TOPIC MAGNETIC EFFECT OF CURRENT & MAGNETIC FORCE OF ON CHARGE 20 SECTION - I : STRAIGHT OBJECTIVE TYPE 20.1 The negatively and uniformly charged nonconducting disc as shown in the figure is rotated clockwise with great angular speed. The direction of the magnetic field at point A in the plane of the disc is (A) into the page (B) out of the page (C) up the page (D) down the page 20.2 A particle is moving with velocity → ˆi 3ˆj and it produces an electric field at a point given by → E 2k It will produce magnetic field at that point equal to (all quantities are in S.. units) (A) 6ˆi 2ˆj c2 (B) 6ˆi 2ˆj c2 (C) zero (D) can not be determined from the given data 20.3 Two observers moving with different velocities see that a point charge produces same magnetic field at the same point A . Their relative velocity must be parallel to r , where r is the position vector of point A with respect to point charge. This statement is : (A) true (B) false (C) nothing can be said → (D) true only if the charge is moving perpendicular to the r 20.4 In the figure shown A B C D E F A was a square loop of side 𝑙 , but is folded in two equal parts so that half of it lies in x z plane and the other half lies in the y z plane. The origin ' O ' is centre of the frame also. The loop carries current ' i '. The magnetic field at the centre is: (A) 0 i ˆi ˆj (B) 0 i ˆi ˆj (C) ˆi ˆj (D) 4 𝑙 0 i ˆi ˆj 𝑙 20.5 If the magnetic field at 'P' in the given figure can be written as K tan 2 then K is : (A) (C) 0 4d 0 d (B) (D) 0 2d 20 d 20.6 The magnetic field at the origin due to the current flowing in the wire as shown in figure below is (A) 0 (ˆi kˆ) 8a (B) (C) 0 (ˆi kˆ) 2a 0 (ˆi kˆ) 8a (D) 0 (ˆi kˆ) 20.7 An infinitely long wire carrying current is along Y axis such that its one end is at point A (0, b) while the wire extends upto + . The magnitude of magnetic field strength at point (a, 0) is 0 b 0 b (A) 1 (B) 1 4a a2 b2 4a a2 b2 0 b (C) (D) None of these 4a a2 b2 20.8 Two infinitely long linear conductors are arranged perpendicular to each other and are in mutually perpendicular planes as shown in figure. If = 2A along the y-axis and = 3A along negative z-axis and AP = AB = 1 cm. The value of magnetic field strength B at P is - (A) (3 × 10–5 T) ˆj + (– 4 × 10–5 T) kˆ (B) (3 × 10–5 T) ˆj + (4 × 10–5 T) kˆ (C) (4 × 10–5 T) ˆj + (3 × 10–5 T) kˆ (D) (– 3 × 10–5 T) ˆj + (4 × 10–5 T) kˆ 20.9 A steady current is set up in a cubic network composed of wires of equal resistance and length d as shown in figure. What is the magnetic field at the centre of cube P due to the cubic network ? 0 2 0 3 (A) 4 d (B) 4 2 d (C) 0 (D) 0
TOPIC MAGNETIC EFFECT OF CURRENT & MAGNETIC FORCE OF ON CHARGE 20 SECTION - I : STRAIGHT OBJECTIVE TYPE 20.1 The negatively and uniformly charged nonconducting disc as shown in the figure is rotated clockwise with great angular speed. The direction of the magnetic field at point A in the plane of the disc is (A) into the page (B) out of the page (C) up the page (D) down the page 20.2 A particle is moving with velocity → ˆi 3ˆj and it produces an electric field at a point given by → E 2k It will produce magnetic field at that point equal to (all quantities are in S.. units) (A) 6ˆi 2ˆj c2 (B) 6ˆi 2ˆj c2 (C) zero (D) can not be determined from the given data 20.3 Two observers moving with different velocities see that a point charge produces same magnetic field at the same point A . Their relative velocity must be parallel to r , where r is the position vector of point A with respect to point charge. This statement is : (A) true (B) false (C) nothing can be said → (D) true only if the charge is moving perpendicular to the r 20.4 In the figure shown A B C D E F A was a square loop of side 𝑙 , but is folded in two equal parts so that half of it lies in x z plane and the other half lies in the y z plane. The origin ' O ' is centre of the frame also. The loop carries current ' i '. The magnetic field at the centre is: (A) 0 i ˆi ˆj (B) 0 i ˆi ˆj (C) ˆi ˆj (D) 4 𝑙 0 i ˆi ˆj 𝑙 20.5 If the magnetic field at 'P' in the given figure can be written as K tan 2 then K is : (A) (C) 0 4d 0 d (B) (D) 0 2d 20 d 20.6 The magnetic field at the origin due to the current flowing in the wire as shown in figure below is (A) 0 (ˆi kˆ) 8a (B) (C) 0 (ˆi kˆ) 2a 0 (ˆi kˆ) 8a (D) 0 (ˆi kˆ) 20.7 An infinitely long wire carrying current is along Y axis such that its one end is at point A (0, b) while the wire extends upto + . The magnitude of magnetic field strength at point (a, 0) is 0 b 0 b (A) 1 (B) 1 4a a2 b2 4a a2 b2 0 b (C) (D) None of these 4a a2 b2 20.8 Two infinitely long linear conductors are arranged perpendicular to each other and are in mutually perpendicular planes as shown in figure. If = 2A along the y-axis and = 3A along negative z-axis and AP = AB = 1 cm. The value of magnetic field strength B at P is - (A) (3 × 10–5 T) ˆj + (– 4 × 10–5 T) kˆ (B) (3 × 10–5 T) ˆj + (4 × 10–5 T) kˆ (C) (4 × 10–5 T) ˆj + (3 × 10–5 T) kˆ (D) (– 3 × 10–5 T) ˆj + (4 × 10–5 T) kˆ 20.9 A steady current is set up in a cubic network composed of wires of equal resistance and length d as shown in figure. What is the magnetic field at the centre of cube P due to the cubic network ? 0 2 0 3 (A) 4 d (B) 4 2 d (C) 0 (D) 0