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1 Magnetism Content of the presentation - Maxwell's general equations on magnetism - Hysteresis curve - Inductance - Magnetic circuit modelling - Eddy.

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Presentation on theme: "1 Magnetism Content of the presentation - Maxwell's general equations on magnetism - Hysteresis curve - Inductance - Magnetic circuit modelling - Eddy."— Presentation transcript:

1 1 Magnetism Content of the presentation - Maxwell's general equations on magnetism - Hysteresis curve - Inductance - Magnetic circuit modelling - Eddy currents and hysteresis losses - Force / torque / power 1990 - 1995 M.sc.EE Student at IET, Aalborg University. 1995 - 1999 Ph.D. Student at IET, Aalborg University. 1999 - 2002 Assistant Professor at IET, Aalborg University. 2002 - Associate Professor at IET, Aalborg University. Few words and mini CV of my self

2 2 Maxwell James Clerk Maxwell 1831 - 1879 Unified theory of the connection between electricity and magnetism

3 3 Maxwells equations in free space Not easy to understand in this form. Practical engineers tend to forget the definition of divergence, curl, surface and line integral

4 4 Ørsted H.C Ørsted 1777-1851 Ørsteds discovery was a deflection of a Compass needle when it is close to a current carrying conductor. But he was not able to describe the physics or mathematics behind the phenomena 1820 {f = Bxil / 90° : f=Bil}

5 5 Amperé André-Marie Ampére 1775 – 1836 Just one week after Ørsteds discovery Ampere showed that two current carrying wires attract or repulse each other, and was able to show that : Thus, for two parallel wires carrying a current of 1 A, and spaced apart by 1 m in vacuum, the force on each wire per unit length is exactly 2 × 10 -7 N/m. I2I2 I1I1 r l It was first in 1826 he published the circuit law in Maxwell’s equation

6 6 Faraday Michael Faraday 1791-1867 {e = Bxlv / 90° : e =Blv} Induction by movement ”generator” Induction by alternating current ”transformer” The Induction law 1821

7 7 Gauss Carl Friedrich Gauss 1777 – 1855 Basically the magnetic induction can’t escape. The equation says that we don’t have a monopole. There will always be a north and a south pole

8 8 Relations in Maxwell’s equations Simplified analogies and the relations in Maxwell’s equations

9 9 Permeability Return μ = μ r μ 0 Where μ r typically is 1000-100000 in magnetic cores

10 10 Analogies

11 11 Faraday’s law Faraday’s law (again)

12 12 Some of the first electrical machines Not useful because it makes AC Improved to a DC machine where Ampere proposed Pixii to use a mechanical commutator Alternator by Pixii 1832 Note it is made with electromagnets (Henry 1828)

13 13 Letz’s law Letz’s law (consequence of Maxwell’s equation)

14 14 Amperé’s law Ampere’s law (again)

15 15 Inductor example Example : Inductor

16 16 Inductor example

17 17 Inductor example No saturation and hysteresis

18 18 Magnetic circuit model Ohm’s law in magnetic circuits

19 19 Magnetic circuit model What about Kirchoff’s current law (KCL) Gauss law

20 20 Magnetic circuit model What about Kirchoff’s voltage law (KVL) Ampere law is similar to Kirchoff’s voltage law

21 21 Magnetic circuit model (Steel and air-gap)

22 22 Magnetic circuit model (Steel and air-gap)

23 23 Core losses Hysteresis losses

24 24 Hysteresis losses

25 25 Hysteresis losses Hysteresis curve at various H-fields

26 26 Hysteresis losses

27 27 Eddy current losses

28 28 Eddy current losses How do we reduce Eddy current losses LAMINATED SOLID

29 29 Eddy current losses

30 30 Eddy current losses in windings Can be a problem with thick wires - Low voltage machines - High speed machines

31 31 Force, torque and power Universal modeling of terminal characteristic of electro-magnetic devices based on energy balance

32 32 Force, torque and power

33 33 Force, torque and power

34 34 Force, torque and power

35 35 Force, torque and power

36 36 Force, torque and power

37 37 Force, torque and power

38 38 Force, torque and power

39 39 Force, torque and power

40 40 Force, torque and power

41 41 Simplified machines

42 42 Simplified machines

43 43 Electromagnetic gearing L gu larger than L g ≈ ∞ Δθ=90

44 44 Electromagnetic gearing Same winding but now enclosing two poles : L A is the same (if end winding is neglected the Resistance is also the same) Δθ=45 Torque doubling

45 45 Normal/radial forces Normal forces Ex. Changing the air gap from 0.3 mm to 0.15 mm Gives a doubling of inductance The Δx is very small i.e a large Force In electrical machines the normal forces versus the tangential force (torque) is typically a factor 10.


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