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Electromagnetic Induction Test - 31

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Electromagnetic Induction Test - 31
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  • Question 1
    1 / -0
    When a current of 5 A flows in the primary coil then the flux linked with the secondary coil is 200 weber. The value of coefficient of mutual induction will be
    Solution
    Coefficient of mutual induction will be the ratio of the flux linked with the secondary coil and the current primary coil.

    $$ M = \dfrac{200}{5} = 40 H $$ 
  • Question 2
    1 / -0
    A straight copper wire is moved in a uniform magnetic field such that it cuts the magnetic lines of force. Then
    Solution
    As the copper wire cuts the magnetic lines of force, the free charges in the wire will experience a force and will get displaced. This displacement of charges in the wire creates a potential difference and hence emf is induced.
  • Question 3
    1 / -0
    The coefficient of mutual induction between two coils is $$1.25 H.$$ If the rate of fall of current in the primary is $$80$$ As$$^{-1}$$, then the induced emf in the secondary coil will be
    Solution
    emf = $$ - M \dfrac{dI}{dt}$$

    $$ = -1.25 \times -80= 100 V $$
  • Question 4
    1 / -0
    The rate of change of magnetic flux density through a circular coil of area 10 m and number of turns 100 is 10$$^3$$ Wb/m$$^2$$/s. The value of induced emf will be
    Solution
    $$emf =$$ rate of change of flux 
           $$=$$ area $$\times $$ number of turns $$\times $$ rate of change of flux density 
           $$= 10 \times  100 \times   1000 \\ =10^6 V $$ 
  • Question 5
    1 / -0
    A coil of area 80 cm$$^2$$ and number of turns 50 is rotating about an axis perpendicular to a magnetic field of 0.05 Tesla at 2000 rotations per minute. The maximum value of emf induced in it will be
    Solution
    $$Max. emf =n A B \omega $$

    $$= 50 \times 0.008 \times 0.05 \times 2000 \dfrac{2 \pi}{60} = \dfrac{4 \pi }{3} V $$
  • Question 6
    1 / -0
    If the turns ratio of a transformer is 2 and the impedance of primary coil is 250 W then the impedance of secondary coil will be
    Solution
    As shown in the image $$ L \propto N^2 $$
    and transformer has coils which cause impedance and impedance of a inductor is $$2 \pi fL$$
    so impedance of each coil $$ \propto N^2 $$
    so impedance of secondary coil $$={ Z }_{ p }{ (\dfrac { { N }_{ S } }{ { N }_{ P } }  })^{ 2 }\\=250*2^2 = 1000 \Omega$$

  • Question 7
    1 / -0
    The coefficient of self induction of a coil is given by
    Solution
    Inductance is the property of a conductor by which a change in current flowing through it induces (creates) a voltage (electromotive force) in both the conductor itself (self-inductance) and in any nearby conductors (mutual inductance). By Lenz's law the induced voltage opposed the the change in current. Hence inductance is defined as 
    $$L = - \dfrac{dI}{dt} $$
  • Question 8
    1 / -0
    Two circular conducting loops of radii $$R_1$$ and $$R_2$$ are laying concentrically in the same plane. If $$R_1$$ > $$R_2$$ then the mutual inductance (M) between them will be proportional to :
    Solution
    Let a current  $$I_1$$ flows through.the outer circular coil of radius $$R_1$$.
    The magnetic field at the centre of the coil is
    $$B_1=\dfrac{μ_0I_1}{2R_1}$$
    As the inner coil of radius $$R_2$$ placed co-axially has small radius $$(R_2<R_1)$$, therefore $$B_1$$ may be taken constant over its cross-sectional area.
    Hence, flux associated with the inner coil is
    $$\phi_2=B_1πR_2^2=\dfrac{μ_0I_1}{2R_1}πR_2^2$$

    As, Mutual Inducatance, $$M=\dfrac{ϕ_2}{I_1}=\dfrac{μ_0πR_2^2}{2R_1}$$

    ∴$$M\propto \dfrac{R_2^2}{R_1}$$
  • Question 9
    1 / -0
    The length of side of a square coil is 50 cm and number of turns in it is 100. If it is placed at right angles to a magnetic field which is changing at the rate of 4 Tesla/s, then induced emf in the coil will be :
    Solution
    emf =|e|= $$\dfrac{d\phi}{dt}$$=NA$$\dfrac{dB}{dt}$$
    rate of change of flux = $$N \times area \times $$ rate of change of magnetic field = $$100 \times 0.5^2 \times 4 = 100 V $$ 
  • Question 10
    1 / -0
    If a spark is produced on removing the load from an AC circuit then the element connected in the circuit is
    Solution
    On removal of load from the circuit, the circuit suddenly becomes an open circuit.
    Thus $$ \dfrac{di}{dt} \rightarrow \infty $$
    For sparking, high voltage must appear across the open ends. This will happen only in case of an inductor as the voltage drop across the inductor is $$ L\dfrac{di}{dt} $$
    Therefore, the circuit has high inductance.
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