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Electrostatic Potential and Capacitance Test - 69

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Electrostatic Potential and Capacitance Test - 69
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  • Question 1
    1 / -0

    Two identical capacitors are connected as shown in the figure. A dielectric slab is introduced between the plates of one of the capacitors so as to fill the gap, the battery remaining connected. The charge on each capacitor will be :(charge on each condenser is $$q_{0}$$;  $$k$$  = dielectric constant )

    Solution
    When capacitors are connected in series the charge present on them must be equal.
    $$\dfrac{Q}{c_{1}}+\dfrac{Q}{c_{2}}=2$$ ------------ (1)
    Now when $$k$$ is introduced $$c_{2}$$ becomes $$kc_{2}$$

    Let $$q_{o}$$ be the charge on capacitor
    given $$c_{1}=c_{2}$$
    $$\Rightarrow 2\dfrac { { q }_{ o } }{ c } =2,\dfrac { { q }_{ o } }{ c } =1$$ from (1)
    $$ c ={ q }_{ o } $$

    After introducing the dielectric, let charge on each plate become $$Q_{ 1 }$$
    $$\Rightarrow \dfrac { Q_{ 1 } }{ { q }_{ o } } +\dfrac { Q_{ 1 } }{ k{ q }_{ 0 } } =2$$
    $$\Rightarrow \dfrac { kQ_{ 1 }+Q_{ 1 } }{ k{ q }_{ o } } =2$$
    $$\Rightarrow Q_{ 1 }=\dfrac { 2kq_{ o } }{ k+1 } $$
    $$\Rightarrow Q_{1}=\dfrac{2q_{o}}{1+ \dfrac{1}{k}}$$
  • Question 2
    1 / -0
    A parallel plate capacitor of capacity $$5 \mu F$$ and plate separation $$6 cm$$ is connected to a $$1V$$ battery and is charged. A dielectric of dielectric constant $$4$$ and thickness $$4 cm$$ is introduced into the capacitor. The additional charge that flows into the capacitor from the battery is:
    Solution

  • Question 3
    1 / -0

    The capacity between the points A and B in the given circuit will be:

    Solution
    The charge distribution is as shown in the figure.
    Using Kirchhoff's law,
    $$ V - q1/C_1 + (q2-q1)/C_3 - q1/C_1 =0 \Rightarrow V = 2q1/C_1 - (q2-q1)/C_3 $$
    $$ V - q2/C_2 + (q1-q2)/C_3 - q2/C_2 =0 \Rightarrow V = 2q2/C_2 - (q1-q2)/C_3 $$
    Therefore,
    $$ C_1C_3 V = 2C_3q1 - C_2 q2 + C_2q1 = (2C_3+C_1)q1 - C_1q2$$
    $$ C_2C_3 V = 2C_3q2 - C_2q1 + C_2q2 = (2C_3 + C_2)q2 - C_2q1$$ 
    Solving these two equations we get,

    $$q1 = \dfrac{C_1(C_2+C_3)V}{C_1+C_2+2C_3} $$

    $$q2 = \dfrac{C_2(C_1 + C_3)V}{C_1+C_2+2C_3} $$

    Equivalent capacitance $$=Q_{net}/V = (q1+q2)/V = \dfrac{2C_1C_2 + C_1C_3 + C_2C_3}{C_1 +C_2 + 2C_3}$$
  • Question 4
    1 / -0

    The capacitance $$C_{AB}$$ in the given network is:

    Solution
    From the given circuit, we get  $$\dfrac{C_1}{C_2} = \dfrac{5}{10} = \dfrac{1}{2}$$
    And  $$\dfrac{C_3}{C_4} = \dfrac{10}{5} = \dfrac{2}{1}$$
    Thus  $$\dfrac{C_1}{C_2}$$ is reciprocal of $$\dfrac{C_3}{C_4}$$
    For this particular type of circuit, the equivalent capacitance is given by-
    $$C_{net} = \dfrac{2C_1C_2 + C_3(C_1+C_2)}{C_1+C_2+2C_3} $$

    $$C_{net} = \dfrac{2(5)(10) + 5(5+10)}{5+10+2(5)} = \dfrac{175}{25} = 7\mu F$$

  • Question 5
    1 / -0
    The equivalent capacitance $$C_{AB}$$ of the circuit shown in the figure is :

    Solution

    The given circuit can be reconstructed as shown (As the potential difference between A and B has to same through all possible paths)

    Using the laws of combination of capacitors,

    $$ C_{net} = C_1 + C_2 + C_3 \,where\,$$

    $$ C_2 = \dfrac{C}{2} , \dfrac{1}{C_1} = \dfrac{1}{C} + \dfrac{1}{C} + \dfrac{1}{(C+ \dfrac{C}{2})} = \dfrac{2}{C} + \dfrac{2}{3C} = \dfrac{8}{3C} \Rightarrow C_1 = \dfrac{3C}{8} $$

    Similarly, $$C_3 = \dfrac{3C}{8} $$

    $$C_{net} = \dfrac{6C}{8} + \dfrac{C}{2} = \dfrac{5C}{4} $$ 

  • Question 6
    1 / -0
    The effective capacity between A and B of the given network is

    Solution

  • Question 7
    1 / -0
    An air filled parallel plate capacitor has a capacitance $$1 pF$$. The separation between the plates is doubled and wax is inserted between the plates, then the capacitance becomes $$2 pF$$. What is the dielectric constant of wax ?
    Solution

    Capacitance of parallel plate capacitor with air ,$$C_a=\dfrac{\varepsilon _{0}A}{d}    ....(1)$$

    Capacitance of parallel plate capacitor with wax ,$$C_w=\dfrac{K\varepsilon _{0}A}{2d}  .....(2)$$

    $$(1)/(2),$$

    $$ \dfrac{C_a}{C_w}=\dfrac{2}{K}$$

    $$\dfrac{1}{2}=\dfrac{2}{K}$$

    $$\therefore K=4$$

  • Question 8
    1 / -0
    An isolated parallel plate capacitor is charged upto a certain potential difference. When a $$3mm$$ thick slab is introduced between the plates then in order to maintain the same potential difference, the distance between the plates is increased by $$2.4mm$$. Find the dielectric constant of the slab. (Assume charge remains constant)
    Solution
    $$C_f=\dfrac {\varepsilon_0A}{d'-t(1-\frac {1}{K})}$$
    $$C_i=C_f$$
    $$\dfrac {\varepsilon_0A}{d}=\dfrac {\varepsilon_0A}{d'-t(1-\dfrac {1}{K})}\Rightarrow d=d'-t(1-\dfrac {1}{K})$$
    $$d'=d-2.4\times 10^{ -3 }$$
    $$t=3mm$$
    $$d=d+(2\cdot 4\times 10^{-3})-3\times 10^{-3}(1-\dfrac {1}{K})$$
    $$K=5$$
  • Question 9
    1 / -0
    The capacity of a parallel plate condenser without any dielectric is C. If the distance between the plates is doubled and the space between the plates is filled with a substance of dielectric constant $$3$$, the capacity of the condenser becomes:
    Solution

    The capacitance of a parallel plate capacitor is given by

    $$C = \dfrac {\varepsilon_o \varepsilon_r A}{d}$$,

    where $$A$$ is the area of the plate and $$d$$ is the distance between them.

    In the first case, there was no dielectric medium, i.e., $$\varepsilon_r = 1$$.

    So we have   $$C = \dfrac {\varepsilon_o A}{d}$$

    In the second case, the distance is doubled, i.e., $$2d$$ and a substance of dielectric constant $$3$$ is inserted between the plates.

    Hence capacitance will change to 

    $$C' = \dfrac {3 \varepsilon_o A}{2d}$$

    So, $$ \dfrac{C'}{C} = \dfrac {3}{2}$$

    $$ \implies C' = \dfrac {3}{2} C$$

  • Question 10
    1 / -0
    A parallel plate capacitor is connected to a cell. It's positive plate A and the negative plate B have charges $$+Q$$ and $$-Q$$ respectively. A third plate C identical to A and B with charge $$+Q$$ is  now introduced midway between the plates A and B parallel to them What is the charge on the inner surface of A ?

    Solution
    Let the capacitance of the A+B system be given by C = $$\dfrac{\epsilon A}{d}$$
    Now when the plate is introduced in middle, the distance of A+C and C+B system is changed to $$\dfrac{d}{2}$$ So the capacitance will be $$\dfrac{2\epsilon A}{d}$$ = 2C
    Now, Total charge in the system is Q assume A+C has q charge and C+B has Q+q charge 
    So, $$\dfrac{q}{2C}$$ + $$\dfrac{Q+q}{2C}$$ = $$\dfrac{Q}{C}$$
    So, q = $$\dfrac{Q}{2}$$

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