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Electric Charges and Fields Test - 22

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Electric Charges and Fields Test - 22
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  • Question 1
    1 / -0
    A hollow metal sphere of radius R is uniformly charged. The electric field due to the sphere at a distance r from the centre 
    Solution
    Charge Q will be distributed over the surface of hollow metal sphere. 
    (i) For r < R (inside)
    By Gauss law, Einˉ.dS=qenε0=0\oint \bar{E_{in}} . \overline{dS} = \dfrac{q_{en}}{\varepsilon_0}= 0
    Ein=0\Rightarrow E_{in} = 0            (qen=0)(\because q_{en} = 0)
    (ii) For r > R (out side)
    Eˉ0.dS=qenε0\oint \bar{E}_0 . \overline{dS} = \dfrac{q_{en}}{\varepsilon_0}
    Here, qen=Q(qen=Q)q_{en} = Q (\because q_{en} = Q)
    E04πr2=Qε0\therefore E_0 4 \pi r^2 = \dfrac{Q}{\varepsilon _0}
    E01r2\therefore E_0 \propto \dfrac{1}{r^2}

  • Question 2
    1 / -0
    Electric field outside a long wire carrying charge q is proportional to :
    Solution
    Using Gauss Law across the cylindrical Gaussian surface,
    E.dS=qencϵ0\displaystyle\int E.dS = \dfrac{q_{enc}}{\epsilon_0}
    E×2πr×l=λ×lϵ0\therefore E\times 2\pi r \times l = \dfrac{\lambda\times l}{\epsilon_0}
    E=λ2πrϵ0\therefore E = \dfrac{\lambda}{2\pi r\epsilon_0}
    Here λ\lambda is the linear charge density on the wire.

  • Question 3
    1 / -0
    An electric line of force in the xyplanexy-plane is given by equation x2+y2=1x^{2} + y^{2} = 1. A particle with unit positive charge, initially at rest at the point x=1,y=0x = 1, y = 0 in the xyplanexy - plane.
    Solution
    Charge will move along the circular line of force because x2+y2=1x^{2} + y^{2} = 1 is the equation of circle in xyplanexy - plane.
  • Question 4
    1 / -0
    Two identical charged spheres suspended from a common distance d(d<<1)d(d < < 1) apart because of their mutual repulsion. The charged begin to leak from both the spheres at a constant rate. As a result, the spheres approach each other with a velocity vv. Then vv varies as a function of the distance xx between the spheres, as
    Solution
    From figure tanθ=Femg=θ\tan \theta = \dfrac {F_{e}}{mg} =\theta
    kq2x2mg=x2l\dfrac {kq^{2}}{x^{2}mg} = \dfrac {x}{2l}
    or x3q2....(1)x^{3}\propto q^{2} .... (1)
    or x3/2q.....(2)x^{3/2} \propto q ..... (2)
    Differentiating eq. (1)(1) w.r.t time
    3x2dxdt2qdqdt3x^{2} \dfrac {dx}{dt}\propto 2q \dfrac {dq}{dt} but dqdt\dfrac {dq}{dt} is constant
    so x2(v)qx^{2}(v) \propto q Replace qq from eq. (2)(2)
    x2(v)x3/2x^{2}(v) \propto x^{3/2} or vx1/2v\propto x^{-1/2}.
  • Question 5
    1 / -0

    Two unlike charges attract each other with a force of 10N. If the distance between them is doubled, the force between them is :

    Solution
    We know F=14πε0q1q2r2=10NF=\dfrac {1}{4\pi \varepsilon_0}\dfrac {q_1q_2}{r^2}=10 N

    if distance is doubled.
    Fnew=14πε0q1q2(2r)2=104F_{new}=\dfrac {1}{4\pi \varepsilon_0}\cdot \dfrac {q_1q_2}{(2r)^2}=\dfrac {10}{4}

    =25N=2\cdot 5 N
  • Question 6
    1 / -0

    Number of electric lines of force emanating from 1C1C of positive charge in vacuum is :

    Solution
    ϕ\phi from 1C1C of charge is =Qenclosedϵo= \dfrac{Q_{enclosed}}{\epsilon_o}
    =18.8501×1012= \dfrac{1}{8.8501\times 10^{-12}}

    =1.129×1011= 1.129\times 10^{11}
  • Question 7
    1 / -0

    A force ‘F’ is acting between two charges in air. If the space between them be completely filled with a medium K=4K=4, the force will be :

    Solution
    By Coulomb's law, the force between two charges (q1,q2)(q_1, q_2) in air is given by F=q1q24πϵ0r2F=\dfrac{q_1q_2}{4\pi\epsilon_0 r^2}  
    where r=r= distance between two charges.
    Now the force between two charges (q1,q2)(q_1, q_2) in medium with dielectric constant K=4K=4 becomes, F=q1q24πKϵ0r2F'=\dfrac{q_1q_2}{4\pi K\epsilon_0 r^2}
    So, F=FK=F4F'=\dfrac{F}{K}=\dfrac{F}{4}
  • Question 8
    1 / -0

    An electron revolves around the nucleus of hydrogen atom in a circle of radius 5×1011 m5\times 10^{-11}\ mThe intensity of electric field at a point in the orbit of the electron is:

    Solution
    We know hydrogen atom consist of one proton and one electron
    R=5×1011mR=5\times 10^{-11} m
    We know attractive force =kq1(q2)r2=9×109×(16×1019)2(5×1011)2=\dfrac {k q_1(q_2)}{r^2}=\dfrac {9\times 10^9\times (1\cdot 6\times 10^{-19})^2}{(5\times 10^{-11})^2}
    We know   F=EqF = E q
    E=Fq\therefore E=\dfrac {F}{q}
    E=9×109×(16×1019)5×1011)2=576×1011N/C.\therefore E=\dfrac {9\times 10^9\times (1\cdot 6\times 10^{-19})}{5\times 10^{-11})^2}=5\cdot 76\times 10^{11} N/C.

  • Question 9
    1 / -0
    A charge q1q_1 exerts a force of 45N45N on a charge of q2=105Cq_{2}=10^{-5} C located at a point 0.2m0.2m from q1q_{1}. The magnitude of q1q_{1} is
    Solution
    As we know electrostatic force between two charges F=kq1q2r2F=\dfrac {k q_1 q_2}{r^2}

    45=(9×109)(q1)(105)(02)2\Rightarrow 45=\dfrac {(9\times 10^9)(q_1)(10^{-5})}{(0\cdot 2)^2}

    q1=45×02×029×109×105\Rightarrow q_1=\dfrac {45\times 0\cdot 2\times 0\cdot 2}{9\times 10^9\times 10^{-5}}

    q1=2×105C\Rightarrow q_1=2\times 10^{-5}C
  • Question 10
    1 / -0
    When we remove polyester or woollen clothes in dark, we can see a spark and hear a crackling sound. Which of the following is responsible for it?
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