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Reciprocity theorem is a fundamental principle in electrical engineering that relates to the behaviour of linear, passive, and bilateral circuits. It states that the ratio of the voltage across a given element to the current through another element in a circuit remains unchanged when the positions of these elements are interchanged. In simpler terms, the reciprocity theorem states that if we have two points in a circuit, say A and B, and we apply a voltage at point A and measure the current at point B, the result will be the same as if we apply the same voltage at point B and measure the current at point A. The reciprocity theorem is a fundamental concept in electrical engineering that establishes a relationship between the electromagnetic fields produced by two sources.
The reciprocity theorem says that in any linear and bilateral network or circuit with one independent source, the response to excitation stays the same even if you swap the source from the input to the output terminals. Since we deal with both voltage and current, this can be seen in four different ways, depending on whether you use voltage or current for excitation and response. This theorem only works for single-source networks and circuits that include dependent sources. It's valid for almost all passive networks and reflects a broader principle of reciprocity in electromagnetism.
This detailed blog will apprise readers of the reciprocity theorem and its applications. This topic is important for upcoming examinations pertaining to Electrical engineering, including SSC JE, GATE Electrical Exam, etc.
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The reciprocity theorem is a fundamental concept in electrical engineering that relates the electromagnetic fields generated by two sources. It states that the ratio of the voltage across a given element to the current through another element in a circuit remains unchanged when the positions of these elements are interchanged.
In terms of electromagnetism it states that the ratio of the electric field produced by one source at a point in space to the current generated by another source at the same point is equal to the ratio of the electric field produced by the second source at the original location of the first source to the current generated by the first source at its own location. This theorem is based on the principle of electromagnetic wave superposition, which states that the total electric field at a given point is the sum of the electric fields produced by all sources in the vicinity. In simpler terms, it means that if we have two sources, the electric field produced by one source at a particular location is the same as the electric field produced by the other source at the same location, but with the sources swapped.
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The reciprocity theorem has various practical applications in the field of electrical engineering. Some notable applications include:
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The reciprocity theorem can be applied to electric circuits, allowing engineers to analyse the behaviour and characteristics of the circuit. Here's how the reciprocity theorem applies to an electric circuit:
In this modified circuit, we have swapped the positions of the input voltage and output current. Now, VS represents the input voltage and current, and the response or output current is denoted by I, which flows through the resistor R1.
In the first circuit, the current flowing through resistor R3 is equal to the current flowing through resistor R1 in the second circuit. This is because the magnitude and polarities of the voltage, VS, are the same in both circuits, and the direction of the output current is also the same in both circuits.
The reciprocity theorem can also be applied to a 2-port network, which is a common component in electrical systems. Here's how the reciprocity theorem applies to a 2-port network:
While the reciprocity theorem is a valuable concept in electrical engineering, it does have certain limitations. Here are a few notable limitations:
The reciprocity theorem has several practical uses in electrical engineering. Here are some notable applications:
Consider two antennas, Antenna A and Antenna B, separated by a distance of \(d\) meters. When Antenna A transmits a power of \(P_1\) watts, the power received by Antenna B is given by the Reciprocity Theorem as the power received by Antenna A when Antenna B transmits the same power. The formula for power received \(P_{\text{received}}\) is given by:
\[P_{\text{received}} = \frac{P_1 \cdot G_{\text{A}} \cdot G_{\text{B}} \cdot \lambda^2}{(4 \pi)^2 \cdot d^2}\]
where \(G_{\text{A}}\) and \(G_{\text{B}}\) are the gains of Antenna A and Antenna B, respectively, and \(\lambda\) is the wavelength.
Given values:
\(P_1 = 100\) W
\(G_{\text{A}} = 4\) (in decibels)
\(G_{\text{B}} = 6\) (in decibels)
\(d = 10\) m
\(\lambda = 2\) m
To find \(P_{\text{received}}\):
\[P_{\text{received}} = \frac{P_1 \cdot G_{\text{A}} \cdot G_{\text{B}} \cdot \lambda^2}{(4 \pi)^2 \cdot d^2} = \frac{100 \cdot 10^{\left(\frac{4}{10}\right)} \cdot 10^{\left(\frac{6}{10}\right)} \cdot 2^2}{(4 \pi)^2 \cdot 10^2} = \frac{100 \cdot 2 \cdot 4}{(4 \pi)^2} \approx 0.509\) W
Hence, \(P_{\text{received}} \approx 0.509\) W.
Given values:
\[P_1 = 100 \, \text{W}\]
\[G_{\text{A}} = 4 \, \text{(in decibels)}\]
\[G_{\text{B}} = 6 \, \text{(in decibels)}\]
\[d = 10 \, \text{m}\]
\[\lambda = 2 \, \text{m}\]
To find: \(P_{\text{received}}\):
\[P_{\text{received}} = \frac{P_1 \cdot G_{\text{A}} \cdot G_{\text{B}} \cdot \lambda^2}{(4 \pi)^2 \cdot d^2} = \frac{100 \cdot 10^{\left(\frac{4}{10}\right)} \cdot 10^{\left(\frac{6}{10}\right)} \cdot 2^2}{(4 \pi)^2 \cdot 10^2} = \frac{100 \cdot 2 \cdot 4}{(4 \pi)^2} \approx 0.509 \, \text{W}\]
Hence, \(P_{\text{received}} \approx 0.509 \, \text{W}\).
Within the purview of this discussion, we covered the exam-oriented details about Reciprocity theorem and its applications in Electrical Engineering. If you are preparing for State and Central level Electrical examinations, get enrolled in AE/JE Electrical Coaching on the Testbook App.
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