Electric Charges and Fields


Electric Charges and Fields

  1. Suppose the charge of a proton and an electron differ slightly. One of them is – e, the other is (e + ∆e). If the net of electrostatic force and gravitational force between two hydrogen atoms placed at a distance d (much greater than atomic size) apart is zero, then ∆e is of the order of [Given mass of hydrogen mh = 1.67 × 10–27 kg]









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    According to question, the net electrostatic force (FE) = gravitational force  (FG)
    ​FE = FG

    or
    1
    ∆e2
    =
    Gm2
    4πε0d2d2

    ⇒ ∆e = m
    G
    K

    1
    = k = 9 × 109
    4πε0

    = 1.67 × 10–27
    6.67 × 10–11
    9 × 109

    ∆e ≈ 1.436 × 10–37 C

    Correct Option: B

    According to question, the net electrostatic force (FE) = gravitational force  (FG)
    ​FE = FG

    or
    1
    ∆e2
    =
    Gm2
    4πε0d2d2

    ⇒ ∆e = m
    G
    K

    1
    = k = 9 × 109
    4πε0

    = 1.67 × 10–27
    6.67 × 10–11
    9 × 109

    ∆e ≈ 1.436 × 10–37 C


  1. Two identical charged spheres suspended from a common point by two massless strings of lengths l, are initially at a distance d (d << l) apart because of their mutual repulsion. The charges begin to leak from both the spheres at a constant rate. As a result, the spheres approach each other with a velocity v. Then v varies as a function of the distance x between the spheres, as :











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    From figure tan θ =
    Fc
    ; θ
    mg

    kq2
    =
    x
    x2 mg2ℓ


    or​ x3 ∝ q2  …(1) ​
    or​ x3/ 2 ∝ q …(2) ​
    Differentiating eq. (1) w.r.t. time
    3x2
    dx
    ∝ 2q
    dq
    but
    dq
    is constant ​
    dtdtdt

    so x2(v) ∝ q Replace q from eq. (2) ​
    x2(v) ∝ x3/2 or v ∝ x–1/2

    Correct Option: C

    From figure tan θ =
    Fc
    ; θ
    mg

    kq2
    =
    x
    x2 mg2ℓ


    or​ x3 ∝ q2  …(1) ​
    or​ x3/ 2 ∝ q …(2) ​
    Differentiating eq. (1) w.r.t. time
    3x2
    dx
    ∝ 2q
    dq
    but
    dq
    is constant ​
    dtdtdt

    so x2(v) ∝ q Replace q from eq. (2) ​
    x2(v) ∝ x3/2 or v ∝ x–1/2



  1. Two pith balls carrying equal charges are suspended from a common point by strings of equal length. The equilibrium separation between them is r. Now the strings are rigidly clamped at half the height. The equilibrium separation between the balls now become​​









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    From figure,  tan θ =
    Fe
    r / 2
    =
    kq2
    mgyr2 / mg

    [ ∵ F =
    kq2
    from coulomb’s law]
    r2

    ⇒ r3 ∝ y ⇒ r'3
    y
    r'
    =
    1
    2r21 / 3

    ⇒ r' =
    r
    32

    Correct Option: A


    From figure,  tan θ =
    Fe
    r / 2
    =
    kq2
    mgyr2 / mg

    [ ∵ F =
    kq2
    from coulomb’s law]
    r2

    ⇒ r3 ∝ y ⇒ r'3
    y
    r'
    =
    1
    2r21 / 3

    ⇒ r' =
    r
    32


  1. A charge ‘q’ is placed at the centre of the line joining two equal charges ‘Q’. The system of the three charges will be in equilibrium if ‘q’ is equal to​​









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    The system of three charges will be in equilibrium.

    For this, force between charge at A and B + force between charge at point O and either at  A or B is zero.

    i.e. ,
    KQ2
    +
    KQq
    = 0
    r2(r / 2)2

    By solving we get,
    q = -
    Q
    4

    Correct Option: B

    The system of three charges will be in equilibrium.

    For this, force between charge at A and B + force between charge at point O and either at  A or B is zero.

    i.e. ,
    KQ2
    +
    KQq
    = 0
    r2(r / 2)2

    By solving we get,
    q = -
    Q
    4



  1. An electron is moving round the nucleus of a hydrogen atom in a circular orbit of radius r. The Coulomb force F between the two is​









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    Charges (–e) on electron and (e) on proton exert a force of attraction given by ​

    Force = (K)
    (-e)(e)
    r̂ =
    -Ke2
    ∵ r̂ =
    r
    r2r3| r |

    Note : Magnitude of Coulomb force is given by
    F =
    1
    .
    q1q2
    4πε0r2

    but in vector form F =
    1
    .
    q1q2
    r
    4πε0r2

    Correct Option: D

    Charges (–e) on electron and (e) on proton exert a force of attraction given by ​

    Force = (K)
    (-e)(e)
    r̂ =
    -Ke2
    ∵ r̂ =
    r
    r2r3| r |

    Note : Magnitude of Coulomb force is given by
    F =
    1
    .
    q1q2
    4πε0r2

    but in vector form F =
    1
    .
    q1q2
    r
    4πε0r2