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Exercises · 1.12

Q.(a) Two insulated charged copper spheres A and B have their centres separated by a distance of 50 cm50\,\text{cm}. What is the mutual force of electrostatic repulsion if the charge on each is 6.5×10−7 C6.5 \times 10^{-7}\,\text{C}? The radii of A and B are negligible compared to the distance of separation.

(b) What is the force of repulsion if each sphere is charged double the above amount, and the distance between them is halved?
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This problem applies Coulomb's Law to calculate the electrostatic force between two point charges. In part (a), the force is 1.521×10−2 N1.521 \times 10^{-2}\,\text{N}. In part (b), when charges are doubled and distance is halved, the force increases by a factor of 16, becoming 0.24336 N0.24336\,\text{N}.

The fundamental principle governing the interaction between stationary electric charges is Coulomb's Law. It describes the electrostatic force as directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between their centres. This "inverse square law" is a recurring theme in physics, appearing in gravitation and light intensity as well.

The reason this law works for spheres with negligible radii is that, for practical purposes, we can treat them as point charges located at their centres. This simplification is crucial because Coulomb's Law is derived for point charges. If the spheres were large compared to their separation, the charge distribution on their surfaces would become non-uniform due to mutual repulsion, making the calculation more complex. However, the problem statement explicitly allows us to treat them as point charges.

The magnitude of the electrostatic force FF between two point charges q1q_1 and q2q_2 separated by a distance rr is given by:

F=k∣q1q2∣r2F = k \frac{|q_1 q_2|}{r^2}

where kk is Coulomb's constant, approximately 9×109 N m2/C29 \times 10^9\,\text{N m}^2/\text{C}^2 in vacuum or air.

Let's apply this law to the given scenarios.

Part (a): Calculating the initial force of repulsion

  1. Identify the given quantities:

    • Charge on sphere A, qA=6.5×10−7 Cq_A = 6.5 \times 10^{-7}\,\text{C}
    • Charge on sphere B, qB=6.5×10−7 Cq_B = 6.5 \times 10^{-7}\,\text{C}
    • Distance of separation, r=50 cmr = 50\,\text{cm}
    • Coulomb's constant, k=9×109 N m2/C2k = 9 \times 10^9\,\text{N m}^2/\text{C}^2
  2. Convert units to SI standard:

    The distance rr is given in centimetres, so we convert it to metres:

    r=50 cm=0.50 mr = 50\,\text{cm} = 0.50\,\text{m}

    The charges are already in Coulombs (C).

  3. Apply Coulomb's Law:

    Substitute the values into the formula F=kqAqBr2F = k \frac{q_A q_B}{r^2}. Since both charges are positive, the force will be repulsive.

    F=(9×109 N m2/C2)(6.5×10−7 C)(6.5×10−7 C)(0.50 m)2F = (9 \times 10^9\,\text{N m}^2/\text{C}^2) \frac{(6.5 \times 10^{-7}\,\text{C})(6.5 \times 10^{-7}\,\text{C})}{(0.50\,\text{m})^2}

    F=(9×109)(6.5)2×(10−7)2(0.50)2F = (9 \times 10^9) \frac{(6.5)^2 \times (10^{-7})^2}{(0.50)^2}

    F=(9×109)42.25×10−140.25F = (9 \times 10^9) \frac{42.25 \times 10^{-14}}{0.25}

    F=(9×109)×(169×10−14)F = (9 \times 10^9) \times (169 \times 10^{-14})

    F=1521×10−5 NF = 1521 \times 10^{-5}\,\text{N}

    F=1.521×10−2 NF = 1.521 \times 10^{-2}\,\text{N}

Part (b): Calculating the force with changed conditions

  1. Identify the new conditions:

    • Each sphere is charged double the amount: qA′=2qA=2×(6.5×10−7 C)=13×10−7 Cq_A' = 2q_A = 2 \times (6.5 \times 10^{-7}\,\text{C}) = 13 \times 10^{-7}\,\text{C}
    • qB′=2qB=13×10−7 Cq_B' = 2q_B = 13 \times 10^{-7}\,\text{C}
    • The distance between them is halved: r′=r2=50 cm2=25 cmr' = \frac{r}{2} = \frac{50\,\text{cm}}{2} = 25\,\text{cm}
  2. Convert units to SI standard:

    r′=25 cm=0.25 mr' = 25\,\text{cm} = 0.25\,\text{m}

  3. Apply Coulomb's Law with new values:

    F′=kqA′qB′(r′)2F' = k \frac{q_A' q_B'}{(r')^2} …

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