Time Period of a Simple Pendulum
- A simple pendulum consists of a string and a bob at the end
- The bob is a weight, generally spherical and considered a point mass
- The bob moves from side to side
- The string is light and inextensible remaining in tension throughout the oscillations
- The string is attached to a fixed point above the equilibrium position
- The time period of a simple pendulum for small angles of oscillation is given by:
- Where:
- T = time period (s)
- L = length of string (from the pivot to the centre of mass of the bob) (m)
- g = gravitational field strength (N kg-1)
A simple pendulum
- The time period of a pendulum does depend on the gravitational field strength, meaning its period would be different on the Earth and the Moon
Small Angle Approximation
- This formula for time period is limited to small angles (θ < 10°) and therefore small amplitudes of oscillation from the equilibrium point
- The restoring force of the pendulum is the weight component acting along the arc of the circle towards the equilibrium position
- It is resolved to act at an angle θ to the horizontal x
- When considering SHM because of small angle approximation it is assumed the restoring force acts along the horizontal
- So sin θ ≅ θ
Forces on a pendulum when it is displaced. Assuming θ < 10°, the small angle approximation can be used to describe the time period of a simple pendulum such as this.
Worked example
A swinging pendulum with a length of 80.0 cm has a maximum angle of displacement of 8°.
Determine the angular frequency of the oscillation.
Answer:
Step 1: List the known quantities
- Length of the pendulum, L = 80 cm = 0.8 m
- Acceleration due to gravity, g = 9.81 m s−2
Step 2: Write down the relationship between angular frequency, ω, and period, T
Step 3: Write down the equation for the time period of a simple pendulum
- This equation is valid for this scenario since the maximum angle of displacement is less than 10°
Step 4: Equate the two equations and rearrange for ω
Step 5: Substitute the values to calculate ω
= 3.50 rad s−1
Angular frequency: ω = 3.5 rad s−1