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8 one ring to that of the other is (a) zero (b) q(Q1 Q2) ( 02 1) / 2 (4 R ) (c) 1 2 0q 2(Q Q ) / (4 R) (d) 1 2 0q(Q Q )( 2 1) / 2(4 R) Explanation: VB = 2 1 1 2 A KQ KQ KQ KQ , V R R2R 2R VA – VB = 1 2KQ KQ1 1 1 1 R R2 2 VA–VB = 1 2 K 1 1 (Q Q ) R 2 , where 0 1 K 4 W = q (VA – VB) (b) 10. A and B are two concentric spheres If A is given a charge Q while B is earthed as shown in figure, then (A) the charge densities of A and B are same B A + + + + + + + + + + + 9 (B) the field inside and outside A is zero (C) the field between A and B is not zero (D) the field inside and outside B is zero Explanation: C Since, B is grounded, therefore VB = 0 A BkQ kQ R R = 0 (R = radius of shell B) QB = QA Now take QA = Q B = 2 Q 4 R But A = 2 Q 4 r (A) is not correct Apply Gauss's theorem. Only (C) is correct. 10 11. Electric charges q, q and 2q are placed at the corners of an equilateral triangle ABC of side L. The magnitude of electric dipole moment of the system is (A) qL (B) 2qL (C) (3)qL (D) 4qL Explanation: C As shown the three charges are equivalent to two dipoles of magnitude q L. Equivalent dipole moment = 2 2(qL) (qL) 2(qL)(qL)cos60 = 3 qL q q -q -q qL qL 60 12. If charges q/2 and 2q are placed at the centre of face and at the corner of a cube, then the total flux through the cube will be (A) o q 2 (B) o q (C) o q 6 (D) o q 8 Explanation: A 11 Flux through the cube when q/2 is placed at the centre of face 1 0 0 q 2 q 2 4 Flux through the cube when 2q is placed at the corner of cube is 2 0 0 2q q 8 4 Now, total flux through the cube 1 2 0 q 2 13. A solid insulating sphere of radius R is given a charge Q. If at a point inside the sphere the potential is 1.5 times the potential at the surface, this point will be (A) at a distance of 2R/3 from the centre (B) at the centre (C) at a distance of 2R/3 from the surface (D) data insufficient Explanation: B 2 2 in 3 0 Q 3R r1 V 4 2R s 0 1 Q V 4 R 12 Given in s 3 V V 2 2 2 3 3 1 3R r 2 R 2R or r = 0 14. A charge +q is fixed at each of the points x = x0, x = 3x0, x = 5x0, . . ., on the x-axis and a charge q is fixed at each of the points x = 2x0, x = 4x0, x = 6x0, . . ., . Here, x0 is a positive quantity. Take the electric potential at a point due to charge Q at a distance r from it to be 0 Q 4 r . Then, the potential at origin due to the above system of charges is (A) 0 (B) (C) 0 0 q 8 x ln 2 (D) 0 0 q ln 2 4 x Explanation: D V = 0 0 0 0 0 q 1 1 1 1 4 x 2x 3x 4x = 0 0 0 0 q 1 1 1 q 1 ln(2) 4 x 2 3 4 4 x 13 16. Find the charge on an iron particle of mass 2.24 mg, if 0.02% of electrons are removed from it. (A) 0.01996 C (B) 0.01996 C (C) 0.02 C (D) 2.0 C Explanation: B As mass Atomic wt. = No. of atoms Avogadro No. No. of atoms = 24 1018 atoms = 24 1018 26 electrons. n = No. of electrons removed = 24 1018 26 0.01 100 = 1248 1014 electron Q = ne = (+ve charge) = 0.01996 C 17. Two small metallic spheres each of mass ‘m’ are suspended together with strings of length ‘’ and placed together. When a quantum of charge ‘q’ is transferred to each, the strings make an angle of 90 with each other. The value of ‘q’ is (A) 0mg (B) 02 mg (C) 04 mg (D) 08 mg Explanation: D 14 T cos 45 = FE = 2 2 2 0 Q 4 (2 ) cos 45 2 2 2 2 0 0 q q 16 (1/ 2) 8 T sin 45 = mg 1 = 2 0 2 mg8 q q = 08 mg . 45 45 FE FE mg mg cos 45 T T 18. Two connected charges of +q and q are at a fixed distance AB apart in a non-uniform electric field, whose lines of force are shown in the figure. The resultant effect on the two charges is (A) a torque in the plane of the paper and no resultant force. (B) a resultant force in the plane of the paper and no torque. A B -q +q (C) a torque normal to the plane of the paper and no resultant force. (D) a torque normal to the plane of the paper and a resultant force in the plane of the paper. Explanation: B