ET 332a Dc Motors, Generators and Energy Conversion Devices 1 Lesson 20 332a.pptx.
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Transcript of ET 332a Dc Motors, Generators and Energy Conversion Devices 1 Lesson 20 332a.pptx.
LESSON 20: NON-LINEAR OPERATION OF COMPOUND MOTORS
ET 332aDc Motors, Generators and Energy Conversion Devices
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Lesson 20 332a.pptx
LEARNING OBJECTIVES
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After this presentation you will be able to:
Determine the operating point of a dc compound motor
Observe the effect of driving a constant torque load on motor performance
Compute the value of field resistance to produce a given speed
Solve non-linear dc motor problems given a magnetization curve.
NON-LINEAR COMPOUND MOTOR CALCULATIONS
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Example 20-1: Compound motor with non-linear magnetic circuit. Ten percent of series field used to offset armature reaction.
240 V, 125 HP, 850 rpm, Ra = 0.0172 ohms RIP = 0.005 ohms Series field resistance Rs = 0.0023 ohmsShunt field resistance Rf = 49.2 ohmsSeries field turns Ns = 4.5 tShunt field turns Nf = 577 t Efficiency at rated load 85.4%Drives a constant torque loadCompute a.) If b.) Ia c.) developed torque d.) Ia when a series R is added to increase speed to 900 rpm. e.) The field resistance in series with the shunt coil to produce the 900 rpm speed.
EXAMPLE 20-1 SOLUTION (1)Lesson 20 332a.pptx
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LoadT= constant
RIP
Interpole
Rf
Ra
Rs
Series Field
Rx
Shunt Field
EaVT
0.0172 W
0.005 W0.0023 W
49.2 W
???? W
240 V
n1 = 850 rpm Nf = 577 t
Ns = 4.5 t
Magnetizationcurve given infigure 11-7 in text
Find Ia from rated output power and efficiency
Answer a.)
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EXAMPLE 20-1 SOLUTION (2)
Answer b.)
EXAMPLE 20-1 SOLUTION (3)
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Answer c.)
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EXAMPLE 20-1 SOLUTION (4)Part d.) Ia2 = ??? Use Fig 11-7 to find the total field mmf.
0 1 2 3 4 5 6 70
0.2
0.4
0.6
0.8
1
1.2Motor Magnetizing Curve
mmf (in 1000 A-t/pole)
Flu
x D
ensi
ty (
T)
.88fnet
1000
EXAMPLE 20-1 SOLUTION (5)Lesson 20 332a.pptx
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For non-linear operation, torque in proportional to Bp∙Ia
For constant torque load, TD1 = TD2
Solve for Ia2
This relates Ia2 to Bp2
Need another equation
EXAMPLE 20-1 SOLUTION (6)Lesson 20 332a.pptx
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Use speeds n1= 850 rpm n2=900 rpm. Speed is inversely proportional to Bp.
SpeedRatio
EXAMPLE 20-1 SOLUTION (7)Lesson 20 332a.pptx
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EXAMPLE 20-1 SOLUTION (7)Solve the quadratic equation using the quadratic formula
EXAMPLE 20-1 SOLUTION (8)Lesson 20 332a.pptx
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LoadT= constant
RIP
Interpole
Rf
Ra
Rs
Series Field
Rx
Shunt Field
EaVT
0.0172 W
0.005 W0.0023 W
49.2 W
???? W
240 V
n1 = 850 rpm Nf = 577 t
Ns = 4.5 t
Part e.) Find the value of Rx to produce 900 rpm with constant T load
Use the value of Bp2 computed from the previous part.
Use the magnetizing curve from the text find the total mmf required to product the computed flux density.
Bp2 0.83 T
Rf 49.2
EXAMPLE 20-1 SOLUTION (9)Lesson 20 332a.pptx
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0 1 2 3 4 5 6 70
0.2
0.4
0.6
0.8
1
1.2Motor Magnetizing Curve
mmf (in 1000 A-t/pole)
Flu
x D
ensi
ty (
T)
.83
fnet
1000
Number of turns in each field winding
Nf 577 t
Shunt
Ns 4.5 t
Series
Fnet = 4000 A-t
Ia21 477.2 A
Current computed from the previous part.
EXAMPLE 20-1 SOLUTION (10)
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4000 A-t/pole
Answer e.)
ET 332aDc Motors, Generators and Energy Conversion Devices
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END LESSON 20