Concept: Faraday’s Law of Electromagnetic Induction
Whenever the magnetic flux linked with a circuit changes, an emf is induced in the circuit. Mathematically,
\[
e = -\frac{d\Phi}{dt}
\]
For a coil of $N$ turns:
\[
e = -N \frac{d\Phi}{dt}
\]
where:
• $e$ = induced emf
• $N$ = number of turns
• $\Phi = BA \cos\theta$ = magnetic flux
---
Step 1: Understanding magnetic flux change
When a magnet is plunged into a coil:
• Magnetic field through the coil changes with time
• Hence flux $\Phi$ changes
• This induces emf according to Faraday’s law
Thus, emf depends on:
\[
e \propto \frac{d\Phi}{dt}
\]
---
Step 2: Expanding the expression for flux
Magnetic flux:
\[
\Phi = BA \cos\theta
\]
Thus:
\[
e = -N \frac{d(BA \cos\theta)}{dt}
\]
This shows emf depends on:
• Magnetic field strength ($B$)
• Area of coil ($A$)
• Orientation ($\theta$)
• Rate of change (motion of magnet)
• Number of turns ($N$)
---
Step 3: Analyze each option carefully
(A) Number of turns
\[
e = -N \frac{d\Phi}{dt}
\]
More turns → more flux linkage → larger emf
\[
\Rightarrow \text{Depends on } N \quad (\text{Important factor})
\]
---
(B) Medium of core
Core material affects magnetic permeability:
\[
B = \mu H
\]
Higher permeability → stronger magnetic field → higher flux
\[
\Rightarrow \text{Affects emf}
\]
---
(C) Insertion speed
\[
e \propto \frac{d\Phi}{dt}
\]
Faster insertion → faster flux change → higher emf
\[
\Rightarrow \text{Strong dependence}
\]
---
(D) Strength of magnet
Stronger magnet → larger magnetic field $B$ → larger flux
\[
\Rightarrow \text{Higher emf}
\]
---
(E) Resistance of coil
This is the key point.
From Faraday’s law:
\[
e = -N \frac{d\Phi}{dt}
\]
No resistance term appears.
Resistance only affects current:
\[
I = \frac{e}{R}
\]
Important distinction:
• EMF depends on flux change
• Current depends on resistance
Thus:
\[
\boxed{\text{EMF is independent of resistance}}
\]
---
Step 4: Physical Interpretation
• EMF is generated due to changing magnetic environment
• Resistance only determines how much current flows AFTER emf is produced
• Even with very large resistance, emf is still induced
---
Final Conclusion:
\[
\boxed{\text{The induced emf does not depend on resistance of the coil}}
\]