To show that the motion of the bob of the simple pendulum is S.H.M
1) Consider a simple pendulum of mass m and length L
L=l+r
where l= length of string and r is the radius of the bob.
2)Let OA be the initial position of pendulum and OB, be its instantaneous position when the string makes an angle θ with the vertical.
In displaced position, two forces are acting on the bob:
a)Gravitational force(weight)mg in the downward direction.
b)Tension T′ in the string.
3)Weight mg can be resolved in to two rectangular components:
a)Radial component mgcosθ along OB and
b)Tangential component mgsinθ perpendicular to OB and directed towards mean position.
4)mgcosθ is balanced by tension T′ in the string,while mgsinθ provides restoring force.
∴F=−mgsinθ
where negative sign shows that force and angular displacement are oppositely directed.Hence, restoring force is proportional to sinθ instead of θ.So, the resulting motion is not S.H.M.
5)If θ is very small then
sinθ≈θ=xL
∴F=−mgxL
∴Fm=−gxL
∴mam=−gxL
∴a=−gxL ....(1)
∴a∝−x since gL=constant
Hence, the motion of the bob of a simple pendulum is simple harmonic.
Expression for the time period:
In S.H.M
a=−ω2x ....(2)
Comparing equations (1) and (2)
ω2=gL
But ω=2πT
(2πT)2=gL
2πT=√gL
T=2π√Lg ....(3)
Equation (3) represents the time period of the simple pendulum.Thus, the period of a simple pendulum depends on the length of the pendulum and acceleration due to gravity.