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{{Short description|Process of simplifying circuit solutions}}
{{about|electronic circuits|transformation of source code|Program transformation}}
'''Source transformation''' is the process of simplifying a circuit solution, especially with mixed sources, by transforming [[voltage]] sources into [[Electric current|current]] sources, and vice versa, using [[Thévenin's theorem]] and [[Norton's theorem]] respectively.<ref name="CPP">CPP. https://www.cpp.edu/~elab/projects/project_08/index.html.</ref>
== Process ==
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Performing a source transformation consists of using [[Ohm's law]] to take an existing [[voltage source]] in [[series circuit|series]] with a [[resistor|resistance]], and replacing it with a [[current source]] in [[parallel circuit|parallel]] with the same resistance, or vice versa. The transformed sources are considered identical and can be substituted for one another in a circuit.<ref name="Nilsson">Nilsson, James W., & Riedel, Susan A. (2002). ''Introductory Circuits for Electrical and Computer Engineering''. New Jersey: Prentice Hall.</ref>
Source transformations are not limited to resistive circuits.
Source transformations are used to exploit the equivalence of a real current source and a real voltage source, such as a [[battery (electricity)|battery]]. Application of Thévenin's theorem and Norton's theorem gives the quantities associated with the equivalence. Specifically, given a real current source, which is an ideal current source <math>I</math> in [[Series and parallel circuits|parallel]] with an [[Electrical impedance|impedance]] <math>Z</math>, applying a source transformation gives an equivalent real voltage source, which is an ideal voltage source in [[Series and parallel circuits|series]] with the impedance. The impedance <math>Z</math> retains its value and the new voltage source <math>V</math> has value equal to the ideal current source's value times the impedance, according to Ohm's Law <math>V=I
== Example calculation ==
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:: <math> V = I\cdot Z, \qquad I = \cfrac VZ</math>
[[Image:Sourcetrans.jpg
▲[[Image:Sourcetrans.jpg||frame|left|Figure 1. An example of a DC source transformation. Notice that the impedance Z is the same in both configurations.]]
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