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Electromagnetic Induction Test - 38

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Electromagnetic Induction Test - 38
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  • Question 1
    1 / -0
    The current $$i$$ in an induction coil varies with time $$t$$ according to the graph shown in the figure. Which of the following graphs shows the induced emf ($$\varepsilon $$) in the coil with time?

    Solution
    When the current is constant, the induced emf is zero as $$emf=-\dfrac { Ldi }{ dt } $$ and when the current decreases at constant rate the emf is a positive constant and when it increase at constant rate it is a negative constant.
  • Question 2
    1 / -0
    In figure, if the current $$i$$ decreases at a rate $$\alpha$$, then $${V}_{A}-{V}_{B}$$ is

    Solution
    For an inductor
    $$ \Delta V = L \cfrac{di}{dt}$$
    Given
    $$\cfrac{di}{dt}= - \alpha$$
    $$V_A-V_B = - \alpha L$$
  • Question 3
    1 / -0
    In the figure shown, a T-shaped conductor moves with constant angular velocity $$\omega$$ in a plane perpendicular, to uniform magnetic field $$\vec { B } $$. The potential difference $${V}_{A}-{V}_{B}$$ is

    Solution
    Since potential difference in a moving conductor is produced in a direction perpendicular to the direction of velocity, potential difference is not produced along the length of AB.
  • Question 4
    1 / -0
    If the instantaneous magnetic flux and induced emf produced in a coil is $$\phi$$ and $$E$$ respectively, then according to Faraday's law of electro magnetic induction:
    Solution
    Farady's law states that time varying magnetic flux can induce an e.m.f.
    E = Electric field, Induced
    $$E = - \cfrac{d \phi}{dt}$$

    $$E = - \cfrac{d \phi}{dt}$$
    $$E =0$$ only if $$ \cfrac{d \phi}{dt} =0$$
    If $$E=0$$, then $$\phi = const.$$
    $$E \ne 0$$, then $$ \phi $$ is changing
  • Question 5
    1 / -0
    In figure, there is a conducting ring having resistance $$R$$ placed in the plane of paper in a uniform magnetic field $${B}_{0}$$. If the ring is rotating in the plane of paper about an axis passing through point $$O$$ and perpendicular to the plane of paper with constant angular speed $$\omega$$ in clockwise direction, then 

    Solution
    The ring can be seen as two rod OCA and  OBA in parallel.

    The motional emf will be induced between O and A = $$\dfrac{1}{2} B (2r)^2 \omega = 2Br^2 \omega $$ with A positibe wrt O

    In both the paths from O - C - A ; and from O - B - A ,  potential increases as one moves from point O to point A.
    Point B and C are at same potential due to symmetry.
    As there is no return path, no current flows even though a potential is developed between points O and A 
  • Question 6
    1 / -0
    A wooden stick of length $$3l$$ is rotated about an end with constant angular velocity $$\omega$$ in a uniform magnetic field $$B$$ perpendicular to the plane of motion. If the upper one-third of its length is coated with copper, the potential difference across the whole length of the stick is

    Solution
    Force on one electron in the rod, at a point r form center, due to the motion = $$F= q \vec v \times \vec B = q_e r \omega B $$

    total emf = $$ \int_{2l}^{3l}{\dfrac{F}{q_e} dr}= \int_{2l}{3l}{ r \omega B dr} $$

    $$= B \omega (\dfrac{9l^2}{2} - \dfrac{4l^2}{2} ) = B \omega \dfrac{ 5 l^2}{2} $$
  • Question 7
    1 / -0
    A horizontal straight conductor when placed along south-north direction falls under gravity; there is
    Solution

    $$\bullet$$We Know induced emf $$\vec E=\vec B.(\vec l \times \vec v)$$

    $$\bullet$$The earth's magnetic field lines are along the north south direction which is parallel to the length of the moving rod. 

    Therefore, no emf is induced along the length in the rod.

    $$Answer:$$

    Hence, option C is the correct answer. 

  • Question 8
    1 / -0
    A metal disc of radius $$a$$ rotates with a constant angular velocity $$\omega$$ about its axis. The potential difference between the center and the rim of the disc is ($$m=$$ mass of electron, $$e=$$ charge on electron)
    Solution
    For second law of Motion,
    $$F=ma$$
    $$eE=mw^2r$$
    $$E=\dfrac{mw^2r}{e}$$
    The potential difference $$V=\int E.dr$$
    $$V=\dfrac{\int_{0}^{a}mw^2r}{e}=\dfrac{mw^2a^2}{2e}$$
  • Question 9
    1 / -0
    Two identical cycle wheels (geometrically) have different number of spokes connected from center to rim. One is having $$20$$ spokes and the other having only $$10$$ (the rim and the spokes are resistanceless). One resistance of value $$R$$ is connected between center and rim. The current in $$R$$ will be
    Solution

  • Question 10
    1 / -0
    A uniform magnetic field exists in a region given by $$\vec { B } =3\hat { i } +4\hat { j } +5\hat { k } $$. A rod of length $$5m$$ along y-axis moves with a constant speed of $$1m$$ $${s}^{-1}$$ along x axis. Then the induced emf in the rod will be
    Solution

    $$ Given, B = 3 + 4 + 5k $$

    $$V = 1  m/s (As \ the \ rod \ moves \ in \

    X-Direction)$$

    $$Length \ of \ rod = 5 m$$

    $$Since, e = -d\phi /dt  \ and \ \phi = B.A $$  

    $$So, e = -d(B.A )/dt$$  

    $$ e = d(B.A)/dt   ( Negative \ sign \ is \

    neglected \ as \ it \ only \ represents  \ the \

    direction)$$ 

    $$ e = B.d(A)/dt   ( Magnetic \ Field \ is \ constant

    )$$ 

    $$ = B.d(l\times b)/dt  ( Where \ l = Length \ and \ b = Breadth

    )$$ 

    $$ = l B. d(b)/dt ---- (1) $$ 

    As $$db/dt$$ is nothing but the velocity with which the rod is moving.

    $$So, db/dt = V $$ 

    Putting  the  above  value  of  $$db/dt$$ in  equation  (1)
    We  have, $$e = l B.V $$

    But, in the above equation it is assumed that the direction of B,  L  and V are mutually perpendicular.

    So,  Only  that component   of  B that  is  in  mutual perpendicular  direction  of  L  and  V will  be  taken into  account.

     $$ So, e = l B.V   = 5 \times 5 \times 1 $$

        $$  e  = 25 V$$
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