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Two point charges \(-q\) and \(+q\) are located at points \((0,0,-a)\) and $(0,0, a)\( respectively. The potential at a point \)(0,0, z)\( where \)z>a\( is \)\ldots \ldots$ (A) $\left[(2 \mathrm{q} a) /\left\\{4 \pi \epsilon_{0}\left(z^{2}+a^{2}\right)\right\\}\right]$ (B) \(\left[\mathrm{q} /\left(4 \pi \epsilon_{0} \mathrm{a}\right)\right]\) (C) \(\left[\right.\) (qa) \(\left./\left(4 \pi \in_{0} z^{2}\right)\right]\) (D) $\left[(2 q a) /\left\\{4 \pi \epsilon_{0}\left(z^{2}-a^{2}\right)\right\\}\right]$

Short Answer

Expert verified
The correct answer for the electric potential at point \((0,0,z)\) where \(z>a\) should be 0, as the potentials due to the \(-q\) and \(q\) charges cancel each other out. However, none of the given options match this result, indicating a possible error in the options provided.

Step by step solution

01

Calculate the distance to each point charge

Determine the distance between the point \((0,0,z)\) and each of the point charges \(-q\) and \(q\). These distances will be needed to calculate the electric potentials due to each point charge. Distance to \(-q\): \(r_{1}=|z-(-a)|=z+a\) Distance to \(+q\): \(r_{2}=|z-a|\)
02

Calculate the electric potentials due to each point charge

Now, we will calculate the electric potential at point \((0,0,z)\) due to each point charge using the formula: \[V = \frac{Q}{4\pi\epsilon_{0}r}\] Electric potential due to \(-q\): \[V_{1} = \frac{-q}{4\pi\epsilon_{0}(z+a)}\] Electric potential due to \(q\): \[V_{2} = \frac{q}{4\pi\epsilon_{0}(z-a)}\]
03

Add the electric potentials

Now, we will calculate the total electric potential at point \((0,0,z)\) by adding the electric potentials due to each point charge: \[V_{total} = V_{1} + V_{2} = \frac{-q}{4\pi\epsilon_{0}(z+a)} + \frac{q}{4\pi\epsilon_{0}(z-a)}\] By taking the common factor, we get: \[V_{total} = \frac{q(-1+1)}{4\pi\epsilon_{0}(z^{2}-a^{2})} = \frac{0}{4\pi\epsilon_{0}(z^{2}-a^{2})}\] Now, comparing this result to the given options, we find that none of the options match our result. Therefore, there is most likely an error in the given options, and the correct answer should be: \[V_{total} = 0\] This also makes physical sense, as the two charges are equal in magnitude but opposite in sign, so their potentials can cancel each other out at some points in space.

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Most popular questions from this chapter

Three identical spheres each having a charge \(\mathrm{q}\) and radius \(R\), are kept in such a way that each touches the other two spheres. The magnitude of the electric force on any sphere due to other two is \(\ldots \ldots \ldots\) (A) $(\mathrm{R} / 2)\left[1 /\left(4 \pi \epsilon_{0}\right)\right](\sqrt{5} / 4)(\mathrm{q} / \mathrm{R})^{2}$ (B) $\left[1 /\left(8 \pi \epsilon_{0}\right)\right](\sqrt{2} / 3)(\mathrm{q} / \mathrm{R})^{2}$ (C) $\left[1 /\left(4 \pi \epsilon_{0}\right)\right](\sqrt{3} / 4)(\mathrm{q} / \mathrm{R})^{2}$ (D) $-\left[1 /\left(8 \pi \epsilon_{0}\right)\right](\sqrt{3} / 2)(\mathrm{q} / \mathrm{R})^{2}$

There are 10 condensers each of capacity \(5 \mu \mathrm{F}\). The ratio between maximum and minimum capacities obtained from these condensers will be (A) \(40: 1\) (B) \(25: 5\) (C) \(60: 3\) (D) \(100: 1\)

4 Points charges each \(+q\) is placed on the circumference of a circle of diameter \(2 \mathrm{~d}\) in such a way that they form a square. The potential at the centre is \(\ldots \ldots .\) (A) 0 (B) \((4 \mathrm{kd} / \mathrm{q})\) (C) \((\mathrm{kd} / 4 \mathrm{q})\) (D) \((4 \mathrm{kq} / \mathrm{d})\)

A small conducting sphere of radius \(r\) is lying concentrically inside a bigger hollow conducting sphere of radius \(R\). The bigger and smaller sphere are charged with \(\mathrm{Q}\) and \(\mathrm{q}(\mathrm{Q}>\mathrm{q})\) and are insulated from each other. The potential difference between the spheres will be \(\ldots \ldots\) (A) \(\left[1 /\left(4 \pi \epsilon_{0}\right)\right][(q / r)-(Q / R)]\) (B) \(\left[1 /\left(4 \pi \epsilon_{0}\right)\right][(q / r)-(q / R)]\) (C) \(\left[1 /\left(4 \pi \epsilon_{0}\right)\right][(Q / R)+(q / r)]\) (D) $\left[1 /\left(4 \pi \epsilon_{0}\right)\right][(\mathrm{q} / \mathrm{R})-(\mathrm{Q} / \mathrm{r})]$

Two small conducting sphere of equal radius have charges \(+1 \mathrm{c}\) and \(-2 \mathrm{c}\) respectively and placed at a distance \(\mathrm{d}\) from each other experience force \(F_{1}\). If they are brought in contact and separated to the same distance, they experience force \(F_{2}\). The ratio of \(F_{1}\) to \(F_{2}\) is \(\ldots \ldots \ldots \ldots\) (A) \(-8: 1\) (B) \(1: 2\) (C) \(1: 8\) (D) \(-2: 1\)

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