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Thevenin's and Norton's Theorems: Simplifying Complex Circuits, Lecture notes of Physics Fundamentals

Thevenin's and norton's theorems, which are used to simplify complex electrical circuits. The theorems allow reducing a network to an equivalent circuit containing a single voltage or current source and resistances. Examples and instructions on how to find thevenin's equivalent circuit and norton's equivalent source.

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2018/2019

Uploaded on 09/18/2019

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Download Thevenin's and Norton's Theorems: Simplifying Complex Circuits and more Lecture notes Physics Fundamentals in PDF only on Docsity! LECTURE # Theveninโ€™s Theorem is a network analysis procedure meant to simplify the computations of a complex network (with several sources and resistances). It does so by reducing a complex network to simple equivalent circuit (Theveninโ€™s Equivalent Circuit) containing a Single Voltage Source in series with a two Resistances. Whereby: The voltage source is the open circuit voltage measured between terminals where its required to determine the current One of the resistors is the Theveninโ€™s equivalent resistance, measured between terminals (where its required to compute current) in a passive circuit While the other resistance represents the load resistance (connected between terminals where its required to find current). Theveninโ€™ s Theorem ย  Active Network with linear Sources and Resistances resistance Rth ย  ๐ดย  ๐ตย  ๐‘น๐‘ณย  ๐‘ฌ๐’•๐’‰ย  ๐‘จย  ๐‘น๐’•๐’‰ย  Equivalent Source, then its possible to determine the Load current, i.e. current between terminals A & B ย  ๐ธ h๐‘กh โˆ’๐‘‡h๐‘’๐‘ฃ๐‘’๐‘›๐‘–๐‘›โ€ฒ ๐‘ ๐‘‰๐‘œ๐‘™๐‘กh๐‘Ž๐‘”๐‘’ย  ย  ๐‘‡h๐‘’๐‘ฃ๐‘’๐‘›๐‘–๐‘›โ€ฒ ๐‘ ๐ธ๐‘ž๐‘ข๐‘–๐‘ฃ๐‘Ž๐‘™๐‘’๐‘›๐‘กh ๐‘†๐‘œ๐‘ข๐‘Ÿ๐‘๐‘’ย  ๐‘ฐ ๐‘ณย  ๐‘น๐‘ณย  ๐‘ฉย  ๐‘น๐‘ณโˆ’๐‘น๐’†๐’”๐’Š๐’”๐’•๐’‚๐’๐’„๐’†๐’๐’‡ ๐’•๐’‰๐’†๐’ƒ๐’“๐’‚๐’๐’„๐’‰๐’˜๐’‰๐’†๐’“๐’†๐’Š๐’•๐’” ๐’“๐’†๐’’๐’–๐’Š๐’“๐’†๐’… ๐’•๐’๐’…๐’†๐’•๐’†๐’“๐’Ž๐’Š๐’๐’†๐’„๐’–๐’“๐’“๐’†๐’๐’•ย  Example # ๐ธย  ๐‘…1ย  ๐ท๐‘’๐‘กh๐‘’๐‘Ÿ๐‘š๐‘–๐‘›๐‘’๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘กh h๐‘กhh๐‘Ÿ๐‘œ๐‘ข๐‘” ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘กh๐‘Ž๐‘›๐‘๐‘’๐‘…2๐‘ข๐‘ ๐‘–๐‘›๐‘”๐‘‡h๐‘’๐‘ฃ๐‘’๐‘›๐‘–๐‘› โ€ฒ ๐‘ ๐‘‡h๐‘’๐‘œ๐‘Ÿ๐‘’๐‘šย  ๐‘น๐Ÿ‘ย ๐‘น๐Ÿย  ๐‘…1=4โ„ฆย  ๐‘…2=8โ„ฆย  ๐‘Ÿ ๐‘–=1โ„ฆย  ๐‘…3=6โ„ฆย  ๐ธ=24๐‘‰ย  ๐‘น๐Ÿ’ย  ๐ท๐‘’๐‘กh๐‘’๐‘Ÿ๐‘š๐‘–๐‘›๐‘’๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘กh h๐‘กhh๐‘Ÿ๐‘œ๐‘ข๐‘” ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘กh๐‘Ž๐‘›๐‘๐‘’๐‘…2๐‘ข๐‘ ๐‘–๐‘›๐‘”๐‘‡h๐‘’๐‘ฃ๐‘’๐‘›๐‘–๐‘› โ€ฒ ๐‘ ๐‘‡h๐‘’๐‘œ๐‘Ÿ๐‘’๐‘šย  LECTURE # Nortonโ€™s Theorem ๐‘ฐ ๐‘ณย  ๐‘ฌย  ๐‘น๐Ÿ‘ย  ๐‘น๐Ÿ’ย  ๐‘น๐Ÿ“ย  ๐‘น๐Ÿ”ย  ๐‘น๐Ÿย  ๐‘น๐Ÿย  ๐‘ฐ ๐‘จย  ๐‘น๐Ÿ=๐‘น๐Ÿ’=๐‘น๐Ÿ”=๐Ÿ’โ„ฆย ๐‘น๐Ÿ=โˆžโ„ฆย  ๐‘น๐Ÿ‘=๐Ÿ”โ„ฆย  ๐‘น๐Ÿ“=๐Ÿโ„ฆย  ๐‘ฌ=๐Ÿ’๐ŸŽ๐‘ฝย  ๐‘ฐ ๐‘จ=๐Ÿ– ๐‘จย  Example # V3=? R1 IA E1 R3 R2 R4 ๐‘น๐Ÿ=๐‘น๐Ÿ’=๐Ÿโ„ฆย  ๐‘น๐Ÿ=๐Ÿ’โ„ฆ,๐‘น๐Ÿ’=๐Ÿ‘โ„ฆย  ๐‘ฌ๐Ÿ=๐Ÿ๐Ÿ”๐‘ฝย ๐‘ฐ ๐‘จ=๐Ÿ– ๐‘จย  Example # 2 ๐ธย  ๐‘…1ย  ๐ท๐‘’๐‘กh๐‘’๐‘Ÿ๐‘š๐‘–๐‘›๐‘’๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘กh h๐‘กhh๐‘Ÿ๐‘œ๐‘ข๐‘” ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘กh๐‘Ž๐‘›๐‘๐‘’๐‘…2๐‘ข๐‘ ๐‘–๐‘›๐‘”๐‘๐‘œ๐‘Ÿ๐‘กh๐‘œ๐‘›โ€ฒ ๐‘ ๐‘‡h๐‘’๐‘œ๐‘Ÿ๐‘’๐‘šย  ๐‘น๐Ÿ‘ย ๐‘น๐Ÿย  ๐‘…1=4โ„ฆย  ๐‘…2=8โ„ฆย  ๐‘Ÿ ๐‘–=1โ„ฆย  ๐‘…3=6โ„ฆย  ๐ธ=24๐‘‰ย  ๐‘น๐Ÿ’ย  ๐ท๐‘’๐‘กh๐‘’๐‘Ÿ๐‘š๐‘–๐‘›๐‘’๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘กh h๐‘กhh๐‘Ÿ๐‘œ๐‘ข๐‘” ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘กh๐‘Ž๐‘›๐‘๐‘’๐‘…2๐‘ข๐‘ ๐‘–๐‘›๐‘”๐‘๐‘œ๐‘Ÿ๐‘กh๐‘œ๐‘›โ€ฒ ๐‘ ๐‘‡h๐‘’๐‘œ๐‘Ÿ๐‘’๐‘šย  ๐‘…4=6โ„ฆย  Example # R1 R4 ๐‘น๐Ÿ=๐‘น3=๐Ÿโ„ฆย  ๐‘น๐Ÿ=๐Ÿ’โ„ฆ,๐‘น๐Ÿ’=๐Ÿ‘โ„ฆย  ๐‘ฌ๐Ÿ=๐Ÿ๐Ÿ”๐‘ฝย ๐‘ฐ ๐‘จ=๐Ÿ– ๐‘จย  R3 R2 E1 V4=? ๐’“=๐Ÿโ„ฆย  Example # ๐‘น๐Ÿ=๐‘น๐Ÿ‘=๐Ÿโ„ฆย  ๐‘น๐Ÿ=๐Ÿ’โ„ฆ,๐‘น๐Ÿ’=๐Ÿ‘โ„ฆย  ๐‘ฐ ๐‘จ=๐Ÿ– ๐‘จย  R1 R3 R2 R4IA V4=? ๐‘ฐ ๐’”๐’„ย  ๐‘น๐‘ตย  ๐‘ฐ ๐‘ณย 
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