The condition of diffraction minima is given by the following equation.
"bsin\u03b8 = m\u03bb"
b – is the split width
m – is the order of diffraction
λ is the wavelength
θ is the diffraction angle
"\u03b8 = sin^{-1}(\\frac{m\u03bb}{b})"
m = 2
b = 0.6 mm
λ = 600 nm
"\u03b8 = sin^{-1}(\\frac{2 \\times 600 \\times 10^{-7}}{0.6 \\times 10^{-1}}) = 0.002 \\;rad"
The angular position of second order minima on either side of the central maxima is twice that of angle θ.
θ’ = 2θ
"\u03b8\u2019 = 2 \\times 0.002 = 0.004\\;rad"
The separation between the second minima from central maxima is
d = θ’f
"d = 0.004 \\times 20 = 0.08 \\;cm"
The intensity distribution is given by the following equation.
"I = I_0(\\frac{sin^2\u03b2}{\u03b2^2})"
I0 is the intensity of principle maximum.
For the first maximum, the value of β is equal to 1.43π.
β = 1.43π
"I_1 = I_0(\\frac{sin^2(1.43\u03c0)}{(1.43\u03c0)^2}) = 0.0472I_0"
Calculate the ratio of intensities of the principle maximum to first order maximum as follows:
"\\frac{I_0}{I_1} = \\frac{I_0}{0.0472I_0} = 21"
The ratio of intensities of the principle maximum to first order maximum is 21.
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