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Reciprocity in linear systems is the principle that a response Rab, measured at a ___location (and direction if applicable) a, when the system has an excitation signal applied at a ___location (and direction if applicable) b, is exactly equal to Rba which is the response at ___location b, when that same excitation is applied at a. This applies for all frequencies of the excitation signal. If Hab is the transfer function between a and b then Hab = Hba, if the system is linear.
In the special case of a modal analysis this is known as Maxwell's reciprocity theorem.[1] In electromagnetism the concept is known as Lorentz reciprocity, a special case of which is the reciprocity theorem of electrical networks.
The reciprocity principle is also used in the analysis of structures.[2] When combined with superposition, symmetry and anti-symmetry, it can be used to resolve complex load conditions.
References
edit- ^ "Experimental modal analysis" (PDF). Archived from the original (PDF) on 2008-09-07.
- ^ Benaroya, Haym (2004). Mechanical Vibration: Analysis, Uncertainties, and Control. CRC Press. ISBN 9780824753801.