Sunday, 26 June 2016

experiment 04: The simple pendulum


Objectives

 
The purposes of this experiment are: (1) to study the motion of a simple pendulum, (2) to

study simple harmonic motion, (3) to learn the definitions of period, frequency, and

amplitude, (4) to learn the relationships between the period, frequency, amplitude and

length of a simple pendulum and (5) to determine the acceleration due to gravity using

the theory, results, and analysis of this experiment.

Theory

 
A simple pendulum may be described ideally as a point mass suspended by a massless

string from some point about which it is allowed to swing back and forth in a place. A

simple pendulum can be approximated by a small metal sphere which has a small radius

and a large mass when compared relatively to the length and mass of the light string from

which it is suspended. If a pendulum is set in motion so that is swings back and forth, its

motion will be periodic. The time that it takes to make one complete oscillation is

defined as the period T. Another useful quantity used to describe periodic motion is the

frequency of oscillation. The frequency f of the oscillations is the number of oscillations

that occur per unit time and is the inverse of the period, f = 1/T. Similarly, the period is

the inverse of the frequency, T = l/f. The maximum distance that the mass is displaced

from its equilibrium position is defined as the amplitude of the oscillation.

When a simple pendulum is displaced from its equilibrium position, there will be a

restoring force that moves the pendulum back towards its equilibrium position. As the

motion of the pendulum carries it past the equilibrium position, the restoring force

changes its direction so that it is still directed towards the equilibrium position. If the

restoring force F



is opposite and directly proportional to the displacement x from the

equilibrium position, so that it satisfies the relationship