Electromagnetic Induction

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Electromagnetic Induction by Mind Map: Electromagnetic Induction

1. A = area of surface

2. The induced emf, E, in any closed circuit is equal to the time rate of change of the magnetic flux through the circuit

3. Faraday's Law

3.1. E <>< d/dt x (Nϕ)

3.2. Middle Finger - Induced Current Direction

3.2.1. Father

3.2.2. Child

4. Unit: Wb (Weber)

5. Fleming's Right Hand Rule

5.1. Thumb - Force Direction

5.2. B = magnetic flux density

6. induced emf as B parallel plane of disc and axis of rotation

7. .

8. .

9. Index - Magnetic Field Direction

10. θ = angle between the magnetic field and the surface S

11. Units of E: V (Volts of induced current)

12. EMF induced in Moving Straight Conductor

12.1. E = Blv

12.1.1. v = velocity

12.2. E = 0, when l or v is parallel to B

13. Use of search coil to measure B

14. .

14.1. where f = 1 / T

14.1.1. T = Period of revolution

14.2. AC Generator

14.2.1. Φ = NBAcosθ

14.3. .

15. BUT, θ = ωt

15.1. Hence, Φ = NBAcos ωt

16. l = length of conductor

17. Applications of EMI

17.1. Use of search coil to measure flux density

17.2. Disc Generator

17.2.1. E = Bπr²f

17.3. Eddy Currents

17.3.1. Magnetic Effect

17.3.1.1. can be reduced by creating slots in the plate

17.3.1.1.1. Eddy currents cannot pass through air gaps

17.3.1.2. Follow Lenz Law

17.3.1.2.1. oppose the motion producing them

17.3.2. Heating Effect

17.3.2.1. coil carrying high frequency ac, causes rapidly changing magnetic flux to induce large eddy currents

18. Currents that are caused in metals moving in a magnetic field

18.1. can be +ve or -ve

19. Q = NBA / R

19.1. R = total resistance of circuit

20. Magnetic flux ϕ

21. ∆Q = ∆Φ / R

22. Lenz's Law

22.1. E = - dϕ / dt

22.1.1. E = - N d(BAcosθ) / dt

22.1.2. Unit: V (Volts)

22.2. If this were not the case, magnet's velocity and KE would be increased indefinitely, but there is no source for the energy, so COE is violated

22.3. derived from Conservation of Energy

23. Note: If l or v is not perpendicular to the field lines

23.1. Component perpendicular to the field should be used

24. N pole induced in top of solenoid when magnet's North is moved towards solenoid to oppose direction of magnet

24.1. Use Right hand grip rule to determine direction of current

25. .

25.1. copper disc rotates at frequency f between poles of magnet

26. Mother

27. Direction of induced emf is such that it tends to oppose the flux-change causing it, and does oppose it if induced current flows

28. Φ = Nϕ

29. N = number of turns in coil

30. Magnetic flux linkage Φ

30.1. Total flux through the coil

30.2. Unit: Wb (Weber)

30.3. Φ = NBAcosθ

31. ;.

31.1. Product of the magnetic flux density & the area normal to the field through which the field is passing

32. Φ = BAcosθ