Natural frequency, measured in terms of eigenfrequency, is the rate at which an oscillatory system tends to oscillate in the absence of disturbance. A foundational example pertains to simple harmonic oscillators, such as an idealized spring with no energy loss wherein the system exhibits constant-amplitude oscillations with a constant frequency. The phenomenon of resonance occurs when a forced vibration matches a system's natural frequency.
In analysis of systems, it is convenient to use the angular frequency rather than the frequency f, or the complex frequency domain parameter .
In a mass–spring system, with mass m and spring stiffness k, the natural angular frequency can be calculated as:
In an electrical network, ω is a natural angular frequency of a response function f( t) if the Laplace transform F( s) of f( t) includes the term , where for a real σ, and is a constant. Natural frequencies depend on network topology and element values but not their input. It can be shown that the set of natural frequencies in a network can be obtained by calculating the poles of all impedance and admittance functions of the network. A pole of the network transfer function is associated with a natural angular frequencies of the corresponding response variable; however there may exist some natural angular frequency that does not correspond to a pole of the network function. These happen at some special initial states.
In LC circuit and RLC circuits, its natural angular frequency can be calculated as:
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