Fair enough.
But it is very simple, actually. You just have to forget about those pulses. They have very little to do with an AC circuit (except that they are a special case of the transient solution to the differential equations describing a series resonant circuit). But that, you have to leave for a little later, when you have undserstood the steady state AC solution.
So, here goes:
You have an inductor and a capacitor connected in series. Fed from an AC voltage source. Right?
There is a current flowing through this circuit. An AC current of a certain amperage. Say I amps. Right?
Now (vector diagram needed) draw one thick arrow from a point from center of a paper to the right. Make it about four inches (ten cm) long. This represents the current. Let's say it is 4 amperes.
As you know. Voltage across an inductor leads current by 90 degrees. Right? Then draw a new arrow pointing from center of paper (where current arrow starts) vertically upwards. Done?
This arrow represents the voltage across the inductor. The phase rotation in a vector diagram is always CCW. So, a leading vector is drawn 90 degrees CCW from the reference vector (the current arrow).
Now. You have half the picture. Any questions? Yes? Ah! If these arrows represent amplitude or RMS? Good question. Well, lets say for now that they represent amplitudes. More on that later.
Look at the circuit diagram. You have two elements (inductor and capacitor) in series. Voltages across the two elements sum (just like the voltage of two batteries sum). So, now you have to add the capacitor voltage to the inductor voltage. In other words, draw a new arrow (representing capacitor voltage) from the inductor voltage arrow tip.
Just one little step left for you now. Are you OK so far? Good.
As you already know (see, you actually knew all these things already!) the capacitor voltage lags the current. So, the capacitor voltage arrow shall be pointing downwards, parallel to the inductive voltage, but in opposite direction. Do that! Yes! from the top of the inductor voltage downwards.
Yes, that means going back towards where it all started.
How long? That depends. Let's say about half-way down the inductor voltage arrow.
Now, when you look at this diagram, you see a reference arrow going to the right, a voltage arrow going up and another voltage arrow going down. The sum of the voltage arrows is the distance from starting point to the tip of the down-pointing arrow. Got it? Good. What's that you said? Yes, right. This is the voltage across the circuit.
Now, resonance. That is when you have equal impedance in inductor and capacitor. Yes, same voltage drop across capacitor as across inductor. BUT DIFFERENT DIRECTIONS!
So, if you make the capacitor voltage longer. Same length as inductor voltage. What do you get? What? Nothing? Oh, yes. You mean there's no distance left between starting point and tip of capacitor voltage? Yes, that's right! No voltage across the circuit!
That is what resonance is about. Current but no voltage, Z = U/I so you have also zero impedance. Got it?
It wasn't that hard. Was it?
This is essentially what the text-books say. Only with fewer words.
There may be quite a few typos in this. I didn't have energy left to proof-read it.
Gunnar Englund
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100 % recycled posting: Electrons, ideas, finger-tips have been used over and over again...