The equivalent capacitance of the system shown in the following circuit is:

   
1. \(9~\mathrm{\mu F}\) 2. \(2~\mathrm{\mu F}\)
3. \(3~\mathrm{\mu F}\) 4. \(6~\mathrm{\mu F}\)

Subtopic:  Combination of Capacitors |
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An electric dipole is placed as shown in the figure.
        
The electric potential (in \(10^2~V\)) at point \(P\) due to the dipole is(\(\epsilon_0\)= permittivity of free space and \(\frac{1}{4 \pi \epsilon_0}=k\)):
1. \((\frac{8}{3})qk\)
2. \((\frac{3}{8})qk\)
3. \((\frac{5}{8})qk\)
4. \((\frac{8}{5})qk\)
Subtopic:  Electric Potential |
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The equivalent capacitance of the arrangement shown in the figure is:
           
1. \(30\) \(\mu\)F 2. \(15\) \(\mu\)F
3. \(25\) \(\mu\)F 4. \(20\) \(\mu\)F
Subtopic:  Combination of Capacitors |
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If a conducting sphere of radius R is charged. Then the electric field at a distance r(r > R) from the centre of the sphere would be, (V=potential on the surface of the sphere):
1. \(\frac{rV}{R^2}\) 2. \(\frac{R^2V}{r^3}\)
3. \(\frac{RV}{r^2}\) 4. \(\frac{V}{r}\)
Subtopic:  Electric Potential |
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Six charges \(+q,\) \(-q,\) \(+q,\) \(-q,\) \(+q\) and \(-q\) are fixed at the corners of a hexagon of side \(d\) as shown in the figure. The work done in bringing a charge \(q_0\) to the centre of the hexagon from infinity is:
(\(\varepsilon_0-\)permittivity of free space)
           
1. zero
2. \(\frac{-q^2}{4\pi\varepsilon_0d}\)
3. \(\frac{-q^2}{4\pi\varepsilon_0d}\Big(3-\frac{1}{\sqrt2}\Big)\)
4. \(\frac{-q^2}{4\pi\varepsilon_0d}\Big(6-\frac{1}{\sqrt2}\Big)\)
Subtopic:  Electric Potential Energy |
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The effective capacitances of two capacitors are 3 \(\mu F\) and 16 \(\mu F\), when they are connected in series and parallel respectively. The capacitance of two capacitors are:
1. 10 \(\mu F\), 6 \(\mu F\) 2. 8 \(\mu F\), 8 \(\mu F\)
3. 12 \(\mu F\), 4 \(\mu F\) 4. 1.2 \(\mu F\), 1.8 \(\mu F\)
Subtopic:  Capacitance |
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The distance between the two plates of a parallel plate capacitor is doubled and the area of each plate is halved. If \(C\) is its initial capacitance, its final capacitance is equal to:
1. \(2C\) 2. \(\frac{C}{2}\)
3. \(4C\) 4. \(\frac{C}{4}\)
Subtopic:  Capacitance |
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When a particle with charge \(+q\) is thrown with an initial velocity \(v\) towards another stationary change \(+Q,\) it is repelled back after reaching the nearest distance \(r\) from \(+Q.\) The closest distance that it can reach if it is thrown with initial velocity \(2v,\) is:

1. \(\frac{r}{4}\) 2. \(\frac{r}{2}\)
3. \(\frac{r}{16}\) 4. \(\frac{r}{8}\)
Subtopic:  Electric Potential Energy |
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Three capacitors, each of capacitance \(0.3~\mu \text{F}\) are connected in parallel. This combination is connected with another capacitor of capacitance \(0.1~\mu \text{F}\) in series. Then the equivalent capacitance of the combination is:

1. \(0.9~\mu\text{F}\) 2. \(0.09~\mu\text{F}\)
3. \(0.1~\mu\text{F}\) 4. \(0.01~\mu\text{F}\)
Subtopic:  Combination of Capacitors |
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A hollow metal sphere of radius \(R\) is given \(+Q\) charges to its outer surface. The electric potential at a distance \(\frac{R}{3}\) from the centre of the sphere will be:

1. \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{9R}\) 2. \(\frac{3}{4\pi \varepsilon_0}\frac{Q}{R}\)
3. \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{3R}\) 4. \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{R}\)
Subtopic:  Electric Potential |
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