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The Indefinite Integral or Anti-derivative

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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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Title:
The Indefinite Integral or Anti-derivative
Description:

An introduction to indefinite integration of polynomials.

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Video Language:
English
Duration:
09:27

English subtitles

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