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Transformers
Lecture 6
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Transformers utilization
As engineers, you should have seen some transformers while you driving or
walking by some substations near power plants, industrial cities or closer to your
houses!
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Practical Transformer
Winding resistance
Flux leakage
Finite permeability
Core losses
Figure 1-a
Contrary to an ideal transformer, a practical transformer has
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Transformer Model
physical reasoning
mathematic model of coupled
circuits
Winding resistance in serieswith leakage inductance
Magnetizing inductance inparallel with core resistance
Figure 1-b
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Referred equivalent circuits
Practical transformer is equivalent to lumped parameters
circuit and ideal transformer
Figure 2
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The ideal transformer can be shifted to either side as in Figures 3 and 4and the
circuit parameters reduced to the appropriate values
Figure 3
Figure 4
E1=E2= aE2
V
2=aV2
I2=I2/a
Xl2=a2xl2
R2=a2R2
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Approximate Equivalent Circuits
I1R1 and I1Xl1 are small
Therefore, |E1| = |V1|
Shunt branch can be moved tosupply terminal
I
small (5% of rated current)Shunt branch removed
Figure 5-a
Figure 5-b-c
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EXAMPLE
An Engineer needs to know the parameters of a 46KVA Transformer which has a2300V/230V winding. His results are:
Open Circuit Test: 230V 11.2A 1150W
Short Circuit Test: 160V 28.0A 1150W
We must first determine which side Low or High the test was performed on.
For the Open Circuit test we compare the tested voltage to the rated voltage of thetransformer.
In this example we see that the Open Circuit Test voltage is the same as the Low siderated operating voltage, thus we know the test was performed on the low side and thehigh side was left open.
Next we need to determine which side the Short Circuit Test was performed on, sowe compare the Current this time.
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Example (continued)
So now we know where the tests were performed.
Open Circuit Test: 230V 11.2A 1150W -H.V. Left open, and tested on Low side
Short Circuit Test: 160V 28.0A 1150W -L.V. Shorted, and tested on High side
So we know that the Open Circuit parameters are Referred to Primary.
So we will use the Referred to Primary parameters for the Open Circuit test.
What we know:
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Example (continued)
Now remember how the Short Circuit Test proved out that the L.V. side was shorted?
This means our equivalent calculations are Referred to the H.V. side. So in effect what weare calculating are ourX2 and R2 values. If we want ourX1 and R1 values, we must divideby our transformation ratio.
To complete our Primary Referred Circuit we must find ourR1 and X1 values. And giventhe fact that the transformer is stepping up voltage from 230 to 2300, we can see that it is a1:10 ratio, orN1 = 1,N2 = 10.
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To complete our Primary Referred Circuit we must find ourR1 and X1 values.And given the fact that the transformer is stepping up voltage from 230 to 2300,we can see that it is a 1:10 ratio, orN
1= 1,N
2= 10.
Now of course one might think this is the end, but that is far from the truth. At
this time we know enough about the circuit to go further if we desire. From herewe can obtain the terminal voltages for simulation, a very important factor indesigning a system!
Example (continued)
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Voltage regulation
No load V2=V1/a
Loaded V2=V1/a V2
Voltage regulation =
Maximum voltage regulation
occur ifL= eq1
%100xVfl
VflVnl
Figure 8 a-b
Figure 8 a
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Efficiency
cucout
out
PPPP
++
=
2
2
2222
222
cos
cos
eqc RIPIV
IV
++
=
Max efficiency occurs for:
Fixed and22
V
Fixed and2V 2I 1cos 2 =
Pc=Core Losses in Watts
Pcu= Copper Losses in Watts
2
2
2 eqc RIP=
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Autotransformer
Another type of transformer is known as the autotransformer.
It consists of a single tapped primary where the center tap is commonto both primary and secondary (not isolated).
some of the turns on the coil are used for the primary and some are
used for the secondary.
an example of a variable autotransformer is known as a variac.
A variac is a single coil with a sweeping arm for the center common,this allows the ratio of primary turns:secondary turns to be alteredeasily.