Posted by Jim on Saturday, March 31, 2012 at 4:11pm.
The condition for an intensity minimum is b sin á = k ë
where b is the slit width.
For 474 nm, there are minima at
sin á = 6.21*10^-3 (k=1)
1.242*10^-3 (k=2)
1.864*10^-2 (k=3)
2.484*10^-2 (k=4)
For 632 nm, there are minima at:
sin á = 8.283*10^-3 (k=1)
1.657*10^-3 (k=2)
2.485*10^-2 (k=3)
Clearly, the k=4 minimum of ë = 474 nm radiation coincides with the k = 3 minimum of 632 nm radiation. The distance from the central maximum is
d = 1.30 m*sin á = 3.23*10^-2 m
= 3.23 cm
For further reading, try
http://www.walter-fendt.de/ph14e/singleslit.htm
The a' symbol in my answer above was meant to be the diffraction angle alpha, and the e with two dots was supposed to be the wavelength, lambda
Let’s use the condition of diffraction minimum for one split of the width b
b•sinα =k1•λ1
b•sinα =k2•λ2,
Since we have superposition of two maxima b•sinα is the same for two wavelengths,
k1•λ1= k2•λ2,
λ1/λ2 = k2/k1,
632/474 = 4/3.
Therefore, k1=3, k2=4.
Now sinα = k1•λ1/b =3•632•10^-9/ 7.63•10^-5 =0.0248.
As the angle is very small tanα = sinα,
x=L• tanα =L• sinα =1.3•0.0248 =0.0323 m = 3.23 cm
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