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A tunnel has been dug through the centre of the earth and a ball is released in it. It executes S.H.M. with time period
\(T=2\pi \sqrt{\frac{R}{g}}=2\pi \sqrt{\frac{64\times 10^{2}}{9.8}}=2\times \frac{22}{7}\times \frac{8\times 10^{3}}{7\times \sqrt{2}}\)
\(=\frac{\sqrt{2}\times 22\times 8\times 1000}{49\times 60}min =84.6\: min\)
A particle moves such that its acceleration ‘a’ is given by a= – bx where x is the displacement from equilibrium position and b is constant. The period of oscillation is
\(T=2\pi \sqrt{\frac{displacement}{acceleration}}=2\pi \sqrt{\frac{x}{bx}}=2\pi /\sqrt{b}\)
A particle of mass 1 kg is moving in S.H.M. with an amplitude 0.02 and a frequency of 60 Hz. The maximum force acting on the particle is
Max. force = mass × max. acceleration= m4 π2 V2a =1 × 4 ×π2× (60)2× 0.02 = 288 π2
An instantaneous displacement of a simple harmonic oscillator is x = A cos (ωt + π/4). Its speed will be maximum at time
Velocity,V=\(\frac{dx}{dt}=-A\: \omega \: sin(\omega +\pi /4)\)
Velocity will be maximum, when
t=π/4 ω
The tension in the string of a simple pendulum is
Tension is maximum at the mean position.
The equation of SHM of a particle is A + 4π2x = 0 where a is instantaneous linear acceleration at displacement x. The frequency of motion is
Comparing A+ω2X=0
ω2=4π2⇒ω=2π,2πv=2πy=1Hz
If the magnitude of displacement is numerically equal to that of acceleration, then the time period is
\(y=\omega ^{2}y,\omega =1,\frac{4\pi ^{2}}{T^{2}}=1\: or\: T^{2}=4\pi ^{2}\)
or T = 2π second.
A particle executing simple harmonic motion along y-axis has its motion described by the equations in y=A sin(ωt)+B.The amplitude of the simple harmonic motion is
The amplitude is a maximum displacement from the mean position
The graph shown in figure represents
At displacement ± a, the velocity is zero. At zero displacement, velocity is maximum
Resonance is an example of