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Moving Charges and Magnetism Test - 48

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Moving Charges and Magnetism Test - 48
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  • Question 1
    1 / -0
    The acceleration of an electron at a certain moment in a magnetic field $$\vec{B}=2\hat{i}+3\hat{j}+4\hat{k}$$ is $$\vec{a}=x\hat{i}+\hat{j}-\hat{k}$$.The value of x is
    Solution
    $$\vec{B}\cdot \vec{F}=0$$ as $$\vec{B}\bot \vec{F}$$
    $$\therefore              \vec{B}\cdot \vec{\alpha} =0$$

    $$ 2x+3-4=0$$
    $$\therefore                x=0.5$$
  • Question 2
    1 / -0
    A charged particle moving along positive x-direction with a velocity $$v$$ enters a region where there is a uniform magnetic field $$\vec{B}=-B\hat{k}$$,from x=0 to x=d.The particle gets deflected at an angle $$\theta$$ from its initial path.The specific charge of the particle is 
    Solution
    $$sin\theta =\displaystyle\dfrac{d}{r}$$

    $$=\dfrac{d}{(mv/Bq)}$$

    $$\therefore \displaystyle\dfrac{q}{m}=\dfrac{vsin\theta}{Bd}$$
  • Question 3
    1 / -0
    If a charged particle projected from origin with some initial velocity $$({v}_{0}\hat { i } )$$ in a uniform magneitc field $$({B}_{0}\hat { i } )$$. At some point of time direction of magnetic field is reversed then which of the following path is/are possible for the charged particle. Here $${v}_{0}$$ and $${B}_{0}$$ are positive constants.
    Solution
    Here as we know that the force due to magnetic field on a particle 
    is $$ F = q (v\times B) $$
    so the force of magnetic field is zero if the velocity of the particle is in the same direction as of the magnetic field so as in this  
    here  $$ v = v_{o} i $$ and $$ B = B_{o} i $$
    so no force on the particle even if you reverse the direction of the magnetic field.
    so particle will always move with a constant velocity in a straight line
    so none of the option is correct.
  • Question 4
    1 / -0
    The force of repulsion between two parallel wires is $$F$$ when each one of them carries a certain current I. If the current in each is doubled, the force between them would be
    Solution
    The force per unit length on a current carrying wire due to another current carrying wire placed at a distance $$d$$ from it is

    $$\dfrac{F}{l}=\dfrac{\mu_0I_1I_2}{2\pi d}$$

    Hence when current in both wires is doubled, the force of repulsion becomes four times of that before.
  • Question 5
    1 / -0
    Two long parallel wires are at a distance of 1m. If both of them carry one ampere of current in same direction, then the force of attraction on unit length of the wires will be
    Solution
    Given: $$I_1= I_2 = 1$$ A              
    Distance between the wires, $$d = 1$$ m

    Force of attraction per unit length, $$f = \dfrac{\mu_0  I_1 I_2}{2\pi  d}$$   $$N/m$$

    $$\therefore $$    $$f = \dfrac{4\pi \times 10^{-7}   \times (1) (1)}{2 \pi  \times 1}  = 2 \times 10^{-7}$$ $$N/m$$
  • Question 6
    1 / -0
    A rectangular loop carrying a current $$i_1$$, is situated near a long straight wire carrying a steady current $$i_2$$. The wire is parallel to one of the sides of the loop and is in the plane of the loop as shown in the figure. Then the current loop will

    Solution
    The magnetic field due to the straight current current carrying wire decreases with increasing distance from the wire. Thus the magnetic field is stronger at the side closer to wire and weaker at the other.
    Force on each segment of wire is $$BIL$$
    Hence force acting on nearer side towards the wire is greater than the force acting on farther side away from wire. Hence the net force on loop is towards the wire.
  • Question 7
    1 / -0
    When a charged particle particle, moving with a velocity v, is subjected to a magnetic field, the force on it is non-zero. This implies that
    Solution
    The force acting on a charge particle moving with velocity $$\vec{v}$$ in a magnetic field $$\vec{B}$$ is given by

    $$\vec{F}=q(\vec{v}\times \vec{B})$$

    $$\implies F=qvBsin\theta$$

    which is non-zero for $$0^{\circ}\neq\theta\neq180^{\circ}$$
  • Question 8
    1 / -0
    A magnetic field cannot exert any force on a :
    Solution

    Hint: Use formula of Lorentz force

    Explanation:

    Force on charge q with velocity $$\vec{v}$$ by magnetic field $$\vec{v}$$ is given by the formula:

    $$\vec{F} = q\ (\vec{v}\ X\ \vec{B})$$

    As given that not any force is exerted, so cross product of $$\vec{v}$$ and $$\vec{B}$$ should be zero. Which is possible if both are parallel to each other or value of one of those is zero. Value of magnetic field is not zero here so velocity must be zero.

    And for only stationary particles velocity is zero. 

    Answer:

    Hence, option D is the correct answer. 

  • Question 9
    1 / -0
    A charged particle moves through a magnetic field in a direction perpendicular to it. Then the
    Solution
    $$\vec{F}=q\vec{v}\times\vec{B}$$
    When $$\vec{v}$$ is perpendicular to $$\vec{B}$$, the charged particle moves in a circular path in a plane perpendicular to $$\vec{B}$$ and the magnetic force $$\vec{F}$$ always act towards the center of the circle with magintude,
    $$F=qvB$$
    Thus, the direction of $$|vec{v}$$ changes but not the magnitude. 
    Hence, speed of particle remains unchanged.
  • Question 10
    1 / -0
    When a charged particle moving with velocity $$\vec V$$ is subjected to a magnetic field of induction $$\vec B$$, the force on it is non-zero. This implies the
    Solution
    Force on a charged particle moving in a magnetic field is 

    $$\vec{F}=q(\vec{v}\times \vec{B})$$

    Let the angle between $$\vec{v}$$ and $$\vec{B}$$ be $$\theta$$

    Hence $$\left|\vec{F}\right|=qvBsin\theta \neq 0$$

    $$\implies sin\theta\neq 0$$

    $$\implies \theta\neq 0^{\circ},180^{\circ}$$
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