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Electrostatic Potential and Capacitance Test - 23

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Electrostatic Potential and Capacitance Test - 23
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  • Question 1
    1 / -0
    The capacitance of a parallel plate capacitor with air as medium is $$6 \mu F$$. With the introduction of a dielectric medium, the capacitance becomes $$30\mu F$$. The permittivity of the medium is :
    $$(\in_0= 8.85 \times 10^{-12} C^2N^{-1} m^{-2})$$ 
    Solution
    Capacitance of air capacitor 
    $$C_0 = \dfrac{\varepsilon_0A}{d} = 6 \mu F$$           ......... (i)
    When a dielectric of permittivity $$\varepsilon_r$$ and dielectric constant K is introduced between the plates, then
    Capacitance, $$C = \dfrac{K \varepsilon_0 A}{d} = 30 \mu F$$       ..... (ii)
    Dividing eq. (ii) by (i), we get
    $$\dfrac{C}{C_0} = \dfrac{\dfrac{K\epsilon_o A}{ d}}{\dfrac{\varepsilon_0 A}{d}} = \dfrac{30}{6}$$
    $$\Rightarrow K = 5$$
    $$\therefore$$ permittivity of the medium
    $$\varepsilon_0 = \varepsilon_0 K$$
    $$= 8.85 \times 10^{-12} \times 5 = 0.44 \times 10^{-10}$$
  • Question 2
    1 / -0
    Two parallel metal plates having charges +Q and -Q face each other at a certain distance between them. If the plates are now dipped in kerosene oil tank, the electric field between the plates will :
    Solution
    Electric field between two parallel plates placed in vacuum is given by
    E = $$\displaystyle \frac{\sigma}{\varepsilon_0}$$
    In a medium of dielectric constant K, E' = $$\displaystyle \frac{\sigma}{\varepsilon_0 K}$$ For kerosene oil K > 1$$\Rightarrow$$ E' is less than E
  • Question 3
    1 / -0
    An electric charge $${10}^{-3}\mu C$$ is placed at the origin $$(0,0)$$ of $$(x,y)$$ co-ordinate system. Two points $$A$$ and $$B$$ are situated at $$(\sqrt {2}, \sqrt {2})$$ and $$(2,0)$$ respectively. The potential difference between the points $$A$$ and $$B$$ will be:
    Solution
    Given :           $$q = 10^{-3}  \mu C =  10^{-9}  C$$

    Distance of A from origin        $$r_A = \sqrt{(\sqrt{2} - 0)^2  + (\sqrt{2} - 0)^2} = 2$$

    Distance of B from origin       $$r_B = 2$$

    Thus potential due to charge at point A          $$V_A = \dfrac{Kq}{r_A}$$      where   $$K = \dfrac{1}{4\pi \epsilon_o}  = 9 \times 10^9$$

    $$\therefore$$    $$V_A = \dfrac{9 \times 10^9  \times 10^{-9}}{2} = 4.5$$  V

    Potential due to the charge at B          
    $$V_B = \dfrac{Kq}{r_B} = \dfrac{9\times 10^9  \times 10^{-9}}{2} = 4.5$$ V

    Potential difference between A and B        
     $$V_{AB} = V_A- V_B = 0$$
  • Question 4
    1 / -0
    A parallel plate capacitor with air as a dielectric has capacitance $$C$$. A slab of dielectric constant $$K$$, having same thickness as the separation between the plates is introduced so as to fill one-fourth of the capacitor as shown in the figure. The new capacitance will be:

    Solution
    The two condensers with $$K$$ and with air are in parallel. With air, $$C_{1} = \dfrac {\epsilon_{0}}{d}\left (\dfrac {3A}{4}\right ) = \dfrac {3\epsilon_{0}A}{4d}$$
    With medium, $$C_{2} = \dfrac {\epsilon_{0}K}{d}\left (\dfrac {A}{4}\right ) = \dfrac {\epsilon_{0}AK}{4d}$$
    $$\therefore C' = C_{1} + C_{2}$$
    or $$C' = \dfrac {3\epsilon_{0}A}{4d} + \dfrac {\epsilon_{0}AK}{4d} = \dfrac {\epsilon_{0}A}{d}\left [\dfrac {3}{4} +\dfrac {K}{4}\right ]$$
    or $$C' = \dfrac {C}{4} (K + 3) \left [\because C = \dfrac {A\epsilon_{0}}{d}\right ]$$.
  • Question 5
    1 / -0
    A parallel plate capacitor of area $$'A'$$ plate separation $$'d'$$ is filled with two dielectrics as shown. What is the capacitance of the arrangement?

    Solution
    $$c_{1} = \dfrac {(A/2)\epsilon_{0}}{d/2} = \dfrac {A\epsilon_{0}}{d}, c_{2} = K \dfrac {A\epsilon_{0}}{d}, c_{3} = K\dfrac {A\epsilon_{0}}{2d}$$
    $$\therefore c_{eq.} = \dfrac {c_{1}\times c_{2}}{c_{1} + c_{2}} + c_{3} = \dfrac {(3 + K)KA\epsilon_{0}}{2d(K + 1)}$$
    $$(\because C_{1}$$ and $$C_{2}$$ are in series and resultant of these two in parallel with $$C_{3})$$.
  • Question 6
    1 / -0
    Space between the plates of a parallel plate capacitor is filled with a dielectric slab. The capacitor is charged and then the supply is disconnected to it. If the slab is now taken out , then:
    Solution
    When a capacitor is charged and then the supply is disconnected charge present on it becomes constant (law of conservation of charge)
    Initial capacitance $$C=\frac {k\varepsilon_0 A}{d}$$ (with slab)
    Final capacitance $$C=\frac {\varepsilon_0 A}{d}$$ (slab removed)
    We know $$Q= CV$$
    As C decreases and Q remains constant V has to increase.
  • Question 7
    1 / -0

    A parallel plate condenser is charged by connecting it to a battery. The battery is disconnected and a glass slab is introduced between the plates. Then, 

    Solution
    $$\rightarrow $$ When the capacitor is charged and battery is removed the charge present on capacitor remains constant. (Law of conservation of charge)
    $$\rightarrow$$ We know $$C=\dfrac {\varepsilon_0 A}{d}$$
    When slab is introduced, $$C=\dfrac {k\varepsilon_0 A}{d}$$
    $$C$$ increases and $$Q$$ is constant.
    We know: $$Q=CV$$ 
    $$\therefore $$ $$V$$ has to decrease.
    We know energy store in capacitor $$=\dfrac{1}{2} QV$$
    $$\therefore $$ as V decreases, energy decreases.
  • Question 8
    1 / -0
    Fill in the blank:

    In order to increase the capacity of a parallel plate condenser,  one should introduce a sheet of  $$\underline{\hspace{0.5in}}$$ between the plates (assume that the space is completely filled).
    Solution
    Dielectric constant is the factor by which the capacitance increases from its value in air when a dielectric is introduced between the plates.
    Mica, among the materials mentioned above, is a dielectric material and hence to be used to increase the capacity.
  • Question 9
    1 / -0
    The capacity of a parallel plate air condenser is $$2\ \mu F$$. If a dielectric of dielectric constant $$4$$ is introduced between the plates, its new capacity is:
    Solution
    We know $$C=\dfrac{\epsilon_{0}A}{d}$$
    When dielectric is added:
    $$C'=\dfrac{K \epsilon_{0}A}{d}$$$$=4\times 2\ \mu F$$$$=8\mu F$$
  • Question 10
    1 / -0
    In an electrical circuit, which of the following quantities is analogous to temperature?
    Solution
    When there is a temperature difference, heat flows from high temperature to low temperature. Similarly, when there is a potential difference electric current flows from high potential to low potential. Hence, potential is analogous to temperature.
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