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Electric Charges and Fields Test - 48

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Electric Charges and Fields Test - 48
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  • Question 1
    1 / -0
    Two small spheres with masses $$M_1$$ and $$M_2$$ hang on weightless, insulating threads with lengths $$L_1$$ and $$L_2$$. The two spheres carry a charge of $$Q_1$$ and $$Q_2$$ respectively. The spheres hang such that they are level with one another and the threads are inclined to the vertical at angles $$\theta_1$$ and $$\theta_2$$. Which of the following conditions is required if $$\theta_1=\theta_2$$.

    Solution
    $$\theta_1=\theta_2$$, if their masses are the same because the force of repulsion due to charges is the same. The force Mg $$\sin\theta$$ opposes the force of repulsion. Even if $$Q_1$$ and $$Q_2$$ are different, the force of repulsion is the same for both as they are mutual.

  • Question 2
    1 / -0
    Two point charges $$-q$$ and $$+q/2$$ are situated at the origin and the point $$(a,0,0)$$ respectively. The point along the x-axis, where the electric field vanishes is
    Solution
    The given situation can be shown as given
    Suppose the field vanished at a distance $$x$$, we have
    $$\cfrac { kq }{ { x }^{ 2 } } =\cfrac { kq/2 }{ { (x-a) }^{ 2 } } $$
    $$\Rightarrow 2{ (x-a) }^{ 2 }={ x }^{ 2 }$$
    $$\sqrt { 2 } (x-a)=x\quad $$
    $$\Rightarrow \sqrt { 2 } x-x=\sqrt { 2 } a$$
    $$\Rightarrow (\sqrt { 2 } -1)x=\sqrt { 2 } a$$
    $$\quad \Rightarrow x=\cfrac { \sqrt { 2 } a }{ \sqrt { 2 } -1 } $$

  • Question 3
    1 / -0
    The smallest electricforce between two changes placed at a distance of 1 m apart is (approximately)
    Solution
    From Coulomb's law, electric force 
    $$F_e =\frac {1}{4\pi \varepsilon _0}\cdot \frac{q_1q_2}{r^2}$$
    For minimum force,
    $$q_1=q_2 = 1.6 \times 10^{-19}C$$
    $$\therefore F_e = \frac {9 \times 10^9 \times 1.6 \times 10^{-19} \times 1.6 \times 10^{-19}}{(1)^2}$$
    $$f_e = 10^{-28} N$$
  • Question 4
    1 / -0
    If the coulombian force acting between two protons separated by a distance r is F, what would be the force acting between two $$\alpha-$$particles separated by a distance 2r ?
    Solution
    Let the charge of proton is q
    Charge of $$\alpha-$$particle
    $$ = 2\times charge \, of \, proton$$
    $$=2q$$

    The force acting between two protons separated by a distance r is
    $$F=k \dfrac {q\cdot q}{r^2}=k \dfrac {q^2}{r^2}$$

    The force acting between two $$\alpha-$$ patricles separated by a distance 2r is
    $$F'=k \dfrac {2q\cdot 2q}{(2r)^2}$$
    $$=k \dfrac {4q^2}{4r^2}$$
    or $$ = k \dfrac {r^2}{r^2}$$
    $$\Rightarrow F'=F$$
  • Question 5
    1 / -0
    The black shapes in the figure are closed surfaces. The electric field lines are in red. For which case the net flux through the surfaces is non-zero?

    Solution
    As charge is enclosed in a, b, so by Gauss's Law there will be a flux enclosed by the given surface.
  • Question 6
    1 / -0
    Eight point charges (can be assumed as small spheres uniformly charged and  their centres at the corner of the cube) having values q each are fixed at vertices of a cube .The electric flux through square surface ABCD of the cube is 

    Solution
    At each vertex, we have effective charge of $$q_v=q/8$$
    So total charge enclosed by the cube is, $$8q_v=q$$

    By Gauss law, total electric flux through the cube is, $$\phi=\dfrac{q}{\epsilon_o}$$
    By symmetry, flux through each face of the cube would be equal.
    So, flux trough ABCD is, $$\dfrac{\phi}{6}=\dfrac{q}{6\epsilon_o}$$

    Option C is correct.
  • Question 7
    1 / -0
    Two identical conducting balls A and B have positive charges $$q_1$$ and $$q_2$$ respectively. But $$q_1\neq q_2$$. The balls are brought together so that they touch each other and then kept in their original positions. The force between them is?
    Solution
    According to coulomb's law, the force of repulsion between them is given by $$F=\displaystyle\frac{q_1q_2}{4\pi \varepsilon_0 r^2}$$
    When the charged spheres A and B are brought in contact, each sphere will attain equal charge $$q'$$
    $$q'=\displaystyle\frac{q_1+q_2}{2}$$
    Now, the force of repulsion between them at the same direction r is
    $$F'=\displaystyle\frac{q'\times q'}{4\pi \varepsilon_0 r^2}=\frac{1}{4\pi \varepsilon_0}\frac{\left(\displaystyle\frac{q_1+q_2}{2}\right)\left(\displaystyle\frac{q_1+q_2}{2}\right)}{r^2}$$
    $$=\displaystyle\frac{\left(\displaystyle\frac{q_1+q_2}{2}\right)^2}{4\pi \varepsilon_0 r^2}$$
    As $$\left(\displaystyle\frac{q_1+q_2}{2}\right)^2 > q_1q_2$$
    $$\therefore F' > F$$.

  • Question 8
    1 / -0
    Let the electrostatic field E at distance r from a point charge q not be an inverse square but, instead an inverse cubic, e.g., $$\vec{E}=k\frac{q}{r^3}\hat{r}$$. Here k is a constant. Consider the following two statements.
    (i) Flux through a spherical surface enclosing the charge is $$\Phi =q_{enclosed}/\epsilon_0$$
    (ii) A charge placed inside uniformly charged shell will experience a force.
    Choose the correct option.
    Solution
    Flux  enclosed is  not constant  since $$\int E.ds$$ over a surface of radius r is  not constant and is inversely proportional to r.  hence (i) is not valid.
    Also $$F = Eq$$, initially distance $$r$$ is inverse square in electric field but now distance r is changed to inverse cube in electric field. hence electric field is changed from initial condition, hence a charge will experience a force. hence (ii) is valid.
  • Question 9
    1 / -0
    A certain charge Q is divided into two parts q and $$Q-q$$. How the charge Q and q must be related so that when q and $$(Q-q)$$ is placed at a certain distance apart experience maximum electrostatic repulsion?
    Solution
    The electrostatic force of repulsion between the charge q and $$(Q-q)$$ at separation r is given by
    $$\displaystyle F=\frac{1}{4\pi \varepsilon_0}$$ $$\frac{q(Q-q)}{r^2}$$ $$=\frac{1}{4\pi \varepsilon_0}$$ $$\frac{qQ-q^2}{r^2}$$
    If F is maximum, then $$\partial F/ \partial q=0$$
    i.e., $$\displaystyle\frac{1}{4\pi \varepsilon_0}\cdot \frac{(Q-2q)}{r^2}=0$$
    As $$\displaystyle\frac{1}{4\pi \varepsilon_0r^2}$$ is constant, therefore
    $$Q-2q=0$$ or $$Q=2q$$
  • Question 10
    1 / -0
    A charge $$Q$$ is situated at the centre of a cube. The electric flux through one of the faces of the cube is
    Solution
    The electric flux through the whole cube:
    $$ \phi = \cfrac{Q}{\varepsilon_0}$$
    Flux through each face will be one sixth of the total:
    $$ \phi = \cfrac{Q}{6\varepsilon_0}$$


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