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## Differential equations

### Course: Differential equations > Unit 1

Lesson 5: Exponential models- Exponential models & differential equations (Part 1)
- Exponential models & differential equations (Part 2)
- Worked example: exponential solution to differential equation
- Differential equations: exponential model equations
- Newton's Law of Cooling
- Worked example: Newton's law of cooling

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# Worked example: exponential solution to differential equation

AP.CALC:

FUN‑7 (EU)

, FUN‑7.F (LO)

, FUN‑7.F.1 (EK)

, FUN‑7.F.2 (EK)

, FUN‑7.G (LO)

, FUN‑7.G.1 (EK)

The solution of the general differential equation dy/dx=ky (for some k) is C⋅eᵏˣ (for some C). See how this is derived and used for finding a particular solution to a differential equation.

## Want to join the conversation?

- Instead of putting the equation in exponential form, I differentiated each side of the equation:

(1/y) dy = 3 dx

ln y = 3x + C

Therefore

C = ln y - 3x

So, plugging in the given values of x = 1 and y = 2, I get that C = ln(2) - 3. If you put this in a calculator, it's a very different value (about -2.307) than what Sal got by raising both sides to the power of e: 2 * e^-3 evaluates to about .0996.

Why did my method not work?(15 votes)- It's important to note that the C you work with is not the same as the C Sal works with. At2:06, Sal gets e^C, which he says is just going to be another arbitrary constant. Thus Sal replaces e^c with C. If you perform e^(-2.307) you should get 0.0996.(25 votes)

- Sal changed e^C (which any arbitrary constant) to C (which is any another constant) and at least according to my knowledge C can't be any another constant as it will always be positive coz e^C can never be negative. We actually limited the value of our arbitrary constant to positive numbers, then shouldn't we mention that C is any constant number greater than zero i.e(C>0) ?(11 votes)
- "Any arbitrary constant" includes complex numbers. Recall that e^(x*j) = cos(x) + j*sin(x). C could be, for example, 5 + π*j, in which case e^C ≈ -7.4.

However, even with complex exponents, e^C can*never*be zero! In this case that does not matter, because we have already limited ourselves to y ≠ 0 by using 1/y as part of the solution. But it is certainly something to keep in mind for other situations.(2 votes)

- At around2:50, Sal decides to consider only the first scenario that he broke the absolute value function into, saying that "it will take the [other, negative part of it] into consideration". How did he know this would happen?(9 votes)
- When dealing with separable equations why in some videos do you put y and the constant on one side and in others (like this one) you only move y over?(5 votes)
- It doesn't matter, the result will be the same. It just changes how you get to that result.(3 votes)

- Wouldn't it be possible to solve for C right after you integrated both sides of the separated equation? ln |y| = 3x + C , when x = 1, y = 2.

Plug in these values and you'd get ln (2) = 3 + C, so C = ln (2) - 3

Then you'd get ln |y| = 3x +ln (2) - 3

So that y = e^(3x+ln (2) -3), because e^ln(2) = 2 you'd get 2e^(3x-3), and this is correct, but the method is different from the one Sal uses, can someone explain to me, why this works, or if there are any steps that aren't correct, so that you'd have to use Sal's method?(3 votes)- What exactly does Sal do (and yes what you did is correct)(2 votes)

- Why do we ultimately get the same specific solution when we solve for C with

y = Ce^(3x)

and substitute C back in and when we use

y = -Ce^(3x)

and substitute C back in?

I might be missing something fairly obvious, but since both functions satisfy our original differential equation and are the reflections of each other over the x-axis, there should be two functions that both pass through the point (1, 2) and satisfy dy/dx = 3y right?

Edit: I think (??) I answered my own question, but I would appreciate it if someone could verify it. In this case, since our two functions have C as a coefficient, and not as something that you add on, the two functions lead to the same specific solution. If you wanted to have the reflection over the x-axis of the solution also pass through the point, you would need to add a constant to it; but then, it wouldn't satisfy our differential equation.(3 votes) - If for whatever reason I had chosen to multiply both sides of the original integral in orange by -1, I would get very different solutions. I have always had a hard time understanding this. can someone help?(2 votes)
- −∫(1 ∕ 𝑦)𝑑𝑦 = −∫3𝑑𝑥 ⇔

⇔ −ln|𝑦| = −3𝑥 + 𝐶, where we can just as well write the right-hand side as −3𝑥 − 𝐶

Multiplying both sides by (−1), we get; ln|𝑦| = 3𝑥 + 𝐶, which is the exact same equation that Sal solved for in the video.(2 votes)

- when I use y=-ce^3x then also I got the same ans y=e^(3x-3) as Sal sir got using y=ce^3x

that means no effect of absolute value here?(2 votes)- I think you may have miscalculated somewhere.

2 = -ce^3 gets a different result than 2 = ce^3(2 votes)

- I solved the integral by using U-substitution (int(1/3y)dy=int(1)dx), but after evaluating, I got ln|3y|=3x+C instead of ln|y|=3x+C. What did I do wrong?

Here are my steps:

int(1/3y)dy=int(1)dx

int(1/3y)dy=x+C

(d/dy)(3y)=3

(1/3)int(3*1/3y)dy=x+C

u=3y

(1/3)int(1/u)du=x+C

(1/3)ln|u|+C=x+C

(1/3)ln|u|=x+C

ln|u|=3x+C

ln|3y|=3x+C(1 vote)- There's nothing wrong.

ln|3𝑦| = 3𝑥 + 𝐶 ⇒ 𝑦 = (1∕3)𝑒^(3𝑥 + 𝐶) ⇒ 𝑑𝑦∕𝑑𝑥 = 𝑒^(3𝑥 + 𝐶) = 3𝑦, which is the equation we started with.

Similarly,

ln|𝑦| = 3𝑥 + 𝐶 ⇒ 𝑦 = 𝑒^(3𝑥 + 𝐶) ⇒ 𝑑𝑦∕𝑑𝑥 = 3𝑒^(3𝑥 + 𝐶) = 3𝑦(3 votes)

- when c=ln(3)/8 how do i set that to base e(1 vote)

## Video transcript

- [Teacher] So, we've got
the differential equation, the derivative of y with
respect to x is equal to three times y. And we want to find
the particular solution that gives us y being equal to two when x is equal to one. So, I encourage you to pause this video and see if you can figure
this out on your own. All right, now, let's
work through it together. So, some of you might
have immediately said, "Hey, this is the form of
a differential equation "where the solution is
going to be an exponential," and you just got right to it. But, I'm not going to go straight to that, I'm just gonna recognize
that this is a separable differential equation and that
I'm gonna solve it that way. So, when I say that it's separable, that means that we can
separate the y's, dy's, on one side, and all the
x's, dx's on the other side. And so, what I can do is
if I divide both sides of this equation by y and
multiply both sides by dx, I get one over y, dy, is equal to three-dx. Now, on the left and right hand sides, I have these clean things
that I can now integrate. That's what people talk about when they say separable
differential equation. Now, here on the left,
if I wanted to write it in a fairly general form, I could write, well, the anti-derivative of one over y is gonna be the natural log
of the absolute value of y. I'm taking the anti-derivative
with respect to y, here. Now, I could add a constant, but I'm gonna add in a constant
on the right-hand side, so there's no reason to
add two arbitrary constants on both sides. I could just add one on one side. So, that is going to be equal to the anti-derivative here is going to be three-x and I'll add the
promised constant, plus c, right over there. And now, let's think
about it a little bit. Well, we can rewrite
this in exponential form. We could say, we could write, that e to the three-x plus c is equal to the natural log of y. I could write the natural of y is equal to e to three-x plus c. Now, I could rewrite this
is equal to e to three-x times e to the c. Now, e to the c is just gonna be some other arbitrary constant, which
I could still denote by c. They're are going to be different values, but we're just trying to just get a sense of what the structure of
this thing looks like. So, we could say this is
going to be some constant times e to the three-x. So, another way of thinking about it. Saying the absolute value
of y is equal to this. This isn't a function yet. We're trying to find
this function solution to this differential equation. So, this would tell us
either y is equal to c, e to the three-x, or y is equal to negative
c, e to the three-x. Well, we've kept it in general terms. I haven't put any... We don't know c is. So, what we could do, instead,
is just pick this one, and then we can solve for c assuming this one right over here. And so, we will see if we
can meet these constraints using this and it'll
essentially take the other one into consideration, whether
we're going positive or negative. So, let's do that. So, when y is equal to two, I'm now going to solve for c to find the particular
solution, x is equal to one, or when x is equal to
one, y is equal to two. So, I could write it like that, and we get two is equal to c times e to the third power, three times one. And so, to solve for
c, I could just divide both sides by e to the third, and so I could, or I
could multiply both sides times e to the negative third, and I could get two e to
the negative third power is equal to c. And so let's now substitute it back in and our particular solutions is gonna be y is equal to c. C is two-e to the negative third power times e to the three-x. Now, I'm taking the product of two things with the same base. I can add the exponents. So, I could say y is equal to two times e to the three-x and I'll add the exponents to three-x minus three, and there you go. This is one way that you could
write the particular solution that meets these constraints for this separable differential equation.