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Welcome to the presentation
on the indefinite integral
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or the antiderivative.
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So let's begin with a
bit of a review of the
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actual derivative.
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So if I were to take
the derivative d/dx.
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It's just the
derivative operator.
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If I were to take the
derivative of the expression
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x squared-- this is an easy
one if you remember the
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derivative presentation.
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Well, this is pretty
straightforward.
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You just take the exponent.
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That becomes the new
coefficient, right.
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You actually multiply it times
the old coefficient, but in
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this case the old coefficient
is 1, so 2 times 1 is 2.
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And you take the variable 2x.
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And then the new exponent
will be one less than
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the old exponent.
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So it'll be 2x to
the 1, or just 2x.
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So that was easy.
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If I had y equals x squared we
now know that the slope at any
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point on that curve,
it would be 2x.
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So what if we wanted
to go the other way?
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Let's say if we wanted to start
with 2x, and I wanted to say
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2x is the derivative of what.
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Well, we know the answer
this question, right?
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Because we just took the
derivative of x squared
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and we figured out 2x.
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But let's say we didn't
know this already.
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You could probably figure it
out intuitively, how you can
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kind of do this operation
that we did here, how
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you can do it backwards.
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So in this case the notation--
well we know it's x squared--
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but the notation for trying to
figure out 2x is the derivative
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of what, we could say that--
let's say 2x is the
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derivative of y.
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So 2x is the derivative of y.
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Let's get rid of this of what.
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Then we can say this.
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We can say that y is equal to--
and I'm going to throw some
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very fancy notation at you and
actually I'll explain why we
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use this notation in a couple
presentations down the road.
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But you just have to know at
this point what the notation
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means or what it tells you to
really do, which really is
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just the antiderivative or
the indefinite integral.
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So we could say that y is
equal to the indefinite
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integral 2x dx.
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And I'm going to explain what
this squiggly line here is and
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dx, but all you have to know is
when you see the squiggly line
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and this dx and then something
in between, all they're asking
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is they want you to figure out
what the antiderivative
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of this expression is.
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And I'll explain later
why this is called the
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indefinite integral.
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And actually this notation
will make a lot more sense
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when I show you what a
definite integral is.
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But let's just take it for
granted right now that an
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indefinite integral-- which I
just drew here, it's kind of
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like a little squirrely thing--
is just the antiderivative.
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So y is equal to the
antiderivative essentially,
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or the indefinite integral
of the expression 2x.
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So what is y equal to?
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Well y is obviously
equal to x squared.
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Let me ask you a question.
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Is y just equal to x squared?
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Because we took the derivative,
and clearly the derivative
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of x squared is 2x.
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But what's the derivative
of x squared-- what's the
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derivative x squared plus 1?
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Well, the derivative of
x squared is still 2x.
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What's the derivative of 1?
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Right, derivative of 1
is 0, so it's 2x plus
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0, or still just 2x.
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Similarly, what's the
derivative of x squared plus 2?
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Well the derivative of
x squared plus 2 once
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again is 2x plus 0.
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So notice the derivative
of x squared plus
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any constant is 2x.
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So really y could be x
squared plus any constant.
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And for any constant
we put a big c there.
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So x squared plus c.
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And you'll meet many calculus
teachers that will mark this
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problem wrong if you forget to
put the plus c when you do
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an indefinite integral.
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So you're saying Sal, OK,
you've showed me some notation,
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you've reminded me that the
derivative of any constant
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number is 0, but this really
doesn't help you solve
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an indefinite integral.
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Well let's think about a way--
a systematic way if I didn't do
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it for you already--
that we could solve an
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indefinite integral.
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Let me clear this.
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A bolder color I think would
make this more interesting.
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Let's say we said y is equal to
the indefinite integral of--
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let me throw something
interesting in there.
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Let's say the indefinite
integral of x cubed dx.
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So we want to figure out some
function whose derivative
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is x to the third.
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Well how can we
figure that out?
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Well just from your intuition,
you probably think, well it's
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probably something times x
to the something, right?
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So let's say that y is
equal to a x to the n.
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So then what is dy/dx, or
the derivative of y is n.
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Well we learned this in
the derivative module.
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You take the exponent, multiply
it by the coefficient.
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So it's a times n.
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And then it's x to
the n minus 1.
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Well in this situation we're
saying that x to the third is
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this expression, it's
the derivative of y.
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This is equal to
x to the third.
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So if this is equal to x to
third, what's a and what's n.
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Well, n is easy to figure out.
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n minus 1 is equal to 3.
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So that means that
n is equal to 4.
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And then what is a equal to?
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Well a times n is equal to 1,
right, because we just have a 1
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in this coefficient, this has
a starting coefficient of 1.
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So a times n is 1.
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If n is 4, than a must be 1/4.
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So just using this definition
of a derivative, I think we now
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figured out what y is equal to.
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y is equal to 1/4
x to the fourth.
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I think you might start
seeing a pattern here.
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Well how did we get
from x to the third to
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1/4 x to the fourth?
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Well, we increased the exponent
by 1, and whatever the new
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exponent is, we multiply it
times 1 over that new exponent.
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So let's think if we can do
a generalized rule here.
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Oh, and of course, plus c.
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I would have failed this exam.
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So let's make a general rule
that if I have the integral
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of-- well, since we already
used a, let's say-- b
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times x to the n dx.
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What is this integral?
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This is an integral sign.
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Well my new rule is, I raise
the exponent on x by 1, so it's
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going to be x to the n plus 1.
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And then I multiply x times
the inverse of this number.
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So times 1 over n plus 1.
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And of course I had that
b there all the time.
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And one day I'll do a more
vigorous-- more rigorous proof
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and maybe it will be vigorous
as well-- as to why this b
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just stays multiplying.
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Actually I don't have to do too
rigorous of a proof if you just
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remember how a derivative is
done, you just multiply this
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times the exponent minus 1.
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So here we multiply the
coefficient times 1 over
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the exponent plus 1.
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It's just the
inverse operation.
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So let's do a couple of
examples like this really fast.
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I have a little time left.
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I think the examples, at
least for me, really
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hit the point home.
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So let's say I wanted to
figure out the integral
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of 5 x to the seventh dx.
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Well, I take the exponent,
increase it by one.
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So I get x to the eighth, and
then I multiply the coefficient
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times 1 over the new exponent.
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So it's 5/8 x to the eighth.
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And if you don't trust me,
take the derivative of this.
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Take the derivative d/dx
of 5/8 x to the eighth.
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Well you multiply 8 times 5/8.
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Well that equals 5 x to the--
and now the new exponent will
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be 8 minus 1-- 5 x
to the seventh.
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Oh, and of course, plus c.
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Don't want to
forget the plus c.
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So I think you have a
sense of how this works.
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In the next presentation I'm
going to do a bunch more
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examples, and I'll also
show you how to kind of
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reverse the chain rule.
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And then we'll learn
integration by parts, which is
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essentially just reversing
the product rule.
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See you in the next
presentation.
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