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Sound is described by a pressure wave which can be written as \(\Delta p=\Delta p_0 \cos (kx-\omega t+\phi)\), where \(\Delta p\) is the change in pressure at \(x\) at time \(t\) from the atmospheric pressure, \(\Delta p_0\) is the maximum change from the atmospheric pressure as the compression and rare faction take place. If two sound waves reach a common place with same frequency, same intensity and a definite phase difference, interference occurs and the intensity becomes \(I=I_0\cos^2 \frac{\phi}{2}\). Depending on \(\phi\) the sound intensity can be high or low. This experiment gives qualitative feel of this intensity variation.
You need two audio speakers, a frequency generator to produce a `monochromatic' sound, a stethoscope, measuring tape.
Frequency Generator: The unit gives an electrical voltage that varies at a chosen fixed frequency. The display shows the frequency. Various knobs control the amplitude and frequency of this signal.
Stethoscope: This is the instrument which is identity of a doctor. We will use it as a sound detector.
Use the minima positions just on the two sides of the central point. The path difference in the situation shown in figure is
For a minimum this should be \(\lambda/2\). The value of \(y\) can be obtained by measuring the distance between two minima on the two sides of the mid points and dividing by two. Calculate the wavelength \(\lambda\) from this. Calculate the speed of sound in air from \(v=n\lambda\).
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