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Q. If n coherent sources of intensity $ \frac{{{p}^{2}}{{t}^{2}}}{m} $ are superimposed at a point the intensity of the point is

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Solution:

The resultant amplitude is $ A=x{{a}_{0}} $ $ l\propto {{A}^{2}} $ $ l=k{{A}^{2}}=k{{x}^{2}}a_{0}^{2}={{x}^{2}}{{l}_{0}} $