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Wave, Motion and Sound - Part II |
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2.
Sound
waves Initially the density of
air around the tuning fork is undisturbed. As the fork prongs go back and
forth or oscillate, the density of the air is pushed and pulled and the air
becomes compressed and rarefied alternately.
Speed of sound depends directly on the elasticity of the medium and
inversely on the density of the medium. For a gaseous medium, elasticity can
be approximated to the pressure of the gas.
In air, the velocity of sound is about 340 m/s. If we change the air
medium to a less denser medium like Helium gas, our voices will sound
shrilly like the cartoon character Mickey mouse. On the other hand, if the
medium surrounding our vocal chord is dense (say with Argon gas), then our
voices will sound hoarse like the cartoon character Goofey. The following table gives
the speed of sound in different mediums at 0°C.
The table below gives the speed of sound in air at different temperatures.
Since sound waves travel because of local air pressure differences, in addition to temperature, humidity and air pressure also changes the velocity of sound. Reflection
of sound waves Take a bell and a hollow tube. Let the tube be placed at an angle to a reflecting surface such as a plate. Keep a screen vertical to the plate. Ask a friend to ring the bell. Take another hollow tube on the other side of the screen and keep it near your ear. Change the angle of the second tube with respect to the plate. At a particular angle, you will be able to hear the ringing of the bell clearly. This is the angle of reflection of the sound wave. You will notice that the angle of reflection = angle of incidence. The conclusion of the experiment is that the sound waves are reflected just like the light waves. Focussing of sound waves occur with concave surfaces just like focussing of light rays with concave mirrors. This is demonstrated by two concave surfaces arranged as shown below. If a source of sound such
as a watch is kept at one focus, the sound of the ticking of the watch is
clearly heard at the other focus. Such examples of sound reflections are a
source of amazement in science museums where whispering galleries surprise
visitors with their own voices reflected back. Also when we are unable to
hear, we cup our hands near our ears in a concave geometry, which then gives
us a better hearing. Sound reflection is also seen in echoes. Since our ears cannot distinguish sounds heard within a gap of 1/10th of a second. Thus an echo can be heard if the sound reflected back takes more than 0.1 second. By taking the speed of sound to be about 340m/s at ordinary temperature and pressure, an echo can be heard if the distance of the reflecting object is more than 17 meters.
One person A stands on a cliff with a gun. Another person stands on the cliff B with a stopwatch. The distance between A and B is known. When the gun is fired by A, there is first a flash of light and then the sound. This is because the speed of light is 3 x 108m/s, many orders of magnitude larger than the speed of the sound. B starts his stopwatch when he sees the flash of light and stops his stopwatch when he hears the sound. The time measured by the stopwatch is the time taken by the sound waves to travel distance AB. Dividing the distance between A and B by the time, we will get the velocity of sound. Since the sound velocity is dependent on various parameters such as air temperature, pressure, wind directions, etc. this experiment has to be performed several times with interchanging positions of A and B; Thus an average velocity of the sound can be determined.
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