(vi) For the positions of antinodes:

or x = even multiple of 
(vii) Nodes: At these point the amplitude of particles is minimum and the change in pressure and density is maximum.
Amin = a1 - a2
or x = odd multiple of 
13. For stationary waves:
1. waves produce nodes antinodes at regular points in limited medium .
2.The distance between to consecution nodes antinodes is 2 / 2
3.Distance between a node and as adjoient antinode is 2 / 4.
4. particles situated between two nodes execute simple harmonic motion whose amplitude are different but frequency are same .
5. Amplitude depends on the position of the particle , maximum amplitude is obtained at antinodes and zero amplitudes at the nodes .
6.The particles situated between two consecutive nodes vibrate in the phase with different amplitudes while the particles situated on either side of a node vibrate in the opposite phase .
14. Vibrations is a stretched string:
1. Transverse progressive wave is produced is a stretched string .
2.node is always formed at fixed and of string .
3.Velocing of the waves produced in a stretched string is

where t = tension and m = mass perurit length of string
If the density of material of string is d, radius is r, then and if T = Mg.

(4) For a string fixed at both the ends, nodes are formed at the ends.
(5) If the length of a string is L & p loops are formed in it , then the frequency of the string

in the condition string is only loop. n1is colled the fundamental frequency. This is also called first harmonic .
(b) If p = 2, then 
In this condition n2 is called the second harmonic or the first overtone.
= 3n1, n3 is called third harmonic or the second overtone.
(d) In the strings all harmonics are produced and their ratio is
n1:n2:n3 ...... = 1:2:3:.....
(e) Some harmonics are shown in the figure .
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