Correct answer Carries: 4.
Wrong Answer Carries: -1.
What determines the visibility of interference fringes when light passes through two slits?
Coherence, or a constant phase difference between the waves from the slits, is essential for a visible, stable interference pattern.
What fundamental principle allows the prediction of a new wavefront’s shape from a known wavefront using secondary wavelets?
Huygens’ principle states that every point on a wavefront acts as a source of secondary wavelets, whose envelope forms the new wavefront.
What is the path difference for the seventh bright fringe in a double-slit experiment?
Constructive interference occurs at \( \Delta = n\lambda \). For the seventh bright fringe, \( n = 7 \), so \( \Delta = 7\lambda \).
What is the shape of the wavefront emitted by a point source at a large distance?
At a large distance from a point source, the spherical wavefront appears plane over a small region.
What prevents the formation of an interference pattern when two independent light sources are used?
Independent sources lack a fixed phase relationship (incoherence), causing rapid phase fluctuations that average out interference effects.
What is the refractive index of a medium if the speed of light in it is \( 2.25 \times 10^8 \, \text{m/s} \) and in vacuum is \( 3.0 \times 10^8 \, \text{m/s} \)?
Refractive index \( n = \frac{c}{v} \).
\( c = 3.0 \times 10^8 \, \text{m/s} \), \( v = 2.25 \times 10^8 \, \text{m/s} \).
\( n = \frac{3.0 \times 10^8}{2.25 \times 10^8} = 1.33 \).
What is the frequency of light with a wavelength of \( 480 \, \text{nm} \) in air, given the speed of light in air is \( 3.0 \times 10^8 \, \text{m/s} \)?
Frequency \( \nu = \frac{c}{\lambda} \).
\( \lambda = 4.8 \times 10^{-7} \, \text{m} \), \( c = 3.0 \times 10^8 \, \text{m/s} \).
\( \nu = \frac{3.0 \times 10^8}{4.8 \times 10^{-7}} = 6.25 \times 10^{14} \, \text{Hz} \).
What distinguishes the interference pattern of a double-slit experiment from the diffraction pattern of a single slit?
Interference involves superposition from two sources, producing evenly spaced fringes, while diffraction from one slit creates a broad central maximum with weaker secondary maxima.
What is the intensity of light transmitted through two polaroids with their pass-axes at \( 45^\circ \) to each other, if the initial intensity after the first polaroid is \( I_0 \)?
Using Malus’ law, \( I = I_0 \cos^2 \theta \).
For \( \theta = 45^\circ \), \( \cos 45^\circ = \frac{\sqrt{2}}{2} \), so \( I = I_0 \left(\frac{\sqrt{2}}{2}\right)^2 = I_0 \times \frac{1}{2} = \frac{I_0}{2} \).
Why does total internal reflection occur only when light travels from a denser to a rarer medium?
In a denser medium, the critical angle exists due to a lower speed, beyond which refraction cannot occur, leading to reflection; this doesn’t happen in the reverse direction.
What happens to the central maximum’s width in a single-slit diffraction pattern if the slit width is reduced to half?
Angular width \( 2\theta = \frac{2\lambda}{a} \). If \( a \) is halved, \( 2\theta \) doubles.
What is the distance of the fifth dark fringe from the central maximum in a double-slit experiment if \( \lambda = 650 \, \text{nm} \), \( d = 0.5 \, \text{mm} \), and \( D = 1.0 \, \text{m} \)?
Dark fringe position \( x_n = \frac{\left(n + \frac{1}{2}\right) \lambda D}{d} \). For the fifth dark fringe, \( n = 4 \).
\( \lambda = 6.5 \times 10^{-7} \, \text{m} \), \( d = 5.0 \times 10^{-4} \, \text{m} \), \( D = 1.0 \, \text{m} \).
\( x_4 = \frac{\left(4 + \frac{1}{2}\right) \times 6.5 \times 10^{-7} \times 1.0}{5.0 \times 10^{-4}} = \frac{4.5 \times 6.5 \times 10^{-7}}{5.0 \times 10^{-4}} = 5.85 \times 10^{-3} \, \text{m} = 5.85 \, \text{mm} \).
What is the nature of the interference pattern formed by incoherent sources?
Incoherent sources produce no stable interference pattern; intensities simply add up, resulting in uniform illumination.
In a single-slit diffraction pattern, what happens to the central maximum’s width if the slit width is tripled?
Angular width \( 2\theta = \frac{2\lambda}{a} \). If \( a \) is tripled, \( 2\theta \) is reduced to one-third.
What is the amplitude of the resultant wave when two coherent waves of amplitude \( a \) interfere with a phase difference of \( \pi/2 \)?
Resultant amplitude \( A = 2a \cos(\phi/2) \).
For \( \phi = \pi/2 \), \( A = 2a \cos(\pi/4) = 2a \times \frac{\sqrt{2}}{2} = a\sqrt{2} \).
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