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L7 1 2Review Polar And Rectangular Forms

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    >> So complex numbers consist of two
    parts: A real part and an imaginary part,
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    and we typically write them then as z a
    complex number is equal to a plus j B.
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    Because there's two parts it requires
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    a complete plane to
    represent them graphically.
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    A real number we can show
    on the real number line,
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    an imaginary number we can show
    along an imaginary number line.
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    But when you've got
    both the real and imaginary part,
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    we form what is known as
    the complex plane where
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    the horizontal axis of the plane
    is referred to as the real axis,
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    and we plot the real value of the
    complex number along the horizontal axis.
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    The vertical axis becomes
    the imaginary axis
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    where we plot the imaginary part
    of our complex number.
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    So, for example here we have
    z is equal to two plus j.
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    We come over one,
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    two units along the real part because
    in this case a the real part is two,
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    and we go up one unit along
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    the imaginary axis because
    our imaginary part is one times j.
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    So, here we'd have one j,
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    two j, three j.
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    You can think of J almost as
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    a unit vector or a quantity
    showing us which axis we're on.
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    The distance along this axis is two.
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    the distance along this axis
    is one times j. All right.
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    We here are representing
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    this real number or
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    this complex number in what is
    known as rectangular coordinates,
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    a horizontal value and a vertical value.
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    As you know we can also represent points in
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    a plane using polar coordinates where
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    the two coordinate values are
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    a angle of rotation away from
    the horizontal axis which we call theta,
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    and the distance from the origin
    out to the point along
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    that ray is known as the magnitude
    of the complex number.
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    So, we can write z in polar form,
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    in terms of this magnitude and an angle.
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    Now, how did the polar and rectangular
    coordinates relate to each other?
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    We can go from rectangular to
    polar using Pythagorean's theorem.
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    So, from rectangular to polar we
    can calculate the magnitude of z.
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    That's simply equal to,
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    using Pythagorean's theorem, the
    square root of the two sides.
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    Well this is A, so it would be
    the square root of A squared,
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    and the distance along
    the imaginary axis is b.
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    So, A squared plus B squared and
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    theta the angle is equal
    to the inverse tangent
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    of the opposite over the adjacent or
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    the inverse of the imaginary over the real
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    or the inverse tangent of b over a.
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    Now, to go from polar coordinates
    back to rectangular coordinates,
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    we again use the right
    triangle and recognize
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    that the distance along
    the horizontal axis is A,
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    that's simply equal to the projection
    of that point down onto
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    the real axis which of course is
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    the magnitude of z times
    the cosine of the angle.
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    So, A then, is equal to
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    the magnitude of z times
    the cosine of the angle theta,
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    and b, the imaginary component is equal
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    to the magnitude of z
    times the sine of theta.
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    Again, is just for
    the projection of this point,
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    onto the imaginary axis.
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    So, that takes us from polar coordinates,
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    back to rectangular coordinates.
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    Now let's just do an example real
    quick to show how this works.
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    In fact let's do it for
    this quantity right there.
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    The complex number z equals two plus j
    given to us in rectangular coordinates,
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    how do we get the polar
    representation of it?
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    While coming down here,
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    the magnitude of z is going to equal
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    the square root of the real part
    squared which is two squared,
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    plus the imaginary part.
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    The imaginary part is
    coming up here one unit,
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    again we don't square the j.
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    The distance there, for
    the geometry in this circuit,
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    in this problem, the distance
    there is one unit,
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    so it'll be one squared and that
    equals the square root of five.
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    Theta is equal to the arc-tangent
    of the imaginary part which is one,
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    it's not J, it's one.
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    Again, this distance is one unit.
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    So, the one imaginary part
    over the real part two,
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    and that turns out to be 26.6 degrees.
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    Now to show how we take it and go back.
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    First of all, this number
    then in polar coordinates,
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    we would represent as square root
    of five angle 26.6 degrees.
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    Okay? Now, how do we take
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    this number in polar form and go
    back into rectangular coordinates?
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    Well, it tells us right here that A,
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    the real part of our number
    is equal to A is
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    equal to the magnitude of Z which we
    found to be the square root of five,
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    times the cosine of the angle which
    is in this case is 26.6 degrees.
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    When you're doing this make sure
    you got your calculator is set in
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    degrees and not radians if
    you're working in degrees.
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    That then of course is going to equal A,
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    the distance along
    the real axis which we know
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    and when you can't do that calculation
    if you find that is equal to two,
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    and b the imaginary part then
    is equal to the square root of
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    five times the sine of 26.6
    degrees which equals one.
Title:
L7 1 2Review Polar And Rectangular Forms
Video Language:
English
Duration:
06:09
CDStunes edited English subtitles for L7 1 2Review Polar And Rectangular Forms Mar 28, 2019, 2:52 PM

English subtitles

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