01. Amperes Law (∞, Length, Solenoid, Toroid)
Moving Charges & Magnetism

153410 The free space inside a current carrying toroid is filled with a material of susceptibility
2×102. The percentage increase in the value of magnetic field inside the toroid will be

1 2%
2 0.2%
3 0.1%
4 1%
Moving Charges & Magnetism

153411 A long solenoid is formed by winding 70 turns cm1. If 2.0 A current flows, then the magnetic field produced inside the solenoid is (μ0=4π×107)TmA1)

1 88×104 T
2 1232×104 T
3 352×104 T
4 176×104 T
Moving Charges & Magnetism

153413 A solenoid of 1200 turns is wound uniformly in a single layer on a glass tube 2 m long and 0.2 m in diameter. The magnetic intensity at the centre of the solenoid when a current of 2 A flows through it is,

1 2.4×103Am1
2 1.2×103Am1
3 1Am1
4 2.4×103Am1
Moving Charges & Magnetism

153414 The magnitude of magnetic induction at mid point O due to current arrangement as shown in Fig will be

1 0
2 μ0lπa
3 μ0l2πa
4 μ0l4πa
Moving Charges & Magnetism

153410 The free space inside a current carrying toroid is filled with a material of susceptibility
2×102. The percentage increase in the value of magnetic field inside the toroid will be

1 2%
2 0.2%
3 0.1%
4 1%
Moving Charges & Magnetism

153411 A long solenoid is formed by winding 70 turns cm1. If 2.0 A current flows, then the magnetic field produced inside the solenoid is (μ0=4π×107)TmA1)

1 88×104 T
2 1232×104 T
3 352×104 T
4 176×104 T
Moving Charges & Magnetism

153412 A long conducting wire having a current i flowing it is bent into a circular coil of N turns. Then it is bent into a circular coil of n turns. The magnetic field is calculated at the centre of coils in both the cases. The ratio of the magnetic field in first case to that of second case is :

1 n:N
2 N:n
3 N2:n2
4 n2:N2
Moving Charges & Magnetism

153413 A solenoid of 1200 turns is wound uniformly in a single layer on a glass tube 2 m long and 0.2 m in diameter. The magnetic intensity at the centre of the solenoid when a current of 2 A flows through it is,

1 2.4×103Am1
2 1.2×103Am1
3 1Am1
4 2.4×103Am1
Moving Charges & Magnetism

153414 The magnitude of magnetic induction at mid point O due to current arrangement as shown in Fig will be

1 0
2 μ0lπa
3 μ0l2πa
4 μ0l4πa
Moving Charges & Magnetism

153410 The free space inside a current carrying toroid is filled with a material of susceptibility
2×102. The percentage increase in the value of magnetic field inside the toroid will be

1 2%
2 0.2%
3 0.1%
4 1%
Moving Charges & Magnetism

153411 A long solenoid is formed by winding 70 turns cm1. If 2.0 A current flows, then the magnetic field produced inside the solenoid is (μ0=4π×107)TmA1)

1 88×104 T
2 1232×104 T
3 352×104 T
4 176×104 T
Moving Charges & Magnetism

153412 A long conducting wire having a current i flowing it is bent into a circular coil of N turns. Then it is bent into a circular coil of n turns. The magnetic field is calculated at the centre of coils in both the cases. The ratio of the magnetic field in first case to that of second case is :

1 n:N
2 N:n
3 N2:n2
4 n2:N2
Moving Charges & Magnetism

153413 A solenoid of 1200 turns is wound uniformly in a single layer on a glass tube 2 m long and 0.2 m in diameter. The magnetic intensity at the centre of the solenoid when a current of 2 A flows through it is,

1 2.4×103Am1
2 1.2×103Am1
3 1Am1
4 2.4×103Am1
Moving Charges & Magnetism

153414 The magnitude of magnetic induction at mid point O due to current arrangement as shown in Fig will be

1 0
2 μ0lπa
3 μ0l2πa
4 μ0l4πa
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Moving Charges & Magnetism

153410 The free space inside a current carrying toroid is filled with a material of susceptibility
2×102. The percentage increase in the value of magnetic field inside the toroid will be

1 2%
2 0.2%
3 0.1%
4 1%
Moving Charges & Magnetism

153411 A long solenoid is formed by winding 70 turns cm1. If 2.0 A current flows, then the magnetic field produced inside the solenoid is (μ0=4π×107)TmA1)

1 88×104 T
2 1232×104 T
3 352×104 T
4 176×104 T
Moving Charges & Magnetism

153412 A long conducting wire having a current i flowing it is bent into a circular coil of N turns. Then it is bent into a circular coil of n turns. The magnetic field is calculated at the centre of coils in both the cases. The ratio of the magnetic field in first case to that of second case is :

1 n:N
2 N:n
3 N2:n2
4 n2:N2
Moving Charges & Magnetism

153413 A solenoid of 1200 turns is wound uniformly in a single layer on a glass tube 2 m long and 0.2 m in diameter. The magnetic intensity at the centre of the solenoid when a current of 2 A flows through it is,

1 2.4×103Am1
2 1.2×103Am1
3 1Am1
4 2.4×103Am1
Moving Charges & Magnetism

153414 The magnitude of magnetic induction at mid point O due to current arrangement as shown in Fig will be

1 0
2 μ0lπa
3 μ0l2πa
4 μ0l4πa
Moving Charges & Magnetism

153410 The free space inside a current carrying toroid is filled with a material of susceptibility
2×102. The percentage increase in the value of magnetic field inside the toroid will be

1 2%
2 0.2%
3 0.1%
4 1%
Moving Charges & Magnetism

153411 A long solenoid is formed by winding 70 turns cm1. If 2.0 A current flows, then the magnetic field produced inside the solenoid is (μ0=4π×107)TmA1)

1 88×104 T
2 1232×104 T
3 352×104 T
4 176×104 T
Moving Charges & Magnetism

153412 A long conducting wire having a current i flowing it is bent into a circular coil of N turns. Then it is bent into a circular coil of n turns. The magnetic field is calculated at the centre of coils in both the cases. The ratio of the magnetic field in first case to that of second case is :

1 n:N
2 N:n
3 N2:n2
4 n2:N2
Moving Charges & Magnetism

153413 A solenoid of 1200 turns is wound uniformly in a single layer on a glass tube 2 m long and 0.2 m in diameter. The magnetic intensity at the centre of the solenoid when a current of 2 A flows through it is,

1 2.4×103Am1
2 1.2×103Am1
3 1Am1
4 2.4×103Am1
Moving Charges & Magnetism

153414 The magnitude of magnetic induction at mid point O due to current arrangement as shown in Fig will be

1 0
2 μ0lπa
3 μ0l2πa
4 μ0l4πa