Thévenin 's theorem - wikipedia Thévenin 's theorem Any black box containing resistances only and voltage and current sources can be replaced by a Thévenin equivalent circuit consisting of an equivalent voltage source in series connection with an equivalent resistance. As originally stated in terms of DC resistive circuits only, Thévenin 's theorem holds that : Any linear electrical network with voltage and current sources and resistances only can be replaced at terminals A-B by an equivalent voltage source V in series connection with an equivalent resistance R. The equivalent voltage V is the voltage obtained at terminals A-B of the network with terminals A-B open circuited. The equivalent resistance R is the resistance that the circuit between terminals A and B would have if all ideal voltage sources in the circuit were replaced by a short circuit and all ideal current sources were replaced by an open circuit. If terminals A and B are connected to one another, the current flowing from A to B will be V / R. This means that R could alternatively be calculated as V divided by the short - circuit current between A and B when they are connected together. In circuit theory terms, the theorem allows any one - port network to be reduced to a single voltage source and a single impedance. The theorem also applies to frequency domain AC circuits consisting of reactive and resistive impedances. It means the theorem applies for AC in an exactly same way to DC except that resistances are generalized to impedances. The theorem was independently derived in 1853 by the German scientist Hermann von Helmholtz and in 1883 by Léon Charles Thévenin ( 1857 -- 1926 ), an electrical engineer with France 's national Postes et Télégraphes telecommunications organization. Thévenin 's theorem and its dual, Norton 's theorem, are widely used to make circuit analysis simpler and to study a circuit 's initial - condition and steady - state response. Thévenin 's theorem can be used to convert any circuit 's sources and impedances to a Thévenin equivalent ; use of the theorem may in some cases be more convenient than use of Kirchhoff 's circuit laws. Contents 1 Calculating the Thévenin equivalent 1.1 Example 2 Conversion to a Norton equivalent 3 Practical limitations 4 A proof of the theorem 5 See also 6 References 7 Bibliography 8 External links Calculating the Thévenin equivalent The equivalent circuit is a voltage source with voltage V in series with a resistance R. The Thévenin - equivalent voltage V is the open - circuit voltage at the output terminals of the original circuit. When calculating a Thévenin - equivalent voltage, the voltage divider principle is often useful, by declaring one terminal to be V and the other terminal to be at the ground point. The Thévenin - equivalent resistance R is the resistance measured across points A and B `` looking back '' into the circuit. The resistance is measured after replacing all voltage - and current - sources with their internal resistances. That means an ideal voltage source is replaced with a short circuit, and an ideal current source is replaced with an open circuit. Resistance can then be calculated across the terminals using the formulae for series and parallel circuits. This method is valid only for circuits with independent sources. 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. The replacements of voltage and current sources do what the sources would do if their values were set to zero. 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. A zero valued current source passes zero current, regardless of the voltage across it ; its replacement, an open circuit, does the same thing. Example Original circuit The equivalent voltage The equivalent resistance The equivalent circuit In the example, calculating the equivalent voltage : V T h = R 2 + R 3 ( R 2 + R 3 ) + R 4 ⋅ V 1 ( displaystyle V_ ( mathrm ( Th ) ) = ( R_ ( 2 ) + R_ ( 3 ) over ( R_ ( 2 ) + R_ ( 3 ) ) + R_ ( 4 ) ) cdot V_ ( mathrm ( 1 ) ) ) = 1 k Ω + 1 k Ω ( 1 k Ω + 1 k Ω ) + 2 k Ω ⋅ 15 V ( displaystyle = ( 1 , mathrm ( k ) Omega + 1 , mathrm ( k ) Omega over ( 1 , mathrm ( k ) Omega + 1 , mathrm ( k ) Omega ) + 2 , mathrm ( k ) Omega ) cdot 15 , mathrm ( V ) ) = 1 2 ⋅ 15 V = 7.5 V ( displaystyle = ( 1 over 2 ) cdot 15 , mathrm ( V ) = 7.5 , mathrm ( V ) ) ( notice that R is not taken into consideration, as above calculations are done in an open - circuit condition between A and B, therefore no current flows through this part, which means there is no current through R and therefore no voltage drop along this part ) Calculating equivalent resistance ( R x ‖ R y ( displaystyle R_ ( x ) R_ ( y ) ) is the total resistance of two parallel resistors ) : R T h = R 1 + ( ( R 2 + R 3 ) ‖ R 4 ) ( displaystyle R_ ( mathrm ( Th ) ) = R_ ( 1 ) + left ( left ( R_ ( 2 ) + R_ ( 3 ) \right ) R_ ( 4 ) \right ) ) = 1 k Ω + ( ( 1 k Ω + 1 k Ω ) ‖ 2 k Ω ) ( displaystyle = 1 , mathrm ( k ) Omega + left ( left ( 1 , mathrm ( k ) Omega + 1 , mathrm ( k ) Omega \right ) 2 , mathrm ( k ) Omega \right ) ) = 1 k Ω + ( 1 ( 1 k Ω + 1 k Ω ) + 1 ( 2 k Ω ) ) − 1 = 2 k Ω. ( displaystyle = 1 , mathrm ( k ) Omega + left ( ( 1 over ( 1 , mathrm ( k ) Omega + 1 , mathrm ( k ) Omega ) ) + ( 1 over ( 2 , mathrm ( k ) Omega ) ) \right ) ^ ( - 1 ) = 2 , mathrm ( k ) Omega. ) Conversion to a Norton equivalent Norton - Thevenin conversion Main article : Norton 's theorem A Norton equivalent circuit is related to the Thévenin equivalent by R T h = R N o ( displaystyle R_ ( mathrm ( Th ) ) = R_ ( mathrm ( No ) ) ! ) V T h = I N o R N o ( displaystyle V_ ( mathrm ( Th ) ) = I_ ( mathrm ( No ) ) R_ ( mathrm ( No ) ) ! ) I N o = V T h / R T h. ( displaystyle I_ ( mathrm ( No ) ) = V_ ( mathrm ( Th ) ) / R_ ( mathrm ( Th ) ). ! ) Practical limitations Many circuits are only linear over a certain range of values, thus the Thévenin equivalent is valid only within this linear range. The Thévenin equivalent has an equivalent I -- V characteristic only from the point of view of the load. The power dissipation of the Thévenin equivalent is not necessarily identical to the power dissipation of the real system. However, the power dissipated by an external resistor between the two output terminals is the same regardless of how the internal circuit is implemented. A proof of the theorem The proof involves two steps. The first step is to use superposition theorem to construct a solution. Then, uniqueness theorem is employed to show that the obtained solution is unique. It is noted that the second step is usually implied in literature. 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 V = V E q − Z E q I. ( displaystyle V = V_ ( mathrm ( Eq ) ) - Z_ ( mathrm ( Eq ) ) I. ) 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. The above expression is obtained by using the fact that the voltage of the black box for a given current I ( displaystyle I ) is identical to the linear superposition of the solutions of the following problems : ( 1 ) to leave the black box open circuited but activate individual voltage source one at a time and, ( 2 ) to short circuit all the voltage sources but feed the circuit with a certain ideal voltage source so that the resulting current exactly reads I ( displaystyle I ) ( Alternatively, one can use an ideal current source of current I ( displaystyle I ) ). Moreover, it is straightforward to show that V E q ( displaystyle V_ ( mathrm ( Eq ) ) ) and Z E q ( displaystyle Z_ ( mathrm ( Eq ) ) ) are the single voltage source and the single series resistor in question. As a matter of fact, the above relation between V ( displaystyle V ) and I ( displaystyle I ) is established by superposition of some particular configurations. Now, the uniqueness theorem guarantees that the result is general. To be specific, there is one and only one value of V ( displaystyle V ) once the value of I ( displaystyle I ) is given. In other words, the above relation holds true independent of what the `` black box '' is plugged to. See also Millman 's theorem Source transformation Superposition theorem Norton 's theorem Maximum power transfer theorem Extra element theorem References Jump up ^ Helmholtz Jump up ^ Thévenin ( 1883a ) Jump up ^ Thévenin ( 1883b ) Jump up ^ Johnson ( 2003a ) Jump up ^ Brittain ^ Jump up to : Dorf Jump up ^ Brenner Jump up ^ Elgerd Jump up ^ Dwight Bibliography Brenner, Egon ; Javid, Mansour ( 1959 ). `` Chapter 12 - Network Functions ''. Analysis of Electric Circuits. McGraw - Hill. pp. 268 -- 269. Brittain, J.E. ( March 1990 ). `` Thevenin 's theorem ''. IEEE Spectrum. 27 ( 3 ) : 42. doi : 10.1109 / 6.48845. Retrieved 1 February 2013. Dorf, Richard C. ; Svoboda, James A. ( 2010 ). `` Chapter 5 - Circuit Theorems ''. Introduction to Electric Circuits ( 8th ed. ). Hoboken, NJ : John Wiley & Sons. pp. 162 -- 207. ISBN 978 - 0 - 470 - 52157 - 1. Dwight, Herbert B. ( 1949 ). `` Sec. 2 - Electric and Magnetic Circuits ''. In Knowlton, A.E. Standard Handbook for Electrical Engineers ( 8th ed. ). McGraw - Hill. p. 26. Elgerd, Olle I. ( 2007 ). `` Chapter 10, Energy System Transients - Surge Phenomena and Symmetrical Fault Analysis ''. Electric Energy Systems Theory : An Introduction. Tata McGraw - Hill. pp. 402 -- 429. ISBN 978 - 0070192300. Helmholtz, H. ( 1853 ). `` Über einige Gesetze der Vertheilung elektrischer Ströme in körperlichen Leitern mit Anwendung auf die thierisch - elektrischen Versuche ( Some laws concerning the distribution of electrical currents in conductors with applications to experiments on animal electricity ) ''. Annalen der Physik und Chemie. 89 ( 6 ) : 211 -- 233. Johnson, D.H. ( 2003a ). `` Origins of the equivalent circuit concept : the voltage - source equivalent '' ( PDF ). Proceedings of the IEEE. 91 ( 4 ) : 636 -- 640. doi : 10.1109 / JPROC. 2003.811716. Johnson, D.H. ( 2003b ). `` Origins of the equivalent circuit concept : the current - source equivalent '' ( PDF ). Proceedings of the IEEE. 91 ( 5 ) : 817 -- 821. doi : 10.1109 / JPROC. 2003.811795. Thévenin, L. ( 1883a ). `` Extension de la loi d'Ohm aux circuits électromoteurs complexes ( Extension of Ohm 's law to complex electromotive circuits ) ''. Annales Télégraphiques. 3 series. 10 : 222 -- 224. Thévenin, L. ( 1883b ). `` Sur un nouveau théorème d'électricité dynamique ( On a new theorem of dynamic electricity ) ''. Comptes rendus hebdomadaires des séances de l'Académie des Sciences. 97 : 159 -- 161. Wenner, F. ( 1926 ). `` Sci. Paper S531, A principle governing the distribution of current in systems of linear conductors ''. Washington, D.C. : Bureau of Standards. External links First - Order Filters : Shortcut via Thévenin Equivalent Source -- showing on p. 4 complex circuit 's Thévenin 's theorem simplication to first - order low - pass filter and associated voltage divider, time constant and gain. Retrieved from `` https://en.wikipedia.org/w/index.php?title= Thévenin % 27s_theorem&oldid = 820564686 '' Categories : Circuit theorems Linear electronic circuits Talk Contents About Wikipedia አማርኛ বাংলা Català Čeština Deutsch Ελληνικά Español Euskara فارسی Français Galego 한국어 हिन्दी Hrvatski Bahasa Indonesia Italiano עברית Magyar മലയാളം Nederlands 日本 語 Polski Português Русский Shqip کوردی Српски / srpski Suomi Svenska Türkçe 中文 23 more Edit links This page was last edited on 15 January 2018, at 10 : 17. Text is available under the Creative Commons Attribution - ShareAlike License ; additional terms may apply. By using this site, you agree to the Terms of Use and Privacy Policy. Wikipedia ® is a registered trademark of the Wikimedia Foundation, Inc., a non-profit organization. About Wikipedia

Question: what is the practical use of thevenin equivalent circuits
Answer: to make circuit analysis simpler and to study a circuit's initial-condition and steady-state response