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Electrostatic Potential and Capacitance Test - 34

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Electrostatic Potential and Capacitance Test - 34
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  • Question 1
    1 / -0
    The two capacitors $$2\mu F$$ and $$6\mu F$$ are put in series, the effective capacity of the system in $$\mu F$$ is:
    Solution
    $$2\mu F, 6\mu F$$ are in series

    $$C_{eq}=\dfrac {C_1C_2}{C_1+C_2}$$

    $$=\dfrac {2\times 6}{(2+6)}=\dfrac {12}{8}=\dfrac {3}{2}\mu F$$
  • Question 2
    1 / -0
    Electrical potential at the centre of a charged conductor is:
    Solution
    Inside a charged conductor there is no electric field that is $$E=0$$.

    And, we know that $$\dfrac{dV}{dr}=-E=0$$

    $$\implies V=constant.$$

    Hence, electric potential at center of charged conductor is same as that on surface and at all points in conductor.

    Answer_(D)
  • Question 3
    1 / -0
    In a cathode ray oscillograph, the focussing of beam on the screen is achieved by
    Solution

  • Question 4
    1 / -0
    When two capacitors of capacities $$3\mu F$$ and $$6\mu F$$ are connected in series and connected to $$120 V,$$ the potential difference across $$3\mu F$$ is:
    Solution
    $$C=\dfrac {3\times 6}{9}=2\mu F$$
    $$V=120 V$$
    $$Q=CV=120\times 2=240\mu C$$
    $$V_3=\dfrac {Q}{3\mu F}=\dfrac {240\mu C}{2\mu F}=80 V$$
  • Question 5
    1 / -0
    If $$C_1=3pF$$ and $$C_2=2pF$$, calculate the equivalent capacitance of the network shown in the figure between points A and B?

    Solution

    The given network shown in figure is equivalent to the arrangement shown in figure, which is further equivalent to arrangement shown in figure.
    Therefore,
    $$\dfrac {1}{C'}=\dfrac {1}{C_1}+\dfrac {1}{C_2}+\dfrac {1}{C_1}$$
    $$=\dfrac {1}{3}+\dfrac {1}{2}+\dfrac {1}{3}=\dfrac {7}{6}$$ or $$C'=\dfrac {6}{7}pF$$
    Here, C" is capacitance of the parallel combination of C' and $$C_2.$$ Therefore,
    $$C"=C'+C_2=\dfrac {6}{7}+2=\dfrac {20}{7}pF$$
    If $$C_{equi}$$ is capacitance of the series combination of $$C_1, C" and C_1$$, then
    $$\dfrac {1}{C_{equi}}=\dfrac {1}{C_1}+\dfrac {1}{C"}+\dfrac {1}{C_1}=\dfrac {1}{3}+\dfrac {7}{20}+\dfrac {1}{3}$$
    $$=\dfrac {61}{60}$$
    or $$C_{equi}=\dfrac {60}{61}\approx 1pF$$

  • Question 6
    1 / -0
    Find the charge appearing on capacitor of capacitance $$4\;\mu F$$ :

    Solution
    As the two capacitances are in series combination, so equivalent capacitance,$$C_{equ}=\dfrac{8\times4}{8+4}=\dfrac{32}{12}=\dfrac{8}{3} \mu F$$
    So, charge on $$4\ \mu F, Q=C_{equ}\times V=\dfrac{8}{3}\times12=32 \ \mu C$$
  • Question 7
    1 / -0
    Condensers of capacities $$2\mu F$$ and $$3\mu F$$ are connected in series and a condenser of capacity $$1\mu F$$ is connected in parallel with them. The resultant capacity is:
    Solution
    $$\dfrac{6}{5}+1=\dfrac{11}{5}=2.2\mu F$$.

  • Question 8
    1 / -0
    What is the equivalent capacitance of the system of capacitors between $$A \mbox{ & } B$$?

    Solution
    The capacitors in the right hand square are in series. So they can be replaced by an equivalent capacitor of capacitance of:
    $$1/(1/C+1/C) = C/2$$
     The next step is to replace C and C/2 by a capacitor having an equivalent capacitance of C and C/2 in parallel.
     $$C+C/2=3C/2$$
    Then, C and 3C/2 are in series. So, they can be replaced by a capacitor having an equivalent capacitance of
    $$1/(1/C+2/3C)=3C/5$$
    Then since in parallel they can be replaced by an equivalent capacitance of $$C+3C/5=8C/5 = 1.6C$$ 
    So the equivalent capacitance is 1.6C.
  • Question 9
    1 / -0
    If $$4\times 10^{20}eV$$ of energy is required to move a charge of 0.25 coulomb between two points, the p.d between them is:
    Solution
    $$\displaystyle V=\frac {W}{Q}=\frac {4\times 10^{20}\times 1.6\times 10^{-19}J}{0.25C}$$
    $$=256 V$$
  • Question 10
    1 / -0
    A capacitor stores $$60\space\mu C$$ charge when connected across a battery. When the gap between the plates is filled with a dielectric, a charge of $$120\space\mu C$$ flows through the battery. The dielectric constant of the material inserted is :
    Solution
    The capacitance before filled with dielectric is $$C=\dfrac{A\epsilon_0}{d}$$
    The capacitance after filled with dielectric is $$C'=\dfrac{Ak\epsilon_0}{d}=kC$$
    Initial charge, $$Q=60 \mu C$$ and total charge after filled with dielectric $$Q'=120+60=180  \mu C$$
    Here, $$Q=CV$$ and $$Q'=C'V=kCV$$
    $$\dfrac{Q'}{Q}=\dfrac{kCV}{CV}$$
    $$k=\dfrac{Q'}{Q}=\dfrac{180}{60}=3$$
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