The Substitution Method: Reversing the Chain Rule for Integration, Schemes and Mind Maps of Differential and Integral Calculus

The substitution method, a technique used in calculus to evaluate integrals by applying the chain rule in reverse. It provides an example of integrating a complex function using this method and discusses the theory behind it.

Typology: Schemes and Mind Maps

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The Substitution Method: Chain Rule in Reverse
Recall that we were motivated by the fundamental theorem of calculus to define the indefinite integral
Zf(x)dx
as all antiderivatives of f(x). That is, if F(x)is an antiderivative of f(x)then we define
Zf(x)dx =F(x) + C
for some constant C.
As a simple example we can compute the following indefinite integral.
Zcos xdx =sin x+C
This is easy because we know that F(x) = sin xis an antiderivative of f(x) = cos x.
So knowing the derivative of sin xlet me integrate cos x. So what about doing some more interesting
derivtives. Consider for instance
F(x) = sin(x3+2x)
Then using the chain rule we see that
F0(x) = cos(x3+2x)(3x2+2)
Well, this means that we now know how to integrate the function f(x) = cos(x3+2x)(3x2+2). Indeed we
get
Zcos(x3+2x)(3x2+2)dx =sin(x3+2x) + C
This integrand is more complicated than just cos x, but really the way we solved it was not much harder.
We just used the chain rule!
Some theory
Okay - let’s try to generalise this example. Suppose that our antiderivative is a composition of two functions.
F(x) = f(g(x))
Then we differentiate using the chain rule to get
F0(x) = f0(g(x))g0(x)
This tells us, by our definition of the indefinite integral, that
ZF0(x)dx =F(x) + C(by definition)
i.e., Zf0(g(x))g0(x)dx =f(g(x)) + C
This is a lot of symbols, so we make our life easier and write u=g(x). Plugging this in gives us
Zf0(u)du
dx dx =f(u) + C
But we also have that Zf0(u)du =f(u) + C
pf3

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The Substitution Method: Chain Rule in Reverse

Recall that we were motivated by the fundamental theorem of calculus to define the indefinite integral ∫ f(x)dx

as all antiderivatives of f(x). That is, if F(x) is an antiderivative of f(x) then we define ∫ f(x)dx = F(x) + C

for some constant C.

As a simple example we can compute the following indefinite integral. ∫ cos xdx = sin x + C

This is easy because we know that F(x) = sin x is an antiderivative of f(x) = cos x.

So knowing the derivative of sin x let me integrate cos x. So what about doing some more interesting derivtives. Consider for instance

F(x) = sin(x^3 + 2x)

Then using the chain rule we see that

F′(x) = cos(x^3 + 2x)(3x^2 + 2 )

Well, this means that we now know how to integrate the function f(x) = cos(x^3 + 2x)(3x^2 + 2 ). Indeed we get (^) ∫

cos(x^3 + 2x)(3x^2 + 2 )dx = sin(x^3 + 2x) + C

This integrand is more complicated than just cos x, but really the way we solved it was not much harder. We just used the chain rule!

Some theory

Okay - let’s try to generalise this example. Suppose that our antiderivative is a composition of two functions.

F(x) = f(g(x))

Then we differentiate using the chain rule to get

F′(x) = f′(g(x))g′(x)

This tells us, by our definition of the indefinite integral, that ∫ F′(x)dx = F(x) + C (by definition)

i.e.,

f′(g(x))g′(x)dx = f(g(x)) + C

This is a lot of symbols, so we make our life easier and write u = g(x). Plugging this in gives us ∫ f′(u) du dx

dx = f(u) + C

But we also have that (^) ∫

f′(u)du = f(u) + C

Putting these two equations together we see that ∫ f′(u) du dx

dx =

f′(u)du

Alright, that was a lot of symbol bashing, but we finally got the thing we wanted out of it. Namely, this theorem gives us rule of sorts, that is the rule we will use for substitutions.

Substitution rule : du dx dx = du

Alright, that’s enough theory for now. Let’s see how this helps us in practice.

The substitution method

Consider the following example. F(x) = ecos^ x

Then using the chain rule we get,

F′(x) = − sin xecos^ x^ (?)

So we can compute the following indefinite integral. ∫ sin xecos^ xdx = −

− sin xecos^ xdx = −ecos^ x^ + C

Note that we had to add a minus sign!

Okay, let’s use our theory to answer the same question without the knowledge of equation (?). That is, we start with the integral ∫ ecos^ x^ sin xdx

And we make the substitution u = cos x. This means that

du dx = − sin x

Now the substitution rule tells us − sin xdx = du

Or equivalently, that −du = sin xdx

We now put this back into our equation

I =

ecos^ x^ sin xdx =

eu(−du) = −

eudu = −eu^ + C

Finally, we put this back in terms of x, giving,

I = −ecos^ x^ + C