The displacement of two light waves, each of amplitude 'a' and frequency \(\omega\), emanating from two coherent sources of light, are given by \(y_1 = a \cos(\omega t)\) and \(y_2 = a \cos(\omega t + \phi)\). \(\phi\) is the phase difference between the two waves. These light waves superpose at a point. Obtain the expression for the resultant intensity at that point.
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Remember that the maximum intensity occurs when \(\phi = 0\) (in phase) and the minimum intensity (possibly zero) occurs when \(\phi = \pi\) (out of phase), demonstrating constructive and destructive interference respectively.
Step 1: Express the resultant displacement.
When two waves superpose, the resultant displacement \(y\) is the sum of the individual displacements:
\[
y = y_1 + y_2 = a \cos(\omega t) + a \cos(\omega t + \phi)
\]
Using the trigonometric identity for the sum of cosines:
\[
y = 2a \cos\left(\frac{\phi}{2}\right) \cos\left(\omega t + \frac{\phi}{2}\right)
\]
Step 2: Determine the resultant intensity.
Intensity is proportional to the square of the amplitude of the wave. The amplitude of the resultant wave is \(2a \cos\left(\frac{\phi}{2}\right)\), so the intensity \(I\) is given by:
\[
I = k \left(2a \cos\left(\frac{\phi}{2}\right)\right)^2 = 4ka^2 \cos^2\left(\frac{\phi}{2}\right)
\]
where \(k\) is a constant of proportionality.