Simple Harmonic Motion
If a body moves in such a way that its acceleration is directed towards a
fixed point in its path and directly proportional to the distance from that
point, the movement of the object is said to be simple
harmonic
E.g.
When a simple pendulum swings to and fro, the acceleration
of its bob is directed towards the centre point of its motion and is
proportional to the distance from that point. Therefore, the motion of a
simple pendulum is SHM.
As you can see, when the weight of the
pendulum bob is resolved, the tension of the string, T,
and the mg cos x cancel each other out, leaving
mg sin x as the net force, as shown above. This
force is responsible for bringing the bob down in a curved path.
Using F = ma for the bob,
mg sin x = ma, where a is the acceleration of the bob.
If the pendulum swings through a small angle
and is measured in radians, sin x is almost
equal to x.
mg. x = m a
gx = a
g d/l = a ( x = d / l radians)
a = (g/l) d
a = k d
a α d
The acceleration of the bob is
directly proportional to the distance from the centre point. Therefore, the
motion of a simple pendulum is simple harmonic.
k = ω2 where ω is the angular speed.
a = ω2 d
ω2 = g/l
ω = √g/l
If the time period is T,
T = 2π/ω
T = 2π/ √g/l
So, the time period of
a simple pendulum depends only on its length; it does not depend on the mass
of the bob. The formula only works for the oscillations through small
angles, as it was something we assumed in the process of proof.
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