DC Machine Example Problems
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Transcript of DC Machine Example Problems
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8/10/2019 DC Machine Example Problems
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Examples
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Andy Knight (/~aknigh/index.html) - Electrical Machines/~aknigh/electrical_machines/machines_main.html)
DC Machine Exampleseparately Excited
separately excited DC motor is rotated at 1000rpm, The variation of armature terminal
oltage as a function of field current is measured under no-load conditions and tabulated
elow:
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
0 30 60 85 102 115 124 130 134
he field winding supply and the field resistance is adjustable. The armature
inding resistance and the armature terminal voltage .a. Calculate the field current if the motor is operated with no-load at 1000 rpm
b. The motor drives a load at 1200 rpm. Calculate the armature voltage at 1200 rpm if the
field resistance
c. Calculate the torque for the above condition
d. The motor supplies a mechanical load of 4000W at 1450rpm. The mechanical rotational
losses are 160W, calculate the efficiency
omments
his question is similar to many DC machine questions and falls into two parts. At the start of
he question, you are given a reasonable amount of data about a specific operating condition.
ou need to then take useful information from this operating condition and apply it to theew operating conditions specified in the rest of the question.
olution
his is a separately excited motor problem:
here are two important pieces of information in the beginning of the question:The information is being given for "no-load" conditions. No-load in machines means
no useable power flow out of the machine. If there is no power flow in a dc machine,
there is no armature current, and therefore the terminal voltage equals the
armature voltage:
You are being given data on the induced armature voltage at a given speed
The data for armature voltage at a given speed allows you to find the nonlinear
relationship between flux and field current, which is independent of speed.
nowing how the data in the question is useful is a significant part of the solution process for
C machine questions.
I
F
V
T
= 2 4 VV
F
= 0 . 2 R
A
= 1 3 0 VV
T
= 6 0 R
F
= 0
I
A
=
E
A
V
T
http://people.ucalgary.ca/~aknigh/electrical_machines/machines_main.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/machines_main.htmlhttp://people.ucalgary.ca/~aknigh/index.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_examples.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_power.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_series.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_sep.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_real.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_comm.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc_volts.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_ac.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_dc.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_basic.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_emreview.htmlhttp://people.ucalgary.ca/~aknigh/electrical_machines/fundamentals/f_main.html -
8/10/2019 DC Machine Example Problems
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a. This question requires you to read data from the table provided. Under no-load
conditions, occurs when
b. Armature voltage is given by
i.e. voltage is a function of and speed. Flux is a function of field current, and since
field voltage and resistance are specified in the question, a first step is to find field
current:
gives
From the table in the question, when: and then
. We need to find for the case when and
There are two possible approaches:
i. In both cases, the field current is constant, therefore flux will be constant.
Armature voltage will be proportional to speed:
Giving
ii. Using the armature voltage equation, find :
Now, at 1200 rpm armature voltage can be found directly from the armature
voltage equation:
Givingc. To find the torque, there are three possible approaches. Two of the approaches require
the calculation of if it has not already been done, two of the approaches require the
calcualtion of the armature current. require the armature current, which can be found
from the armature loop equation
I
i. Using power equations:
= 1 3 0 VV
T
= 0 . 7 AI
F
= E
A
= V
F
I
F
R
F
= 0 . 4 A
I
F
= 1 0 0 0 r p m
= 0 . 4 AI
F
= 1 0 2 VE
A
E
A
= 1 2 0 0 r p m
= 0 . 4 AI
F
= E
1 2 0 0
E
1 0 0 0
1 2 0 0
1 0 0 0
= 1 2 2 . 4 VE
A
= 0 . 4
I
F
= 0 . 4
I
F
=
E
A
= =
2
6 0
1 0 0
3
= 0 . 9 7 4
E
A
1 2 0 0
=
= 1 2 0 0
2
6 0
= 1 2 2 . 4 VE
A
= + V
T
E
A
I
A
R
A
= 3 8 . 0 A
A
P
c
= = E
A
I
A
-
8/10/2019 DC Machine Example Problems
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ii. Using the torque equation directly: . This approach requires the
calculation of , if not already done in the armature voltage calculation.
iii. Rearranging the torque-speed equation:
d. The final part of the question includes mechanical losses. In this case
No information is available on the flux in the machine, so armature voltage or current
cannot be directly determined from the armature voltage equation or torque equation.
The preferred approach is to consider the power in the armature circuit:
Solving the quadratic for armature current results in two values, or
. The correct answer will be the one that results in the lowest power
loss, . The armature voltage can be found by solving the armature
circuit equation
At this point, the armature losses can be found, but this is a separately excited machineand it is important to remember to account for power flow in the field circuit. To find
the field current that gives at 1450 rpm, it is necessary to calculate
armature voltage that would be induced at the same field current with a rotational
speed of 1000 rpm.
gives which, from the table, corresponds to a field current
Finally, efficiency can be found from
giving
eries Motor Exam le
P
c
= = E
A
I
A
=
1 2 2 . 4 3 0 I
A
1 2 0 0
= 3 7 N
= I
A
=
V
T
R
A
(
)
2
= P
c
=
+ P + a a P
4 0 0 0 + 1 6 0 = 4 1 6 0 W
= + V
T
I
A
E
A
I
A
I
2
A
R
A
+ = 0 I
2
A
R
A
V
T
I
A
P
c
= 6 1 6 AI
A
I A = 3 3 . 7 5 A
= 3 3 . 7 5 AI
A
= +
V
T
E
A
I
A
R
A
= 1 2 3 . 2 5 AE
A
= 1 2 3 . 2 5 A
E
A
= E
A
1 0 0 0
E
A
1 4 5 0
1 0 0 0
1 4 5 0
= 8 5 . 0 VE
A
1 0 0 0
= 0 . 3 AI
F
P
=
P
+
P
P
= + + = 3 9 5 WI
2
A
R
A
I
2
F
R
F
P
a a
=
4 0 0 0
4 3 9 5
= 9 1 . 0 %
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8/10/2019 DC Machine Example Problems
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Andy Knight (mailto:[email protected])
series DC motor has combined armature and field resistance of . When
onnected to a supply of at standstill, the motor develops a torque of 1500Nm.
a. Calculate the armature current at standstill and combined motor constant
b. Calculate the torque when the speed is 500 rpm
c. Calculate the output power and efficiency when operating at 500 rpm (neglect
mechanical losses)
olution
his is a series motor problem:
a. At standstill, the angular velocity is zero, therefore the armature voltage is zero
. The full terminal voltage is dropped across the winding
resistances and gives
Using the torque equation for a series excited DC machine, , the combined
motor constant can be found:b. To find the torque it is possible to either substitute directly into the series motor torque-
speed equation, or to first find the armature currents:
i.
Re-arranging the torque speed equation and submitting for kc and speed gives
ii. Alternately, substitute into in the armature loop equation to
obtain and solve for armature current.
and use the torque equation .
c. To find efficiency neglecting rotational losses:
+ = 1 . 2 R
A
R
S
= 4 8 VV
T
c
( = c = \ 0 ) E
A
I
A
= + ( + ) V
T
I
A
R
A
R
S
= 4 0 AI
A
= c
I
2
A
c= 1 5 0 0 / 1 6 0 0 = 0 . 9 3 7 5
N
A
2
=
V
T
c
1
+ R
A
R
S
c
= =
2
6 0
5 0
3
= 0 . 8 5 4 N
= c E
A
I
A
= ( c + + ) V
T
I
A
R
A
R
S
= 0 . 9 5 5 AI
A
= c I
2
A
= = =
P
c
P
E
A
I
A
V
T
I
A
E
A
V
T
a = 9 7 . 0 %
mailto:[email protected]