An electron having charge \(e\) and mass \(m\) is moving in a uniform electric field \(E.\) Its acceleration will be:
1. \(\dfrac{e^2}{m}\)
2. \(\dfrac{E^2e}{m}\)
3. \(\dfrac{eE}{m}\)
4. \(\dfrac{mE}{e}\)

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\(ABC\) is an equilateral triangle. Charges \(+q\) are placed at each corner. The electric intensity at \(O\) will be:
| 1. | \(\dfrac{1}{4\pi\epsilon _0}\dfrac{q}{r^{2}}\) | 2. | \(\dfrac{1}{4\pi\epsilon _0}\dfrac{q}{r^{}}\) |
| 3. | zero | 4. | \(\dfrac{1}{4\pi\epsilon _0}\dfrac{3q}{r^{2}}\) |

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| 1. | \(\frac{Q}{4\pi \varepsilon_0R^2}\) | 2. | \(\frac{Q}{4\pi \varepsilon_0R}\) |
| 3. | zero | 4. | \(\frac{Q}{2\pi \varepsilon_0R^2}\) |
| 1. | \({E}_{1}\;{=}\;\dfrac{\mathit{\sigma}}{{\mathit{\epsilon}}_{0}}{;}\;{E}_{2}\;{=}\;{0}{;}\;{E}_{3}\;{=}\;\dfrac{\mathit{\sigma}}{{\mathit{\epsilon}}_{0}}~\) |
| 2. | \({E}_{1}\;{=}\;{E}_{2}\;{=}\;{E}_{3}\;{=}\;{0} \) |
| 3. | \({E}_{1}\;{=}\;{0}{;}\;{E}_{2}\;{=}\;\dfrac{\mathit{\sigma}}{2{\mathit{\epsilon}}_{0}}{;}\;{E}_{3}\;{=}\;\dfrac{\mathit{\sigma}}{{\mathit{\epsilon}}_{0}}~~\) |
| 4. | \({E}_{1}\;{=}\;\dfrac{\mathit{\sigma}}{{\mathit{\epsilon}}_{0}}{;}\;{E}_{2}\;{=}\;{0}{;}\;{E}_{3}\;{=}\;\dfrac{\mathit{\sigma}}{2{\mathit{\epsilon}}_{0}}\) |
A metallic solid sphere is placed in a uniform electric field. The lines of force follow the path(s) shown in the figure as:

1. \(1\)
2. \(2\)
3. \(3\)
4. \(4\)

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A cube of side a has a charge \(q\) at each of its vertices. The net electric field intensity at its centre is:
(\(r\) is the distance between a corner and the centre, and \(k=1/4\pi \varepsilon_0\) )
1. zero
2. \(kq/r^2\)
3. \(12kq/r^2\)
4. \(6kq/r^2\)

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