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Question: A beam of light of wavelength 600 nm from a distinct source falls on a single slit \( 1.0mm \) wide ...

A beam of light of wavelength 600 nm from a distinct source falls on a single slit 1.0mm1.0mm wide and the resulting diffraction pattern is observed on a screen 2 m away. The distance between the first dark fringes on either side of the central bright fringe is?

Explanation

Solution

Hint : In single slit diffraction, the dark fringe is located at an integral multiple of the wavelength. The difference between the locations of the dark fringes on either side gives us the distance between them.

Formula used: In this solution we will be using the following formula;
y=mλDdy = \dfrac{{m\lambda D}}{d} where yy is the location of the dark fringes from the central maximum, mm is the mth place of the particular dark fringe on either side of the central maximum. (given as m=....3,2,1,0,1,2,3,....m = .... - 3, - 2, - 1,0,1,2,3,.... ), λ\lambda is the wavelength of the light, DD is the distance of the screen from the slit, and dd is the width of the single slit.

Complete step by step answer
In single slit diffraction, a light wave is incident on a single slit of a particular width, a diffraction pattern, quite similar but different to double slit, is obtained on a screen at a distance away. In this diffraction pattern, the location of the dark fringes is given as
y=mλDdy = \dfrac{{m\lambda D}}{d} where mm is the place (integer position) of the particular dark fringe, λ\lambda is the wavelength of the light, DD is the distance of the screen from the slit, and dd is the width of the single slit. mm takes the values …-3, -2, -1, 0, 1, 2, 3… depending on which side of the central maximum it is.
Hence, for the first dark fringe on one side, we have
y=(1)λDdy = \dfrac{{\left( 1 \right)\lambda D}}{d} , inserting all known values, we get
y=600×109(2)0.001=0.0012my = \dfrac{{600 \times {{10}^{ - 9}}\left( 2 \right)}}{{0.001}} = 0.0012m
Similarly, for the bright fringe on the other side, the distance is simply
y=(1)λDdy = \dfrac{{\left( { - 1} \right)\lambda D}}{d} , which by insertion of known values will give
y=600×109(2)0.001=0.0012my = \dfrac{{ - 600 \times {{10}^{ - 9}}\left( 2 \right)}}{{0.001}} = - 0.0012m
The distance between them is hence,
Δy=0.0012(0.0012)=0.0024m\Delta y = 0.0012 - \left( { - 0.0012} \right) = 0.0024m
Δy=2.4mm\therefore \Delta y = 2.4mm .

Note
Alternatively, since the location of the bright fringes are equal from on both sides from the central maximum, then the distance between then is simply twice the distance of one from the central maximum as in:
Δy=2λDd\Delta y = 2\dfrac{{\lambda D}}{d}
Hence, by insertion of values again
Δy=2600×109(2)0.001=0.0024m\Delta y = 2\dfrac{{600 \times {{10}^{ - 9}}\left( 2 \right)}}{{0.001}} = 0.0024m