Chapter 13: Problem 58
Suppose the electrostatic potential at some points in space are given by \(V=\left(x^{2}-2 x\right)\). The electrostatic field strength at \(x=1\) is (A) Zero (B) \(-2\) (C) 2 (D) 4
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Chapter 13: Problem 58
Suppose the electrostatic potential at some points in space are given by \(V=\left(x^{2}-2 x\right)\). The electrostatic field strength at \(x=1\) is (A) Zero (B) \(-2\) (C) 2 (D) 4
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Two equal negative charges \(-q\) are fixed at points \((0, a)\) and \((0,-a)\) on the \(y\)-axis. A positive charge \(Q\) is released from rest at a point \((2 a, 0)\) on the \(x\)-axis. The charge \(Q\) will (A) execute SHM about the origin. (B) move to the origin and remain at rest there. (C) move to infinity. (D) execute oscillatory but not SHM.
If there are \(n\) capacitors in parallel connected to \(\mathrm{V}\) volt source, then total energy stored is equal to (A) \(\mathrm{CV}\) (B) \(\frac{1}{2} n \mathrm{CV}^{2}\) (C) \(\mathrm{CV}^{2}\) (D) \(\frac{1}{2 n} \mathrm{CV}^{2}\)
Assertion: When an uncharged capacitor of capacitance \(C\) is charged by a cell of emf \(V\), the energy stored by capacitor is \(\frac{1}{2} C V^{2}\), and energy supplied by battery is \(C V^{2}\). Reason: In charging an uncharged capacitor, energy is lost in the form of heat. (A) A (B) \(\mathrm{B}\) (C) \(\mathrm{C}\) (D) \(\mathrm{D}\)
The electric field intensity at a point at a distance \(2 \mathrm{~m}\) from a charge \(q\) is \(E\). The amount of work done in bringing a charge of 2 coulomb from infinity to this point will be (A) \(2 E \mathrm{~J}\) (B) \(4 E \mathrm{~J}\) (C) \(\frac{E}{2} \mathrm{~J}\) (D) \(\frac{E}{4} \mathrm{~J}\)
The electric potential \(V\) is given as a function of distance \(x\) (metre) by \(V=\left(5 x^{2}+10 x-9\right)\) v. Magnitude of electric field at \(x=1\) is (A) \(20 \mathrm{~V} / \mathrm{m}\) (B) \(6 \mathrm{~V} / \mathrm{m}\) (C) \(11 \mathrm{~V} / \mathrm{m}\) (D) \(-23 \mathrm{~V} / \mathrm{m}\)
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