Continue to Site

Welcome to EDAboard.com

Welcome to our site! EDAboard.com is an international Electronics Discussion Forum focused on EDA software, circuits, schematics, books, theory, papers, asic, pld, 8051, DSP, Network, RF, Analog Design, PCB, Service Manuals... and a whole lot more! To participate you need to register. Registration is free. Click here to register now.

Capacitor charging/discharging equation, maths

Status
Not open for further replies.

drk15

Newbie level 3
Joined
Oct 9, 2012
Messages
4
Helped
0
Reputation
0
Reaction score
0
Trophy points
1,281
Activity points
1,315
Hello,
Can anybody explain me the capacitor charge/discharge equation derivation in detail?
Places I check, they start at either complicated point or in other easier version, some of the steps are omitted.

Any pointers/ links will be helpful too.

Thanks.
 

Places I check, they start at either complicated point or in other easier version, some of the steps are omitted.

Better you give the link reference and pinpoint what exactly you did not understand, instead of raising an open ended question.
 

Places I check, they start at either complicated point or in other easier version, some of the steps are omitted

Please cite a reference so that we can start with a starting point; otherwise I will have to draw some diagrams to begin...

-Begin at the beginning and go on till you come to the end; then stop- Lewis Caroll
 

The mathematical constant e is in the formula. I experimented with a graphing program until I found that the equation below creates a plot which resembles the classic discharge graph. It assumes time constant=1.
V starts at 1V.
0.368 = 1/e.

V = 0.368 ^ t

After 5 seconds (5 time constants) the capacitor is nearly discharged, as according to convention.
 

    V

    Points: 2
    Helpful Answer Positive Rating
After 5 seconds (5 time constants) the capacitor is nearly discharged, as according to convention.

Another interesting concept is the half-time; this is the time needed for the voltage to drop by 50%. In the example above, you will have voltage reduce by 50% after 0.6931 secs. This number is ln(2) and also crops up when you expect it the least.
 
  • Like
Reactions: BradtheRad

    V

    Points: 2
    Helpful Answer Positive Rating

    BradtheRad

    Points: 2
    Helpful Answer Positive Rating
If the OP had shown few more interest in this issue since the opening of the thread, we could also explore the similarity among mathermatical models of different physical phenomens, for example understanding the discharge of the capacitor as the discharge of a fluid, which flows with more intensity as more charged is the deposit of liquid. The fact is that certain concepts have to be acquired intuitively before one proceed to learn something few palpable to human senses, such as the electric current.
 
Can anybody explain me the capacitor charge/discharge equation derivation in detail...

I do not know how much detail you want, but I can try.

I am not drawing a diagram and you need to have a diagram to get most out of this description...

1. Consider a power supply (battery) of const voltage V and zero internal resistance; it can supply infinite current.

2. We have resistor of resistance R connected in series with a capacitor of capacitance C. The positive end of the battery is connected to the resistor via a switch and the free end of the capacitor is connected to the negative end of the battery.

3. Set up initial conditions: at time t=0, the capacitor has no potential across it and the switch is closed.

4. Now consider the case at time t; the current is i(t) and the voltage is v(t). The total voltage across the circuit is V=i(t).R + v(t); v(t) is the voltage across the capacitor.

5. Capacitor formula is C=dQ/dV; or CdV=dQ; also dQ=i(t)dt; therefore CdV=i(t)dt; The voltage across the capacitor will be then integral (1/C)(i(t)dt) with limit from 0 to t. Put this in the previous equation.

6. Hence is final equation is V= V(t) + (1/RC)(dV(t)/dt)

7. This equation is a simple differential equation and can be solved easily.
 

Hello,
Thanks you all for your responses.
here is more on my question.

I am going through this(attachment)

I dont get how it goes to vN(t) = K e -t/RC step.

Thank you
 

Attachments

  • rc.png
    rc.png
    160.7 KB · Views: 123

If you are clear about the previous step, then it is simple. Rearrange the equation to get:

RC dV/dt=-V; more rearragement and you get : (dV/dt)/V=-(1/RC); or dV/V=-(1/RC)dt; then integrate to obtain: ln(V)=-t/(RC); or V=V(0) exp(-t/RC)
 

Thank you very much. It is clear now. I made mistakes while doing this on my own.
 

Status
Not open for further replies.

Part and Inventory Search

Welcome to EDABoard.com

Sponsor

Back
Top