Principle of superposition
Principle of superposition
When two or more waves propagating in a medium arrive at the same point simultaneously, a new wave is produced. This phenomenon is called superposition of According to Young the net displacement at any point of the medium is equal to the algebraic sum of displacements of individual waves arriving at that point simultaneously. This is called the principle of superposition and holds good as long as the amplitude of the waves is not too large. This principle is of extreme importance and can be applied to many types of waves e.g. sound waves, light waves, wave pulses etc. The superposition of harmonic waves gives rise to interference, beats and standing waves.
To recognize the types of waves, the following
equations must be known.
Equation of a straight line
y = mx + c
Equation of circle of radius ‘a’ is x2 + y2 = a2
Equation of ellipse
a = semi-major axis
b = semi-minor axis
Equation of parabola is
y2 = 4 a x ( fig .a )
This is parabola symmetrically about x-axis and
x2 = 4 a y (fig . b)
This is parabola symmetrical about y – axis
When two waves of slightly different frequencies travel along the same straight line and along the same direction, they superimpose in such a way that the resultant intensity alternatively increases or decreases. This phenomenon of waxing and waning of sound is called beats. One waxing and one waning forms one beat.
For the sake of simplicity we assume the two waves of slightly different frequencies n1 and n2 (at x =0 ) are represented as
From Young’s principle of superposition
Let n1 = n and n2 = n + such that
; then equation (1) gives
is the amplitude of resultant and obviously depends on time.
The amplitude A = 2a ….(3)
is maximum for where r is an integer.
The instant of maximum are given by
Obviously time interval between two consecutive maxima
Frequency of maxima = ( n1 – n2 ) sec -1
The amplitude is minimum for
The time interval between two consecutive minima
The number of beats produced per second.
Remark: When the prongs of a turning fork are loaded, the frequency of fork decreases and when they are filed; the frequency of fork increases.
When two wave trains of same frequency and amplitude travel with the same velocity along the
same straight line in opposite directions, they superimpose to, produce a new type of wave called stationary wave or standing wave.
The name stationary for such type of waves is justified because there is no flow of energy along the
wave. Let the incident wave propagating along Y- axis be
and the wave reflected from the boundary traveling along negative X-axis is
The positive and negative signs are used: if the boundary is free or rigid respectively.
Case (i). If boundary is free: then equation (2) is,
The resultant displacement due to these incident and reflected waves is
is the amplitude of resultant wave.
At positions where , the displacement is maximum. Such points are called antinodes and are given by
The separation between two consecutive antinodes is
At positions where = 0, the displacement is always zero. Such points are called nodes and are given by
The separation between two consecutive nodes is
From (7) and (8) it is obvious that at free boundary always an antinodes is farmed. Midway between the antinodes, there are nodes.
The separation between a node and neighboring antinodes is
Case (ii) If the boundary is rigid , then
Amplitude of resultant disturbance,
The positions of maximum displacement or antinodes are
The positions of zero displacement or nodes are
Thus a node is always formed at rigid boundary lowest.
Fundamental tone, harmonics and overtones:
The sound of frequency produced by a musical instrument is called the fundamental tone. The sounds of other frequencies produced by the musical instrument are called overtones. The overtones whose frequencies are integral multiplies of the fundamental frequency are called the harmonics. The fundamental tone is also called the first harmonic. If first harmonic is n, then the tones of frequencies 2n, 3n, 4n … are called the second, the third and the fourth harmonic respectively. If frequencies of sound emitted by an instrument are n, 1.5n, 2n, 2.5n, 3n etc, then the notes of frequencies 1.5n, 2n, 2.5n, 3n are overtones, while those of frequencies 2n, 3n are second and third harmonics respectively.
Stationary Waves in Strings Fixed at Both Ends:
For transverse vibrations in string, we have
Speed of waves v = n
where T is tension in string and m is mass per unit length of string
When the string is plucked in the middle, it vibrates in one loop with nodes at fixed ends and antinodes in the middle; so that length of string
This tone is emitted is called the fundamental or first harmonic.
If the wire is plucked at one fourth of its length, the string vibrates in two loops, so that
This tone is called the second harmonic or first overtone.
In the string is plucked at one sixth of its length, the string vibrates in three loops, so that
This tone is called third harmonic or second overtone.
In general when the string vibrates in p-loops, the frequency
This tone is called the pth. Thus in the case of string fixed at both ends, all harmonics even and odd are present.
If N is frequency of tuning fork for a given length ‘l’ of a string vibrating in p-loops under 2; tension T, then Melde’s law states
T.p2 = constant or = constant
Vibrations of Air columns in Organ Pipes
The minimum frequency produced in a pipe is called fundamental and other notes are called overtones.
Open organ pipe :
An antinodes is always formed at the open end. Accordingly different notes produced in open pipe are shown in fig. In fundamental mode if is wavelength, then
For first overtone if is the wavelength , then
This frequency is double of fundamental frequency and is therefore called second harmonic.
For second overtone, if is the wavelength, then
This is the third harmonic Frequencies
Frequencies n1 : n2 : n3 : … = 1 : 2: 3:… i.e. in open organ pipe all harmonics even or odd are present.
Stationary Waves and Harmonics in Closed Organ Pipe:
A node is always formed at closed end and antinodes at open end. Accordingly different harmonies produced in closed organ pipe are shown in fig.
In fundamental mode, if is the wavelength of vibrations, then
Frequency of first overtone, if is the wavelength , then
This frequency is three times of fundamental. Therefore in closed pipe the first overtone is third
For second overtone; if is the wavelength, then
Thus in closed pipe
n1 : n2 : n3 : … = 1 : 3 : 5 : …
Hence in closed organ pipe only odd harmonics are present.
End Correction :
So far we have considered that the antinodes is formed exactly at the open end of the pipe; but actually due to finite momentum of the particles the reflection takes place a little above the open end; that is why the antinodes is formed a little above the open end. For this a correction is applied being known as end correction.This is denoted by ‘c’ and its value to 0.6r. r being radius of the pipe. If lo is the length of pipe, then for closed pipe ‘l’ is replaced by lo + e while for open pipe ‘I’ is replaced by 1o + 2e .
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