oh_well1500
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Indeed - the confusion arises from a lack of engineering knowledge, resonant systems can have currents and voltages higher than the supplying circuit quite easily due to the physics involved.What is confusing me FvM, is I built the circuit, with a 12.8 mH inductor, in parallel with a capacitor bank of 550 uF, and I am measuring 60 amps on the cap bank line, 60 amps on the inductor line, and 20 amps on the input current before the node.
No. It's a voltage driven resonator. I = V/X.I fear FvM has missed the point - if you have L & C of a similar size to above but the L is sized for resonance at 60Hz then the currents in the L & C will be " Q " times the current to the parallel pair - even for a Q of 4 -5 this will cook the L & C very quickly.
I fear you are ignoring the Z of the lines back to the transformer . . . very few things are purely volt driven - and even then it doesn't matter - if there is any current to the parallel pair ( 60 Hz resonant ) then there will be Q times this inside the LC.No. It's a voltage driven resonator. I = V/X.
Sure. But current "inside LC" is V/X and not dependant on Q as long as V is near to nominal grid voltage.if there is any current to the parallel pair ( 60 Hz resonant ) then there will be Q times this inside the LC.
I think you're confusing parallel and series resonant circuits. What FvM (and I think everyone else) is proposing is a parallel inductor. For parallel LC circuits, Q=R*sqrt(C/L), where R is the resistance of the drive source. For typical AC mains, R will be so low as to completely dampen the resonance. Even with a relatively high R of 0.5ohm, you'd get Q=0.5*sqrt(550e-6/12.8e-3)=0.10, and that's assuming the L and C themselves are perfectly lossless.I fear FvM has missed the point - if you have L & C of a similar size to above but the L is sized for resonance at 60Hz then the currents in the L & C will be " Q " times the current to the parallel pair - even for a Q of 4 -5 this will cook the L & C very quickly.
So - to get a constructive discussion - what needs to be corrected in the simulation of post#27 to show "the problem"?any simple simulation confirms this.
any simple simulation confirms this.
Contradicting statements. I'd appreciated at least a hint which parameters or conditions are missing in the considerations.Ah yes - as said above - it's what you don't see that trips the unsuspecting soul.
Yes, true, we don´t know source side.The problem is we do not know exactly the mains supply Z - it can be a lot more complex than all the assumptions - this regularly catches people out . . .
Where else should they be? ... I mean they need a connection to the phase lines somehow.If there are switchable PFC caps nearby on the 400V 3 phase line
I don´t understand. Is it better outside a building? In the rain?i.e. in a nearby building
This is your assumption. Without proof so far.it can be a lot more complex than all the assumptions
What exactly? Change the color of snow?this can cause very interesting things to happen.
There is a good reason why voltage driven LC parallel resonance also is called "anti resonance".if you have L & C of a similar size to above but the L is sized for resonance at 60Hz then the currents in the L & C will be " Q " times the current to the parallel pair - even for a Q of 4 -5 this will cook the L & C very quickly.
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