1. 2 sec
2.
Consider a mass m suspended from one end of a string of length L fixed at the other end as shown in figure. Suppose P is the instantaneous position of the pendulum. At this instant its string makes an angle θ with the vertical.
The forces acting on the bob are (1) weight of bob Fg(mg) acting vertically downward. (2) Tension T in the string.
The gravitational force Fg can be divided into a radial component FgCosθ and tangential component
FgSinθ. The tangential component FgSinθ produces a restoring torque.
Restoring torque τ = – Fg sinθ . L
τ = – mg sinθ . L _____(1)
-ve sign shown that the torque and angular displacement θ are oppositely directed. For rotational motion of bob,
τ = Iα ______(2)
Where I is moment of inertia about the point of suspension and α is angular acceleration. From eq (1) and eq (2).
Iα = – mgsinθ . L
If we assume that the displacement θ is small, sinθ ≈ θ
∴ Iα = -mgθ . L
Iα + mgθ L = 0
Compairing eq (3) with standard differential equation
∴ period of simple pendulum,
for simple pendulum I = mL2
Substituting I = mL2 we get
The above equation gives that T is independent of mass.