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Moving Charges and Magnetism Test - 67

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Moving Charges and Magnetism Test - 67
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  • Question 1
    1 / -0
    A moving coil galvanometer of resistance $$100 \space \Omega$$ is used as an ammeter using a resistance $$0.1 \space \Omega$$. The maximum deflection current in the galvanometer is $$100 \space \mu A$$.Find the minimum current in the circuit so that the ammeter shows maximum deflection.    
    Solution
    $$I_g G = \left (I - I_g \right )S$$. 
    Here, $$I_g = 100 \times 10^{-6} A$$
    $$G = 100 \space \Omega, S = 0.1 \space \Omega$$

    $$\therefore  I = I_g \left ( \dfrac{G} {S} + 1 \right ) = 100 \times 10^{-6} \left ( \dfrac{100} {0.1} + 1 \right )$$
    $$ = 100 \times 10^{-6} \times 1000.1 = 100.01 mA$$
  • Question 2
    1 / -0
    A magnetic field $$ \vec{B} = B_{0}\hat{j} $$ exists in the region $$ a  < x < 2a $$ and $$ \vec{B} = -B_{0}\hat{j} $$ , in the region $$ 2a < x < 3a $$ , where $$ B)_{0} $$ is a positive constant . A positive point charge moving with a velocity $$ \vec{v} = v_{0} \hat{i} $$ , where $$ v_{0} $$ is a positive constant , enters the magnetic field at $$ x = a $$ . The trajectory of the charge in this region can be like 

    Solution
     Force experienced by charge q is F = q(V × B) 
    In the region, x = a to  x = 2a, 
    $$F_1 = q(V_0i × B_0j) = qV_0B_0 \ k$$…..(i × j = k) 

    F1 is along positive z axis. In the region, x = 2a to 3a,

    $$ F_2 = q(V_0i × – B_0j) = – qV_0B_0\ k$$
     F2 is directed along negative z axis 

    ∵  F1 & F2 are perpendicular to velocity V. 
  • Question 3
    1 / -0
    Two infinite long wires, each carrying current I , are lying along x and y -axis , respectively .A charged particle, having a charge q and mass m, is projected with a velocity u along the straight line OP. the path of the particle is ( neglect gravity) 
    Solution
     $$\overrightarrow B$$ (magnetic field) at all the points lying on OP is zero  because both the wire cancels the effect of each other so u will not be affected by the magnetic force. Hence, it moves on a straight line.
  • Question 4
    1 / -0
    Bolt-savart law indicates that the moving electrons (velocity v) produce a magnetic field b such that
    Solution
    By Biot-savart law, $$ dB=\dfrac{I.dlsin\theta }{r^{2}} $$
    Or $$ dB= \dfrac{I\times dl}{r} $$
    acc to Biot-Savart law , if magnetic field is not perpendicular to the motion of charge then it will not move in helical path, which is not possible for motion of a charge in magnetic field. 
    So the magnetic field is perpendicular to the direction of flow of charge verifies answer 'a'.
  • Question 5
    1 / -0
    Two parallel wires are carrying electric currents of equal magnitude and in the same direction. They exert
    Solution
    Two straight conductors carry current in same direction, then attractive force acts between them.
  • Question 6
    1 / -0
    The radius of curvature of the path of the charges particles in a uniform magnetic field is directly proportional to
    Solution
    The radius of the circular path in the magnetic field is given by:

    $$r=\dfrac{mv}{qB}$$

    We know that $$mv$$ is the momentum of the body.

    $$\therefore r=\dfrac {p}{qB}$$

    $$\Rightarrow r\propto p$$
  • Question 7
    1 / -0
    Tick the most appropriate answer.
    Which of the following methods is used to magnetize a magnetic without touching it by a magnet?
    Solution
    Using electric current we can magnetize a magnetic material without touching it by a magnet.
  • Question 8
    1 / -0
    A magnetic field 
    Solution
    The force exerted by the magnetic field is given by:
    $$\vec F=q\vec v \times \vec B$$

    So, the force is exerted only when the charge particle is moving across the magnetic field lines.
  • Question 9
    1 / -0
    A proton (mass $$=1.67\times 10^{-27} kg$$ and charge $$=1.6\times 10^{-19}C$$) enters perpendicular to a magnetic field of intensity $$2$$ weber $$/m^2$$ with a velocity $$3.4\times 10^7\ m/sec$$. The acceleration of the proton should be
    Solution
    The force experienced by the proton due to the magnetic field provides an acceleration to it.
    $$F=ma=qvB $$

    $$\Rightarrow a=\dfrac {qvB}{m}$$

    $$=\dfrac {1.6\times 10^{-19}\times 2\times 3.4\times 10^{7}}{1.67\times 10^{-27}}$$

    $$=6.5\times 10^{15}\ m/sec$$
  • Question 10
    1 / -0
    Lorentx force can be calculate dby using the formula
    Solution
    Lorentz force is given by
    $$\vec F=\vec {F_e}+\vec {F_m}$$

    $$=q\vec E+q(\vec v \times \vec B)$$

    $$=q [\vec E+(\vec v\times \vec B)]$$
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