Solution:
As we know;
nλ = dsinθ
i.e,
given d = 1/1000 mm => 10^-6 m or 1 micrometre
and
The n th-order maximum for each wavelength occurs at a specific angle.
All wavelengths are seen at θ =0, corresponding to n=0 as sinθ = 0 at 0 degrees.
next,the zeroth-order maximum (m=1) is observed at the angle that satisfies the relationship sin θ =λ/d
and the second-order maximum (m=2) is observed at a larger angle θ ....
Now using d= 10^-6 m
we get;
nλ = (10^-6) sinθ
and sinθ can take values between [0,1] as the angle takes values between: [0,90 ] degrees.
On an average:
nλ = (10^-6) (1/2)
=> nλ = 5 x 10^-7 m
For n = 1,2,3,4 . . .
=> λ = 5 x 10^-7 m , 2.5 x 10^-7 m , 1.667 x 10^-7 m
or
λ = 500 nm , 250 nm , 167 nm ,and so on . . . .
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