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Wave Optics Test - 32

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Wave Optics Test - 32
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  • Question 1
    1 / -0
    The wavefront of a light beam is given by the equation $$x+2y+3z=c$$ (where $$c$$ is arbitrary constant of light). What is the angle made by the light with the y-axis is
    Solution
    the wavefront equations must be of form $$ax+by+cz=1$$ where $$a^{2}+b^{2}+c^{2}=1$$ (a,b,c are cosines of angles made with x,y,z axes respectively)

    applying this to the given equation ,
    $$1^{2}+2^{2}+3^{2}=c^{2}$$
    $$c^{2}=14$$
    $$c=\sqrt{14}$$
    angle made with y-axis is $$cos ^{-1}\dfrac{2}{\sqrt{14}}$$
    option $$C$$ is correct. 
  • Question 2
    1 / -0
    In Young's interference experiment, if the slits are of unequal width, then
    Solution
    Unequal width of slits will cause unequal intensity of lights entering from both slits.
    As a result, during interference complete cancelling of light intensity will not take place at regions of otherwise dark fringe.
    As the value of $$\beta$$ does not depend on intensity of light, there will be no shifting of fringes as well as no change in fringe width.
    Answer. B) the positions of minimum intensity will not be completely dark.
  • Question 3
    1 / -0
    In a double-slit experiment, instead of taking slits of equal width, one slit is made twice as wide as the other. Then, in the interference pattern
    Solution
    Net intensity at any point on the screen due to two slits with incident intensities $$I_1,I_2$$ is given by
    $$I=I_1+I_2+2\sqrt{I_1I_2}\cos\phi$$
    When the slits are equal, $$I_1=I_2$$
    Thus $$I'=I_!+I_1+2\sqrt{I_1I_1}\cos\phi$$
    Not let the intensity due to second slit be $$I_2>I_1$$
    Then $$I''=I_1+I_2+2\sqrt{I_1I_2}\cos\phi>I'$$ for any $$\phi$$
  • Question 4
    1 / -0
    The resolving power of an electron microscope operated at 16 kV is R. The resolving power of the electron microscope when operated at 4 kV is
    Solution
    $$\sqrt{\dfrac{16}{4}}=\dfrac{R}{x}$$

    $$x=\dfrac{R}{2}$$

    option $$B$$ is correct 
  • Question 5
    1 / -0
    One of the two slits in YDSE is painted over, so that it transmits only light waves having intensity half of the intensity of the light waves having half of the intensity of the light waves through the other slit. As a result of this
    Solution
    Case 1: When slit are of equal width, if $$ { I }_{ o }$$ is intensity of light then,
    $$ { I }_{ max }={ I }_{ o }+{ I }_{ o }+2\sqrt { { I }_{ o }{ I }_{ o } } =4{ I }_{ o }$$
    $$ { I }_{ min }={ I }_{ o }+{ I }_{ o }-2\sqrt { { I }_{ o }{ I }_{ o } } =0$$
    Case 2: When one of the slit is painted over, its intensity would reduce to half then,
    $$ { I }_{ newmax }={ I }_{ o }/2+{ I }_{ o }+2\sqrt { { I }_{ o }{ I }_{ o }/2 } =2.932{ I }_{ o }$$
    $$ { I }_{ newmin }={ I }_{ o }/2+{ I }_{ o }-2\sqrt { { I }_{ o }{ I }_{ o }/2 } =0.068{ I }_{ o }$$
    Therefore, dark fringes get brighter and bright fringes get darker

  • Question 6
    1 / -0
    A certain region of a soap bubble reflects red light of vacuum wavelength $$\lambda=650nm$$. What is the minimum thickness that this region of the soap bubble could have? Take the index of reflection of the soap film to be $$1.41$$
    Solution
    By equation of destructive interference,
    thickness, $$t = \dfrac{1}{2}\dfrac{(m+0.5)\lambda}{1.41}$$
    where $$m$$ is any non-negative integer,
    $$\lambda=650*10^{-9}$$.
    For minimum thickness, take $$m=0$$
    So, $$t=1.152*10^{-7}\approx1.2*10^{-7}$$
  • Question 7
    1 / -0
    Light from a source travel out with a velocity c. If the source moves away from the observer with a velocity v, then relative velocity of light w.r.t observer is
    Solution
    Consider two particles with velocity u and w. The expression for the relative velocity can be given by

    $$ v = \dfrac{w-u}{1-\dfrac{wu}{c^2}} $$

    If one of the particles is light, $$w=c$$.

    This gives relative velocity of light $$v=c$$.
  • Question 8
    1 / -0

    Directions For Questions

    When light from two sources (say slits $${S}_{1}$$ and $${S}_{2}$$) interfere, they form alternate dark and bright fringes. Bright fringe is formed at all points where the path difference is an odd multiple of half wavelength. At the condition of equal amplitudes, $${A}_{1}={A}_{2}=a$$, the maximum intensity can also be indicated with phase factor as $$I=2{a}^{2}\cos ^{ 2 }{ \left( \phi /2 \right)  } $$.

    ...view full instructions

    If the path difference between the slits $${S}_{1}$$ and $${S}_{2}$$ is $$\lambda$$, the central fringe will have an intensity of
    Solution
    Path difference at the central fringe will be the same as the path difference at the slits i.e. $$\lambda$$.
    Hence, the waves reaching the central fringe will be $$180^o$$ out of phase and will result in destructive interference. Hence, the intensity of the central fringe will be 0. 
  • Question 9
    1 / -0
    A thin slice is cut out of a glass cylinder along a plane parallel to its axis. The slice is placed on a flat glass plae as shown in figure. The observed interference fringes from this combination shall be

    Solution
    The locus of the equal path difference consists in lines going parallel to the axis of cylinder. 
    Therefore, interference fringes will be straight. 
  • Question 10
    1 / -0
    Resolving power of a telescope increases with
    Solution
    Resolving power $$= \displaystyle \dfrac{\lambda}{d \lambda}$$ plane transmission granting 

    Resolving power for telescope

    $$= \displaystyle \frac{1}{\text{limit of resolution}} = \dfrac{d}{1.22 \lambda} = \dfrac{d_0}{d_1}$$

    by increasing the aperture of objective resolving power can be increased.
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