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Electric Charges and Fields Test - 72

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Electric Charges and Fields Test - 72
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  • Question 1
    1 / -0
    Two point charges $$q$$ and $$-4q$$ are placed at points $$A$$ and $$B$$ respectively, at a distance $$d$$ apart as shown in the figure. The null point (the point where electric field is zero) is :

    Solution

    Let the third charge is placed at distance\[x\] which is the null point.

    So by using Coulombs law we get

    $$\dfrac{{Kq}}{{{x^2}}} = \dfrac{{K4q}}{{{{\left( {d - x} \right)}^2}}}$$

    By solving the above equation we get

    $$d - x = 2x$$

    Hence the distance of the third charge is$$x = \dfrac{d}{3}$$

    The magnitude can be determined by the equilibrium condition. The charge on the position$$B$$will exert a force towards itself and the charge on position$$A$$will exert force away from it. Hence the third charge should be placed in between these two charges.

     

  • Question 2
    1 / -0
    A cubical region of side $$'a'$$ has its centre at the origin. It encloses three fixed point charges, $$-q$$ at $$(0, -a/4, 0), +3q$$ at $$(0, 0, 0)$$ and $$-q$$ at $$(0, +a/4, 0)$$. Choose the incorrect option

    Solution

  • Question 3
    1 / -0
    Two equal and opposite point charges are kept in a box. A vacuum is created in the box by evacuating the air inside the box. Then the electrostatic force between the two charges will:
    Solution

    The electrostatic force between two charge are given as

    $$F = \dfrac{{Qq}}{{4\pi {\varepsilon _0}{r^2}}}$$

    The electrostatic force is inversely proportional to that of the dielectric permittivity.

    The permittivity of free space (vacuum) is 1 and hence the electrostatic field in vacuum is more as there is no resistance to the field.

     

     

  • Question 4
    1 / -0
    A particle of charges $$q_{0}$$ is moved around a charges $$+q$$ along the semicircle path of radius $$r$$ from $$A$$ to $$B$$ (see figure). The work done by the Coulomb force is

    Solution

  • Question 5
    1 / -0
    A charged particle $$q$$ is placed at the centre $$O$$ of cube of side $$L (ABCDEFGH)$$. Another same charge $$q$$ is placed at a distance $$L$$ from $$O$$, then the electric flux through $$ABCD$$ is

    Solution

  • Question 6
    1 / -0
    Two charges $$q_{1}$$ and $$q_{2}$$ are moving with velocity $$\vec {V_{1}}$$ and $$\vec {V_{2}}$$ parallel to each other in vacuum as shown. Then,

    Solution

  • Question 7
    1 / -0
    Two point charges $$+q$$ and $$-4q$$ are placed at $$(-a, 0)$$ and $$(+a, 0)$$. Take electric field intensity to be positive if it is along positive $$x-$$direction. The variation of the electric field intensity as one moves along the $$x-$$axis is: 
    Solution

  • Question 8
    1 / -0
    To construct an air filled capacitor which can store $$ 12 \mu C $$ of charge, What can be the minimum plate area of the capacitor? (Dielectric strength of air is $$3\times 10^6 V/m$$ )
    Solution

  • Question 9
    1 / -0
    Three charge $$+4q,\ Q$$ and $$q$$ are placed in a straight line of length $$\ell$$ at points distance $$0,\ \ell/2$$ and $$\ell$$ respectively. What should be the value of $$Q$$ in order to make the net force on $$q$$ to be zero?
    Solution
    Two forces are acting on $$q$$, one due to $$4q$$ and second due to $$Q$$.
    $${F}_{1}=\dfrac{1}{4\pi\epsilon}\left(4q\right)\dfrac{q}{l^2}$$ and
    $${F}_{2}=\dfrac{1}{4\pi\epsilon}\left(Q\right)\dfrac{q}{l^2/4}$$ 
    And $${F}_{1}+{F}_{2}=0$$
    $$\Rightarrow \dfrac{1}{4\pi\epsilon}\left(4q\right)\dfrac{q}{l^2}+\dfrac{1}{4\pi\epsilon}\left(4Q\right)\dfrac{q}{l^2}=0$$
    $$\Rightarrow \dfrac{1}{4\pi\epsilon}\left(\left(4q\right)+\left(4Q\right)\right)\dfrac{q}{1^2}=0$$
    $$\Rightarrow \dfrac{1}{\pi\epsilon}\left(\left(q\right)+\left(Q\right)\right)\dfrac{q}{1^2}=0$$
    $$\therefore Q=-q$$

  • Question 10
    1 / -0
    Consider a hemispherical surface of radius $$r$$, a positive point charge $$q$$ is kept at the centre of hemisphere. The electric flux through this hemisphere is :
    Solution
    if this charge is put at the centre of a sphere then net flux
    $$=\phi =q/\varepsilon_0$$ ( hauss s law)
    $$\Rightarrow$$ But this is hemisphere and it contain only half of the field lines and halve flux will become halved
    Hence net flux through hemisphere $$=\dfrac{q}{2\varepsilon_0}$$

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