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Electrostatic Potential and Capacitance Test - 47

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Electrostatic Potential and Capacitance Test - 47
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  • Question 1
    1 / -0
    Three capacitors of capacitance 1.0,2.01.0,2.0 and 5.0μF5.0\mu F are connected in series to a 10V10V source. The potential difference across the 2.0μF2.0\mu F capacitor is
    Solution
    Ceq=1017μF,Q=10017μC{ C }_{ eq }=\cfrac { 10 }{ 17 } \mu F,Q=\cfrac { 100 }{ 17 } \mu C\quad
    \therefore Potential difference across 2μF2\mu F capacitor
    =10017μC2μF=5017V=\cfrac { \cfrac { 100 }{ 17 } \mu C }{ 2\mu F } =\cfrac { 50 }{ 17 } V
  • Question 2
    1 / -0
    A metal plate of thickness d/2d/2 is introduced in between the plates of a parallel plate air capacitor with plate separation of dd. Capacity of the metal plate :
    Solution
    C=ϵoAdC=\dfrac{\epsilon_oA}{d}
    when a dielectric is filled ,thickness t
    C1=ϵoAdt+tKC_1=\dfrac{\epsilon_oA}{d-t+\frac{t}{K}}
    for metal k= infinity ,t=d2t=\dfrac{d}{2}
    C1=2ϵoAd=2CC_1=\dfrac{2\epsilon_oA}{d}=2C
  • Question 3
    1 / -0
    An electron enters into a space between the plates of parallel plate capacitor at an angle of α\alpha with the plates and leaves at an angle of β\beta to the plates. The ratio of its KEKE while leaving to entering the capacitor will be :
    Solution
    We know that Electric field is always perpendicular to the plates of the capacitor.

    Let the speed of the electron be v1v_1 when it enters the gap between the plates and v2v_2 when it leaves the plates.

    As the electron only experiences force in the direction perpendicular to the plates, by the conservation of momentum in the direction parallel to the plates, we have
    v1cos(α)=v2cos(β)v2v1=cosαcosβv_1\textrm{cos}(\alpha) = v_2\textrm{cos}(\beta) \Rightarrow \dfrac{v_2}{v_1} = \dfrac{\textrm{cos}\alpha}{\textrm{cos}\beta}

    The ratio of kinetic energy is given by (v2v1)2=(cosαcosβ)2(\dfrac{v_2}{v_1})^2 = (\dfrac{\textrm{cos}\alpha}{\textrm{cos}\beta})^2
  • Question 4
    1 / -0
    Given below are three schematic graphs of potential energy V(r)V(r) versus distance rr for three atomic particles: electron (e)(e^{-}), proton (p+)(p^{+}) and neutron (n)(n), in the presence of a nucleus at the origin OO. The radius of the nucleus is r0r_{0}. The scale on the V-axis may not be the same for all figures. The correct pairing of each graph with the corresponding atomic particle is.

    Solution
    The interaction forces between the sub-atomic particles are
    (i) Electrostatic forces and (ii) Nuclear forces/Strong forces.

    The nuclear forces are very large in magnitude compared to electrostatic forces, but they are short distance forces. They only act within the nucleus.

    Thus, within the nucleus, the potential is governed by nuclear forces and outside the nucleus, it is governed by the electrostatic forces.

    Case 1: Neutron\textrm{Case 1: Neutron}
    Neutron is a chargeless particle. Thus, outside the nucleus, electrostatic potential energy of neutron is zero.
    But, within the nucleus, the nuclear forces (attractive) bind the neutron to the nucleus. Hence potential energy is negative.
    Thus, Potential energy of neutron corresponds to figure (1)

    Case 2: Proton\textrm{Case 2: Proton}
    proton is a positively charged particle. Thus, outside the nucleus, electrostatic forces on the proton are repulsive. Thus, potential energy of proton is positive.
    But, within the nucleus, the nuclear forces (attractive) bind the proton to the nucleus. Hence potential energy is negative.
    Thus, Potential energy of proton corresponds to figure (2)

    Case 3: Electron\textrm{Case 3: Electron}
    Electron is a negatively charged particle. Thus, outside the nucleus, electrostatic forces on the electron are attractive. Thus, potential energy of electron is negative.
    But, within the nucleus, the nuclear forces and the electrostatic forces are of the same order (since electron is not a intra nuclear particle).
    Thus, Potential energy of electron corresponds to figure (3)
  • Question 5
    1 / -0
    How many 6μF6\mu F, 200V200 V condensers are needed to make a condenser of 18μF18\mu F, 600V600 V?
    Solution
    Place three 200V, 6μF6\mu F capacitors in series to get 1 equivalent 600V, 2μF2\mu F capacitor. Now place 9 of these equivalent 600V, 2μF2\mu F capacitors in parallel to obtain an equivalence of 18μF18\mu F at 600 Volts. All this requires a total of 27 6μF6\mu F capacitors. Nine rows connected in parallel with 3 capacitors connected in series in each row.
  • Question 6
    1 / -0
    The minimum value of effective capacitance that can be obtained by combining 33 capacitors of capacitances 1pF1 pF, 2pF2 pF and 4pF4 pF is
    Solution
    Minimum capacitance is obtained when these three capacitors are connected in series with each other.
    Effective capacitance of series combination 1Ceff =1C1+1C2+1C3\dfrac{1}{C_{eff}}  = \dfrac{1}{C_1} + \dfrac{1}{C_2} + \dfrac{1}{C_3}
    \therefore  1Ceff =11+12+14\dfrac{1}{C_{eff}}  = \dfrac{1}{1} + \dfrac{1}{2} + \dfrac{1}{4}
        \implies  Ceff=47pFC_{eff} = \dfrac{4}{7}p F
  • Question 7
    1 / -0
    Two identical parallel plate capacitance C each are connected in series with a battery of emf, E as shown, If one of the capacitors is now filled with a dielectric of dielectric constant k, the amount of charge which will flow through the battery is ??(neglect internal resistance of the battery)

    Solution
    Inital charge on both the capacitor Q=CE2Q=\dfrac{CE}{2}
    final chargeQf=kCEK+1Q_f=\dfrac{kCE}{K+1}
    charge flow from batter is QfQ=k12(k+1)CEQ_f-Q=\dfrac{k-1}{2(k+1)}CE
  • Question 8
    1 / -0
    A charge 10nC10nC is situated in a medium of relative permittivity 1010. The potential due to this charge at a distance of 0.1m0.1 m is :
    Solution
    Relative permittivity of the charge  ϵr=10\epsilon_r =10
    Magnitude of charge  q=10nC=108Cq = 10nC = 10^{-8} C
    Potential at a distance 0.1m0.1m,   Vp=q4πϵdV_p = \dfrac{q}{4\pi \epsilon d}  
    where ϵ=ϵrϵo\epsilon = \epsilon_r \epsilon_o
    \therefore  Vp=q4πϵoϵrdV_p = \dfrac{q}{4\pi \epsilon_o \epsilon_r d}
    Or  Vp=9×109×10810×0.1=90VV_p = \dfrac{9\times 10^9 \times 10^{-8}}{10 \times 0.1} =90 V
  • Question 9
    1 / -0
    An insulator plate is passed between the plates of a capacitor. Then, current :

    Solution

  • Question 10
    1 / -0
    Two charges +6μC+6\mu C and 4μC-4\mu C are placed 15cm15 cm apart as shown. At what distances from AA to its right, the electrostatic potential is zero?

    Solution
    Let the potential be zero at point PP at a distance xx from the charge +6×106C+6\times { 10 }^{ -6 }C at AA as shown in above figure. Potential at PP
    V=14πε 0[6×106x(4×106) 15x ]V=\dfrac { 1 }{ 4\pi { \varepsilon  }_{ 0 } } \left[ \dfrac { 6\times { 10 }^{ -6 } }{ x } -\dfrac { \left( -4\times { 10 }^{ -6 } \right)  }{ 15-x }  \right]
    0=14πε 0[6×106x4×10615x ]0=\dfrac { 1 }{ 4\pi { \varepsilon  }_{ 0 } } \left[ \dfrac { 6\times { 10 }^{ -6 } }{ x } -\dfrac { 4\times { 10 }^{ -6 } }{ 15-x }  \right]
    0=6×106x4×10615x0=\dfrac { 6\times { 10 }^{ -6 } }{ x } -\dfrac { 4\times { 10 }^{ -6 } }{ 15-x }
    6×106x=4×10615x \dfrac { 6\times { 10 }^{ -6 } }{ x } =\dfrac { 4\times { 10 }^{ -6 } }{ 15-x }
    6(15x)=4x\Rightarrow 6\left( 15-x \right) =4x
    906x=4x\Rightarrow 90-6x=4x
    10x=90\Rightarrow 10x=90
    x=9010=9cm\Rightarrow x=\dfrac { 90 }{ 10 } =9 cm
    The other possibility is that point of zero potential PP may lie on ABAB produced at a distance xx from the charge +6×106C+6\times { 10 }^{ -6 }C at AA as shown in the figure.
    Potential at PP
    V=14πε 0[6×106x+(4×106) (15x)  ]V=\dfrac { 1 }{ 4\pi { \varepsilon  }_{ 0 } } \left[ \dfrac { 6\times { 10 }^{ -6 } }{ x } +\dfrac { \left( -4\times { 10 }^{ -6 } \right)  }{ \left( 15-x \right)  }  \right]
    0=14πε 0[6×106x4×106(x15)  ]0=\dfrac { 1 }{ 4\pi { \varepsilon  }_{ 0 } } \left[ \dfrac { 6\times { 10 }^{ -6 } }{ x } -\dfrac { 4\times { 10 }^{ -6 } }{ \left( x-15 \right)  }  \right]
    0=6×106x4×106(x15) 0=\dfrac { 6\times { 10 }^{ -6 } }{ x } -\dfrac { 4\times { 10 }^{ -6 } }{ \left( x-15 \right)  }
    6×106x=4×106x15\Rightarrow \dfrac { 6\times { 10 }^{ -6 } }{ x } =\dfrac { 4\times { 10 }^{ -6 } }{ x-15 }
    6x=4x15\Rightarrow \dfrac { 6 }{ x } =\dfrac { 4 }{ x-15 }
    6x90=4x\Rightarrow 6x-90=4x
    2x=90\Rightarrow 2x=90
    x=902=45cm\Rightarrow x=\dfrac { 90 }{ 2 } =45 cm

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