1. | 9×10−3 J | 2. | 9×10−3 eV |
3. | 2 eV/m | 4. | zero |
Three charges Q, +q and +q are placed at the vertices of an equilateral triangle of side l as shown in the figure. If the net electrostatic energy of the system is zero, then Q is equal to:
1. | −q2 | 2. | −q |
3. | +q | 4. | zero |
A charge q1=5×10−8 C is kept at 3 cm from a charge q2=−2×10−8 C. The potential energy of the system relative to the potential energy at infinite separation is:
1. | 3×10−4 J | 2. | −3×10−4 J |
3. | 9×10−6 J | 4. | −9×10−6 J |
Two charges q1 and q2 are placed 30 cm apart, as shown in the figure. A third charge q3 is moved along the arc of a circle of radius 40 cm from C to D. The change in the potential energy of the system is q34πε0k, where k is:
1. | 8q2 | 2. | 8q1 |
3 | 6q2 | 4. | 6q1 |
An elementary particle of mass m and charge +e is projected with velocity v at a much more massive particle of charge Ze, where Z>0. What is the closest possible approach of the incident particle?
1. | Ze22πε0mv2 | 2. | Ze4πε0mv2 |
3. | Ze28πε0mv2 | 4. | Ze8πε0mv2 |
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 an initial velocity 2v, is:
1. | r4 | 2. | r2 |
3. | r16 | 4. | r8 |
Four equal charges Q are placed at the four corners of a square of each side a. Work done in removing a charge −Q from its centre to infinity is:
1. 0
2. √2Q24πε0a
3. √2Q2πε0a
4. Q22πε0a
A charge of 10 e.s.u. is placed at a distance of 2 cm from a charge of 40 e.s.u. and 4 cm from another charge of 20 e.s.u. The potential energy of the charge 10 e.s.u. is: (in ergs)
1. | 87.5 | 2. | 112.5 |
3. | 150 | 4. | 250 |
Figure shows a ball having a charge q fixed at a point A. Two identical balls having charges +q and –q and mass ‘m′ each are attached to the ends of a light rod of length 2a
1. | √2q3πε0ma3 | 2. | q√3πε0ma3 |
3. | q√6πε0ma3 | 4. | √2q4πε0ma3 |