An Ideal Transformer Example: Difference between revisions

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<math>\ =(45+j27)\Omega</math>
<math>\ =(45+j27)\Omega</math>


Since <math>{i_{1}}=\frac{e_{1}}{R_{th}}</math>,
Since <math>{i_{1}}=\frac{e_{1}}{Z_{th}}</math>,


<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 10:55, 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: Ideal Circuit.jpg

Contributors

Christopher Garrison Lau I

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