Two identical conducting spheres \(A\) and \(B\) carry an equal charge. They are separated by a distance much larger than their diameters and the force between them is \(F.\) A third identical conducting sphere \(C\) is uncharged. The sphere \(C\) is first touched to \(A\) then to \(B\) and then removed. As a result, the force between \(A\) and \(B\) would be equal to:
1. \(\dfrac{3F}{4}\)

2. \(\dfrac{F}{2}\)

3. \(\dfrac{3F}{8}\)

4. \(F\)
Subtopic:  Coulomb's Law |
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Let a total charge \(2Q\) be distributed in a sphere of radius \(R\), with the charge density given by \(\rho(r)=kr \), where \(r\) is the distance from the centre. Two charges \(A\) and \(B\), of \(-Q \) each, are placed on diametrically opposite points, at equal distance, a from the centre. If \(A\) and \(B\) do not experience any force, then:
1. \(a=8^{-1/4}R\)
2. \(a=2^{-1/4}R\)
3. \(a=\frac{3R}{2^{1/4}}\)
4. \(a=R/\sqrt{3}\)

Subtopic:  Coulomb's Law |
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Three charges \(+Q, q, +Q\) are placed respectively, at a distance, \(0,~d/2\) and \(d\) from the origin, on the \(x\text-\)axis. If the net force experienced by \(+Q,\) placed at \(x=0,\) is zero, then the value of \(q\) is:
1. \(\frac{-Q}{4}\)

2. \(\frac{+Q}{2}\)

3. \(\frac{+Q}{4}\)

4. \(\frac{-Q}{2}\)
Subtopic:  Coulomb's Law |
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Consider the force \(F\) on a charge \(q\)  due to a uniformly charged spherical shell of radius \(R\) carrying charge \(Q\) distributed uniformly over it. Which one of the following statements is true for \(F\), if \(q\) is placed at a distance \(r\) from the centre of the shell? 

1. \( F=\dfrac{1}{4 \pi \varepsilon_0} \dfrac{Q q}{r^2} \text { for } r>R \)
2. \( \dfrac{1}{4 \pi \varepsilon_0} \dfrac{Q q}{R^2}>F>0 \text { for } r<R \)
3. \( F=\dfrac{1}{4 \pi \varepsilon_0} \dfrac{Q q}{r^2} \text { for all } r \)
4. \(F=\dfrac{1}{4 \pi \varepsilon_0} \dfrac{Q q}{r^2} \text { for } r<R \)
Subtopic:  Coulomb's Law |
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Two electrons are fixed at a distance of \(2d\) apart. A proton is placed at the midpoint between them and is displaced slightly by a distance \(x\) \((x\ll d)\) perpendicular to the line joining the two fixed electrons. The proton will undergo simple harmonic motion with an angular frequency given by:
(here, \(m\) is the mass of the proton, \(q\) is the magnitude of the charge, and \(\varepsilon_0\)​ is the permittivity of free space)

1. \(\sqrt{\left( {\dfrac{2 q^2}{\pi \varepsilon_0 m d^3}}\right)}\)

2. \(\sqrt{\left (\dfrac{\pi \varepsilon_0 {md}^3}{2 {q}^2} \right )}\)

3. \(\sqrt{\left ({\dfrac{ q^2}{2\pi \varepsilon_0 m d^3}}\right)}\)

4. \(\sqrt{\left( \dfrac{2\pi \varepsilon_0 {md}^3}{m{q}^2}\right)}\)

Subtopic:  Coulomb's Law |
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Two small spheres each of mass \(10~\text{mg}\) are suspended from a point by threads \(0.5~\text{m}\) long. They are equally charged and repel each other to a distance of \(0.20~\text m.\). The charge on each of the spheres is \(\frac{a}{21} \times 10^{-8} \mathrm{~C}.\) The value of '\(a\)' will be:
(given \(g=10~\mathrm{ms^{-2}}\))

1. \(25\) 2. \(30\)
3. \(40\) 4. \(20\)
Subtopic:  Coulomb's Law |
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Two identical conducting spheres, each with negligible volume, carry initial charges of \(2.1~\text{nC}\) and \(-0.1~\text{nC},\) respectively. The spheres are brought into contact, allowing charge to redistribute, and are then separated by a distance of \(0.5~\text m.\) The electrostatic force acting between the spheres is: 
\(\left ( 4 \pi \varepsilon_0=\frac{1}{9 \times 10^9}~\text{in SI units} \right )\) 
1. \(36 \times 10^{-7}~\mathrm{N}\)
2. \(36 \times 10^{-9}~\mathrm{N}\)
3. \(18 \times 10^{-7}~\mathrm{N}\)
4. \(18 \times 10^{-9}~\mathrm{N}\)

Subtopic:  Coulomb's Law |
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Two identical charged particles, each having a mass \(10\) g and charge \(2.0 \times 10^{-7}\) C, are placed on a horizontal table with a separation of \(L\) between them such that they stay in limited equilibrium. If the coefficient of friction between each particle and the table is \(0.25\), the value of \(L\) is: [Use \(g = 10\) ms-2]
1. \(12\) cm 
2. \(10\) cm 
3. \(8\) cm 
4. \(5\) cm 
Subtopic:  Coulomb's Law |
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Three identical charged balls each of charge \(2C\) are suspended from a common point \(P\) by silk threads of \(2~\text{m}\) each (as shown in the figure). They form an equilateral triangle of side \(1~\text{m}\). The ratio of the net force on a charged ball to the force between any two charged balls will be:
        
1. \(1:1\)
2. \(1:4\)
3. \(\sqrt 3 :2\)
4. \(\sqrt 3:1\)
Subtopic:  Coulomb's Law |
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Two point charges, \(Q\) each, are placed at a distance \(d\) apart. A third point charge \(q\) is placed at a distance \(x\) from the mid-point on the perpendicular bisector. The value of \(x\) at which charge \(q\) will experience the maximum Coulomb's force is:
1. \(x = d\)
2. \(x = \dfrac{d}{2}\)
3. \(x = \dfrac{d}{\sqrt 2}\)
4. \(x = \dfrac{d}{2\sqrt 2}\)
Subtopic:  Coulomb's Law |
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