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Wave Optics question

2019 · Shift 2 · Q42
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Wave Optics question

2019 · Shift 2 · Q42

JEE AdvancedPhysicsWave OpticsMultiple correct+4 / −1
In a Young's double slit experiment, the slit separation d is 0.3 mm and the screen distance D is 1 m. A parallel beam of light of wavelength 600 nm is incident on the slits at angle α\alphaα as shown in figure. JEE Advanced 2019 Paper 2 Offline Physics - Wave Optics Question 17 English On the screen, the point O is equidistant from the slits and distance PO is 11.0 mm. Which of the following statement(s) is/are correct?
  1. A
    For α\alphaα = 0, there will be constructive interference at point P.
  2. B
    For α=0.36π\alpha = {{0.36} \over \pi }α=π0.36​ degree, there will be destructive interference at point P.
  3. C
    For α\alphaα=α=0.36π\alpha = {{0.36} \over \pi }α=π0.36​ degree, there will be destructive interference at point O.
  4. D
    Fringe spacing depends on α\alphaα.
View written solutionFree

Correct answer: B

  1. Given data
  • Slit separation: d=0.3 mm=3×10−4 md = 0.3\text{ mm} = 3\times 10^{-4}\text{ m}d=0.3 mm=3×10−4 m
  • Screen distance: D=1 mD = 1\text{ m}D=1 m
  • Wavelength: λ=600 nm=6×10−7 m\lambda = 600\text{ nm} = 6\times 10^{-7}\text{ m}λ=600 nm=6×10−7 m
  • Distance PO=11.0 mm=1.1×10−2 mPO = 11.0\text{ mm} = 1.1\times 10^{-2}\text{ m}PO=11.0 mm=1.1×10−2 m

In YDSE, fringe width is

β=Dλd\beta = \frac{D\lambda}{d}β=dDλ​

So,

β=1⋅6×10−73×10−4=2×10−3 m=2 mm\beta = \frac{1\cdot 6\times 10^{-7}}{3\times 10^{-4}} = 2\times 10^{-3}\text{ m} = 2\text{ mm}β=3×10−41⋅6×10−7​=2×10−3 m=2 mm

Thus point PPP is at

POβ=112=5.5\frac{PO}{\beta} = \frac{11}{2} = 5.5βPO​=211​=5.5

fringe widths from OOO.


  1. Path difference with oblique incidence

If the incident beam makes angle α\alphaα, then there is an initial path difference at the slits:

Δi=dsin⁡α\Delta_i = d\sin\alphaΔi​=dsinα

At a point at transverse distance yyy on the screen, the geometric path difference due to position is

Δg=dyD\Delta_g = \frac{dy}{D}Δg​=Ddy​

Hence net path difference is

Δ=dyD−dsin⁡α\Delta = \frac{dy}{D} - d\sin\alphaΔ=Ddy​−dsinα

(up to sign convention; only condition for maxima/minima matters).

Therefore,

  • Bright fringe: Δ=nλ\Delta = n\lambdaΔ=nλ
  • Dark fringe: Δ=(n+12)λ\Delta = \left(n+\tfrac12\right)\lambdaΔ=(n+21​)λ

  1. Check option A: α=0\alpha=0α=0 at point PPP

For α=0\alpha=0α=0,

Δ=dyD\Delta = \frac{dy}{D}Δ=Ddy​

At PPP, y=11 mmy=11\text{ mm}y=11 mm, so

Δ=(3×10−4)(11×10−3)1=3.3×10−6 m\Delta = \frac{(3\times10^{-4})(11\times10^{-3})}{1} = 3.3\times10^{-6}\text{ m}Δ=1(3×10−4)(11×10−3)​=3.3×10−6 m

Now,

Δλ=3.3×10−66×10−7=5.5\frac{\Delta}{\lambda} = \frac{3.3\times10^{-6}}{6\times10^{-7}} = 5.5λΔ​=6×10−73.3×10−6​=5.5

So,

Δ=5.5λ=(5+12)λ\Delta = 5.5\lambda = \left(5+\tfrac12\right)\lambdaΔ=5.5λ=(5+21​)λ

This is destructive, not constructive.

So A is false.


  1. Evaluate α=0.36π\alpha = \dfrac{0.36}{\pi}α=π0.36​ degree

Convert to radians:

α=0.36π⋅π180=0.36180=0.002 rad\alpha = \frac{0.36}{\pi}\cdot \frac{\pi}{180} = \frac{0.36}{180} = 0.002\text{ rad}α=π0.36​⋅180π​=1800.36​=0.002 rad

Since angle is small,

sin⁡α≈0.002\sin\alpha \approx 0.002sinα≈0.002

Thus,

dsin⁡α=3×10−4×0.002=6×10−7 m=λd\sin\alpha = 3\times10^{-4}\times 0.002 = 6\times10^{-7}\text{ m} = \lambdadsinα=3×10−4×0.002=6×10−7 m=λ

So oblique incidence introduces path difference of exactly one wavelength.


  1. Check option B: destructive interference at PPP

At PPP,

Δg=dyD=5.5λ\Delta_g = \frac{dy}{D} = 5.5\lambdaΔg​=Ddy​=5.5λ

Net path difference:

Δ=5.5λ−λ=4.5λ\Delta = 5.5\lambda - \lambda = 4.5\lambdaΔ=5.5λ−λ=4.5λ

Since

4.5λ=(4+12)λ4.5\lambda = \left(4+\tfrac12\right)\lambda4.5λ=(4+21​)λ

it is destructive interference.

So B is true.


  1. Check option C: destructive interference at OOO

At point OOO, y=0y=0y=0, so

Δ=−dsin⁡α=−λ\Delta = -d\sin\alpha = -\lambdaΔ=−dsinα=−λ

Magnitude of path difference is λ\lambdaλ, i.e. an integral multiple of wavelength. Hence interference is constructive, not destructive.

So C is false.


  1. Check option D: fringe spacing depends on α\alphaα

Position of bright fringes is given by

dyD−dsin⁡α=nλ\frac{dy}{D} - d\sin\alpha = n\lambdaDdy​−dsinα=nλ

So,

yn=Dsin⁡α+nDλdy_n = D\sin\alpha + n\frac{D\lambda}{d}yn​=Dsinα+ndDλ​

This shows that α\alphaα only shifts the whole fringe pattern by Dsin⁡αD\sin\alphaDsinα. The spacing between consecutive fringes is still

β=Dλd\beta = \frac{D\lambda}{d}β=dDλ​

which is independent of α\alphaα.

So D is false.


  1. Final conclusion

Only option B is correct.

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