Do the capacitors always charge exponentially?

In summary: Depending on how it is connected, it could act as a current source, a voltage source, or something in between. It all depends on the specific circuit and how it is designed.
  • #1
Femme_physics
Gold Member
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The way I see it, the more the plates charge, the harder it is to charge them. Therefor capacitors always charge exponentially and linearly. Is that right?
 
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  • #2
It depends on how the capacitor is charged.

If the capacitor is charged from a constant voltage source, it will be charged exponentially as you say.

If the capacitor is charged from a constant current source, it will be charged linearly (as in your recent thread).
The current source will have to work harder and harder to keep its current constant though. ;)

If the capacitor is charged in another way, it will yet be different.
 
  • #3
So since we have a transistor mediating between the voltage source and capacitor (like in my last exercise), that means it charges from a constant current source, yes?
 
  • #4
Femme_physics said:
So since we have a transistor mediating between the voltage source and capacitor (like in my last exercise), that means it charges from a constant current source, yes?

Yes.

It also involves the zener diode that forces the voltage at the base of the BJT (:wink:) to remain constant.
 
  • #5
Capacitors, from every chart I've seen, charge exponentially. Capacitors are reactive and not linear devices, so they charge in a curve, exponential way.

I read above how they can charge linearly with current. This could be right, but I know nothing about this method.
 
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  • #6
remember basic relation for a capacitor: Q = C X V , charge Q = capacitance C X voltage V

so V = Q / C

which would make dV/dt = dQ/dt X 1/C

that should light up the brain cells

If dQ/dt (current) is constant, so is dV/dt (slope of voltage)

so - a capacitor charged by a constant current gives a straight line not exponential.

Observe Voltage would be 1/C X ∫current

and if current's integral is an exponential, that's what voltage will be.

is that any help?


Now draw yourself a simple circuit, battery and resistor and capacitor and switch all in series.
Initial condition is zero volts on cap, and zero current of course 'cause the switch is open..
Now close switch.
Current commences because battery pushes it through resistor
commencing buildup of voltage on cap
which subtracts from voltage across resistor
lowering current
lowering rate of charge
so we have a process whose rate depends on its value
and isn't that the definition of exponential growth?

So your initial statement could be elegant-ized to "Capacitor in series with just resistance charges exponentially . 'Cause that's how Mother Nature designed e^x. "

Pardon my simplistic approach. I have to do such thought exercises myself before i can believe the equations because i make so many math mistakes.
You always ask penetrating questions. I think it belies a very analytical mind.


old jim
 
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  • #7
If you "charge" a capacitor through an inductor, it will charge "sinusoidally", even with a constant voltage source:
[tex]
\mathcal{E} - \frac{Q}{C} - L \, \frac{dI}{dt} = 0
[/tex]
[tex]
I = \frac{dQ}{dt}
[/tex]
[tex]
\ddot{Q} + \frac{1}{L C} \, Q = \frac{\mathcal{E}}{L}
[/tex]
Define:
[tex]
\omega_0 = \frac{1}{\sqrt{L C}}
[/tex]
and the solution, with the inital conditions [itex]Q(0) = 0, I(0) = 0[/itex], is:
[tex]
Q(t) = \mathcal{E} \, C \, \left[1 - \cos \left( \omega_0 \, t \right) \right]
[/tex]
 
  • #8
PS

the more the plates charge, the harder it is to charge them.

Indeed. Just like squeezing a spring.



edit late entry:

indeed the sinewaves are another exponential .

ei t = cos t + i sin t

Euler was one heavy thinking dude !
 
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  • #9
I like Serena said:
It depends on how the capacitor is charged.

If the capacitor is charged from a constant voltage source, it will be charged exponentially as you say.

If the capacitor is charged from a constant current source, it will be charged linearly (as in your recent thread).
The current source will have to work harder and harder to keep its current constant though. ;)

If the capacitor is charged in another way, it will yet be different.

Woa there A constant voltage source has zero source resistance. The capacitor will charge 'instantly' because the voltage across it will suddenly become equal to the supply volts. You must make it clear that a series R is involved if you want to avoid misunderstanding.

If charged with a 'constant current', then Q=CV rules and the voltage across it will increase linearly with time with no limit.
 
  • #10
sophiecentaur said:
Woa there A constant voltage source has zero source resistance. The capacitor will charge 'instantly' because the voltage across it will suddenly become equal to the supply volts. You must make it clear that a series R is involved if you want to avoid misunderstanding.

It's still exponential. :)

In the extreme theoretical case where the resistance is zero, the exponential function turns into a step response.
 
  • #11
I like Serena said:
It's still exponential. :)

In the extreme theoretical case where the resistance is zero, the exponential function turns into a step response.

You said "constant voltage". That has a specific meaning. There are a lot of misunderstanding about this topic and it is essential to be as clear as possible. I try to look at people's posts as if I were a total beginner and see what I could make of them. That's why I am so picky. :smile: They were just that fussy when I was at School and I am eternally grateful.

A step function is not just a very fast exponential function; no time is involved for the transition.
 
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  • #12
Femme_physics said:
So since we have a transistor mediating between the voltage source and capacitor (like in my last exercise), that means it charges from a constant current source, yes?
Only if the transistor is arranged to operate as a constant current source. The transistor circuit could be designed to provide some other characteristic, perhaps something non-linear, so you mustn't assume it to be a constant current source without analysing it.
 
  • #13
Hmm. How would I know if the transistor acts as a constant current source or not?
 
  • #14
Femme_physics said:
Hmm. How would I know if the transistor acts as a constant current source or not?
You would need to look at the circuit or add one that you had designed. What is the exact context of all this? Do you not believe the theory?
If all you want is to verify the theory by looking at waveforms on a scope then use a low voltage (low output resistance source) and a moderately high series resistance or a high voltage and a very high resistance (effectively a current source) to show the extremes. Don't ask what would constitute low or high because it would depend on the capacitor value. Basically, all you are doing is using a shortish time constant for one - so you get a recognisable exponential curve because the volts on the capacitor will go from zero to almost the supply volts - and a very long time constant for the other, which will give you a curve that looks like a straight diagonal line whilst the capacitor volts are low. Of course, when using the high voltage supply, you would need to cut it off when the capacitor volts get too high. If you actually want a good constant current supply then there are tons of circuits available.
 
  • #15
Femme_physics said:
Hmm. How would I know if the transistor acts as a constant current source or not?
You derive equations for its voltages and currents, to establish which variables influence the current charging the capacitor. Just like you did in that other memorable thread. :smile:

If the equation for the charging current involves terms which are fixed and constant (so that means it cannot include a term related to the capacitor's voltage, since that voltage changes as the capacitor charges) then it will be constant current charging.

You don't need to painstakingly analyze every circuit at each encounter. Having thoroughly examined each once or twice, the essential details will remain with you. Honest. :wink:
 
  • #16
Hmm... ok then, I think I understand. But as far as the constant voltage issue from before... I am in basic electronics and we're only working with ideal voltage sources. I'm not sure how can a capacitor charge "instantly" if everything in nature takes time. Even if it's 0.000000000000000000000000000000001 nanosecs
 
  • #17
Well, if you connect an ideal voltage source across an ideal capacitor you have one embarrassing situation. :eek: It's best to think in terms of elements approaching the ideal, and describe the situation accordingly. Leave the ideal for the idealists. :wink:
 
  • #18
Femme_physics said:
Hmm... ok then, I think I understand. But as far as the constant voltage issue from before... I am in basic electronics and we're only working with ideal voltage sources. I'm not sure how can a capacitor charge "instantly" if everything in nature takes time. Even if it's 0.000000000000000000000000000000001 nanosecs

It does not charge instantly if you connect it to an ideal current source. It charges linearly and indefinitely in time, according to:
[tex]
Q = I \, t
[/tex]

EDIT:
As for an ideal voltage source, it ought to charge instantaneously according to:
[tex]
Q = C \, V
[/tex]
But, the electric field inside the capacitor will change as a Heaviside step funciton:
[tex]
E = \frac{V}{d} \, \theta(t)
[/tex]
and the displacement current density is:
[tex]
J_{\mathrm{disp.}} = \frac{\partial D}{\partial t} = \epsilon_0 \, \frac{\partial E}{\partial t} = \frac{\epsilon_{0} \, V}{d} \, \delta(t)
[/tex]
This delta-like displacement current will cause an impule in the magnetic field, which, in turn will cause an induced emf that will oppose the sudden rise of the electric current (Lenz Law).

So, if you do not neglect the displacement current, you will have a finite charge time.
 
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  • #19
I'm not sure how can a capacitor charge "instantly" if everything in nature takes time. Even if it's 0.000000000000000000000000000000001 nanosecs

indeed we wind up with division by zero
so we evaluate its limit instead
that was the fun of freshman calculus...

Dick has brought up self inductance of the space between the plates, i think,,,, but my math isn't that good.

i do know a very fast current pulse has a tremendous magnetic field. In the power plant we noticed effects of lightning stroke on nearby loops of instrument system ground wires.

old jim
 
  • #20
If you charge a capacitor through a smaller and smaller resistor, you'll get something like this.

attachment.php?attachmentid=49057&stc=1&d=1342125120.jpg


The curve comes closer and closer to a so called step response.

When we consider ideal wires, an ideal capacitor, an ideal constant voltage source, and an ideal switch, the graph will ideally be a step response.

But you're right, that's not realistic!
It's just an ideal and abstract approximation of reality.

(There! I included a smiley!)
.
 

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  • #21
Thanks for these references... I'm still not entirely sure how would I figure out what is a current source and what is a voltage source. I only know that a mediating transistor where the collector current loads the capacitor makes it a current source... but what other possible example can there be? Or is there a rule of thumb?
 
  • #22
If you have a symbol in your circuit with the text "current source" next to it, it is also a current source. ;)

Note that your mediating transistor also needs constant voltage between the base and the emitter, before it will behave like a current source.
In your previous threads you have seen a couple of examples of that (for instance a zener diode).

What you need is that the current is the same whether the capacitor is full or empty.
If you can calculate the current in both those cases and it is the same, you have a current source.
 
  • #23
I see.. but what if the zener diode wasn't there?
 
  • #24
Well, for instance a separate voltage source (connected between base and emitter) would also do the trick...
 
  • #25
But if there was only an ideal wire there? Still linear charge?
 
  • #26
My imagination is falling short.
Picture?
 
  • #28
Okay.
So did you calculate Ie and Ic?
 
  • #29
No, because I don't know if it makes sense that they'll give me an exercise like that..but I'm too tired to retrace the data anyway, I should get some sleep before the test :) Although I'm printing some papers for the upcoming 30 mins

Any chance you'll be nice to tell me what's going on here? Pretty please?
 
  • #30
Nice? Nice? NICE?
But... I'M NOT A NICE PERSON!
Rawwr.What papers are you printing?
 
  • #31
Low pass filters, wiki article on logic gates...general official references to have with me, since I can't use google during the test :(
 
  • #32
Yes. It's best to be prepared!Tbh the circuit doesn't look as if it makes much sense.

Since Vb=0, I think Ve will become 0.7V always.
At first the capacitor would charge, up to 0.7V (exponentially), and then it would stop.

So no, not a constant current source.
 
  • #33
In that case I'll just print two of your replies

It depends on how the capacitor is charged.

If the capacitor is charged from a constant voltage source, it will be charged exponentially as you say.

If the capacitor is charged from a constant current source, it will be charged linearly (as in your recent thread).
The current source will have to work harder and harder to keep its current constant though. ;)

If the capacitor is charged in another way, it will yet be different.

If you have a symbol in your circuit with the text "current source" next to it, it is also a current source. ;)

Note that your mediating transistor also needs constant voltage between the base and the emitter, before it will behave like a current source.
In your previous threads you have seen a couple of examples of that (for instance a zener diode).

What you need is that the current is the same whether the capacitor is full or empty.
If you can calculate the current in both those cases and it is the same, you have a current source.

Should do the job :) thanks
 
  • #34
Don't forget to trust your visual cues! ;)
 
  • #35
Good point!
 

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