Question #41432

A particle executing simple harmonic motion has velocities
4cms(−1)
at
6cm
and
6cm−1
at
4cm
respectively from the equilibrium position.Determine the amplitude of oscillation

Expert's answer

Answer on Question #41432, Physics, Mechanics | Kinematics | Dynamics

A particle executing simple harmonic motion has velocities 4cms14\mathrm{cms}^{-1} at 6cm and 6cms16\mathrm{cms}^{-1} at 4cm respectively from the equilibrium position. Determine the amplitude of oscillation

Solution:

Simple harmonic motion is typified by the motion of a mass on a spring when it is subject to the linear elastic restoring force given by Hooke's Law.

Now since F=kxF = -kx is the restoring force and from Newton's law of motion force is given as F=maF = ma, where mm is the mass of the particle moving with acceleration aa. Thus acceleration of the particle is


a=Fm=kxma = \frac{F}{m} = \frac{-kx}{m}


but we know that acceleration a=dv/dt=d2x/dt2a = dv/dt = d^2 x/dt^2.

Thus,


d2xdt2=kxm\frac{d^2 x}{dt^2} = \frac{-kx}{m}


This differential equation is known as the simple harmonic equation.

The solution is


x=Acos(ω0t+ϕ)x = A \cos(\omega_0 t + \phi)


where AA is amplitude of oscillation, ω0\omega_0 and ϕ\phi are all constants.

We know that velocity of a particle is given by


v=dxdtv = \frac{dx}{dt}


Now differentiating the displacement of particle xx with respect to tt

v=dxdt=Aω0(sin(ω0t+ϕ))v = \frac{dx}{dt} = A \omega_0 \left( -\sin(\omega_0 t + \phi) \right)


From trigonometry we know that


sin2x+cos2x=1\sin^2 x + \cos^2 x = 1


Thus,


A2sin2(ω0t+ϕ)=A2A2cos2(ω0t+ϕ)=A2x2A^2 \sin^2(\omega_0 t + \phi) = A^2 - A^2 \cos^2(\omega_0 t + \phi) = A^2 - x^2


Or


sin(ω0t+ϕ)=1x2A2\sin(\omega_0 t + \phi) = \sqrt{1 - \frac{x^2}{A^2}}


putting this in for velocity we get,


v=Aω01x2A2v = -A \omega_0 \sqrt{1 - \frac{x^2}{A^2}}


so it is proportional to ω0\omega_0.

Thus,


v2=A2ω02(1x2A2)=ω02(A2x2)v^2 = A^2 \omega_0^2 \left(1 - \frac{x^2}{A^2}\right) = \omega_0^2 (A^2 - x^2)


We have that


v1=4cms1,v _ {1} = 4 \mathrm {c m s} ^ {- 1},x1=6cm,x _ {1} = 6 \mathrm {c m},v2=6cms1,v _ {2} = 6 \mathrm {c m s} ^ {- 1},x2=4cm,x _ {2} = 4 \mathrm {c m},


Thus,


v12v22=A2x12A2x22\frac {v _ {1} ^ {2}}{v _ {2} ^ {2}} = \frac {A ^ {2} - x _ {1} ^ {2}}{A ^ {2} - x _ {2} ^ {2}}


Substitute


4262=A262A242\frac {4 ^ {2}}{6 ^ {2}} = \frac {A ^ {2} - 6 ^ {2}}{A ^ {2} - 4 ^ {2}}1636=A236A216\frac {1 6}{3 6} = \frac {A ^ {2} - 3 6}{A ^ {2} - 1 6}36(A236)=16(A216)3 6 (A ^ {2} - 3 6) = 1 6 (A ^ {2} - 1 6)20A2=10402 0 A ^ {2} = 1 0 4 0A2=52A ^ {2} = 5 2A=7.2cmA = 7. 2 \mathrm {c m}


Answer. A=7.2cmA = 7.2\mathrm{cm}

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