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The replacements of voltage and current sources do what the sources would do if their values were set to zero. November Learn how and when to remove this template message. Theorem in circuit analysis. From Wikipedia, the free encyclopedia.
The equivalent circuit is a voltage source with voltage V Th in series with a resistance R Th. By using superposition of specific configurations, it can be shown that for any linear “black box” circuit which contains voltage sources and resistors, its voltage is a linear function of the corresponding current as follows.
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Unsourced material may be challenged and removed. It is noted that the second step is usually implied in literature. Here, the first term reflects the linear summation of contributions from each voltage source, while the second term measures the contributions from all the resistors.
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Circuit theorems Linear electronic circuits.
The theorem also applies to frequency domain AC circuits consisting of reactive and resistive impedances. This article needs additional citations for verification. Now, the uniqueness theorem guarantees that the result is general. This page was last edited on 27 Decemberat The first step is to use superposition theorem to construct a solution. Please help improve this article by adding citations to reliable sources.
Resistance can then be calculated across the terminals using the formulae for series and parallel circuits. Original circuit The equivalent voltage The equivalent resistance The equivalent circuit. The resistance is measured after replacing all voltage- and current-sources with their internal resistances.
This method is valid only for circuits with independent sources. In circuit theory terms, the theorem allows any one-port network to be reduced to a single voltage source and a single impedance.
Thévenin’s theorem – Wikipedia
Retrieved from ” https: That means an ideal voltage source is replaced with a short circuit, and an ideal current source is replaced with an open circuit. A zero valued current source passes zero current, regardless of the voltage across it; its replacement, an open circuit, does the same thing.
Then, uniqueness theorem is employed to show that the obtained solution is unique. If there are dependent sources in the circuit, another method must be used such as connecting a test source across A and B and calculating the voltage across or current through the test source.
In other words, the above relation holds true independent of what the “black box” is plugged to. A zero valued voltage source would create a potential difference of zero volts between its terminals, regardless of the current that passes through it; its replacement, a short circuit, does the same thing.
The proof involves two steps.