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Electromagnetic Induction Test - 35

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Electromagnetic Induction Test - 35
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  • Question 1
    1 / -0
    Two coils, A and B, are lined such that emf $$\epsilon$$ is induced in B when the current in A is changing at the rate $$I$$. If $$i$$ current is now made to flow in B, the flux linked with A will be :
    Solution
    Let $$M=$$ mutual inductance between A and B.

    $$\epsilon_B=M\dfrac {di_A}{dt}$$ or $$\epsilon_B=MI$$ or 

    $$M=\epsilon_B/I$$

    where $$I=di_A/dt$$

    $$\phi_A=Mi_B=(\epsilon_B/I)i_B$$

    $$\therefore \phi_A=(\epsilon /I)i$$                                              $$ (\because i=i_B)$$
  • Question 2
    1 / -0
    Coils in the resistance boxes are made from doubled up insulated wires
    Solution
    The wire is doubled back on itself. As a result ,there are equal and opposite currents in each section of the coil. Therefore ,the coil has no net magnetic field and no net induced e.m.f.
    Thus, it is done to minimize the inductance of coils.
  • Question 3
    1 / -0
    If a current increases from zero to one ampere in 0.1 second in a coil of 5 mH, then the magnitude of the induced e.m.f. will be
    Solution
    $$\varepsilon=L\times (rate \ of \ change \ of \ current)$$

    $$=(5\times 10^{-3})(1/0.1)$$

    $$=0.05V$$.
  • Question 4
    1 / -0
    The SI unit of inductance, the henry can be written as
    Solution
    $$ e = \dfrac{d\phi}{dt} = L\dfrac{dI}{dt} $$

    $$\Rightarrow [volt] = \dfrac{[weber]}{[second]} = [L]\dfrac{[Ampere]}{[second]}$$

    also,
    Energy dissipated(E) $$ = VIt$$

    $$\Rightarrow [Joule] = [volt][Ampere][second] \ Rightarrow [volt-second] = \dfrac{[Joule]}{[Ampere]}$$

    so units of self inductance L is,

    $$[L] = \dfrac{weber}{Ampere} = \dfrac{volt - second}{Ampere} = \dfrac{Joule}{Ampere^2}$$
  • Question 5
    1 / -0
    A copper ring is suspended by a thread in a vertical plane. If one end of a magnet is brought horizontally towards the ring in plane of ring as shown, the ring will

    Solution
    Answer is B.

    The magnetic flux is given by $$\phi= BA cos \theta$$ where $$\theta$$ is angle between magnetic field and area of ring.
    in this case the area vector is out of the plane, hence $$\theta=90^\circ{}$$,
    $$\Rightarrow \phi =0$$
    The ring will not move from the magnet, as there is no change in flux through ring and current in it will be zero. Ring will not behave as a magnet.
  • Question 6
    1 / -0
    A generator has an e.m.f. of 440 volt and internal resistance of 400 ohm. Its terminals are connected to a load of 4000 ohm. The voltage across the load is:
    Solution
    Total resistance of the circuit$$=4000+400=4400\ W$$
    Current flowing $$i=\dfrac {V}{R}=\dfrac {440}{4400}=0.1\ A$$.
    Voltage across load $$V_L = Ri=4000\times 0.1=400\ V$$.
  • Question 7
    1 / -0
    A rectangular coil of single turn, having area A, rotates in a uniform magnetic field B with an angular velocity $$\omega$$ about an axis perpendicular to the field. If initially the plane of the coil is perpendicular to the field, then the average induced emf when it has rotated through $$90^o$$ is:
    Solution
    Initially flux, $$\phi=BA cos 0=BA$$
    After rotating through an angle $$90^o$$.
    Flux through the coil is zero.
    So, $$\Delta \phi=BA$$

    Angular speed $$=w$$, so, time period $$=\dfrac {2\pi}{\omega}=T$$

    $$\dfrac {T}{4}$$ is time taken to rotate $$90^o$$.

    So, $$\dfrac {\Delta \phi}{\Delta t}=\dfrac {BA}{T/4}=\dfrac {2BA\omega}{\pi}$$
  • Question 8
    1 / -0
    A coil has 200 turns and area of $$70 cm^2$$. The magnetic field perpendicular to the plane of the coil is $$0.3 Wb/m^2$$ and take 0.1 sec to rotate through $$180^o$$. The value of the induced e.m.f. will be
    Solution
    Change in flux $$=2BAN$$

    $$\therefore$$ Induced e.m.f. $$=\dfrac {2\times 0.3\times 200\times 70\times 10^{-4}}{0.1}$$

    $$=8.4V$$
  • Question 9
    1 / -0
    According to Faraday's law of electromagnetic induction:
    Solution
    According to Faraday's Law of electromagnetic induction, if magnetic flux through a coil changes, it leads to an induced emf across the coil. Hence, electric field is produced by time-varying magnetic fields.
  • Question 10
    1 / -0
    If coefficient of self induction of a coil is 1 H, an e.m.f. of 1 V is induced, if
    Solution
    Induced EMF $$E =-L\dfrac{di}{dt}$$...(i)

    Given $$E=1\ V$$, $$L=1  \ H$$

    $$\Rightarrow \dfrac{di}{dt} =1 A/s$$
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