Question #65193

A plane light wave of wavelength 580 nm falls on a long narrow slit of width 0.5 mm. (i) Calculate the angles of diffraction for the first two minima. (ii) How are these angles influenced if the width of slit is changed to 0.2 mm? (iii) If a convex lens of focal length 0.15 m is now placed after the slit, calculate the separation between the second minima on either side of the central maximum.

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Answer on Question #65194, Physics / Optics

A plane light wave of wavelength 580 nm falls on a long narrow slit of width 0.5 mm. (i) Calculate the angles of diffraction for the first two minima. (ii) How are these angles influenced if the width of slit is changed to 0.2 mm? (iii) If a convex lens of focal length 0.15 m is now placed after the slit, calculate the separation between the second minima on either side of the central maximum.

Solution:

The general condition for a minimum for a single slit is:


mλ=asinθm \lambda = a \sin \theta


where m=1,2,3,4m = 1, 2, 3, 4 and so on

- aa is the width of the slit,

- θ\theta is the angle of incidence at which the minimum intensity occurs, and

- λ\lambda is the wavelength of the light

(i)

The angle of diffraction for the first minimum:


θ1=sin1(λa)=sin1(580×1090.5×103)=0.0665\theta_1 = \sin^{-1} \left(\frac{\lambda}{a}\right) = \sin^{-1} \left(\frac{580 \times 10^{-9}}{0.5 \times 10^{-3}}\right) = 0.0665{}^\circ


The angle of diffraction for the second minimum:


θ1=sin1(2λa)=sin1(2×580×1090.5×103)=0.1329\theta_1 = \sin^{-1} \left(\frac{2\lambda}{a}\right) = \sin^{-1} \left(\frac{2 \times 580 \times 10^{-9}}{0.5 \times 10^{-3}}\right) = 0.1329{}^\circ


(ii)

The angle of diffraction for the first minimum:


θ1=sin1(λa)=sin1(580×1090.2×103)=0.1662\theta_1 = \sin^{-1} \left(\frac{\lambda}{a}\right) = \sin^{-1} \left(\frac{580 \times 10^{-9}}{0.2 \times 10^{-3}}\right) = 0.1662{}^\circ


The angle of diffraction for the second minimum:


θ1=sin1(2λa)=sin1(2×580×1090.2×103)=0.3323\theta_1 = \sin^{-1} \left(\frac{2\lambda}{a}\right) = \sin^{-1} \left(\frac{2 \times 580 \times 10^{-9}}{0.2 \times 10^{-3}}\right) = 0.3323{}^\circ


(iii) Distance of nth secondary minima from central maxima


yn=nλfay_n = \frac{n\lambda f}{a}


where f is focal length of converging lens.


y2=2×580×109×0.150.2×103=0.87×103 my_2 = \frac{2 \times 580 \times 10^{-9} \times 0.15}{0.2 \times 10^{-3}} = 0.87 \times 10^{-3} \text{ m}


Thus, the separation between the second minima on either side of the central maximum is


Δy=2y2=1.74×103 m\Delta y = 2y_2 = 1.74 \times 10^{-3} \text{ m}


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