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Electrostatic Potential and Capacitance Test - 49

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Electrostatic Potential and Capacitance Test - 49
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  • Question 1
    1 / -0
    Effective capacitance between A and B in the figure shown is (all capacitances are in $$\mu F$$).

    Solution
    The points C and D will be at same potentials since, $$\displaystyle\frac{3}{6}=\frac{4}{8}$$. Therefore, capacitance of $$2\mu F$$ will be unaffected. So, the equivalent circuit can be shown as the effective capacitance in upper in series, is given by
    $$C_1=\displaystyle\frac{3\times 6}{3+6}=\frac{18}{9}=2\mu F$$
    The effective capacitance in lower arm in series is given by
    $$C_2=\displaystyle\frac{4\times 8}{4+8}=\frac{32}{12}=\frac{8}{3}\mu F$$
    Hence, the resultant capacitance in parallel given by
    $$C=C_1+C_2=2+\displaystyle\frac{8}{3}=\frac{14}{3}\mu F$$.

  • Question 2
    1 / -0
    Two identical air filled parallel plate capacitors are charged to the same potential in the manner shown by closing the switch S. If now the switch S is opened and the space between the plates is filled with a dielectric of relative permittivity $$\displaystyle { \varepsilon  }_{ r }$$, then :

    Solution
    After switch S is opened, as the Capacitor A is connected across the battery, its potential difference is fixed at steady state (i.e., when capacitor is fully charged).

    Capacitor B is isolated, so its charge gets fixed. But as we insert the dielectric, its capacitance changes, thus its potential difference also changes.

    Option C is correct.
  • Question 3
    1 / -0
    Three capacitors connected in series have an effective capacitance of $$4 \mu F$$. If one of the capacitance is removed, the net capacitance of the capacitor increases to $$6 \mu F$$. The removed capacitor has a capacitance of
    Solution
    Let there are three capacitors with capacitances $$C_1,C_2 , C_3$$ respectively and $$ C_1 $$ is removed.
    In first case, $$\dfrac{1}{C_{eq1}}=\dfrac{1}{C_1}+\dfrac{1}{C_2}+\dfrac{1}{C_3} $$ ...(1)
    In second case, $$\dfrac{1}{C_{eq2}}=\dfrac{1}{C_2}+\dfrac{1}{C_3} $$ ...(2)
    From (1) and (2),  $$\dfrac{1}{C_{eq1}}=\dfrac{1}{C_1}+\dfrac{1}{C_{eq2}} $$ 
    or $$1/4=1/C_1+1/6$$
    or $$C_1=12\, \mu F$$

  • Question 4
    1 / -0
    The electrostatic potential energy of two point charges, $$1$$ $$\mu$$C each, placed $$1$$ meter apart in air is?
    Solution

    $$\textbf{Step 1: Formula of Potential energy}$$ 

    Electrostatic potential energy is given by $$U$$ between two charges placed at a separtion $$r$$ is given by 
    $$\Rightarrow\ \  U=\dfrac { k{ q }_{ 1 }{ q }_{ 2 } }{ r} $$

    $$\textbf{Step 2: Calculations}$$
    Putting values, $$k=9\times { 10 }^{ 9 }\dfrac { N.{ m }^{ 2 } }{ { C }^{ 2 } } ,$$ 
    $${ q }_{ 2 }={ q }_{ 1 }=1\mu C=1\times { 10 }^{ -6 }C,$$
    $$r=1m$$

    $$\\ \Rightarrow U\\ $$$$ =\dfrac { 9\times { 10 }^{ 9 }\times 1\times { 10 }^{ -6 }\times 1\times { 10 }^{ -6 } }{ 1 } =9\times { 10 }^{ -3 }J\\ $$

    Hence, correct option is $$C$$.
  • Question 5
    1 / -0
    Capacitance of a capacitor made by a thin metal foil is $$\displaystyle 2\mu F$$. If the foil is folded with paper of thickness 0.15 mm, dielectric constant of paper is 2.5 and width of paper is 400 mm, the length of the foil will be :
    Solution
    Here, let the length be $$l$$
    width is, $$b=400mm=0.4m$$
    thickness, $$t=0.15mm=15\times10^{-5}m$$

    As capacitance for parallel plate capacitor is, 
    $$C=K\epsilon_0A/d=K\epsilon_0(l\times b)/t$$
    $$\implies l=Ct/K\epsilon_0b=2\times10^{-6}\times15\times10^{-5}/(2.5\times8.85\times10^{-12}\times0.4)=33.91m$$

    Option D is correct.
  • Question 6
    1 / -0
    The potential of a large liquid drop when eight liquid drops are combined is $$20\ V$$. Then, the potential of each single drop was :
    Solution
    Volume of $$8$$ drops $$=$$ Volume of big drop
    $$\therefore \left (\dfrac {4}{3}\pi r^{3}\right ) \times 8 = \dfrac {4}{3} \pi R^{3}$$
    $$\Rightarrow 2r = R .... (i)$$
    According to charge conservation
    $$8q = Q .... (ii)$$
    We have
    $$V \propto \dfrac {1}{r}$$
    or $$\dfrac {V_{1}}{V_{2}} = \dfrac {r_{2}}{n}$$
    $$\Rightarrow  \dfrac {20}{V_{2}} = \dfrac {2r}{r}$$
    $$\Rightarrow V_{2} = 10\ V$$
  • Question 7
    1 / -0
    If a dielectric introduced between the plates of a parallel plate condenser, then which of the following is possible :
    Solution
    If a dielectric medium of dielectric constant $$K$$ is filled completely between the plates then capacitance increases by $$K$$ times
    $$C' = \dfrac {K\epsilon_{0}A}{d}$$
    $$\Rightarrow C' = KC$$.
  • Question 8
    1 / -0
    The capacity of a parallel plate capacitor with no dielectric substance but with a separation of 0.4 cm is $$\displaystyle 2\mu F$$. The separation is reduced to half and it is filled with a dielectric substance of value 2.8. The final capacity of the capacitor is
    Solution
    Initial capacitance   $$\displaystyle C = 2uF=\frac { { \varepsilon  }_{ 0 }{ A }}{ d } $$
    New capacitance  $$\displaystyle { C }^{ \prime  }=\frac { K{ \varepsilon  }_{ 0 }A }{ { d }^{ \prime  } } =\frac { 2.8\times { \varepsilon  }_{ 0 }A }{ (d/2)  } =5.6\frac { { \varepsilon  }_{ 0 }A }{ d } $$
    $$\displaystyle \Rightarrow  { C }^{ \prime  }= 5.6\times 2=11.2\mu F$$
  • Question 9
    1 / -0
    The capacity of a parallel plate capacitor with no dielectric substance but with a separation of $$0.4cm$$ is $$2\mu F$$. If the separation is reduced to half and it is filled with a dielectric substance of value $$2.8$$, then the final capacity of the capacitor is
    Solution
    Given, $$C=\cfrac { { \varepsilon  }_{ 0 }A }{ d } =2\mu F$$
    and $$C'=\cfrac { K{ \varepsilon  }_{ 0 }A }{ d' } =\cfrac { 2.8{ \varepsilon  }_{ 0 }A }{ d/2 } =\cfrac { 5.6{ \varepsilon  }_{ 0 }A }{ d } $$
    $$\Rightarrow C'=5.60\times 2=11.2\mu F$$
  • Question 10
    1 / -0
    Two capacitors of capacitance $$C$$ are connected in series. If one of them is filled with a substance of dielectric constant $$K$$, what is the effective capacitance?
    Solution
    When a substance of dielectric constant $$K$$ is filled in the capacitor, its capacity
    $${ C }_{ m }=\cfrac { K{ \varepsilon  }_{ 0 }A }{ d } =K{ C }_{ o }$$
    Here, $${ C }_{ o }=C$$
    $$\therefore { C }_{ m }==KC$$
    Now two capacitors of capacities $$KC$$ and $$C$$ are connected in series, therefore their effective capacitance
    $$\cfrac { 1 }{ C' } =\cfrac { 1 }{ KC } +\cfrac { 1 }{ C } =\cfrac { 1+K }{ KC } \Rightarrow C'=\cfrac { KC }{ (1+K) } $$
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