3\pi t+\sqrt 3 \cos 3\pi t)$ Their amplitudes are in the ratio of :
Physics
Oscillations and Simple Harmonic Motion
136 QuestionsOscillations and simple harmonic motion focus on amplitude, damped vibrations, and force equations. These physics principles are essential for various engineering and civil services examinations. Review these problems to understand the core mechanics of oscillating bodies.
Oscillations and Simple Harmonic Motion Questions
The amplitude of vibrations measured on the Richter's scale increase by steps of about
The direction of motion of a particle at any instant is given by
The number of cycles an oscillator completes in each second is called its _______________.
Frequency of vibration of a particle is 10 Hz. If the amplitude of vibration is doubled, what will be the change in frequency of vibration
A particle performs 20 vibrations in 5 secs. The time period of vibration is
A particle vibrates 10 times in 1 sec. What is the time period of vibration of the particle
The equation of motion of a particle is $x = a cos(\alpha t)^2$. The motion is
In the equations below, A, B, $\omega$ and $\phi$ are constants; $y$ and $t$ are variables; $t$ represents time. Only one of the following equations does not represent SHM. Which one is that?
Uniform circular motion can also be represented by a simple harmonic oscillator.
State whether given statement is True/False?
In periodic motion, the displacement is
A thin spherical shell of mass $M$ and radius $R$ has a small hole. A particle of mass $m$ is released at its mouth. Then
A particle oscillating in simple harmonic motion is :
A block of mass $M$ is performing $SHM$ with amplitude $A$ on a smooth horizontal surface$.$ At the extreme position a small block of mass $m$ falls vertically and sticks to$M.$ then$,$ amplitude of oscillation will be
A simple harmonic oscillator of angular frequency $2$ rad/s is acted upon by an external force $F = \sin t$ N. If the oscillator is at rest in its equilibrium position at $t= 0$, its position at later times is proportional to: