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ELECTROMAGNETIC INDUCTION
Presented by-
ACHUYT BHARALEE
Roll No- PHP22108
Dept of Physics
Tezpur University
EMF, Terminal Voltage & Internal Resistance:
οƒ˜ More bulb in parallel it will more dimmer.
οƒ˜ More current drawn leads to voltage drop!
οƒ˜ For understanding this we have to know EMF.
οƒ˜ EMF= Electromotive Force; It’s an energy.
οƒ˜ EMF is the maximum P.D between two electrodes when no
current is drawn from a cell or it is the amount of energy
deliver per unit electric charge by a power source.
οƒ˜ Charges moves through the battery get resistance which called
Internal Resistance.
οƒ˜ Due to Internal resistance heat is generated.
οƒ˜ The P.D across the load when the ckt is closed.
𝑽𝑻 = 𝒆 βˆ’ 𝑰𝒓
Faraday’s Law:
οƒ˜ In 1831 M. Faraday report some experiments.
1. Expt: Move a loop of wire through a non uniform magnetic field.
2. Expt: Move a magnet but this time hold the loop still.
3. Expt: Both the loop and magnet is at rest but the magnetic field intensity is change
with time.
οƒ˜ From all the experiments we get a same result, that there is current is flowing through
the wire with changing magnetic field.
οƒ˜ i.e.; there is create a electric field whenever there change the magnetic flux.
οƒ˜ So a current is flowing.
οƒ˜ Due to the electric field there create a accumulation of charges.
οƒ˜ So at this point we actually get a EMF; called Motional EMF.
οƒ˜ Hence current is flowing.
Direction of the current!
οƒ˜ We always see that the current is flowing in such a direction that
the direction of magnetic field created for the current is always
opposite to the parental magnetic field.
οƒ˜ Lenz’s law states that an induced electric current flows in a
direction such that the current opposes the change that induced it.
οƒ˜ Lenz’s law based on conservation of energy.
Mathematically- πœ€ = 𝐸. 𝑑𝑙 = βˆ’
𝑑
𝑑𝑑
𝐡. 𝑑𝑆 = βˆ’
π‘‘πœ™
𝑑𝑑
𝜡 Γ— 𝑬 =
𝝏𝑩
𝝏𝒕
Self Induction:
οƒ˜ A current caring coil can produce a magnetic field around it.
οƒ˜ By Faraday’s law changing magnetic flux can create an induce EMF.
οƒ˜ But by Lenz’s law induce EMF will oppose the change of current.
οƒ˜ The phenomenon of production of opposing EMF in a coil when current through the
coil changes is called Self Induction.
πœ™ ∝ 𝐼
π‘πœ™ = 𝐿𝐼
οƒ˜Where L is the coefficient of self induction.
οƒ˜If changing current through the coil of N
turns produced self induce emf then it will be
πœ€ = βˆ’π‘
π‘‘πœ™
𝑑𝑑
πœ– = βˆ’πΏ
𝑑𝐼
𝑑𝑑
Mutual Inductance:
οƒ˜For changing current in coil 1 there will be changing magnetic flux though the coil 2.
οƒ˜For changing magnetic flux there will induce an emf in coil 2.
οƒ˜So there will be current flowing in such direction that the magnetic field produce by this
current oppose the parental magnetic field.
οƒ˜This property of two neighbouring coils that any change of current in flowing in the
other developing mutually induced emf called as Mutual Induction.
πœ€π‘€ = βˆ’π‘2
π‘‘πœ™2
𝑑𝑑
πœ€π‘€ = βˆ’π‘€
𝑑𝐼1
𝑑𝑑
𝑁2πœ™2 ∝ 𝐼1
𝑁2πœ™2 = 𝑀𝐼1
M is called coefficient of mutual inductance.
οƒ˜ If a changing current in coil A produces mutually induced emf in coil B then -
THANK YOU

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Electromagnetic Induction .pptx

  • 1. ELECTROMAGNETIC INDUCTION Presented by- ACHUYT BHARALEE Roll No- PHP22108 Dept of Physics Tezpur University
  • 2. EMF, Terminal Voltage & Internal Resistance: οƒ˜ More bulb in parallel it will more dimmer. οƒ˜ More current drawn leads to voltage drop! οƒ˜ For understanding this we have to know EMF. οƒ˜ EMF= Electromotive Force; It’s an energy. οƒ˜ EMF is the maximum P.D between two electrodes when no current is drawn from a cell or it is the amount of energy deliver per unit electric charge by a power source. οƒ˜ Charges moves through the battery get resistance which called Internal Resistance. οƒ˜ Due to Internal resistance heat is generated. οƒ˜ The P.D across the load when the ckt is closed. 𝑽𝑻 = 𝒆 βˆ’ 𝑰𝒓
  • 3. Faraday’s Law: οƒ˜ In 1831 M. Faraday report some experiments. 1. Expt: Move a loop of wire through a non uniform magnetic field. 2. Expt: Move a magnet but this time hold the loop still. 3. Expt: Both the loop and magnet is at rest but the magnetic field intensity is change with time. οƒ˜ From all the experiments we get a same result, that there is current is flowing through the wire with changing magnetic field. οƒ˜ i.e.; there is create a electric field whenever there change the magnetic flux. οƒ˜ So a current is flowing.
  • 4. οƒ˜ Due to the electric field there create a accumulation of charges. οƒ˜ So at this point we actually get a EMF; called Motional EMF. οƒ˜ Hence current is flowing. Direction of the current! οƒ˜ We always see that the current is flowing in such a direction that the direction of magnetic field created for the current is always opposite to the parental magnetic field. οƒ˜ Lenz’s law states that an induced electric current flows in a direction such that the current opposes the change that induced it. οƒ˜ Lenz’s law based on conservation of energy. Mathematically- πœ€ = 𝐸. 𝑑𝑙 = βˆ’ 𝑑 𝑑𝑑 𝐡. 𝑑𝑆 = βˆ’ π‘‘πœ™ 𝑑𝑑 𝜡 Γ— 𝑬 = 𝝏𝑩 𝝏𝒕
  • 5. Self Induction: οƒ˜ A current caring coil can produce a magnetic field around it. οƒ˜ By Faraday’s law changing magnetic flux can create an induce EMF. οƒ˜ But by Lenz’s law induce EMF will oppose the change of current. οƒ˜ The phenomenon of production of opposing EMF in a coil when current through the coil changes is called Self Induction.
  • 6. πœ™ ∝ 𝐼 π‘πœ™ = 𝐿𝐼 οƒ˜Where L is the coefficient of self induction. οƒ˜If changing current through the coil of N turns produced self induce emf then it will be πœ€ = βˆ’π‘ π‘‘πœ™ 𝑑𝑑 πœ– = βˆ’πΏ 𝑑𝐼 𝑑𝑑
  • 7. Mutual Inductance: οƒ˜For changing current in coil 1 there will be changing magnetic flux though the coil 2. οƒ˜For changing magnetic flux there will induce an emf in coil 2. οƒ˜So there will be current flowing in such direction that the magnetic field produce by this current oppose the parental magnetic field. οƒ˜This property of two neighbouring coils that any change of current in flowing in the other developing mutually induced emf called as Mutual Induction.
  • 8. πœ€π‘€ = βˆ’π‘2 π‘‘πœ™2 𝑑𝑑 πœ€π‘€ = βˆ’π‘€ 𝑑𝐼1 𝑑𝑑 𝑁2πœ™2 ∝ 𝐼1 𝑁2πœ™2 = 𝑀𝐼1 M is called coefficient of mutual inductance. οƒ˜ If a changing current in coil A produces mutually induced emf in coil B then -