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Question: Define oscillatory motion....

Define oscillatory motion.

Explanation

Solution

Hint: A motion is said to be oscillatory if its diagram in displacement-time graph is either
A. Sinusoidal with constant amplitude. (undamped)
B. Sinusoidal with decreasing amplitude. (damped)

Complete step-by-step answer:
We first need to know about the simple harmonic motion where the force on a body is proportional to its displacement from a mean position. Its equation of motion can be given by,
md2ydt2+Rdydt+ky=0m\dfrac{d^2y}{dt^2}+R\dfrac{dy}{dt}+ky=0
Where R is the damping force per unit velocity of the object. k is called the force constant. The equation is modified as,
d2ydt2+2bdydt+ω02y=0\dfrac{d^2y}{dt^2}+2b\dfrac{dy}{dt}+\omega_0^2y=0
Here, 2b=Rm2b=\dfrac{R}{m} and ω02=km\omega_0^2=\dfrac{k}{m}
Undamped oscillatory motion- In this case, R=0 \Rightarrow b=0. Hence the equation reduces to,
d2ydt2+ω02y=0\dfrac{d^2y}{dt^2}+\omega_0^2y=0
The solution will be, y=A.cos(ω0tθ)y=A.cos(\omega_0t-\theta)
Where, A is the amplitude of oscillation and θ\theta depends on the initial conditions. Its diagram looks like…..

Its energy is given by,
E=Ek+Ep=12m(dydt)2+12mω02y212ˉmω02A2E=E_k+E_p=\dfrac{1}{2}m(\dfrac{dy}{dt})^2+\dfrac{1}{2}m\omega_0^2y^2\\\=\dfrac{1}{2}m\omega_0^2A^2
Damped oscillation- In case b0b\neq 0, oscillation can only be observed if bω0b\leq \omega_0 and in all the other cases no oscillation will be observed.
If bω0b\geq \omega_0 ,the motion is called over damped.
If b=ω0b=\omega_0, the motion is said to be critically damped.
In these two cases there is no oscillation. For oscillation (damped), bω0b\leq \omega_0
In this case, the solution is given by, y=A.ebt.cos(ωtθ)y=A.e^{-bt}.cos(\omega t-\theta)
Here, ω=ω02b2\omega=\sqrt{\omega_0^2-b^2}

The diagram will look like this.
In this case, the amplitude decreases as , A1=AebtA_1=Ae^{-bt}
Its energy can be shown to be E=12mω02A2e2btE=\dfrac{1}{2}m\omega_0^2A^2e^{-2bt}

Note: There is another type of oscillation that is called forced oscillation. In this case, the system is forced to move in oscillation by an oscillatory external force.