Question #39082

Show that all Fresnel half-period zones have the same area.

Expert's answer

Answer on Question #39082, Physics, Optics

Show that all Fresnel half-period zones have the same area.

Solution.

Let the light source SS extends monochromatic spherical wave, PP - the point of observation. Through the point OO passes spherical wave surface. It is symmetric with respect to the line SPSP .



To determine the resultant effect at PP , Fresnel subdivided the wavefront into a number of circular zones I, II, III etc. Let PO=bPO = b . The radii of zones equal b+λ2,b+2λ2,b+3λ2b + \frac{\lambda}{2}, b + \frac{2\lambda}{2}, b + \frac{3\lambda}{2} ... etc. The area enclosed between O and O1O_1 , O1O_1 and O2O_2 , O2O_2 and O3O_3 etc. are known as half period zones. Each zone differs from its neighbour by a phase difference of π\pi or a path difference of λ/2\lambda / 2 . The area enclosed by the first circle of radius OO1OO_1 is called the first half period zone. The area enclosed by the annular strip O1O2O_1O_2 is known as second half period zone and so on. Thus, the annular area between (n-1)th circle and nth is the nth half period zone.

The area of the nth zone:


Sn=πOOn2OOn12=π[(POn2PO2)(POn12PO2)]=π[POn2POn12]==π[(b+nλ2)2(b+(n1)λ2)2]==π[b2+n2λ24+bnλb2(n1)2λ24bλ(n1)]==π[bλ+λ24(n2n21+2n)]=π[bλ+λ24(2n1)]\begin{array}{l} S _ {n} = \pi O O _ {n} ^ {2} - O O _ {n - 1} ^ {2} = \pi \left[ \left(P O _ {n} ^ {2} - P O ^ {2}\right) - \left(P O _ {n - 1} ^ {2} - P O ^ {2}\right) \right] = \pi \left[ P O _ {n} ^ {2} - P O _ {n - 1} ^ {2} \right] = \\ = \pi \left[ \left(b + \frac {n \lambda}{2}\right) ^ {2} - \left(b + \frac {(n - 1) \lambda}{2}\right) ^ {2} \right] = \\ = \pi \left[ b ^ {2} + \frac {n ^ {2} \lambda^ {2}}{4} + b n \lambda - b ^ {2} - \frac {(n - 1) ^ {2} \lambda^ {2}}{4} - b \lambda (n - 1) \right] = \\ = \pi \left[ b \lambda + \frac {\lambda^ {2}}{4} (n ^ {2} - n ^ {2} - 1 + 2 n) \right] = \pi \left[ b \lambda + \frac {\lambda^ {2}}{4} (2 n - 1) \right] \\ \end{array}

bλb \gg \lambda so λ2\lambda^2 term is negligible.

Thus,


Snπbλ.S _ {n} \approx \pi b \lambda .


The area of each half period zone (πbλ)(\pi b\lambda) is approximately same and independent of the order of zone.

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