SIMPLE HARMONIC MOTION
INTRODUCTION:
Things move. They sometimes move in random fashion, sometimes
along a path of some sort, sometimes in a repeating motion. Let’s first
explore the latter, and narrow that further to things moving back and
forth. Indeed, if you look at something going around and around from
the side, it appears to be going back and forth anyway. The simplest back and forth, or vibrating motion is called simple harmonic motion.
In your imagination if not actually, take a string about 3 feet long and
tie a reasonably large weight (two or three pounds) to one end, the
other to a hook at the top center of your doorway or some other place
where it can swing freely. You have made a pendulum, which is one
example of something moving in Simple Harmonic Motion (See fig.
Figure 2-1
SIMPLE HARMONIC MOTION
REVEIW OF LITERATURE
1.FRIDAY’S PHYSICAL LAW -
SIMPLE HARMONIC MOTION
First we know that simple harmonic motion is a function of a sin/cosine . But Friday gives in his law that it is also a restoring force.
2. SUNIL KUMAR SINGH: He given some suggestions about the simple harmonic motion.
3.Dr.HAYWARD
4.Dr.STEPHEN
5.Sc.SWIFF
THEORY
Simple Harmonic Motion
Idea: Any object that is initially displaced slightly from a stable equilibrium point will oscillate about its equilibrium position. It will, in general, experience a restoring force that depends linearly on the displacement x from equilibrium:
Hooke’s Law:
|
Fs = – kx |
(1) |
where the equilibrium position is chosen to have x -coordinate x = 0 and k is a constant that depends on the system under consideration. The units of k are:
|
[k] = . |
(2) |
Definitions:
- Amplitude ( A ): The maximum distance that an object moves from its equilibrium position. A simple harmonic oscillator moves back and forth between the two positions of maximum displacement, at x = A and x = – A .
- Period ( T ): The time that it takes for an oscillator to execute one complete cycle of its motion. If it starts at t = 0 at x = A , then it gets back to x = A after one full period at t = T .
- Frequency ( f ): The number of cycles (or oscillations) the object completes per unit time.
|
f = . |
(3) |
- The unit of frequency is usually taken to be 1 Hz = 1 cycle per second.
- Simple Harmonic Oscillator: Any object that oscillates about a stable equilibrium position and experiences a restoring force approximately described by Hooke’s law. Examples of simple harmonic oscillators include: a mass attached to a spring, a molecule inside a solid, a car stuck in a ditch being “rocked out” and a pendulum.
Note:
- The negative sign in Hooke’s law ensures that the force is always opposite to the direction of the displacement and therefore back towards the equilibrium position (i.e. a restoring force).
- The constant k in Hooke’s law is traditionally called the spring constant for the system, even when the restoring force is not provided by a simple spring.
- The motion of any simple harmonic oscillator is completely characterized by two quantities: the amplitude, and the period (or frequency
A simple harmonic motion can be conceived as a “to and fro” motion along an axis (say x-axis). In order
to simplify the matter, we choose origin of the reference as the point about which particle oscillates. If we
start our observation from positive extreme of the motion, then displacement of the particle “x” at a time
“t” is given by
x=Acoswt
where “w” is angular frequency and “t” is the time. The figure here shows the positions of the particle
executing SHM at an interval of “T/8”. The important thing to note here is that displacements in different
intervals are not equal, suggesting that velocity of the particle is not uniform. This also follows from the
nature of cosine function. The values of cosine function are not equally spaced with respect to angles.
Simple harmonic motion
A simple harmonic motion can be conceived as a “to and fro” motion along an axis (say x-axis). In order
to simplify the matter, we choose origin of the reference as the point about which particle oscillates. If we
start our observation from positive extreme of the motion, then displacement of the particle “x” at a time
“t” is given by :
http://cnx.org/content/m15572/latest/ (5 of 17)11/18/2008 9:04:29 PM
Simple harmonic motion
x=Acoswt
where “w” is angular frequency and “t” is the time. The figure here shows the positions of the particle
executing SHM at an interval of “T/8”. The important thing to note here is that displacements in different
intervals are not equal, suggesting that velocity of the particle is not uniform. This also follows from the
nature of cosine function. The values of cosine function are not equally space with respect to angles. The solution of the differential equation of simple harmonic motion is:
A general equation describing simple harmonic motion is:
CHARACTERSTICS OF SHM
1 THE MOTION OF THE BODY EXECUTING SHM IS PERODIC AND ‘TO AND FRO’
.
THE GRAPH REPRESENTING AMPLITUDE OF SIMPLE HARMONIC MOTION
APPLICATIONS
1. The pendulum -
Show the movement of a simple pendulum bob and explain
SHM. When the bob is hanging downward it is in
equilibrium position. When it is disturbed, it
executes SHM. Gravity pulls it back to equilibrium
position but momentum carries it past that position to
another point. It relies on acceleration due to
gravity to deep swinging. Try different lengths of
string and different weights of bobs and see what
happens. Which moves slower, a heavy bob or a light
bob? What difference in acceleration is observed due
to length of string? What else did you observe?
2. The metronome -
This inverted compound pendulum executes SHM when set
into motion by a force. The period of swing can be
altered by varying the position of the small weight on
the arm of the metronome. How does the weight set near
the top of the arm affect the swing of the arm, faster
or slower? What happens when the weight is moved to
the bottom of the arm? Is the swing equal on each side
of the position of equilibrium?
3. A diving board -
This oscillates with SHM after the diver has started
into his dive. Before this when the diver is bouncing
to gain maximum height, the board undergoes forced
oscillation. Observe a diver as he makes a dive, or
set up a simulation of a dive in the classroom.
SUMMARY
They sometimes move in random fashion, sometimes
along a path of some sort, sometimes in a repeating motion. Let’s first
explore the latter, and narrow that further to things moving back and
forth. Indeed, if you look at something going around and around from
the side, it appears to be going back and forth anyway. The simplest back and forth, or vibrating motion is called simple harmonic motion.
Suggestions:
As a student I am not able to give any suggestions about the simple harmonic motion.
