Chapter 13: Problem 16
The ratio of the forces between two small spheres with same charges when they are in air to when they are in a medium of dielectric constant \(K\) is (A) \(1: K\) (B) \(K: 1\) (C) \(1: K^{2}\) (D) \(K^{2}: 1\)
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Chapter 13: Problem 16
The ratio of the forces between two small spheres with same charges when they are in air to when they are in a medium of dielectric constant \(K\) is (A) \(1: K\) (B) \(K: 1\) (C) \(1: K^{2}\) (D) \(K^{2}: 1\)
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Two point charges \(+8 q\) and \(-2 q\) are located at \(x=0\) and \(x=L\), respectively. The location of a point on the \(x\)-axis at which the net electric field due to these two point charges is zero (A) \(2 L\) (B) \(\frac{L}{4}\) (C) \(8 L\) (D) \(4 L\)
A long string with a charge of \(\lambda\) per unit length passes through an imaginary cube of edge \(a\). The maximum flux of the electric field through the cube will be (A) \(\lambda a / \varepsilon_{0}\) (B) \(\frac{\sqrt{2} \lambda a}{\varepsilon_{0}}\) (C) \(\frac{6 \lambda a^{2}}{\varepsilon_{0}}\) (D) \(\frac{\sqrt{3} \lambda a}{\varepsilon_{0}}\)
Two spheres of radii \(r\) and \(R\) carry charges \(q\) and \(Q\), respectively. When they are connected by a wire, there will be no loss of energy of the system if (A) \(q r=Q R\) (B) \(q R=Q r\) (C) \(q r^{2}=Q R^{2}\) (D) \(q R^{2}=O r^{2}\)
Two equal positive charges \(+q\) each are fixed a certain distance apart. A third equal positive charge \(+q\) is placed exactly midway between them. Then the third charge will (A) move at an angle of \(45^{\circ}\) to the line joining the two charges. (B) move at an angle of \(90^{\circ}\) to the line joining the two charges. (C) move along the line joining the two charges. (D) stay at rest.
A charged particle \(q\) is shot towards another charged particle \(Q\) which is fixed, with a speed \(v\). It approaches \(Q\) up to a closest distance \(\mathrm{r}\) and then returns. If \(q\) was given a speed \(2 v\), the closest distance of approach would be (A) \(r\) (B) \(2 r\) (C) \(r / 2\) (D) \(r / 4\)
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