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Electrostatic Potential and Capacitance Test - 22

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Electrostatic Potential and Capacitance Test - 22
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  • Question 1
    1 / -0
    Effective capacitance of parallel combination of two capacitors $$C_1$$ and $$C_2$$ is $$10\mu F$$. when these capacitors are individually connected to a voltage source of $$1V$$, the energy stored in the capacitor $$C_2$$ is 4 times that of $$C_1$$. If these capacitors are connected in series, their effective capacitance will be:
    Solution
    Given that $$C_1 + C_2 = 10\mu F$$ (Parallel combination)       ...(1)

    They are now connected to the same voltage source of $$1V$$.

    The energy stored in the two capacitors are given by

    $$E_1 = \dfrac{1}{2}C_1V^2$$         $$E_2 = \dfrac{1}{2}C_2V^2$$

    Given that $$E_2 = 4E_1$$

    $$\therefore \dfrac{1}{2} C_2V^2 = 4 \times C_1V^2$$

    $$\therefore C_2 = 4C_1$$        ....(ii)

    From (i) and (ii),

    $$C_1 + C_2 = C_1 + 4C_1 = 10\mu F$$.

    $$5C_1 = 10\mu F$$, $$C_1 = 2\mu F$$

    $$C_2 = 10\mu F-C_1 = 10 \mu F - 2\mu F = 8\mu F$$.

    When $$C_1$$ and $$C_2$$ are connected in series, the equivalent capacitance of the combination is given by 

    $$C_{series} = \dfrac{C_1C_2}{C_1+C_2} = \dfrac{2\times 8}{2+8}\mu F = 1.6\mu F$$

  • Question 2
    1 / -0
    The equivalent capacitance between $$A$$ and $$B$$ in the circuit given below is:

    Solution
    $$C_1 = 5 + 5 + 2 = 12 \mu F$$
    $$C_2 = 4 + 2 = 6 \mu F$$
    $$1/ C_{Eq} = 1/6 + 1/12 + 1/6 = 5/12$$
    $$C_{Eq} = 2.4 \mu F$$

  • Question 3
    1 / -0
    Figure shows a network of capacitors where the numbers indicates capacitances in micro Farad. The value of capacitance C if the equivalent capacitance between point A and B is to be 1 $$\mu F$$ is : 

  • Question 4
    1 / -0
    Three capacitances, each of $$3\mu F$$, are provided. These cannot be combined to provide the resultant capacitance of :
    Solution
    We are provided with 3 capacitors each of capacitance 3 $$ \mu F $$
    We prove that the rest of the three combinations can be obtained with a combination of these.
    $$ 1 \mu F $$ = Combining all three of them in series
    $$ 2 \mu F $$ = Combining 2 in parallel and 1 in series with them
    $$ 4.5 \mu F $$ = Combining 2 in series and 1 in parallel combination
    Hence, only the 6 $$ \mu F $$ combination is not possible
  • Question 5
    1 / -0
    A sheet of aluminium foil of negligible thickness is introduced between the plates of a capacitor. The capacitance of the capacitor
    Solution
    The capacitance without aluminium foil is $$C=\dfrac{A\epsilon_0}{d}$$ 

    The capacitance with aluminium foil is $$C'=\dfrac{A\epsilon_0}{d-t}$$

    If thickness $$(t)$$ of foil is negligible so $$d-t \sim d.$$ Hence, $$C=C'$$ 
  • Question 6
    1 / -0
    Three capacitors each of $$4\ \mu F$$ are to be connected in such a way that the effective capacitance is $$6\ \mu F$$. This can be done by connecting them:
    Solution
    For capacitor is series, equivalent capacitance is given by:
    $$C_{S}=\dfrac{C_1C_2}{C_1+C_2}$$

    For capacitor is parallel, equivalent capacitance is given by:
    $$C_{P}=C_1+C_2$$

    In the given configuration, equivalent capacitance is given by
    $$C_{eq}=C_s+C$$, where $$C= 4\ \mu F$$
    and $$C_s=\dfrac{C \times C}{C+C}=\dfrac{C}{2}$$

    $$\therefore C_{eq}=C+\dfrac{C}{2}=6\ \mu F$$

  • Question 7
    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

    $$ V_A = \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{r_A} =  \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{\sqrt{2+2}}=  \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{2}$$

    $$ V_B= \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{r_B}=  \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{\sqrt{4+0}}= \dfrac{1}{4 \pi \epsilon } \dfrac{ q}{2} $$

    $$ V_A - V_B =0 $$

  • Question 8
    1 / -0
    A parallel plat capacitor is made of two circular plates separated by a distance of $$5 mm$$ and with a dielectric of dielectric constant $$2.2$$ between them. When the electric field in the dielectric is $$3 \times 10^4$$V/m, the charge density of the positive plate will be close to:
    Solution
    Answer is C.
    By formula of electric field between the plates of a capacitor $$ \displaystyle E = \dfrac{\sigma}{K\varepsilon_0}$$
    $$\sigma  = EK\varepsilon_0 = 3 \times 10^4 \times 2.2 \times 8.85 \times 10^{-12}$$
                           $$= 6.6 \times 8. 85 \times 10^{-8}$$
                           $$= 5.841 \times 10^{-7}$$
                           $$\cong 6 \times 10^{-7} C/m^2$$
  • Question 9
    1 / -0
    A parallel plate capacitor C with plates of unit area and separation d is filled with a liquid of dielectric constant $$K = 2.$$The level of liquid is $$\dfrac{d}{3}$$ initially. Suppose the liquid level decreases at a constant speed V, the time constant as a function of time $$t$$ is :

    Solution

    At time t the level of liquid is,

    $$ \dfrac { d }{ 3 }$$$$ -Vt\\ { C }_{ eq }=\dfrac { \dfrac { { \epsilon  }_{ 0 }KA }{ \dfrac { d }{ 3 } -Vt } \cdot \dfrac { { \epsilon  }_{ 0 }A }{ \dfrac { 2d }{ 3 } +Vt }  }{ \dfrac { { \epsilon  }_{ 0 }KA }{ \dfrac { d }{ 3 } -Vt } +\dfrac { { \epsilon  }_{ 0 }A }{ \dfrac { 2d }{ 3 } +Vt }  } =\dfrac { { \epsilon  }_{ 0 }KA }{ K\left( \dfrac { 2d }{ 3 } +Vt \right) +\dfrac { d }{ 3 } -Vt } \\ =\dfrac { 2{ \epsilon  }_{ 0 } }{ \left( \dfrac { 4d }{ 3 } +2Vt \right) +\dfrac { d }{ 3 } -Vt } =\dfrac { 2{ \epsilon  }_{ 0 } }{ \left( \dfrac { 5d }{ 3 } +Vt \right)  } =\dfrac { 6{ \epsilon  }_{ 0 } }{ 5d+3Vt } \\ \tau =R{ C }_{ eq }=\dfrac { 6{ \epsilon  }_{ 0 }R }{ 5d+3Vt } $$

  • Question 10
    1 / -0
    A parallel plate air capacitor of capacitance C is connected to a cell of emf V and then disconnected from it. A dielectric slab of dielectric constant K, which can just fill the air gap of the capacitor, is now inserted in it. Which of the following is incorrect?
    Solution
    $$C_f = KC_i$$
    $$Q_i =C_iV$$
    $$U_i = \frac{1}{2}C_iV^2$$
    $$U_f = \frac{1}{2}\frac{Q_f ^2}{C_f}$$
    After the capacitor is disconnected from the battery, charge on the capacitor cannot change.
    $$\therefore Q_f =Q_i$$
    $$ \therefore U_f = \frac{1}{2} \frac{Q_f ^2}{C_f}= \frac{1}{2}\frac{C_i ^2V^2}{KC_i}$$
    $$ \Delta U = U_f -U_i = \frac{1}{2}\frac{C_i ^2V^2}{KC_i} - \frac{1}{2}C_i V^2= \frac{1}{2}C_i V^2 ( \frac{1}{K} -1)=\frac{1}{2}C V^2 ( \frac{1}{K} -1) $$ since $$C_i= C$$ as given

    Option(A) is correct.

    Option (B) :
    Charge on the capacitor remains same since battery is disconnected.

    Option (C):
    C increases K times.
    Since $$Q = CV$$ and Q remains same, V decreases K times.

    Option D:
    The energy stored in the capacitor $$U_f$$ decreases K times.






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