Lab Manual: To Determine the Length of the Equivalent Simple Pendulum (Ring Pendulum)
1. Aim
To determine the length of the equivalent simple pendulum for a given ring pendulum and to verify the relationship between the time periods of the ring pendulum and its equivalent simple pendulum.
2. Apparatus Used
- A metal ring with known diameter
- A rigid support stand
- A knife-edge for suspension
- A stopwatch (least count = 0.1 s)
- A meter scale (least count = 0.1 cm)
- A vernier caliper (least count = 0.01 cm)
3. Diagram

A labeled diagram showing the ring suspended from a knife-edge, oscillating about an axis perpendicular to its plane.
4. Theory
A ring pendulum is a rigid body oscillating about a horizontal axis passing through its periphery. The time period of oscillation of a ring pendulum is given by:
where:
- \( I \) = Moment of inertia of the ring about the axis of suspension
- \( m \) = Mass of the ring
- \( l \) = Distance from the suspension point to the center of mass (equal to the radius \( R \) of the ring)
- \( g \) = Acceleration due to gravity
The moment of inertia of the ring about the suspension axis (using the parallel axis theorem) is:
The equivalent simple pendulum is a hypothetical simple pendulum with the same time period as the ring pendulum. Its length \( L \) is given by:
Thus, the length of the equivalent simple pendulum should be equal to the diameter of the ring.
5. Formula
- Time period of ring pendulum:
\[ T_{ring} = 2\pi \sqrt{\frac{2R}{g}} \]
- Length of equivalent simple pendulum:
\[ L = 2R \]
6. Procedure
- Measure the diameter of the ring using a vernier caliper and record it.
- Suspend the ring from a rigid support using a knife-edge so that it can oscillate freely in its plane.
- Displace the ring slightly and release it to allow small oscillations.
- Measure the time for 20 complete oscillations using a stopwatch and calculate the time period \( T \).
- Repeat the experiment for different suspension points (if possible) and record observations.
- Calculate the equivalent length \( L \) using the formula and compare it with the theoretical value \( 2R \).
7. Observation Table
S.No. | Diameter of Ring (2R) (cm) | Time for 20 Oscillations (s) | Time Period \( T \) (s) | \( L = \frac{gT^2}{4\pi^2} \) (cm) | Theoretical \( L = 2R \) (cm) |
---|---|---|---|---|---|
1 | |||||
2 | |||||
3 |
8. Calculations
Sample Calculation:
Given: \( R = 15 \, \text{cm} \), \( T = 1.1 \, \text{s} \), \( g = 980 \, \text{cm/s}^2 \)
Theoretical \( L = 2R = 30 \, \text{cm} \)
9. Result
The experimentally determined length of the equivalent simple pendulum is ____ cm, which closely matches the theoretical value of ____ cm (diameter of the ring).
10. Precautions
- Ensure that the ring oscillates in a vertical plane without any wobbling.
- Use a stopwatch with a small least count for accurate time measurement.
- Keep the amplitude of oscillation small (≤ 5°) to ensure simple harmonic motion.
- Repeat the experiment multiple times to minimize errors.
11. Viva Voce Questions
- What is a compound pendulum? How does it differ from a simple pendulum?
- Derive the expression for the time period of a ring pendulum.
- What is the equivalent simple pendulum?
- Why should the amplitude of oscillation be small?
- How does the moment of inertia affect the time period of a ring pendulum?
- What is the parallel axis theorem, and how is it applied here?
- What are the sources of error in this experiment?