An Ideal Transformer Example: Difference between revisions
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<math>\ =(45+j27)\Omega</math> |
<math>\ =(45+j27)\Omega</math> |
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Since <math>{i_{1}}=\frac{e_{1}}{ |
Since <math>{i_{1}}=\frac{e_{1}}{Z_{th}}</math>, |
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<math>{i_{1}}=\frac{120\sqrt{2}}{45+j27} A</math> |
<math>{i_{1}}=\frac{120\sqrt{2}}{45+j27} A</math> |
Revision as of 09:55, 21 January 2010
Consider a simple, transformer with two windings. Find the current provided by the voltage source.
- Winding 1 has a sinusoidal voltage of ° applied to it at a frequency of 60Hz.
- The combined load on winding 2 is
Solution
Given: and
Substituting ,
Therefore,
Now the Thevenin equivalent impedance, , is found through the following steps:
Since this is an ideal transformer and
So we can substitute,
Now, substituting:
Since ,
Since this is an ideal transformer, it can be modeled by this simple circuit:
Contributors
Reviwed By
Andrew Sell - Chris, everything looks fine, though I would do some extra formatting if possible to help make the problem flow a little smoother as you read it, and locate the picture a little higher to help bring the solution together.
Read By
John Hawkins