The Experiments of Faraday and Henry
PHXII06:ELECTROMAGNETIC INDUCTION

358688 In electromagnetic induction, the induced charge in a coil is independent of

1 Time
2 Change in the flux
3 Resistance in the circuit
4 None of the above
PHXII06:ELECTROMAGNETIC INDUCTION

358689 If a coil of 40 turns and area \(4.0\;\,c{m^2}\) is suddenly removed from a magnetic field, it is observed that a charge of \(2.0 \times {10^{ - 4}}\,C\) flows into the coil. If the resistance of the coil is \(80 \Omega\), the magnetic flux density in \(Wb/{m^2}\) is:

1 0.5
2 1.0
3 1.5
4 2.0
PHXII06:ELECTROMAGNETIC INDUCTION

358690 A long solenoid of diameter \(0.1\;\,m\) has \(2 \times 10^{4}\) turns per meter. At the centre of the solenoid, a coil of 100 turns and radius \(0.01\,\;m\) is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to \(0\;A\) from \(4\;A\) in \(0.05\;s\). If the resistance of the coil is \(10 \pi^{2} \Omega\). The total charge flowing through the coil during this time is :-

1 \(16 \mu \mathrm{C}\)
2 \(32 \mu \mathrm{C}\)
3 \(16 \pi \mu \mathrm{C}\)
4 \(32 \pi \mu \mathrm{C}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358691 A thin circular ring of area \(A\) is perpendicular to uniform magnetic field of induction \(B\). A small cut is made in the ring and a galvanometer is connected across the ends such that the total resistance of the circuit is \(R\). When the ring is suddenly squeezed to zero area, the charge flowing through the galvanometer is

1 \(\dfrac{B R}{A}\)
2 \(\dfrac{A B}{R}\)
3 \(A B R\)
4 \(\dfrac{B^{2} A}{R^{2}}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358688 In electromagnetic induction, the induced charge in a coil is independent of

1 Time
2 Change in the flux
3 Resistance in the circuit
4 None of the above
PHXII06:ELECTROMAGNETIC INDUCTION

358689 If a coil of 40 turns and area \(4.0\;\,c{m^2}\) is suddenly removed from a magnetic field, it is observed that a charge of \(2.0 \times {10^{ - 4}}\,C\) flows into the coil. If the resistance of the coil is \(80 \Omega\), the magnetic flux density in \(Wb/{m^2}\) is:

1 0.5
2 1.0
3 1.5
4 2.0
PHXII06:ELECTROMAGNETIC INDUCTION

358690 A long solenoid of diameter \(0.1\;\,m\) has \(2 \times 10^{4}\) turns per meter. At the centre of the solenoid, a coil of 100 turns and radius \(0.01\,\;m\) is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to \(0\;A\) from \(4\;A\) in \(0.05\;s\). If the resistance of the coil is \(10 \pi^{2} \Omega\). The total charge flowing through the coil during this time is :-

1 \(16 \mu \mathrm{C}\)
2 \(32 \mu \mathrm{C}\)
3 \(16 \pi \mu \mathrm{C}\)
4 \(32 \pi \mu \mathrm{C}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358691 A thin circular ring of area \(A\) is perpendicular to uniform magnetic field of induction \(B\). A small cut is made in the ring and a galvanometer is connected across the ends such that the total resistance of the circuit is \(R\). When the ring is suddenly squeezed to zero area, the charge flowing through the galvanometer is

1 \(\dfrac{B R}{A}\)
2 \(\dfrac{A B}{R}\)
3 \(A B R\)
4 \(\dfrac{B^{2} A}{R^{2}}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358688 In electromagnetic induction, the induced charge in a coil is independent of

1 Time
2 Change in the flux
3 Resistance in the circuit
4 None of the above
PHXII06:ELECTROMAGNETIC INDUCTION

358689 If a coil of 40 turns and area \(4.0\;\,c{m^2}\) is suddenly removed from a magnetic field, it is observed that a charge of \(2.0 \times {10^{ - 4}}\,C\) flows into the coil. If the resistance of the coil is \(80 \Omega\), the magnetic flux density in \(Wb/{m^2}\) is:

1 0.5
2 1.0
3 1.5
4 2.0
PHXII06:ELECTROMAGNETIC INDUCTION

358690 A long solenoid of diameter \(0.1\;\,m\) has \(2 \times 10^{4}\) turns per meter. At the centre of the solenoid, a coil of 100 turns and radius \(0.01\,\;m\) is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to \(0\;A\) from \(4\;A\) in \(0.05\;s\). If the resistance of the coil is \(10 \pi^{2} \Omega\). The total charge flowing through the coil during this time is :-

1 \(16 \mu \mathrm{C}\)
2 \(32 \mu \mathrm{C}\)
3 \(16 \pi \mu \mathrm{C}\)
4 \(32 \pi \mu \mathrm{C}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358691 A thin circular ring of area \(A\) is perpendicular to uniform magnetic field of induction \(B\). A small cut is made in the ring and a galvanometer is connected across the ends such that the total resistance of the circuit is \(R\). When the ring is suddenly squeezed to zero area, the charge flowing through the galvanometer is

1 \(\dfrac{B R}{A}\)
2 \(\dfrac{A B}{R}\)
3 \(A B R\)
4 \(\dfrac{B^{2} A}{R^{2}}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358688 In electromagnetic induction, the induced charge in a coil is independent of

1 Time
2 Change in the flux
3 Resistance in the circuit
4 None of the above
PHXII06:ELECTROMAGNETIC INDUCTION

358689 If a coil of 40 turns and area \(4.0\;\,c{m^2}\) is suddenly removed from a magnetic field, it is observed that a charge of \(2.0 \times {10^{ - 4}}\,C\) flows into the coil. If the resistance of the coil is \(80 \Omega\), the magnetic flux density in \(Wb/{m^2}\) is:

1 0.5
2 1.0
3 1.5
4 2.0
PHXII06:ELECTROMAGNETIC INDUCTION

358690 A long solenoid of diameter \(0.1\;\,m\) has \(2 \times 10^{4}\) turns per meter. At the centre of the solenoid, a coil of 100 turns and radius \(0.01\,\;m\) is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to \(0\;A\) from \(4\;A\) in \(0.05\;s\). If the resistance of the coil is \(10 \pi^{2} \Omega\). The total charge flowing through the coil during this time is :-

1 \(16 \mu \mathrm{C}\)
2 \(32 \mu \mathrm{C}\)
3 \(16 \pi \mu \mathrm{C}\)
4 \(32 \pi \mu \mathrm{C}\)
PHXII06:ELECTROMAGNETIC INDUCTION

358691 A thin circular ring of area \(A\) is perpendicular to uniform magnetic field of induction \(B\). A small cut is made in the ring and a galvanometer is connected across the ends such that the total resistance of the circuit is \(R\). When the ring is suddenly squeezed to zero area, the charge flowing through the galvanometer is

1 \(\dfrac{B R}{A}\)
2 \(\dfrac{A B}{R}\)
3 \(A B R\)
4 \(\dfrac{B^{2} A}{R^{2}}\)