Reciprocity Theorem
Reciprocity Theorem (Voltage and Current) formulas
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\( \dfrac{ V_1 }{ I_2 } \;=\; \dfrac{ V_2 }{ I_1 } \) | ||
Symbol | English | Metric |
\( V_1 \) = Voltage Source 1 | \(V\) | \(V\) |
\( I_2 \) = Current Produced at One Point | \(A\) | \(A\) |
\( V_2 \) = Voltage Source 2 | \(V\) | \(V\) |
\( I_1 \) = Current Produced at One Point | \(A\) | \(A\) |
Reciprocity theorem is a principle in electrical engineering and circuit theory that applies to linear, bilateral, and time-invariant networks. It states that in such a network, the ratio of a response (such as voltage or current) at one point to an excitation (such as a voltage or current source) at another point remains the same if the positions of the excitation and response are interchanged, provided the network contains only linear and bilateral components.
In simpler terms, if a voltage source at one location produces a specific current at another location, then placing the same voltage source at the second location will produce the same current at the first location. This theorem is rooted in the symmetry of Maxwell’s equations and is widely used in analyzing electrical circuits, antennas, and other systems to simplify calculations and understand mutual interactions.
Reciprocity Theorem (Impedance) formulas
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\( Z_{12} \;=\; Z_{21} \) | ||
Symbol | English | Metric |
\( Z_{12} \) = Impedance from Port 1 | \(V\) | \(V\) |
\( Z_{21} \) = Impedance from Port 2 | \(A\) | \(A\) |
The reciprocity theorem in electrical circuit theory doesn't have a single, specific formula but is expressed as a principle about the interchangeability of excitation and response in a linear, bilateral, time-invariant network.