Showing posts with label Stretched String. Show all posts
Showing posts with label Stretched String. Show all posts

Vibrations of Sound in Closed Pipe and Open Pipe

Vibrations of the transverse waves in a closed pipe

A pipe that is open at one end and closed at other end is called as a closed pipe.

When a sound wave is passed, at the closed end it reflects back. There is a formation of node at the close the end and anti node at the open end. Different modes of vibration are possible and in each mode of the vibration different frequency is generated. These frequencies are called harmonics and they are in a systematic way. We can derive the equation for the ratios of the frequencies as shown below.



In a closed pipe, the first and second harmonics are having the ratios of frequencies 1:3. Basing on this concept we can derive the equation for the velocity of the sound using this to vibrations as shown below. We need to calculate the vibrating lengths at which a booming sound is heard. At that particular length of the air, the frequency of the tuning fork and the frequency of the air column are coinciding with each other. They are said to be in resonance and it together produces a large booming sound.



Different modes of vibration in open pipe

The pipe that is open at both the ends is called as open pipe. When it is exposed to a sound wave at both the ends there is a formation of anti node. Under different modes of vibration different frequencies are available and the ratio is derived as shown below.



Problem and solution

A pipe that is open at both the ends as a fundamental frequency n. When one by fourth of its length is immersed in water, what will be the fundamental frequency?

When the pipe is immersed in water it becomes a closed pipe. It will further have only three by fourth of the length is one by fourth is immersed in water.




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Stretched String Problems and Solutions

Problem and solution

A sonometer wire has a length of 114 cm between the two fixed ends. Where shall we place two movable bridges to divide the wire into three segments whose fundamental frequency surrender ratio of  1:3:4 ?

When the tension and linear density of the wire is kept constant, frequency of the wire is inversely proportional to its length. Taking this law into consideration the problem is solved as shown below.



Problem and solution

A wire with density and length given and extension under a load is given in the below problem.We need to calculate the frequency of the wire under fundamental mode using the formula for the frequency of a stretched string.



This problem  is based on law of tension.When frequency is changed its tension will change as shown below.












Frequency of the tuning fork is directly proportional to thickness of the fork, velocity of the wave and inversely proportional to Squire of its length.

Speed of a longitudinal wave in a medium

The velocity of a wave in a medium can be expressed as the ratio of Squire root of  modulus of elasticity of the medium to the density of the medium. It is assumed that the propagation of the sound happens in a isothermal way. Anyway practically it is found that the temperature of the particles of the medium is not going to remain constant during the propagation of the wave. It is rather in adiabatic process when the heat energy of the system remains constant but the temperature increases.


It can be further proved that velocity of sound is independent of pressure.When ever pressure changes its volume also changes which generates same change in density and hence the ratio of pressure to density remain constant.



we can further compare this velocity with RMS velocity of a gas as shown below.Both of them depend on the absolute temperature similarly.



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Wave Motion an introduction