Demo Video: Simple Harmonic Motion (SHM) of a Pendulum | Nagwa Demo Video: Simple Harmonic Motion (SHM) of a Pendulum | Nagwa

Demo Video: Simple Harmonic Motion (SHM) of a Pendulum

In this demonstration, we will see pendulums display simple harmonic motion and we will reveal the impact of pendulum length on the period of oscillation.

03:49

Video Overview

A pendulum is an object that consists of a mass on the end of a string, wire, or thin rod. The string, wire, or rod is attached to a surface so that the mass hangs below it.

When the pendulum hangs straight down, it is in its equilibrium position. The weight of the mass is balanced by the tension in the string. There is no net force acting on the mass at the end of the pendulum, so it does not move.

When the mass on the end of the pendulum is raised to one side by hand, the weight of the mass still acts straight downward, but the tension in the string acts diagonally upward. The tension only partly counterbalances the weight of the mass. This results in a net force that is perpendicular to the string.

When the pendulum is released, the net force accelerates the mass, and the mass moves closer to its equilibrium position. However, when the mass reaches its equilibrium position, it has a sideways velocity, and it overshoots its equilibrium position. The mass moves past the equilibrium position, and since the string keeps the mass at a fixed distance away from where the pendulum is attached to the surface, the mass moves upward as well as to the side.

When the mass is on the other side of the equilibrium position, the resultant force due to the weight of the mass and the tension in the string is in the opposite direction. The mass is accelerated in the opposite direction, and it moves closer to the equilibrium position again. The mass will overshoot its equilibrium position again.

The pendulum will keep overshooting its equilibrium position; it will oscillate.

Although the mass of the pendulum determines its weight, it does not affect the period of the oscillation. For amplitudes less than approximately 1 radian (about 57), the amplitude of the oscillation does not affect the period either. The period of the oscillation, 𝑇, depends only on the length of the string, 𝑙, and the acceleration due to gravity, 𝑔: 𝑇=2𝜋𝑙𝑔.

Since on the surface of Earth, the acceleration due to gravity is roughly constant, the main factor that can be used to change the period of the oscillation of a pendulum is its length.

Consider a pendulum that has a length of 0.5 m. The acceleration due to gravity is 9.81 m/s2. Then, the period of the pendulum is 𝑇=2𝜋0.59.81/𝑇=1.42.mmss(3s.f.)

The amplitude of the oscillation will gradually decrease over time. The kinetic energy of the pendulum will gradually be lost due to air resistance and due to friction at the point where the pendulum is attached to the surface above it.

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