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Moving Charges and Magnetism Test - 43

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Moving Charges and Magnetism Test - 43
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  • Question 1
    1 / -0

    Directions For Questions

    Two long straight conducting wires with linear mass density $$'\lambda'$$ are suspended using cords so that both of them are horizontal and parallel to each other at a distance $$'d'$$ apart. The back ends of the wires are connected by a low resistance slack wire. A charged capacitor is now added across the wires such that its positive terminal is connected to far end and negative terminal is connected to near end as shown in figure. The capacitance of the capacitor is $$C$$. These connections are also made by slack wires. Assume that time to discharge is negligible. Initial charge on capacitor is $$Q_0$$.

    ...view full instructions

    The wires 1 and 2

    Solution
    It is evident from the question that current in the two is in opposite direction so on using the formulas of current carrying straight conductor we can say that they will repel each other.
  • Question 2
    1 / -0
    A charge of $$0.04 C$$ is moving in a magnetic field of $$0.02 T$$ with a velocity $$10 m/s$$ in a direction making an angle $$30^o$$ with the direction of field. The force acting on it will be :
    Solution
    Force on the moving charge is,
     $$\vec F=q(\vec{v} \times \vec{B})= qvB \sin \theta= 0.04 \times 10 \times 0.02 \sin 30^o= 0.04 \times 10 \times 0.02 \times 0.5 = 4 \times 10^{-3} \:N$$
  • Question 3
    1 / -0
    When a conductor is rotated in a perpendicular magnetic field then, it's free electrons
    Solution
    Force on electron = $$ -q_e \vec v \times \vec B $$
    the force is perpendicular to the magnetic field. 
  • Question 4
    1 / -0
    Two wires carry currents of  $$100\  A$$ and  $$200\  A$$ respectively and they repel each other with a force of  $$0.4\  N/m$$. The distance between them will be :
    Solution
    Force due to two parallel current carrying conductor is,
    $$F = \dfrac{\mu_0}{4\pi} \dfrac{2i_1i_2}{r}=10^{-7}\dfrac{  2 \times 100 \times 200}{r}$$
    $$\therefore  0.4 \times r = 4 \times 10^{-3} $$
    $$\therefore r = 10^{-2}\: m = 1\: cm$$
  • Question 5
    1 / -0
    A neutron, a proton, an electron and an $$\alpha-$$particle enter a region of uniform magnetic field with equal velocities. The magnetic field is perpendicular to the plane of paper and directed into it. The tracks of particles are labeled in the figure. The neutron follows the track

    Solution
    Neutron does not carry any charge.
    Hence, there is no force on the neutron and it travels undeflected.
  • Question 6
    1 / -0
    An electron accelerated through a potential difference V passes through a uniform transverse magnetic field and experiences a force F. If the accelerating potential is increased to 2V, the electron in the same magnetic field will experience a force
    Solution
    $$F=Bqv$$
    But $$\frac {1}{2}mv^2=eV$$ or $$v=\sqrt {\frac {2eV}{m}}$$
    $$\therefore F=Bq\sqrt {\frac {2eV}{m}}$$
    $$\Rightarrow F\propto \sqrt V$$ and
    $$F\propto \sqrt {2V}$$
    $$\frac {F'}{F}=\sqrt 2$$ or $$F'=\sqrt 2F$$
  • Question 7
    1 / -0
    An electron and a proton are injected into a uniform magnetic field perpendicular to it with the same momentum. If both particles are fired with same momentum into a transverse electric field, then
    Solution
    let, momentum of electron and proton be p.
    Transverse electric force on particle provides the centripetal force to support the circular motion.
    If r is radius of curvature, $$ F_e = F_c $$

    i.e. $$qE = m \dfrac{v^2}{r} $$.

    Solving the above equation we get r = $$ \dfrac {p^2}{mqE} $$ 

    where, $$p = momentum = mv$$

    Given $$q$$ ,$$p$$ and $$E$$ are constant. So, we can say that $$ r \propto \dfrac{1}{m} $$

    Radius of curvature is higher for a lighter mass particle which is an electron and vice versa for proton.
  • Question 8
    1 / -0
    An electron is moving along positive $$x-$$axis. To get it moving on an anticlockwise circular path in $$x-y$$ plane, a magnetic field is applied
    Solution
    For the particle to move anti-clockwise, force should be in $$\hat{j}$$ direction.

    $$\vec{F} = -e(\vec{v} \times \vec{B})=-e( v\hat{i} \times \vec{B})$$

    $$ \Rightarrow \vec{B}= B\hat{k}$$ since LHS is in $$\hat{j}$$ direction.
  • Question 9
    1 / -0
    A conducting rod PQ is moving parallel to X-axis in a uniform magnetic filed directed in positive Y-direction. The end P of the rod will become
    Solution
    Force of positive charges in rod = $$ q \vec v \times \vec B $$
    As $$v$$ is along x axis and $$B$$ is along y axis the force will be along the z axis. Therefore the positive charges will move towards the end P and it will become positive charged.

  • Question 10
    1 / -0
    An electron and a proton are injected into a uniform magnetic field perpendicular to it with the same momentum. If the two particles are injected into a uniform transverse electric field with same kinetic energy, then
    Solution
    Let, Kinetic energies of electron and proton be K.
    Transverse electric force on particle provides the centripetal force to support the circular motion in this case.
    If r is radius of curvature, $$ F_e = F_c $$

    i.e. qE = m $$\dfrac{v^2}{r} $$.

    Solving the above equation we get r = $$ \dfrac {2K}{qE} $$ where K = Kinetic Energy = $$\dfrac {mv^2}{2}$$

    Here, q,E and K are constant. So, radius of curvature is same for both of them.
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