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### Course: Electrical engineering > Unit 2

Lesson 4: Natural and forced response- Capacitor i-v equations
- A capacitor integrates current
- Capacitor i-v equation in action
- Inductor equations
- Inductor kickback (1 of 2)
- Inductor kickback (2 of 2)
- Inductor i-v equation in action
- RC natural response - intuition
- RC natural response - derivation
- RC natural response - example
- RC natural response
- RC step response - intuition
- RC step response setup (1 of 3)
- RC step response solve (2 of 3)
- RC step response example (3 of 3)
- RC step response
- RL natural response
- Sketching exponentials
- Sketching exponentials - examples
- LC natural response intuition 1
- LC natural response intuition 2
- LC natural response derivation 1
- LC natural response derivation 2
- LC natural response derivation 3
- LC natural response derivation 4
- LC natural response example
- LC natural response
- LC natural response - derivation
- RLC natural response - intuition
- RLC natural response - derivation
- RLC natural response - variations

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# RC natural response - derivation

We derive the natural response of an RC circuit and discover it has an exponential form. Created by Willy McAllister.

## Want to join the conversation?

- At about0:55I am confused by the direction of i_c.

Is this the direction of the current that charged the capacitor (before switching?).

I don't understand how one can then apply KCL at1:34. It seems to me that i_r should = i_c in size and direction.(18 votes)- The direction of i_c is arbitrarily designated according to the passive sign convention; see https://www.khanacademy.org/science/electrical-engineering/ee-circuit-analysis-topic/circuit-elements/v/ee-passive-sign-convention for more on the passive sign convention, because it's really important to the application of all these equations.

As for KCL, the span between the two components still counts as a node, and so the (two) branches still have their currents sum to zero. The issue you're running into is the desire to have all the arrows drawn in the "right" orientation before you've analyzed the circuit. You are correct, the current is the same throughout the node; that's why he invoked KCL. But it is perfectly valid, or even (as in this case) useful to draw arrows in orientations you know to be impossible, and just get a negative result for some (meaning it's in the opposite direction of how you drew it).

So, yes, the current in both ends of the node is necessarily the same amount, directed to the left. But because we drew i_c as pointing to the right, opposite the direction of i_r, it necessarily must equal the NEGATIVE of i_r. Had we drawn both pointing to the left, they would both equal +[amount], or if we had drawn them both to the right they would both be -[amount], but the all the relationships remain the same; we just lose the passive sign convention.(9 votes)

- At7:52, why it is told that -(t/RC) has to have no units before we evaluate? What is the reason behind this thing?(4 votes)
- The term -(t/RC) is in the exponent. Exponents have to be pure numbers with no dimensions. That's because exponents are really a shorthand notation for a multiplication operation. If I write 2^3 it means multiply 2 by itself 3 times. If I write something like 3^(4 ohms) where there are dimensions in the exponent, I can't make sense of it: multiply 3 by itself "4 ohms" times?(9 votes)

- Solving the ODE:

dv/dt + v/RC = 0

dv/dt = -v/RC

dv/v = -dt/RC

∫dv/v = -∫dt/RC

ln(v) = -t/RC + k

v = e^(-t/RC + k)

= K e^(-t/RC)

v(t) = v_0 e^(-t/RC)(7 votes)- What law or property allows dropping the constant K from the exponent e^(-t/RC + k) to get Ke^(-t/RC)?(3 votes)

- at1:32you use the formula iC = C dv/dt

silly question but what is 'd'?(3 votes)- Hello Doug,

This is the notation of calculus - d stands for delta or change. You would think of this as "a change in voltage per unit time."

In English the equation reads The current on the capacitor equals the product of capacitance and the speed at which the voltage is changing.

If the voltage is changing quickly the capacitor will have a high current.

Regards,

APD(3 votes)

- at10:50(probably a stupid question), why don't you also account for current from the capacitor?(2 votes)
- We account for the current in the capacitor back at1:30where we develop the original differential equation.(2 votes)

- At1:37, I get confused. You state that according to KCL,

i_R + i_C = 0,

but I thought that is only the case when they are flowing at the same time. In here i_C stops flowing once you turn the switch, right? So how do you know if i_C and I_R are the same magnitude in opposite directions? Why isn't it possible for i_R to be of a different magnitude than i_C?(2 votes)- In the previous video there was a battery and switch connected to the R and C. The battery provided some charge that flowed through R and got stored on the plates of C. As charge was being added to the capacitor, its voltage increased, (q = Cv) or (v = q/C). At some time in the past, the voltage on the capacitor became equal to the battery voltage. When that happened, you have 0 volts across the resistor, which means v = iR or 0 = iR, telling us i = 0. So just before we flip the switch, capacitor current = resistor current = 0.

Now we throw the switch and the battery basically vanishes. The circuit becomes just R and C connected at both ends, and there is some charge stored on the capacitor. That's where this video starts. There is only one loop in the circuit, which means there is only one current. Just before the switch is flipped, the current is 0. Just after the switch flips, charge starts flowing out of the capacitor and into the resistor. Moving charge is a current, and it is flowing in both R and C.

I use a notation trick that maybe causes some confusion. The point of this video is to show you how to derive an equation for what happens next. Looking ahead, I planned out how to get a nice looking equation that didn't have too many minus signs. With this foresight, I labeled the one current with two names i_R and i_C. I did this so I could use the i-v equations for R (Ohm's Law) and C (i = Cdv/dt) in the upcoming steps.

Please let me know if this helps you understand what's going on here.(2 votes)

- In your prior video (RC natural response) you show the current flowing in the opposite direction out of the capacitor as that shown in this video. In the last video you said you were going to " say more about why you chose that current direction later" , BUT you didn't. Also, you failed to explain why you show current flowing in 2 (opposite) directions in the same node from the capacitor source.(2 votes)
- How would this circuit change if the current went through the capacitor first, then the resistor?(1 vote)
- This RC circuit is symmetric and there is a single loop. That means there is only one current, and it flows in both R and C at the same time. There isn't a sense that current flows in the resistor "first". It flows everywhere all at once.(2 votes)

- So question, around3:47the variable e was introduced, what does it represent? K was the initial voltage. S became time/sec. I don't know where e came from or what it represents.(1 vote)
- e is the "base of the natural logarithm". It is a number, 2.718... This number shows up in a lot of places in physics, chemistry, biology, and engineering. Sal provides this introduction to e: https://www.khanacademy.org/math/algebra2/exponential-and-logarithmic-functions/e-and-the-natural-logarithm/v/e-through-compound-interest(2 votes)

- Admittedly my Calculus is horribly rusty (I took it almost 30 years ago). At the @4:47mark, you say that "the S comes down..." How does that happen? I guess I'm missing a step in solving the equation that brings S from an exponent into part of the constant. I want to say it is e^s would be S(e^s-1)dx, but I'm not sure if that's correct.(1 vote)
- I think you are remembering the derivative of x^n

as in

d x^n/dx = n x^(x-1)

We are doing something different, where the independent variable (t) is up in the exponent and the base is the natural number "e".

The derivative of e^t (with no "s" coefficient) is

de^t/dt = e^t

(the exponential is its own derivative)

If we slip in a coefficient s the answer becomes,

d e^st/dt = s e^st

This happens where I said "comes down".

Sal does a proof of the derivative of e^x here:

https://www.khanacademy.org/math/ap-calculus-ab/ab-differentiation-1-new/ab-2-7/a/proof-the-derivative-of-is

When you slip in the s coefficient the derivative is determined by the "chain rule". All these things you learned back in your calc class all those years ago. Hope this knocked off a little rust. Good luck!(2 votes)

## Video transcript

- [Voiceover] Now what I want
to to do for the RC circuit is a formal derivation of exactly what these two curves look like. And then we'll have a
precise definition of the natural response. What I want to do now is
draw our circuit again. There's R, there's C. And we have some initial voltage, we said, on the capacitor, which is V naught. And what we want to find is V of T. And there's R, and there's C. So let me also label the
currents in these guys. This is the current in the resistor, and this is the current in the capacitor. So now I'm gonna write
the two voltage current relationships for these two components. And Ohm's Law tells me
that equals one over R times V. And the current in a
capacitor, this is iR, current in a capacitor
equals C times dv, dt. That's the two currents in our devices. Now, gonna use Kirchhoff's
Current Law on this node right here, and that says
that all the currents flying out of that node
have to add up to zero. So let's do that. Let's say iC plus iR equals zero. This is KCL, Kirchhoff's Current Law. C dv, dt, plus one over
R, times V, equals zero. Now I'm just gonna divide through by C just to be tidy. Dv, dt plus one over RC,
times V, equals zero. So what we have here,
this expression here is referred to as an ordinary
differential equation. It has a derivative in it,
and that's what makes it a differential equation,
and you can go look up ODE and search for this in
Khan Academy and elsewhere and in the mathematical
videos, you'll find out different ways to solve this equation. Now we're gonna do the same thing here, and we're gonna try to find
an expression for V of t. We're gonna define V of
t in a way that makes this equation true. So we plug the function
in here, whatever it is, and then we take its derivative
and plug that in here and that has to make this
whole expression true. There's a couple of different
ways to do this, and the one that we're gonna use
here is we're gonna guess at an answer. So what we need is, we need
a function whose derivative looks kind of like
itself, because this thing has to add up to zero. So that means that the function
V and the function dv, dt they have to be of the
same form so that they have a chance of adding up to zero. The function that I know
whose derivative looks like itself is the exponential. So we're gonna propose that
there's gonna be an exponential and the way we do it is say,
we'll put in some constant here that we can adjust,
and then we'll put some constant out here. So this is our guess. Our guess is gonna be that
the solution for V of t is gonna be something of
the form, some constant times e to another constant, s, times t. The way we test our guess
is to put it back into the equation and see if it works. And if it does, then we made a good guess. If it doesn't work,
then we have to go back and try something else. So one of the things we
need, we're gonna plug v of t in right here. We're gonna need derivative
of v with respect to time. So let's take a derivative here. Equals d dt of k, e to the st. And that equals K, and the S comes down. And e to the st remains. So we just took the derivative
of our proposed solution and now we're gonna plug
it into the equation and see what happens. So now I'm gonna plug in
the derivative that we had, plus the proposed solution,
and see if our equation comes out true. So dv, dt is sk, e to the st, plus one over RC stays here. And we plug in V, and V was ke to the st. And that'll all equal zero. Now I'm gonna factor out,
here's the common term for each one of these, so
we'll just factor that out. So now we get ke to the st,
times S plus one over RC equals zero. Okay, now let's take
a little peek at this. We have to make this
zero by the way we pick K and S. How can we make this zero? There's three terms in
here, there's three terms in the product. There's this, this, and that. Any three of these terms could be zero. The first one, K is
zero, that's a boring one because it says if we have
a circuit with no energy it sits there with no energy. So that's not so interesting. Now, e to the st, we
can make that go to zero but that takes a long time
because we have to let t go to infinity. S would have to be a negative
number, and t would have to go to infinity, which
is a long time to wait for something to happen,
so that's not a very interesting solution either. So here's the interesting one. The interesting one is
when S plus RC equals zero so the interesting solution
is S plus one over RC equals zero, and that says that
S equals minus one over RC. That makes this solution true. And if that's the case,
now we can say v of t, we're making good progress here, k, some k, times e to the minus t over RC. Now something really
interesting just happened here. Look up here where we
have this RC term here. See this right here? This whole exponent has to
have no units by the time we evaluate it. That means that RC has
to have units of time. RC is a measure, it's in seconds. RC is the units of R times
C, ohms times farads, is actually seconds. This whole exponent has to
have no units by the time we evaluate it. And that means that RC
has to have units of time. And it's actually ohms times farads, comes out to be seconds. Now we solve for S, and that means we only have to find K. Let's work on K now. K is a variable here, time is a variable, and voltage is a variable. If we knew V and T at
the same time, we would be able to figure out K. And there's a time when we do know that. And that is t equals zero. At t equals zero we know that
the battery was hooked up and there's a bunch of
charge on the capacitor so we know that the
voltage on the capacitor at time zero, is equal to V naught. So now we have a pair of variables here. We know v and t at the same time, so let's plug that into our
proposed solution and see how k pops up. So we're gonna put these two
into our proposed solution and see what happens to k. V, at time equals zero,
is V naught, and that's equal to k times e to
the minus t, minus zero at time zero, over RC. Now this whole expression
is e to the zero, or one. So it drops out of the expression and all we get is k equals V naught. K is the starting
voltage on the capacitor. And that gives us to our
final answer, which is v of t equals V naught, starting voltage, e to the minus time over RC. We can go one small step
further and find out what is i of t. Well, i of t is equal to v of t over R, that's just Ohm's Law, and so i of t equals V naught over R,
e to the minus t over RC. That is the natural
response of an RC circuit.