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Curious case of the charging capacitor

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rstofer:
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/capeng2.html#c4

T3sl4co1l:
The lesson is this: a real physical circuit has R, L and C elements.  The voltage source* and capacitor circuit is a fiction, adequate to explore conservation of charge, but completely inadequate for any other aspect -- such as time or frequency behavior, or energy or power balance.

*Or capacitors of different charge, or any combination.  Two capacitors in series, with some initial voltage on one, is equivalent to one capacitor of series equivalent value, plus one voltage source equal to the difference in initial voltages. :)

The case with just L and C (no D) is actually identical to the C and C case, if you separate the solution properly:

With no D, of course, the resonant wave continues on forever -- the diode simply stops it at a convenient point, turning the resonant energy into potential energy (capacitor final voltage and charge).  If we leave it resonate instead, then we have a mean value on the capacitor, equal to the voltage source, and therefore the mean charge as well.  And if we look at the energy in the capacitor, it's also oscillating up and down, with the average equal to the half charge value.  Presto -- we've separated the energy components into a oscillating component, and a static component!  The oscillating component, obviously, has equal energy -- it's oscillating up and down with amplitude equal to the average.  If we calculate the energy of that sine wave by itself (Parseval's theorem), we find the same answer again.

Incidentally, if you try simulating this, you may find the sine wave grows or shrinks over time, even with all components carefully set to zero ohms resistance.  This is a consequence of numerical stability: it's very hard to calculate something with quite that much accuracy, when you're doing it incrementally, one tiny step at a time!  This isn't a bad illustration of it actually, and getting a feel for how it varies with the various TOL parameters, and integration method (simulation settings).

Tim

IanB:

--- Quote from: ZeroResistance on February 20, 2019, 05:25:56 am ---I'm going to revisit the classic capacitor charging case, which I just came across

1. Is it true that half the energy fed by the power supply in charging the capacitor is lost, I mean if 100uJ is supplied by the power supply of 10VDC, finally the energy stored in the capacitor @ 10VDC would only be 50uJ.
If this is true can charging a capacitor be considered inefficient?
Following on are there efficient ways charging a capacitor?

2. This case is of charging a capacitor with another capacitor. Eg. If I have a 1uF capacitor charged to 10VDC and another 1uF capacitor uncharged. If I connect both of these in parallel the final derived energy is again half the energy that we started off with. So where did the other half go?
And if this is true then how come charge pumps achieve high efficiencies?

On subsequent searches I also found several posts indicating that this is likely due to energy loss in the resistance
wires.

I would like to hear the views of the learned audience at eevblog on this subject.

TIA

PS: Would the above cases still be true if the capacitor was charged with constant current?

--- End quote ---

I posted this a while back. It was something curious to me at the time:

https://www.eevblog.com/forum/projects/why-trying-to-store-energy-in-a-capacitor-can-be-less-efficient-than-you-think/

About resonance, if the series resistance is large enough the system will be over damped and oscillations will be quenched. Then the simple analysis becomes (more) valid.

Jwillis:
Voltage doubler/multiplier work by taking the peek to peek AC current and charging two capacitors one positive and one negative .This is done with diodes one diode directs the first 0 to 180 degree half cycle of the  AC  positive to one capacitor and the second diode directs 180 to 360 degree half cycle of The AC    to the second capacitor. For example you have 5 volts AC supply , one capacitor  is charged to  +5 volts from the first half cycle .the other capacitor is charged - 5 volts from the second half of AC cycle . As one is being charged the other is being discharged. The quantitative addition  of positive  5 volts and negative 5 volts is 10 volts . Add another diode and capacitor (Tripler) adds another 5 volts for 15 volts total so on and so on. But as your voltage increases at the out the available current at output halves  in a doubler and is 1/3 rd for a tripler. So if your available current is 1 amp at the AC source only 0.5 amps is available  after the doubler and 0.3 amps available after a tripler .  But that's in a perfect world condition.Actual available current and voltage  will be much different than expected  due to combined losses of capacitor reactance and voltage drops across the diodes. Also Reactance is directly proportional to frequency but for the sake of simplicity I didn't include that relationship.

Models tend to fail because they assume a zero resistance between the voltage source and in the capacitor.But the reality is resistance is there however small it may be .Look at the the time constant  T=R X C .If the resistance (including the resistance of the capacitor) always remains zero ,charge would also remain zero.This can be verified with  Kirchhoff’s voltage law Vs - R x I(t) - Vc .Capacitor would remain a dead short.

not1xor1:

--- Quote from: Doc Daneeka on February 20, 2019, 06:10:39 am ---Yes in a real circuit the energy goes into the resistance. As soon as you add a resistor to the model there is no problem and the model works perfectly

--- End quote ---

in the real world part of the energy (how much depends on the features of the circuit) is also radiated as EM waves

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