1. Lesson 4: Solving Magnetic Circuits with Electrical Analogies ET 332a Dc Motors, Generators and Energy Conversion Devices 1

2. 2 Learning Objectives After this presentation you will be able to:  Convert a magnetic structure to a electric circuit analogy  Solve a complex magnetic circuit using the mathematical relationships of magnetic circuits  Compute the inductance of a coil  Define Hysteresis power loss in magnetic circuits and determine power losses.

3. Magnetic-Electric Circuit Analogies 3 Sources = windings and current flowing into coils Core Reluctances = length, area and permeability of core carrying a given flux Air Gap Reluctances = length, area and permeability of free space (air) used to compute these quantities Known flux or Flux Density One of these quantities must be given to find the permeability of core sections. Remember, reluctance is non-linear and depends on the level of flux carried by a core section.

4. Magnetic Circuit Example 3 4 Converting the magnetic circuit to an electrical analogy The magnetic core at the left has the following core segment lengths L af = L cd = L bc =L ed = 1.0 m L ab =L fe = 0.8 m The air gap length is L ag = 0.5 cm Flux density in the air gap is B ag = 0.2T Coil turns: N =80 t Core cross sectional area: A = 0.04 m 2 Coil Resistance: R=2.05  Fringing negligible 1.) Find battery V to produce B ag 2.) Compute  r for each core leg 1.0 m 0.8 m Using magnetization curve (B-H) from text 0.5 cm B ag = 0.2 T

5. Example 3 5 Convert diagram to schematic diagram F tot R gap R be R bcde  gap  bcde  total R abfe Electrical analog

6. Example 3 Solution Method 6 Part 1: Find flux in air gap Determine H of air gap Determine H for center core Find MMF to drive flux in center core Find flux in right leg Find F tot Use Ohms law to find V

7. Example 3 Solution –Part 1 7 0.3 m 0.69 m H ag Remember, permeability is constant in air gap

8. 8 Example 3 Solution –Part 1 Solution continued H=0.47 Oersteds

9. 9 Example 3 Solution –Part 1 Solution continued H ag = 159,155 A-t/m H 0.3 =H 0.69 = 37.4 A-t/m F 0.3 F 0.69 F ag F gap

10. 10 Example 3 Solution –Part 1 Solution continued H=3.49 Oersteds B=1.45 T

11. 11 Example 3 Solution –Part 1 Solution continued H bcde = 277.7A-t/m B bcde = 1.45 T 0.008 Wb=  gap 0.058 Wb=  bcde

12. 12 Example 3 Solution –Part 1 Solution continued Wb H=37 Oersteds B=1.65 T

13. 13 Example 3 Solution –Part 1 Solution continued H bcde = 2944 A-t/m B bcde = 1.65 T 0.008 Wb=  gap 0.058 Wb=  bcde 0.066 Wb=  total F abef

14. 14 Example 3 Solution –Part 1 Solution continued

15. Example 3 Solution –Part 2 Computing Relative Permeabilities 15 Part 2 Solution Method:Find B and H for each section (From Part 1) Compute permeability of each section Compute relative permeability

16. 16 Example 3 Solution –Part 2 Computing Relative Permeabilities Part 2 solution continued

17. Example 4- Electric Circuit Analogy with Given Reluctances 17 Coil has 140 turns A1A2 tt 11 22 R1R1 R2R2 22 11 0.25 Wb =  t F tot R3R3 R 1 = 10,500 A-t/Wb R 2 = 30,00 A-t/Wb R 3 = 40,00 A-t/Wb Find coil I,  2 and MMF drop across R 3 I=? FR3FR3

18. Example 4 Solution 18

19. Example 4 Solution 19 Solution continued

20. Example 4 Solution 20 Check the previous result using flux division

21. Magnetic Circuits and Inductance 21 Magnetic structures are modeled as inductors. These structures also have a dc resistance due to winding resistance Define inductance in terms of coil parameters Product of flux and turns -flux linkages = N  lambda  Remember Substitute

22. 22 Magnetic Circuits and Inductance Define flux linkages in terms of magnetic coil parameters Inductance, L, defined as flux linkages per amp so …… Where: L = inductance (H)  = permeability of core material (Wb/A-t-m) N = number of turns in coil A = cross-sectional area of core (m 2 ) l = length of core (m) Note:

23. 23 Inductance Calculation Example A 100 turn coil with a cross-section area of 0.025 m 2 is 20 cm long. The core material has a relative permeability of 2750. Find the inductance of this coil.

24. Hysteresis in Magnetic Circuits 24 Coercive Force - force required to bring flux to zero Hysteresis occurs in ac circuits area inside loop represents power lost smaller area less losses (J/cycle/m 3 ) H -H B -B a o b c d f e Initial magnetization : oa Demagetization: abc Change poles: cd Reverse magnetization : defa

25. Power Loss Due to Hysteresis 25 Hysteresis losses depend on: frequency flux density mass of core iron Relationship Where:P h = hysteresis losses (W/unit mass) f = frequency of flux wave (Hz) B max = Maximum flux density (T) k h = constant (depends on material and unit system n = exponent varies with material ( 1.4 -1.6)

26. Hysteresis Power Loss Example 26 Knowing one set of conditions, can use proportions to find another. A power transformer has a silicon steel core (n = 1.6) This power transformer operates at 60 Hz with a P h of 2.5 kW. What are the hysteresis losses when it operates at 50 Hz

27. Hysteresis Power Loss Example Solution 27 Set up proportion Cross multiply and solve for P h50

28. END LESSON 4: SOLVING MAGNETIC CIRCUITS WITH ELECTRICAL ANALOGIES ET 332a Dc Motors, Generators and Energy Conversion Devices 28