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Electromagnetic Induction Test - 22

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Electromagnetic Induction Test - 22
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  • Question 1
    1 / -0
    Complete the following statement. For electromagnetic induction to occur:
    Solution
    Current is induced in a coil when flux through the coil changes. The flux through the coil changes when a magnet moves relative to the coil and coil is at rest relative to the magnet.
    Hence the correct answer is option B.
  • Question 2
    1 / -0
    A helicopter rises vertically with a speed of 100 m/s. If helicopter has length 10 m and horizontal component of earth's magnetic field is $$5\times 10^{-3} Wb/m^2$$, then the induced emf between the tip of nose and tail of helicopter is:
    Solution
    In case of motional emf, the motion of the conductor in the field exerts a force on the free charge in the conductor, so that one end of the conductor becomes positive, while the other negative resulting in a potential difference across its ends due to which a non-conservative electric field is set up in the conductor. In steady state the magnetic force on the free charge is balanced by the electric force due to induced field. 
    $$qE = qvB$$
    or $$q\left(\frac{V}{l}\right)=qvB$$
    ie, $$V=Bvl$$ 
    So, the induced emf between tip of nose and tail of helicopter is given by
     $$e=Bvl$$
    $$=5\times 10^{-3}\times 10\times 100$$
    $$=5V.$$
  • Question 3
    1 / -0
    If circular coil with $$N_{1}$$ turns is changed in to a coil of $$N_{2}$$ turns. What will be the ratio of self inductances in both cases.
    Solution

    If circular coil with N1 turns is changed in to a coil of N2 turns. 

    $$L=\dfrac{Nd \phi}{dt} $$
    $$L_1=\dfrac{N_1d \phi}{dt} $$
    $$L_2=\dfrac{N_2d \phi}{dt} $$ 
     L is in Henries
            N is the Number of Turns
            Φ is the Magnetic Flux
            Ι  is in Amperes
    $$\dfrac{L_1}{L_2}=\dfrac{N_1}{N_2} $$
  • Question 4
    1 / -0
     If coil is placed perpendicular to field lines then number of lines passing through coil are :
    Solution
    The magnitude of the induced emf in a circuit is proportional to the time rate of magnetic flux linked with the circuit.

    Consider a rectangular loop which rotates in a uniform magnetic field, around an axis in the plane of the loop and passing through the centres of opposite sides.

    If the area of the loop is A and the field strength is B and the normal to the loop makes an angle phi with the field direction at any instant, the flux through the loop at any time is B A cos phi. The flux is a maximum when the loop is normal to the field $$(\phi =0)$$ and zero when the loop is aligned parallel to the field $$(\phi =90).$$

    If the loop rotates with angular velocity w, then we can substitute phi = wt, and we can then write flux at any instant $$= A B cos wt.$$

    The induced emf is $$E =\dfrac{ - d (A B cos wt)}{dt}$$

    $$E= A B w sin wt.$$

    The answer to your question follows from that last expression. The induced emf is a sinusoidal function. It will be a minimum (that is zero), when phi = wt = 0, when the plane of the coil is normal to the field, and it will be maximum when $$\phi = wt = 90$$, or when the plane of the loop is parallel to the field
  • Question 5
    1 / -0
     Alternative current generator is basically based upon :
    Solution
    Alternative current generator is based on Faraday's Law.
    Faraday's Law states that when the magnetic flux linking a circuit changes,an emf is induced in the circuit proportional to the rate of change of flux linkage.
  • Question 6
    1 / -0
    Flux density under trailing pole tips in case of generator will :
    Solution
    LPT=leading pole tip
    TPT=tailling pole top
    Considering armature reaction.
    where GNA=Geometrical axis
    MNA=Magnetic neutral axis
    here clearly see that TPT side flux increases due to armature in case of generator.

  • Question 7
    1 / -0
    Alternating current is flowing in inductance L and resistance R. The frequency of source is $$\displaystyle\frac{\omega}{2\pi}$$. Which of the following statement is correct.
    Solution
    $$\begin{array}{l} \, \, As\, frequency\, approaches\, zero\, or\, DC,\, the\, inducators\, reac\tan  ce\, would\, decrease\, tozero\, , \\ acting\, like\, a\, short\, circuit.\, this\, means\, inductive\, reac\tan  ce\, is\, proportional\, to\, fequency \\ \, \, \, \, \, \, \, \, \, \, \, \, \, so\, ,\, for\, low\, frequency\, the\, { { limimiting } }\, \, value\, of\, impedance\, is\, L,\, and\, \, alternating\,  \\ current\, is\, flowing\, in\, inductance\, L\, and\, resistance\, R.\, \, The\, frequency\, of\, source\, is\, \frac { \omega  }{ { 2\pi  } } . \\ so\, the\, correct\, option\, is\, A. \end{array}$$
  • Question 8
    1 / -0
    In a transformer, coefficient of mutual inductance between primary and secondary coil is 0.2 H. When current changes by 5 Na in the primary, then: the induced era in the secondary will be 
    Solution
    $$e = M\dfrac{di}{dt} = 0.2\times5 = 1 V$$
  • Question 9
    1 / -0
    The dimensions of self-inductance L are :
    Solution
    Self-inductance L $$= \dfrac {e}{\Delta i/\Delta t}=\dfrac{e\Delta t}{\Delta i}$$
    $$\therefore $$ Unit of L$$=\dfrac{Volt-second}{Ampere}$$
    $$=\dfrac{(Joule/Coulomb)second}{Ampere}$$
    $$=\dfrac{Newton-metre-second}{Coulomb-ampere}$$
    $$\Rightarrow $$ Unit of L$$= \dfrac{Newton-metere}{Ampere^2}$$
    $$\therefore [L]=\dfrac{[MLT^2][L]}{[A^2]}=[ML^2T^{-2}A^{-2}]$$
  • Question 10
    1 / -0
    A coil carrying electric current is placed in uniform magnetic field, then :
    Solution
    As magnetic field is uniform so its rate of change with time is zero. By Faraday's law of induction, no emf is induced.

    But current carrying coil experience torque inside magnetic field, which is cross product of magnetic moment of the coil and the magnetic field.
    $$\vec{\tau}=\vec{M}\times\vec{B}$$

    Option A is correct.
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