Convex lens is illuminated by a plane wave which is propagating along z-axis. Sketch and nd out
mathematical expressions of wavefronts within each part of the optical system. Focus of both lenses are
f. The pattern t(x; y) is given as 1/2*[1+ cos(2x=10)]
Given data:
Pattern "t(x,y)=\\dfrac{1}{2}[1+cos(2\\pi x\/10)]"
"= \\frac{1}{2}[2cos^2(\\frac{\\pi x}{10})]=cos^2(\\pi x\/10)"
(a) Wave front behavior at f
"\\bar u =-f" [wave focus on focal point means intense wave form arises at focal point]
"\\dfrac{1}{v}-\\dfrac{1}{(-f)}=\\dfrac{1}{f}\\\\\\Rightarrow \\dfrac{1}{v}=0\\\\\\Rightarrow v= \\infty"
Image at infinity but density is squared
(b) Wave front behavior at 2f
[On 2f position wave normalize the wave front ]
"\\bar u =-2f\\\\\\dfrac{1}{v}=\\dfrac{1}{u}+\\dfrac{1}{f}=\\dfrac{1}{(-3f)}+\\dfrac{1}{f}=\\dfrac{2}{3f}\\\\\\Rightarrow So\\ Size = (\\dfrac{3}{2})times"
As the wave front is squared , So it is always it the positive direction
"\\dfrac{-v}{u}=\\dfrac{3}{2}" [At 2f] ; "\\dfrac{-v}{u}=\\infty" [At f]
(Magnification here infinity represent the order of t(x,y) is vary much less than order at f)
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