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I've read many times some statements about resonators like this (reference):

Resonant circuits are circuits, which offers a high impedance or low impedance (for parallel and series resonance respectively) to the source at a particular frequency of operation. The frequency at which the resonant circuit has a very high or low impedance is called its resonant frequency.The frequency selectivity property of resonant circuits are exploited in building filter circuits

1) It's a basic concept that is written everywhere, but I cannot understand in practice how resonators may filter an input signal. Precisely, let's consider a parallel RLC circuit:

enter image description here

It may represents different kinds of resonators. It's simple to find that the input impedance of the parallel RLC circuit which represents the resonator is the following one (in terms of real and imaginary parts):

enter image description here

If we look at the graph, I understand the initial statement: this graph is very frequency - selective.

But let's look at the RLC circuit: what does it filter? There is an input voltage signal. If I take the voltage across one of RLC components, it will be the same of the source. I'd say that this circuit, given an input voltage signal, gives an output filtered current. So, how should I read this filtered current (from a circuital point of view).

2) What If the parallel RLC circuit is only a model (not a real circuit) of a cavity/waveguide resonator (i.e. a closed tube of metal in which there is my electromagnetic source)? My electromagnetic source (consider a simple antenna) generates an EM field with some frequencies, and the cavity selects only specific frequency. How may I read the filtered signal?

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  • \$\begingroup\$ The voltage is understood to have an internal resistance/impedance, so the equivalent Thevenin circuit of the source, together with the equivalent impedance of the parallel RLC network, will form a voltage divider, with the probe across the equivalent Z of the RLC. What you see in the picture is conceptual, more than strictly physical. \$\endgroup\$ Commented Jan 3, 2021 at 21:19

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The circuit you show isn't a useful filter. The current from the voltage source is nicely bandpass filtered, but in the real world that's not terribly useful.

A useful model for an RF filter would be something like this, with a source that has a real source impedance (represented by R1), and a load that also has some real impedance, not to mention that the inductance will come with its own bit of effective impedance. This should have a band-pass characteristic, with the center frequency of the filter determined mostly by the values of L and C and it's width determined by L, C, and the resistances.

schematic

simulate this circuit – Schematic created using CircuitLab

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