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Moving Charges and Magnetism Test - 59

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Moving Charges and Magnetism Test - 59
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  • Question 1
    1 / -0
    The incorrect statement of the following is:
    Solution
    Movement of charge in a straight line results in a magnetic field being generated from the relation $$F=qvB\sin\theta$$
  • Question 2
    1 / -0
    A proton and an alpha particle are separately projected in a region , where a uniform magnetic field exists. The initial velocities are perpendicular to the direction of magnetic field . If both the particles move along circles of equal radii , the ratio of momentum of proton to alpha particle( $$\dfrac{P_p}{P_a}$$)
    Solution

  • Question 3
    1 / -0
    If an electron of velocity $$(2\hat{i}+3\hat{j})$$ is subjected to magnetic field of $$4\hat{k}$$, then its:-
    (a) path will change
    (b) speed does not change
    (c) path must be circular
    (d) momentum is constant.
    Solution
    As shown, the Lorentz Force on the electron is: $$e(\vec{V} \times \vec {B})$$
    In this case, it is given by:
    $$e((2\hat { i } +3\hat { j } )\times 4\hat { k } )=e(3\hat { i } -8\hat { j } )$$

    which shows that the force acts at some angle to the velocity.
    Hence its path would change.

    Also, a magnetic field always acts perpendicular to s=displacement, therefore no work is done. Hence, the change in kinetic energy is zero (Work-Energy theorem). Therefore the speed will not change.
  • Question 4
    1 / -0
    A charged particle moves in a uniform magnetic field perpendicular to it, with a radius of curvature 4 cm. On passing through a metallic sheet it looses  half of its kinetic energy, then the radius of curvature of the particle is :
    Solution
    $$R= \dfrac{mv}{qB} =\dfrac{m}{qB}\sqrt{\dfrac{2(KE)}{m}}= \dfrac{\sqrt{2m}}{qB}\sqrt{KE}$$

    $$\Rightarrow \dfrac{R_1}{R_2}= \dfrac{\sqrt{KE}}{\sqrt{KE/2}}$$

    $$\Rightarrow R_2= \dfrac{R_1}{\sqrt2}=\dfrac{4}{\sqrt2}= 2\sqrt2cm$$
  • Question 5
    1 / -0
    The coil of a tangent galvanometer is put in the magnetic meridian
    Solution

  • Question 6
    1 / -0
    The charged particles traverse identical helical paths in a completely opposite sense in a uniform magnetic field $$B={ B }_{ 0 }\hat { k }$$.
    Solution
    As the two charged particles travers identical helical path the pitchof their helices will be same 
    Now pitch will be same 
    Now pitch $$=$$ Time for one circle completion $$\times$$ speed 
    $$ \Rightarrow P = T \times v\cos \theta = \dfrac{2\pi m}{qB} v\cos\theta$$       (Time period under uniform magnetic field $$= \dfrac{2\pi m}{qB})$$
    As $$ P_{1}=P_{2}$$
    $$ \Rightarrow \dfrac{2\pi m_{1}}{q_{1}B_{0}} v\cos \theta = \dfrac{2\pi m_{2}}{q_{2}B_{0}} v\cos\theta $$
    $$ \Rightarrow \dfrac{q_{1}}{m_{1}} = \dfrac{q_{2}}{m_{2}}$$
    So the have equal charge to mass eatio magnitude
    But they are moving in opposite direction so one is $$+Ve$$ charge and another $$-Ve$$
    $$ \Rightarrow \dfrac{q_{1}}{m_{1}} + \dfrac{q_{2}}{m_{2}} = 0 $$
  • Question 7
    1 / -0
    A positively charged particle moving with constant speed due east enters a region of uniform magnetic field directed vertically upwards this particle will-
    Solution
    By right-hand rule force, $$\vec F= q\vec V \times \vec B$$ will be towards south so the charge will start moving in a circular path.
    As the force is in the perpendicular direction so it will not do any work so speed will not change.
    Option C is correct.
  • Question 8
    1 / -0
    A charged particle of mass 1 $$\mu $$ g and charge 1 $$\mu $$ C having speed 2m/s moves in a magnetic field 1 $$\hat{K} $$ Tesla. At a certain instant its velocity is $$\bar{V}=\hat{i}+\hat{j}+m\hat{k} $$ . The value of 'm' is ________________.
  • Question 9
    1 / -0
    A current carrying wire and a rectangular loop are placed as shown in figure then-

    Solution
    Since, there is an attractive force between $$PS$$ and the adjacent wire and the repulsive force between $$QR$$ and the adjacent wire but $$B\alpha \dfrac1{R}\implies$$ the attractive force prevails and rectangular loop is attracted to the adjacent current wire. 
  • Question 10
    1 / -0
    The magnetic field strength at a point P distant r due to an infinite straight wire as shown in the figure carrying i is :

    Solution
    We know,

    Magnetic field due to semi-infinite wire,
    $$B=\dfrac{\mu_0I}{4\pi R}(\cos\theta_1+\cos\theta_2)$$

    $$B_1=\dfrac{\mu_0I}{4\pi R}(1+\cos(45^0))$$

    $$B_2=\dfrac{\mu_0I}{4\pi R}(1+\cos(45^0))$$

    $$\overrightarrow B_{net}=\overrightarrow {B_1}+ \overrightarrow{B_2}$$

    $$\overrightarrow B=\dfrac{\mu_0 I}{4\pi R}(2+\sqrt 2)$$

    Option $$\textbf D$$ is the correct answer.

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