Lesson 22 SelfExcited Dc Generators ET 332 a

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Lesson 22: Self-Excited Dc Generators ET 332 a Dc Motors, Generators and Energy Conversion

Lesson 22: Self-Excited Dc Generators ET 332 a Dc Motors, Generators and Energy Conversion Devices Lesson 22 332 a. pptx 1

Learning Objectives After this presentation you will be able to: Explain how a self-excited

Learning Objectives After this presentation you will be able to: Explain how a self-excited dc generator operates Ø Explain how voltage builds in self-excited dc generators Ø Use magnetization curves and dc machine formulas to find an unloaded generator’s terminal voltage Ø Identify the voltage characteristics of compound generators. Ø Lesson 22 332 a. pptx 2

Self-Excited Generator Connection With field switch open only residual flux can produce Ea Residual

Self-Excited Generator Connection With field switch open only residual flux can produce Ea Residual magnetism in pole pieces causes induced voltage Shunt field is connected in parallel with armature Racir + n Rf Fr VT If Prime mover provides mechanical power Lesson 22 332 a. pptx 3

Voltage Buildup in Self-Excited Generators 1. ) Residual magnetism causes Ea 0 with If=0

Voltage Buildup in Self-Excited Generators 1. ) Residual magnetism causes Ea 0 with If=0 2. ) Close switch and parallel armature and field Ea=VT Racir + n Rf Fr VT If I f 2 Ea 0 3. ) Ea 0/Rf = If 1 causes Ea to increase due to field flux increase 4. ) Ea increases to Ea 1 causing If 2 Ea 1 5. ) Process repeats until operating point reached Lesson 22 332 a. pptx 4

Self-Excited Generator Graphical Analysis Operating Point Magnetizing curve Rf Ea Operating point occurs when

Self-Excited Generator Graphical Analysis Operating Point Magnetizing curve Rf Ea Operating point occurs when magnetizing curve and field R lines intersect Ea 1 Ea 0 If 1 Lesson 22 332 a. pptx If 5

Field Resistance and Voltage Buildup Analytic methods Reluctance is nonlinear w. r. t. If

Field Resistance and Voltage Buildup Analytic methods Reluctance is nonlinear w. r. t. If In field circuit and so Equate field and armature circuit equations Non-linear equation with respect to (w. r. t. ) If. Difficult to solve. Lesson 22 332 a. pptx 6

Field Resistance and Voltage Buildup R 4 R 2 R 3 R 1 Ea

Field Resistance and Voltage Buildup R 4 R 2 R 3 R 1 Ea R 4 is critical resistance Ea will not build up due to excessive field resistance R 4 > R 3 > R 2 > R 1 If Lesson 22 332 a. pptx 7

Voltage Buildup and Speed of rotation effects the voltage buildup. Lower speed - lower

Voltage Buildup and Speed of rotation effects the voltage buildup. Lower speed - lower Ea Adjusting the rheostat controls terminal voltage. Critical resistance prevents voltage buildup at all speeds Lesson 22 332 a. pptx 8

Self-Excited Generator Example 22 -1: Given a generators magnetization curve (Fig 12 -4, p

Self-Excited Generator Example 22 -1: Given a generators magnetization curve (Fig 12 -4, p 443, text). Self-excited generator ratings: 125 Vdc, 50 k. W, 1750 rpm. No-load voltage with rheostat shorted 156 V Determine: a. ) field circuit resistance b. ) field rheostat setting for no-load voltage of 140 Vdc c. ) armature voltage if rheostat is set at 14. 23 ohms d. ) rheostat setting that will give critical resistance e. ) armature voltage at 80% rated speed and rheostat shorted f. ) rheostat setting for no-load voltage of 140 Vdc at 1750 rpm if field is separately excited from 120 Vdc source Lesson 22 332 a. pptx 9

Example 22 -1 Solution (1) Part a. ) Field circuit resistance (rheostat shorted) For

Example 22 -1 Solution (1) Part a. ) Field circuit resistance (rheostat shorted) For voltage of 156 Vdc, graph gives current of 4. 7 A Use Ohm’s Law to find the value of field resistance Answer Lesson 22 332 a. pptx 10

Example 22 -1 Solution (2) Part b. ) Rheostat setting to give Ea =

Example 22 -1 Solution (2) Part b. ) Rheostat setting to give Ea = 140 Vdc Field current value from graph is 3. 2 A Subtract off field resistance to find rheostat setting 140 V 33. 2 W 3. 2 A Answer Lesson 22 332 a. pptx 11

Example 22 -1 Solution (3) Part c. ) Find value of Ea when field

Example 22 -1 Solution (3) Part c. ) Find value of Ea when field rheostat increased to: Total field circuit resistance is: Graph this equation: Ea = 47. 421∙If The value of Ea is where the above equation intersects the magnetization curve. Lesson 22 332 a. pptx 12

Example 22 -1 Solution (4) Part d. ) Find the critical resistance value. Critical

Example 22 -1 Solution (4) Part d. ) Find the critical resistance value. Critical resistance has the same value as the slope of the linear part of the generator’s magnetization curve. Select two points and compute the slope Rcrit Ans Plot the line Ea = 59. 4∙If This is the critical resistance line Lesson 22 332 a. pptx 13

Example 22 -1 Solution (5) Part e. ) Armature voltage at 80% rated speed

Example 22 -1 Solution (5) Part e. ) Armature voltage at 80% rated speed and rheostat shorted out. Multiply the rated speed Ea curve data by 0. 80 to get new curve then plot the line Ea = 33. 2∙If line. The intersection is the solution Ea = 115 V Ans Lesson 22 332 a. pptx 14

Example 22 -1 Solution (6) Part f. ) Find the field rheostat for separately

Example 22 -1 Solution (6) Part f. ) Find the field rheostat for separately excited operation for a 120 V dc source if Ea = 140 V dc Separately excited source voltage and Rf from part a. ) 33. 191 W 3. 2 A 120 V If =3. 2 A Ans Lesson 22 332 a. pptx 15

Terminal Voltage Characteristic Increasing load increases Ia. R drop. Rated Increase load until breakdown

Terminal Voltage Characteristic Increasing load increases Ia. R drop. Rated Increase load until breakdown occurs VT Ia Breakdown Rated Constant I Region Lesson 22 332 a. pptx 16

Compound Generator Connections Short shunt connection Avoids series field drop Lesson 22 332 a.

Compound Generator Connections Short shunt connection Avoids series field drop Lesson 22 332 a. pptx Long shunt connection Preferred in calculations 17

Compound Generator Characteristics Loading effects on induced voltage Over Compounded Flat Compounded Ff =

Compound Generator Characteristics Loading effects on induced voltage Over Compounded Flat Compounded Ff = shunt field mmf Fs = series field mmf Fd = demagnetizing mmf Series field flux related to load. Increasing load increases field flux which increase Ea. Lesson 22 332 a. pptx Under Compounded Shunt Generator Differentially Compounded 18

End Lesson 22 ET 332 a Dc Motors, Generators and Energy Conversion Devices Lesson

End Lesson 22 ET 332 a Dc Motors, Generators and Energy Conversion Devices Lesson 22 332 a. pptx 19