A double-slit interference experiment is done in a ripple tank. The slits are 4.90 cm apart, and a viewing screen is 1.56 m from the slits. The wave speed of the ripples in water is 0.027 m/s, and the frequency of the oscillator producing the ripples is 5.10 Hz. How far from the centerline of the screen will the first order maxima be found?
Let's call the position on the screen away from the centreline \(y\), the distance from the slits to the screen \(D\) = 1.56 m, the separation of the slits \(d\) = 4.9 cm, and the angle of diffraction \(\theta\). The wavelength \(\lambda\) is the wavespeed divided (0.027 m/s) by the frequency (5.1 Hz). The difference in path length from each slit to a point \(y\) on the screen is \(d\sin\theta\) where \(y\) is related to \(theta\) by \[\tan\theta=\frac{y}{D}\] The condition for the first order maximum is that the difference in path length must be 1 wavelength. \[d\sin\theta=\lambda\] \(y\) may be worked out thus: \[y=D\tan\sin^{-1}\Big(\frac{\lambda}{d}\Big)\] or you could use the small-angle approximation \[y = \frac{\lambda D}{d}\] In case the LaTeX on this website doesn't render for you (it doesn't for me), I've attached my answer compiled as a PDF
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