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Mathematical Expression Editor
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We introduce antiderivatives.
Computing derivatives is not too difficult. At this point, you should be able to take
the derivative of almost any function you can write down. However, undoing
derivatives is much harder. This process of undoing a derivative is called taking an
antiderivative.
A function is called an antiderivative of on an interval if for all in the
interval.
How many antiderivatives does have?
The functions , , , and so on, are all antiderivatives of .
It is clear that any function , where is a constant, is an antiderivative of . Why?
Because, .
Could there exist any other antiderivative of , call it , such that is not a sum of and
a constant? In that case, for all we would have
Recall: Any function whose derivative is equal to on some interval is equal to a
constant on that interval. This means that the function , for some constant . This
implies that , for all x.
The Family of Antiderivatives
If is an antiderivative of , then the function has a whole family of antiderivatives.
Each antiderivative of is the sum of and some constant .
So, when we write , we denote the entire family of antiderivatives of . Alternative
notation for this family of antiderivatives was introduced by G.W. Leibniz
(1646-1716):
Let be a function. The family of of all antiderivatives of is denoted by
This is called the indefinite integral of .
It follows that where is any antiderivative of and is an arbitrary constant.
Now we are ready to ”integrate” some famous functions.
Fill out these basic antiderivatives. Note each of these examples comes directly from
our knowledge of basic derivatives.
Basic Indefinite Integrals
It may seem that one could simply memorize these antiderivatives and antidifferentiating
would be as easy as differentiating. This is not the case. The issue comes up when
trying to combine these functions. When taking derivatives we have the
product rule and the chain rule. The analogues of these two rules are much
more difficult to deal with when taking antiderivatives. However, not all is
lost.
Consider the following example.
Find an antiderivative of the function defined by
expression
, for all in some interval .
Differentiate each choice.
In the last choice we get .
It is easy to recognize an antiderivative: we just have to differentiate it, and check
wether , for all in .
Notice, that the function is the sum of the two functions, and , where and , for in
.
We know antiderivatives of both functions: and , for in , are antiderivatives of and ,
respectively. So, in this example we see that the function is an antiderivative
of . In other words, ”the sum of antiderivatives is an antiderivative of a
sum”.
Is this true in general?
Let’s check whether this rule holds for any eligible pair of functions and
defined on some interval .
Let , , and be four functions defined on some
interval such that is an antiderivative of and is an antiderivative of ,
i.e.
and for all in some interval .
Find an antiderivative of the function .
Differentiate the function .
Since , it follows that is an antiderivative of .
To summarize: The sum of antiderivatives is an antiderivative of a sum.
We have proved the following theorem.
The Sum Rule for Antiderivatives If is an antiderivative of and is an antiderivative
of , then is an antiderivative of .
We can write equivalently, using indefinite integrals,
.
Next, we will try to prove an analogue of the constant multiple rule for derivatives.
Let’s consider the following example.
Find an antiderivative of the function , where ,
for all in some interval .
Differentiate each choice for . In the first choice we get .
It is easy to recognize an antiderivative: we just have to differentiate it, and check
wether , for all in .
Notice, in this example the function is a constant multiple of ,
where . On the other hand, we know that the function , defined by is an
antiderivative of .
If we differentiate the function , we get that
, for in .
In other words, “a constant multiple of an antiderivative is an antiderivative of a
constant multiple of a function.” Is this always true?
Let’s check whether this rule holds for any constant and any eligible function
defined on some interval .
Let be a constant, let be a function defined on some
interval and let be an antiderivative of , i.e.
, for all in some interval .
Find an antiderivative of the function .
Differentiate the function .
Since , it follows that is an antiderivative of . To summarize: The constant
multiple of an antiderivative is an antiderivative of a constant multiple of a
function.
We have proved the following theorem.
The Constant Multiple Rule for
Antiderivatives If is an antiderivative of , and is a constant, then is an
antiderivative of .
We can write equivalently, using indefinite integrals, .
Let’s put these rules and our knowledge of basic derivatives to work.
Find the antiderivative
of .
By the theorems above , we see that
The sum rule for antiderivatives allows us to integrate term-by-term. Let’s see an
example of this.
Compute:
Let’s start by simplifying the problem using the sum rule and constant
multiple rule for antiderivatives,
Now we may integrate term-by-term to find
While the sum rule for antiderivatives allows us to integrate term-by-term, we cannot
integrate factor-by-factor, meaning that in general
A student claims that . Determine whether the student is correct or incorrect.
If the student were correct, then the derivative of with respect to would have to be .
However:
Hence, the student is incorrect!
Computing antiderivatives
Unfortunately, we cannot tell you how to compute every antiderivative, we view them
as a sort of puzzle. Later we will learn a hand-full of techniques for computing
antiderivatives. However, a robust and simple way to compute antiderivatives is
guess-and-check.
Tips for guessing antiderivatives
(a)
If possible, express the function that you are integrating in a form that is
convenient for integration.
(b)
Make a guess for the antiderivative.
(c)
Take the derivative of your guess.
(d)
Note how the above derivative is different from the function whose
antiderivative you want to find.
(e)
Change your original guess by multiplying by constants or by adding
in new functions.
Compute:
Before guessing the solution, let’s express the function in the
form convenient for integration. Due to Sum Rule, it is more convenient
to have a sum of functions, instead of a single, complicated term.
Now, we can apply the Sum Rule. Now we can finish the problem.
Compute:
Start with a guess of Take the derivative of your guess to see if it is
correct: We’re off by a factor of , so multiply your guess by this constant to get the
solution,
Compute:
Start with a guess of Take the derivative of your guess to see if it is
correct: Therefore,
Compute:
Start with a guess of Take the derivative of your guess to see if it is
correct: We’re off by a factor of , so multiply our guess by this constant to get the
solution,
Compute:
Start by rewriting the indefinite integral as Now start with a
guess of Take the derivative of your guess to see if it is correct: We’re off
by a factor of , so multiply our guess by this constant to get the solution,
Compute:
We try to guess the antiderivative. Start with a guess of Take the
derivative of your guess to see if it is correct: Ah! So we need only multiply our
original guess by . We now find
Compute:
We notice that the numerator is the derivative of the denominator, i.e.,
the function that we are integrating has the form . Take the derivative of your guess
to see if it is correct: Therefore,
Compute:
We’ll start with a guess of Take the derivative of your guess to see if it is
correct: We are only off by a factor of , so we need to multiply our original guess by
this constant to get the solution,
Final thoughts
Computing antiderivatives is a place where insight and rote computation meet.
We cannot teach you a method that will always work. Moreover, merely
understanding the examples above will probably not be enough for you to
become proficient in computing antiderivatives. You must practice, practice,
practice!
Differential equations
Differential equations show you relationships between rates of functions.
A differential equation is simply an equation with a derivative in it. Here is an
example:
Which one is a differential equation?
When a mathematician solves a differential equation, they are finding functions
satisfying the equation.
Which of the following functions solve the differential
equation
We can directly check that any function is a solution to our differential equation .
Could there be any others? It turns out that these are the only solutions. But
showing that we didn’t miss any is a bit tricky.
Well, suppose we have some mysterious function and all we know is that . Let’s
define a new function . Since our denominator is never 0, the quotient rule tells
us that But we know that a function with a 0 derivative is constant, so .
Plugging this back into our formula for tells us that . Now we rearrange to get
.
This shows us that any solution to our differential equation must be one of the
functions we’ve already found. Our argument relies on some features that are special
to this problem; proving that we’ve found all the possible solutions to an arbitrary
differential equation is a very difficult task!
A function is called a general solution of the differential equation. Since there are
infinitely many solutions to a differential equation, we can impose an additional
condition (say ), called an initial condition. When we are asked to find a function
that satisfies both the differential equation (DE) and the initial condition (IC), this is
called an initial value problem (IVP). Let’s try one out.
Solve the initial value
problem (IVP):
The figure below shows several solutions of the differential equation.
The figure suggests that the only solution to the initial value problem is the function .
We can verify this result.
Since all solutions of the differential equation have the form and , it follows that
Therefore, So, the unique solution to the given initial value problem is the function
.
Solve the initial value problem (IVP):
First, we have to solve the differential equation. The solution is clearly an
antiderivative of . where is an arbitrary constant. We have found the general
solution of the DE and this family of solutions is illustrated by the figure below.
Now we must find the solution that also satisfies the initial condition .
Since it follows that Therefore, The function is the solution of the initial value
problem and it is shown in the figure above.
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