03. Inductance (Self and Mutual Induction)
Electro Magnetic Induction

154885 An ideal choke draws a current of $8 \mathrm{~A}$ when connected to an AC supply of $100 \mathrm{~V}, 50 \mathrm{~Hz}$. A pure resistor draws a current of $10 \mathrm{~A}$ when connected to the same source. The ideal choke and the resistor are connected in series and then connected to the AC source of $150 \mathrm{~V}, 40$ Hz. The current in the circuit becomes:

1 $\frac{15}{\sqrt{2}} \mathrm{~A}$
2 $8 \mathrm{~A}$
3 $18 \mathrm{~A}$
4 $10 \mathrm{~A}$
Electro Magnetic Induction

154886 When the current changes from $+2 \mathrm{~A}$ to $-2 \mathrm{~A}$ in 0.05 seconds, an emf of $8 \mathrm{~V}$ is induced in a coil. The coefficient of self inductance of the coil is

1 $0.2 \mathrm{H}$
2 $0.4 \mathrm{H}$
3 $0.8 \mathrm{H}$
4 $0.1 \mathrm{H}$
Electro Magnetic Induction

154887 If a current of $5 \mathrm{~A}$ in a coil of self inductance 2 $\mathrm{mH}$ is cut off in time $0.1 \mathrm{~s}$, the induced emf in the coil is

1 $0.1 \mathrm{~V}$
2 $0.01 \mathrm{~V}$
3 $0.2 \mathrm{~V}$
4 $0.02 \mathrm{~V}$
Electro Magnetic Induction

154888 A uniformly wound coil of self inductance $1.2 \times$ $10^{-4} \mathrm{H}$ and resistance $3 \Omega$ is broken up into two identical coils. These coils are then connected parallel across a $6 \mathrm{~V}$ battery of negligible resistance. The time constant for the current in the circuit is (neglect mutual inductance)

1 $0.4 \times 10^{-4} \mathrm{~s}$
2 $0.2 \times 10^{-4} \mathrm{~s}$
3 $0.5 \times 10^{-4} \mathrm{~s}$
4 $0.1 \times 10^{-4} \mathrm{~s}$
Electro Magnetic Induction

154890 A condenser of capacity $20 \mu \mathrm{F}$ is first charged and then discharged through a $10 \mathrm{mH}$ inductance. Neglecting the resistance of the coil, the frequency of the resulting vibrations will be

1 356 cycles $/ \mathrm{hr}$
2 356 cycles/sec
3 $356 \times 10^{3}$ cycles $/ \mathrm{sec}$
4 3.56 cycles $/ \mathrm{sec}$
Electro Magnetic Induction

154885 An ideal choke draws a current of $8 \mathrm{~A}$ when connected to an AC supply of $100 \mathrm{~V}, 50 \mathrm{~Hz}$. A pure resistor draws a current of $10 \mathrm{~A}$ when connected to the same source. The ideal choke and the resistor are connected in series and then connected to the AC source of $150 \mathrm{~V}, 40$ Hz. The current in the circuit becomes:

1 $\frac{15}{\sqrt{2}} \mathrm{~A}$
2 $8 \mathrm{~A}$
3 $18 \mathrm{~A}$
4 $10 \mathrm{~A}$
Electro Magnetic Induction

154886 When the current changes from $+2 \mathrm{~A}$ to $-2 \mathrm{~A}$ in 0.05 seconds, an emf of $8 \mathrm{~V}$ is induced in a coil. The coefficient of self inductance of the coil is

1 $0.2 \mathrm{H}$
2 $0.4 \mathrm{H}$
3 $0.8 \mathrm{H}$
4 $0.1 \mathrm{H}$
Electro Magnetic Induction

154887 If a current of $5 \mathrm{~A}$ in a coil of self inductance 2 $\mathrm{mH}$ is cut off in time $0.1 \mathrm{~s}$, the induced emf in the coil is

1 $0.1 \mathrm{~V}$
2 $0.01 \mathrm{~V}$
3 $0.2 \mathrm{~V}$
4 $0.02 \mathrm{~V}$
Electro Magnetic Induction

154888 A uniformly wound coil of self inductance $1.2 \times$ $10^{-4} \mathrm{H}$ and resistance $3 \Omega$ is broken up into two identical coils. These coils are then connected parallel across a $6 \mathrm{~V}$ battery of negligible resistance. The time constant for the current in the circuit is (neglect mutual inductance)

1 $0.4 \times 10^{-4} \mathrm{~s}$
2 $0.2 \times 10^{-4} \mathrm{~s}$
3 $0.5 \times 10^{-4} \mathrm{~s}$
4 $0.1 \times 10^{-4} \mathrm{~s}$
Electro Magnetic Induction

154890 A condenser of capacity $20 \mu \mathrm{F}$ is first charged and then discharged through a $10 \mathrm{mH}$ inductance. Neglecting the resistance of the coil, the frequency of the resulting vibrations will be

1 356 cycles $/ \mathrm{hr}$
2 356 cycles/sec
3 $356 \times 10^{3}$ cycles $/ \mathrm{sec}$
4 3.56 cycles $/ \mathrm{sec}$
Electro Magnetic Induction

154885 An ideal choke draws a current of $8 \mathrm{~A}$ when connected to an AC supply of $100 \mathrm{~V}, 50 \mathrm{~Hz}$. A pure resistor draws a current of $10 \mathrm{~A}$ when connected to the same source. The ideal choke and the resistor are connected in series and then connected to the AC source of $150 \mathrm{~V}, 40$ Hz. The current in the circuit becomes:

1 $\frac{15}{\sqrt{2}} \mathrm{~A}$
2 $8 \mathrm{~A}$
3 $18 \mathrm{~A}$
4 $10 \mathrm{~A}$
Electro Magnetic Induction

154886 When the current changes from $+2 \mathrm{~A}$ to $-2 \mathrm{~A}$ in 0.05 seconds, an emf of $8 \mathrm{~V}$ is induced in a coil. The coefficient of self inductance of the coil is

1 $0.2 \mathrm{H}$
2 $0.4 \mathrm{H}$
3 $0.8 \mathrm{H}$
4 $0.1 \mathrm{H}$
Electro Magnetic Induction

154887 If a current of $5 \mathrm{~A}$ in a coil of self inductance 2 $\mathrm{mH}$ is cut off in time $0.1 \mathrm{~s}$, the induced emf in the coil is

1 $0.1 \mathrm{~V}$
2 $0.01 \mathrm{~V}$
3 $0.2 \mathrm{~V}$
4 $0.02 \mathrm{~V}$
Electro Magnetic Induction

154888 A uniformly wound coil of self inductance $1.2 \times$ $10^{-4} \mathrm{H}$ and resistance $3 \Omega$ is broken up into two identical coils. These coils are then connected parallel across a $6 \mathrm{~V}$ battery of negligible resistance. The time constant for the current in the circuit is (neglect mutual inductance)

1 $0.4 \times 10^{-4} \mathrm{~s}$
2 $0.2 \times 10^{-4} \mathrm{~s}$
3 $0.5 \times 10^{-4} \mathrm{~s}$
4 $0.1 \times 10^{-4} \mathrm{~s}$
Electro Magnetic Induction

154890 A condenser of capacity $20 \mu \mathrm{F}$ is first charged and then discharged through a $10 \mathrm{mH}$ inductance. Neglecting the resistance of the coil, the frequency of the resulting vibrations will be

1 356 cycles $/ \mathrm{hr}$
2 356 cycles/sec
3 $356 \times 10^{3}$ cycles $/ \mathrm{sec}$
4 3.56 cycles $/ \mathrm{sec}$
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Electro Magnetic Induction

154885 An ideal choke draws a current of $8 \mathrm{~A}$ when connected to an AC supply of $100 \mathrm{~V}, 50 \mathrm{~Hz}$. A pure resistor draws a current of $10 \mathrm{~A}$ when connected to the same source. The ideal choke and the resistor are connected in series and then connected to the AC source of $150 \mathrm{~V}, 40$ Hz. The current in the circuit becomes:

1 $\frac{15}{\sqrt{2}} \mathrm{~A}$
2 $8 \mathrm{~A}$
3 $18 \mathrm{~A}$
4 $10 \mathrm{~A}$
Electro Magnetic Induction

154886 When the current changes from $+2 \mathrm{~A}$ to $-2 \mathrm{~A}$ in 0.05 seconds, an emf of $8 \mathrm{~V}$ is induced in a coil. The coefficient of self inductance of the coil is

1 $0.2 \mathrm{H}$
2 $0.4 \mathrm{H}$
3 $0.8 \mathrm{H}$
4 $0.1 \mathrm{H}$
Electro Magnetic Induction

154887 If a current of $5 \mathrm{~A}$ in a coil of self inductance 2 $\mathrm{mH}$ is cut off in time $0.1 \mathrm{~s}$, the induced emf in the coil is

1 $0.1 \mathrm{~V}$
2 $0.01 \mathrm{~V}$
3 $0.2 \mathrm{~V}$
4 $0.02 \mathrm{~V}$
Electro Magnetic Induction

154888 A uniformly wound coil of self inductance $1.2 \times$ $10^{-4} \mathrm{H}$ and resistance $3 \Omega$ is broken up into two identical coils. These coils are then connected parallel across a $6 \mathrm{~V}$ battery of negligible resistance. The time constant for the current in the circuit is (neglect mutual inductance)

1 $0.4 \times 10^{-4} \mathrm{~s}$
2 $0.2 \times 10^{-4} \mathrm{~s}$
3 $0.5 \times 10^{-4} \mathrm{~s}$
4 $0.1 \times 10^{-4} \mathrm{~s}$
Electro Magnetic Induction

154890 A condenser of capacity $20 \mu \mathrm{F}$ is first charged and then discharged through a $10 \mathrm{mH}$ inductance. Neglecting the resistance of the coil, the frequency of the resulting vibrations will be

1 356 cycles $/ \mathrm{hr}$
2 356 cycles/sec
3 $356 \times 10^{3}$ cycles $/ \mathrm{sec}$
4 3.56 cycles $/ \mathrm{sec}$
Electro Magnetic Induction

154885 An ideal choke draws a current of $8 \mathrm{~A}$ when connected to an AC supply of $100 \mathrm{~V}, 50 \mathrm{~Hz}$. A pure resistor draws a current of $10 \mathrm{~A}$ when connected to the same source. The ideal choke and the resistor are connected in series and then connected to the AC source of $150 \mathrm{~V}, 40$ Hz. The current in the circuit becomes:

1 $\frac{15}{\sqrt{2}} \mathrm{~A}$
2 $8 \mathrm{~A}$
3 $18 \mathrm{~A}$
4 $10 \mathrm{~A}$
Electro Magnetic Induction

154886 When the current changes from $+2 \mathrm{~A}$ to $-2 \mathrm{~A}$ in 0.05 seconds, an emf of $8 \mathrm{~V}$ is induced in a coil. The coefficient of self inductance of the coil is

1 $0.2 \mathrm{H}$
2 $0.4 \mathrm{H}$
3 $0.8 \mathrm{H}$
4 $0.1 \mathrm{H}$
Electro Magnetic Induction

154887 If a current of $5 \mathrm{~A}$ in a coil of self inductance 2 $\mathrm{mH}$ is cut off in time $0.1 \mathrm{~s}$, the induced emf in the coil is

1 $0.1 \mathrm{~V}$
2 $0.01 \mathrm{~V}$
3 $0.2 \mathrm{~V}$
4 $0.02 \mathrm{~V}$
Electro Magnetic Induction

154888 A uniformly wound coil of self inductance $1.2 \times$ $10^{-4} \mathrm{H}$ and resistance $3 \Omega$ is broken up into two identical coils. These coils are then connected parallel across a $6 \mathrm{~V}$ battery of negligible resistance. The time constant for the current in the circuit is (neglect mutual inductance)

1 $0.4 \times 10^{-4} \mathrm{~s}$
2 $0.2 \times 10^{-4} \mathrm{~s}$
3 $0.5 \times 10^{-4} \mathrm{~s}$
4 $0.1 \times 10^{-4} \mathrm{~s}$
Electro Magnetic Induction

154890 A condenser of capacity $20 \mu \mathrm{F}$ is first charged and then discharged through a $10 \mathrm{mH}$ inductance. Neglecting the resistance of the coil, the frequency of the resulting vibrations will be

1 356 cycles $/ \mathrm{hr}$
2 356 cycles/sec
3 $356 \times 10^{3}$ cycles $/ \mathrm{sec}$
4 3.56 cycles $/ \mathrm{sec}$