elec 3105 basic em and power engineering rotating dc motor part 2 electrical
DESCRIPTION
Motor / Generator Action Linear relation between speed and torque Current flows in a direction to charge the battery. Motor Slide extracted from linear motor and modified for loop motor. Stall torque Generator LinkTRANSCRIPT
ELEC 3105 Basic EM and Power Engineering
Rotating DC MotorPART 2 Electrical
Motor / Generator Action
BrVemf
2
Equivalent circuit
emfVbat
V
R
terminalv
Expression of Vemf
Loop
Slide extracted from linear motor and modified for loop motor.
I
emfbatVIRV
BrRrB
Vbat
22
rBI2
Motor / Generator Action
BrRrB
Vbat 22
Linear relation betweenspeed and torque
rBVbat
loadno 2
RVrB bat2
0
Current flows in a direction to charge the battery.
Motor
Slide extracted from linear motor and modified for loop motor.
Stall torque
GeneratorLink
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
E = motor voltageRa = armature resistanceLa = armature inductanceV = Applied motor voltageIa = armature current
= magnetic fluxRf = field resistanceLf = field inductanceVf = Field voltageIf = field current
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
In steady state operation: FIELD SIDE
πΌ π=π π
π πΞ¦=
2ππΌ ππreluctance
Magnetic circuit
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
In steady state operation: ARMATURE SIDE
πΈ=ππΈΞ¦ππ
Motor constant
Back emf
Motor / Generator Action
BrVemf
2
Equivalent circuit
emfVbat
V
R
terminalv
Expression of Vemf
Loop
Slide extracted from linear motor and modified for loop motor.
I
emfbatVIRV
BrRrB
Vbat
22
rBI2
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
In steady state operation: ARMATURE SIDE
πΈ=ππΈΞ¦ππ
Motor constant
Back emf
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
In steady state operation: ARMATURE SIDE
π πππ£=ππΞ¦ πΌπ
Motor constant
Developed torque
ππΈ=ππ Same motor constant in emf and developed torque
Motor / Generator Action
BrVemf
2
Equivalent circuit
emfVbat
V
R
terminalv
Expression of Vemf
Loop
Slide extracted from linear motor and modified for loop motor.
I
emfbatVIRV
BrRrB
Vbat
22
rBI2
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
In steady state operation: ARMATURE SIDE
π πππ£=ππΞ¦ πΌ π
Motor constant
Developed torque
ππΈ=ππ Same motor constant in emf and developed torque
πΈ=ππΈΞ¦ππ
Motor constant
Back emf
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
Power flow: ARMATURE SIDE; Conservation of energy
π=πΌππ π+πΈKVL
POWER π πΌ π= πΌπ2 π π+πΌ ππΈ
Power in
Armature copper loss
Power developed
Motor / Generator Action
BrVemf
2
Equivalent circuit
emfVbat
V
R
terminalv
Expression of Vemf
Loop
Slide extracted from linear motor and modified for loop motor.
I
emfbatVIRV
BrRrB
Vbat
22
rBI2
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
Power flow: ARMATURE SIDE; Conservation of energy
ππππ£= πΌππΈ=ππππππ£
Power developed
π πππ π π ππ
ππππ£
Electrical Mechanicalcopper
π πΌ π= πΌπ2 π π+πΌ ππΈ
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
Power flow: ARMATURE SIDE πππ’π‘=ππππ£βππππ‘
π πππ π π ππ
ππππ£
Electrical Mechanical
ππππ‘
πππ’π‘
Rotational lossCopper
Electrical Equivalent
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
Motor sequence πππ’π‘=ππππ£βππππ‘
πππ π πππ£
Speed of rotation limiting loop
πΈπΌπ ππππ£
Shunt Connected Field
V
aIπ ππΏπ
E
ππ ,π πππ£πΏ π
π πR
π πππ£=ππΞ¦ πΌπ
π=πΌππ π+πΈ
πΈ=ππΈΞ¦ππ
π πππ£=πΞ¦ππ π
β π2Ξ¦2
π πππ
Developed torque Rotation rate
Shunt Connected Field
V
aIπ ππΏπ
E
ππ ,π πππ£πΏ π
π πR
π πππ£=πΞ¦ππ π
β π2Ξ¦2
π πππ
Similar type of graph
Shunt Connected Field
V
aIπ ππΏπ
E
ππ ,π πππ£πΏ π
π πR
π πππ£=πΞ¦ππ π
β π2Ξ¦2
π πππ
π πππ£
ππ
πΎΞ¦ππ π
ππΞ¦
MotorGenerator
Force motor to spin backwards
Generator
Force motor to spin to fast
Series Connected Field
V
aIπ ππΏπ
E
ππ ,π πππ£
πΏ ππ π
Universal motor design: works for D.C. and for A.C.
π πππ£=ππΞ¦ πΌ π
π=πΌ π(π ΒΏΒΏπ+π π )+πΈ ΒΏ
πΈ=ππΈΞ¦ππ
π πππ£=πβ² πΌπ2 Since Ξ¦β πΌπ
Series Connected Field
V
aIπ ππΏπ
E
ππ ,π πππ£
πΏ ππ π
Universal motor design: works for D.C. and for A.C.
π πππ£=πβ² [ ππ π+π π+πβ²ππ ]
2
π πππ£
ππ
1ππ
2
Maximum Power Transfer
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π ππ=πΌ ππ π+πΈ
Power developed in the motor ππππ£=πΈ πΌπ
ππππ£=πΈ (π βπΈ )/π π
ππππ£=πΈπ βπΈ2
π π
Find maximum with respect to the motor voltage
Maximum Power Transfer
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π ππ=πΌ ππ π+πΈ
For extremes of a function, take derivatives and set to zero
ππππ£=πππ₯πππ’π hπ€ πππΈ=π2
ππππ£ πππ₯ = π£2
4 π π
Calculation example
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
A 120 volt dc motor has an armature resistance of 0.70 Ξ©. At no-load, it requires 1.1 A armature current and runs at 1000 rpm. Find the output power and torque at 952 rpm output speed. Assume constant flux.
π πππ£=ππΞ¦ πΌππ=πΌππ π+πΈ
πΈ=ππΈΞ¦ππ
Solution provided in class
Calculation example
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
A permanent magnet dc motor has the following information: 50 hp, 200 V, 200 A, 1200 rpm and armature resistance of 0.05 Ξ©. Determine the output power if the voltage is lowered to 150 V and the current is 200 A. Assume rotational losses are proportional to speed. Determine the rotational loss, armature resistance, no-load rpm, machine constant, efficiency?
π πππ£=ππΞ¦ πΌππ=πΌππ π+πΈ
πΈ=ππΈΞ¦ππ
Solution provided in class
Calculation example
V
fV
aI π ππΏπ
E
ππ ,π πππ£
πΏ π
π π
An 80 V dc motor has constant field flux, separately excited, and a nameplate speed of 1150 rpm with 710 W output power. The nameplate armature current is 10 A and the no-load current is 0.5 A. Assume constant rotational losses.
π πππ£=ππΞ¦ πΌππ=πΌππ π+πΈ
πΈ=ππΈΞ¦ππ
Solution provided in class