Chapter 9: Optics – Interference, Diffraction & Polarization (Set-3)

Diffraction of light is more pronounced when

A Aperture ≫ wavelength
B Aperture ≈ wavelength
C Aperture = infinity
D Light is incoherent

Fraunhofer diffraction refers to

A Diffraction with source and screen at finite distances
B Diffraction with source at infinity and screen at infinity (parallel rays)
C Near-field diffraction
D Reflection only

Fresnel diffraction refers to

A Far-field diffraction
B Near-field diffraction with curvature of wavefront important
C No diffraction
D Laser diffraction only

In single-slit Fraunhofer diffraction, minima occur when

A d sinθ = mλ
B a sinθ = mλ
C a sinθ = (m + ½)λ
D 2a sinθ = λ

The central maximum in single-slit diffraction is

A Narrower than side maxima
B Twice as wide as other maxima
C Equal width to other maxima
D Zero

Intensity in single-slit diffraction pattern is proportional to

A (sinβ/β)²
B cosβ
C tanβ
D sinβ

In single-slit diffraction, β =

A πa/λ sinθ
B a/λ
C θ/a
D None

Condition for principal maxima in single-slit diffraction is

A a sinθ = mλ
B a sinθ = (2m+1)λ/2
C No simple condition exists
D d sinθ = mλ

If slit width decreases in single-slit diffraction, the central maximum

A Narrows
B Widens
C Disappears
D Moves sideways

Diffraction effects dominate when

A Using very large lenses
B Aperture becomes small
C Light intensity increases
D Light is polarized

Double-slit diffraction pattern is

A Pure interference
B Pure diffraction
C Interference pattern modulated by single-slit diffraction envelope
D Random

In double-slit diffraction, fringe visibility decreases when

A Slits wider
B Slits narrower
C Wavelength decreases
D None

In diffraction gratings, principal maxima occur at

A a sinθ = mλ
B d sinθ = mλ
C 2d = mλ
D d/λ = m

Grating resolving power is given by

A λ/d
B
C mN
D N/d

Diffraction grating gives very sharp maxima because

A Large number of slits interfere
B Wide slits
C Light intensity low
D Source is incoherent

In Fresnel diffraction, the shape of fringes depends on

A Aperture shape
B Wavelength
C Geometry of obstacle
D All the above

Fresnel zones are

A Concentric circles representing regions of constructive/destructive interference
B Spectral regions
C Lens coatings
D Polarized domains

A zone plate focuses light due to

A Refraction
B Reflection
C Diffraction
D Polarization

A zone plate behaves like

A A diverging lens
B A converging lens (multiple focal points)
C Mirror
D Prism

In zone plate, the radii of zones follow

A rₙ ∝ n
B rₙ² ∝ n
C rₙ³ ∝ n
D rₙ constant

Diffraction through circular aperture results in

A No pattern
B Airy pattern
C Newton’s rings
D White centre

Angular resolution of a telescope (Rayleigh criterion) is

A 1.22 λ/a
B a/1.22λ
C λ/a²
D d/λ

Reducing aperture diameter does what to resolution?

A Improves it
B Worsens it
C No effect
D Random

The resolving power of a grating increases with

A Number of slits
B Decreasing slits
C Wavelength
D None

Missing orders occur in double-slit diffraction when

A d sinθ = mλ
B a/d = integer ratio leading to cancellation of certain maxima
C λ very small
D Slits very narrow

Intensity at the central maximum of a single slit is approximately

A Four times the secondary maximum
B Half of it
C Same as side lobes
D Zero

Grating spacing d decreases when

A Slits decrease in number
B Slits per unit length increase
C λ increases
D Light intensity decreases

For equal slit widths, diffraction envelope depends on

A Slit separation
B Wavelength
C Individual slit width
D Number of slits

In multiple-slit diffraction, principal peaks become

A Narrower and more intense
B Broader and weaker
C Random
D Disappear

Half-period zones in Fresnel theory contribute

A Additively
B Alternately with opposite phases
C Nothing
D Only destructively

Obstructing alternate Fresnel zones (zone plate idea)

A Eliminates diffraction
B Enhances one constructive contribution → focusing
C Creates polarization
D Creates dispersion

In single-slit diffraction, if wavelength increases, the diffraction pattern

A Widens
B Narrows
C Disappears
D No effect

For a given aperture, shorter wavelengths give

A Better resolution
B Worse resolution
C No change
D Zero diffraction

The grating element (d) is

A Width of single slit
B Total width of slit + spacing
C Twice the slit width
D Always 1 mm

A transmission grating works due to

A Reflection
B Refraction
C Diffraction + interference
D Polarization filtering

In Fresnel diffraction at straight edge, fringes are

A Uniform
B Non-uniform, hyperbolic
C Circular
D Absent

Fraunhofer diffraction uses

A Divergent waves
B Plane-wave illumination (far field)
C Spherical waves
D No optical elements

The first minima in circular aperture diffraction occurs at angle satisfying

A a sinθ = λ
B 1.22 λ/D
C λ/2D
D D/λ

The energy in diffraction pattern is

A Lost
B Redistributed
C Constant only at centre
D Infinite

In multi-slit interference, secondary maxima

A Strong
B Very weak
C Equal to main maxima
D Random

The free spectral range of a grating is

A λ²/d
B λ/m
C d/λ
D λ/N

A zone plate exhibits

A Chromatic aberration
B No focusing properties
C Monochromatic focus only
D Infinite focal points

Higher orders in diffraction grating appear at

A Smaller angles
B Larger angles
C No angle
D Always zero angle

If grating is illuminated with white light, different wavelengths

A Overlap
B Separate into spectra
C Disappear
D Become monochromatic

Diffraction efficiency depends strongly on

A Groove shape
B Wavelength
C Incidence angle
D All of these

Fresnel’s half-period theory explains

A Why diffraction cannot occur
B Why contributions partially cancel
C Why central maximum is bright
D Both B and C

In single-slit diffraction, if slit width doubles, width of central maximum

A Doubles
B Halves
C Increases four times
D Unchanged

Zone plate focal length decreases when

A Wavelength increases
B Zone radii decrease
C Zone spacing constant
D All above

Grating with 600 lines/mm has grating spacing

A 1/600 mm
B 600 mm
C 0.6 mm
D 6 mm

A circular aperture produces

A Rectangular diffraction
B Airy disc pattern
C Flat-top pattern
D Random fringes