# Diffraction In Wave Optics

Diffraction

• Diffraction is the phenomenon by virtue of whichlight bendswhile passing through aslit or an opening.
• The extent of bending depends upon the diameter of the slit.
• Both Interference and Diffraction are closely related to each other.
• Young replaced the two slits by a single slit in his single slit experiment.Therefore this experiment is also referred as Young’s single slit experiment.
• When the light passed through one slit a different type of pattern was observed on the screen.
• The pattern which was observed had a central maximum band and which was very wide as compared to interference pattern.
• There were alternate dark and bright bands and their intensity was decreasing on both the sides.
• The central maxima,was very wide whereas corresponding secondary maxima and minima were reduced in the intensity.
• The change in the pattern was formed due to diffraction instead of interference.

Conclusion:-

2. Alternate dark and bright bands on either side.
3. Intensity was decreasing on both sides.

Diffraction Fringe Pattern

Wave Optics - Diffraction Watch More Videos at: By: Mr. Pradeep Kshetrapal, Tutorials Point In. Jan 29, 2015 Diffraction in Wave Optics Overview The phenomenon of bending of the light and the obstacle is called diffraction. It is exhibited by not only the light waves but also by sound waves, Matter waves and water waves.

• In diffraction there is an incoming wave which passes through a single slit and as a result diffraction pattern was obtained on the screen.

## Diffraction In Wave Optics Worksheet

Diffraction pattern Maxima

• The incident wavefront is parallel to the plane of the slit. This shows they are in phase with each other.
• From the given figure:-
• Path difference =NP – LP
• =>NQ = a sinθ where a=width of the slit.
• The slit was divided into smaller parts M1, M2, N and L, and when contribution from each part is added up.
• At the central point θ =0. This implies path difference =0.
• This means all the parts of the slit will contribute completely. Therefore the intensity is the maximum.
• Central Maximum occurs at θ =0.

Problem:-The light of wavelength 600nm is incident normally on a slit of width 3mm.Calcluate the linear width of central maximum on a screen kept 3m away from the slit?

Wavelength λ =600nm =600 x10-9m.

Width of the slit a =3mm=3x10-3m.

Distance of the screen D=3m.

Condition for minima:-a sinθ =nλ

=>a sin θ =λ

=>sin θ = (λ/a) = (600 x10-9)/ (3x10-3)

=>θ =(600 x10-9)/(3x10-3)

=>(x/D) = (600 x10-9)/ (3x10-3)

=> x= (600 x 10-9 x3)/ (3 x10-3)

x=600 x 10-6m.

Therefore width =2x = 1200 x 10-6m

Width = 1.2 mm

Diffraction pattern Secondary Maxima

Scientist Fresnel found that secondary maxima occurred when the value of θ is:

• θ =(n+(1/2)) (λ/a)
• For n=1 =>θ =(3λ)/(2a) = (1.5λ/a) (equation 1)
• Where = (3λ)/ (2a) it lies midway between 2 dark fringes.
• Suppose if the slit is divided into 3 parts ,
• Consider the first 2/3rd part of the slit ,
• Path difference = (2/3) a x θ
• =(2/3) a x(3λ/2a) using (equation 1)
• Path difference =λ.
• The λ is getting divide into 2 halves with path difference =λ/2 and λ/2.
• Each of λ/2 gets cancel with another λ/2.
• Contribution from (2/3rd) part gets cancel out with each other.
• Therefore only (1/3rd) contributes to I(Intensity).
• Intensity ≠ 0.
• Intensity is reduced.
• For n=2 => θ =(5 λ)/(a)
• Only (1/5th) part will contribute.
• For n=3 =>θ =(7 λ)/(2a)
• Only (1/7th) part contributes.

Slit divided into 3 parts

Diffraction pattern for Minima

## Diffraction In Wave Optics

• Condition to get minima on the diffraction pattern:
• θ = (n λ/a); n= (+-) 1, (+-2)…
• For n=1, =>θ = (λ/a)
• Suppose the slit is divided into small parts. For every M1in the portion LM there exists another M2 in MN.
• From the figure it is clear that the contribution from all elements inLM (M1) will cancel out the contribution from all elements MN (M2).
• Therefore net intensity I=0 at θ = (λ/a).
• Minima occur at θ = (nλ/a). => aθ =nλ
• => a sinθ =nλ.
• Path difference = (nλ/a).
• Minima will occur ata sin θ =n λ. Where a =width of the slit,λ = wavelength of the light used.

Problem:- A beam of light consisting of two wavelengths, 650 nm and 520 nm, is used to obtaininterference fringes in a Young’s double-slit experiment.

(a) Find the distance of the third bright fringe on the screen from the centralmaximum for wavelength 650 nm.

(b) What is the least distance from the central maximum where the bright fringes dueto both the wavelengths coincide?

Wavelength of the light beam, λ1 =650nm

Wavelength of another light beam,λ2 =520nm

Distance of the slits from the screen = D

Distance between the two slits = d

(a) Distance of the nth bright fringe on the screen from the central maximum is given bythe relation,

x=nλ1(D/d)

For third bright fringe, n=3

Therefore x=3x650(D/d) =1950(D/d) nm

(b) Let the nth bright fringe due to wavelength and (n − 1)th bright fringe due towavelength λ1coincide on the screen. We can equate the conditions for bright fringesas:

2=(n-1)λ1

520n=650n-650

650=130n

Therefore, n=5.

Hence, the least distance from the central maximum can be obtained by the relation:

Note: The value of d and D are not given in the question.

Problem:- In a double-slit experiment the angular width of a fringe is found to be 0.2° on a screenplaced 1 m away. The wavelength of light used is 600 nm. What will be the angularwidthof the fringe if the entire experimental apparatus is immersed in water? Take refractiveindex of water to be 4/3.

Distance of the screen from the slits, D = 1 m

Wavelength of light used, λ1 =600nm

Angular width of the fringe in air θ1 =0.2o

## Wave Optics Class 12

Angular width of the fringe in water = θ2

Refractive index of water, μ= (4/3)

Refractive index is related to angular width as:

μ = (θ12)

θ2 = (3/4)θ1

## Diffraction In Wave Optics Theory

= (3/4)x0.2 =0.15

Therefore, the angular width of the fringe in water will reduce to 0.15°.

Problem:- A parallel beam of light of wavelength 500 nm falls on a narrow slitand the resulting diffraction pattern is observed on a screen 1 maway. It is observed that the first minimum is at a distance of 2.5mm from the centre of the screen. Find the width of the slit.

Wavelength of light beam, λ = 500 nm = 500 × 10−9 m

Distance of the screen from the slit, D = 1 m

For first minima, n = 1

Distance between the slits = d

Distance of the first minimum from the centre of the screen can be obtained as:

x = 2.5 mm = 2.5 × 10−3 m

It is related to the order of minima as:

n λ =x(d/D)

d= (n λD/x)

d= (1x500x10-9x1)/ (2.5 x10-3) = 2x 10-4 m

d=0.2mm

Therefore, the width of the slits is 0.2 mm.