31 NEET previous-year questions on Wave Optics, each with the correct answer and a step-by-step solution. Filter by topic and expand any question to see how to solve it.
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d/λD
λD/d
D/λd
λ/dD
Solution
.
A surface of constant intensity
A surface of constant phase
A line of light propagation
A point source
Solution
Wavefront: surface where every point has the same phase.
Two sources of any kind
Coherent sources
Equal amplitude only
Equal frequency only
Solution
Coherent: same f and constant phase difference.
Longitudinal
Transverse
Stationary
Circular
Solution
Only transverse waves can be polarised.
sin θ_B = n
tan θ_B = n
cos θ_B = n
cot θ_B = n
Solution
.
0.5 mm
1.0 mm
1.5 mm
2.0 mm
Solution
m = 1.5 mm.
λD/a
2λD/a
λa/D
a/λD
Solution
.
Parallel
Anti-parallel
Perpendicular
Same intensity
Solution
At θ_B, reflected and refracted rays are exactly 90° apart.
500 nm
600 nm
750 nm
450 nm
Solution
Shift in fringes nm.
I = I_0 cos θ
I = I_0 sin θ
I = I_0 cos² θ
I = I_0 sin² θ
Solution
.
I_1 + I_2
(√I_1 + √I_2)²
(√I_1 - √I_2)²
I_1·I_2
Solution
.
I_0
2 I_0
4 I_0
0
Solution
Equal coherent sources: .
a sin θ = λ
a sin θ = λ/2
a cos θ = λ
a sin θ = 2λ
Solution
First minimum at .
D/(1.22λ)
1.22λ/D
D·λ
λ/(1.22D)
Solution
.
I_0
I_0/2
I_0/4
I_0/8
Solution
After first: . After second at 60°: .
Unpolarised
Plane-polarised perpendicular to plane of incidence
Plane-polarised parallel to plane of incidence
Circularly polarised
Solution
Reflected ray fully polarised perpendicular to plane of incidence.
Doubled
Halved
Quadrupled
Same
Solution
. New .
Plane
Spherical
Cylindrical
Disturbed
Solution
A plane wavefront stays plane (just slows down) when entering a uniform medium.
(n - 1)t
(n - 1)tD/d
nt
t
Solution
Shift .
λD/d
2λD/d
3λD/d
7λD/(2d)
Solution
. n = 3 → .
Same intensity
Half intensity
Zero
Quarter intensity
Solution
for unpolarised through ideal polariser.
5 mm
10 mm
50 mm
100 mm
Solution
m = 10 mm.
0.6 µrad
6 µrad
60 µrad
500 nrad
Solution
rad ≈ 0.6 µrad.
Increases
Decreases by factor 1.33
Stays same
Doubles
Solution
λ' = λ/n inside water. β shrinks by factor n.
I_0
I_0/2
I_0/4
0
Solution
Crossed polarisers: cos² 90° = 0.
30°
45°
56.3°
60°
Solution
.
Tangent to wavefront
Along wavefront
Perpendicular to wavefront
Parallel to source
Solution
Ray direction is the normal to the wavefront.
Same
Half
Twice
Four times
Solution
Central max is twice as wide as the side maxima.
3
6
9
12
Solution
Shift in fringes .
5I
9I
3I
8I
Solution
.
5:3
9:1
4:1
3:1
Solution
.
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