Normal vector from plane equation Video Lecture

What I want to do in
this video is make sure
that we're good at
picking out what
the normal vector
to a plane is, if we
are given the
equation for a plane.
So to understand that, let's
just start off with some plane
here.
Let's just start off--
so this is a plane,
I'm drawing part
of it, obviously it
keeps going in every direction.
So let's say that is our plane.
And let's say that this is a
normal vector to the plane.
So that is our normal
vector to the plane.
It's given by ai
plus bj plus ck.
So that is our normal
vector to the plane.
So it's perpendicular.
It's perpendicular
to every other vector
that's on the plane.
And let's say we have
some point on the plane.
We have some point.
It's the point x sub p.
I'll say p for plane.
So it's a point on the plane.
Xp yp zp.
If we pick the origin.
So let's say that
our axes are here.
So let me draw our
coordinate axes.
So let's say our coordinate
axes look like that.
This is our z-axis.
This is, let's say
that's a y-axis.
And let's say that
this is our x-axis.
Let's say this is our
x-axis coming out like this.
This is our x-axis.
You can specify this
is a position vector.
There is a position vector.
Let me draw it like this.
Then it would be behind the
plane, right over there.
You have a position vector.
That position vector would
be xpi plus ypj plus zpk.
It specifies this
coordinate, right here,
that sits on the plane.
Let me just call that something.
Let me call that
position vector,
I don't know-- let
me call that p1.
So this is a point on the plane.
So it's p-- it is p1
and it is equal to this.
Now, we could take another
point on the plane.
This is a particular
point of the plane.
Let's say we just say, any
other point on the plane, xyz.
But we're saying that
xyz sits on the plane.
So let's say we take this
point right over here, xyz.
That clearly, same logic, can
be specified by another position
vector.
We could have a position
vector that looks like this.
And dotted line.
It's going under the
plane right over here.
And this position
vector, I don't know,
let me just call it p, instead
of that particular, that P1.
This would just be
xi plus yj plus zk.
Now, the whole reason
why I did this set up
is because, given some
particular point that I know
is on the plane, and any other
xyz that is on the plane,
I can find-- I can construct--
a vector that is definitely
on the plane.
And we've done this
before, when we
tried to figure out what the
equations of a plane are.
A vector that's
definitely on the plane
is going to be the difference
of these two vectors.
And I'll do that in blue.
So if you take the yellow
vector, minus the green vector.
We take this position,
you'll get the vector
that if you view
it that way, that
connects this point
in that point.
Although you can
shift the vector.
But you'll get a vector that
definitely lies along the plane
So if you start
one of these points
it will definitely
lie along the plane.
So the vector will
look like this.
And it would be lying
along our plane.
So this vector lies
along our plan.
And that vector is p minus p1.
This is the vector p minus p1.
It's this position vector minus
that position vector, gives you
this one.
Or another way to view
it is this green position
vector plus this blue vector
that sits on the plane
will clearly equal this
yellow vector, right?
Heads to tails.
It clearly equals it.
And the whole reason
why did that is we
can now take the dot product,
between this blue thing
and this magenta thing.
And we've done it before.
And they have to be equal to 0,
because this lies on the plane.
This is perpendicular
to everything
that sits on the
plane and it equals 0.
And so we will get the
equation for the plane.
But before I do
that, let me make
sure we know what the components
of this blue vector are.
So p minus p1, that's
the blue vector.
You're just going to subtract
each of the components.
So it's going to be x minus xp.
It's going to be x minus
xpi plus y minus ypj plus z
minus zpk.
And we just said,
this is in the plane.
And this is, this
right, the normal vector
is normal to the plane.
You take their dot product--
it's going to be equal to zero.
So n dot this vector is
going to be equal to 0.
But it's also equal to this
a times this expression.
I'll do it right over here.
So these-- find some good color.
So a times that, which is ax
minus axp plus b times that.
So that is plus by minus byp.
And then-- let me make
sure I have enough colors--
and then it's going to
be plus that times that.
So that's plus cz minus czp.
And all of this is equal to 0.
Now what I'm going to do is,
I'm going to rewrite this.
So we have all of these
terms I'm looking for, right?
Color.
We have all of the x terms-- ax.
Remember, this is any
x that's on the plane,
will satisfy this.
So ax, by and cz.
Let me leave that on
the right hand side.
So we have ax plus by
plus cz is equal to--
and what I want
to do is I'm going
to subtract each of
these from both sides.
Another way is, I'm going
to move them all over.
Let me do it-- let me
not do too many things.
I'm going to move them
over to the left hand side.
So I'm going to add
positive axp to both sides.
That's equivalent of
subtracting negative axp.
So this is going
to be positive axp.
And then we're going to have
positive byp plus-- I'll
do that same green-- plus byp,
and then finally plus czp.
Plus czp is going
to be equal to that.
Now, the whole reason why
did this-- and I've done this
in previous videos, where we're
trying to find the formula,
or trying to find the
equation of a plane,
is now we say, hey, if
you have a normal vector,
and if you're given a point
on the plane-- where it's
in this case is
xp yp zp-- we now
have a very quick way of
figuring out the equation.
But I want to go the other way.
I want you to be
able to, if I were
to give you a equation for
plane, where I were to say, ax
plus by plus cz, is equal to d.
So this is the general
equation for a plane.
If I were to give
you this, I want
to be able to figure out the
normal vector very quickly.
So how could you do that?
Well, this ax plus by
plus cz is completely
analogous to this part
right up over here.
Let me rewrite all this over
here, so it becomes clear.
This part is ax
plus by plus cz is
equal to all of this stuff
on the left hand side.
So let me copy and paste it.
So I just essentially
flipped this expression.
But now you see this, all of
this, this a has to be this a.
This b has to be this b.
This c has to be this thing.
And then the d is all of this.
And this is just
going to be a number.
This is just going to
be a number, assuming
you knew what the
normal vector is,
what your a's, b's
and c's are, and you
know a particular value.
So this is what d is.
So this is how you could get
the equation for a plane.
Now if I were to give
you equation or plane,
what is the normal vector?
Well, we just saw it.
The normal vector, this a
corresponds to that a, this b
corresponds to that b, that
c corresponds to that c.
The normal vector to
this plane we started off
with, it has the
component a, b, and c.
So if you're given
equation for plane here,
the normal vector to this
plane right over here,
is going to be ai
plus bj plus ck.
So it's a very easy thing to do.
If I were to give you
the equation of a plane--
let me give you a
particular example.
If I were to tell you that
I have some plane in three
dimensions-- let's say it's
negative 3, although it'll
work for more dimensions.
Let's say I have negative 3
x plus the square root of 2
y-- let me put it this
way-- minus, or let's say,
plus 7 z is equal to pi.
So you have this crazy--
I mean it's not crazy.
It's just a plane
in three dimensions.
And I say what is a normal
vector to this plane?
You literally can just pick
out these coefficients,
and you say, a normal
vector to this plane
is negative 3i plus
the square root of 2
plus 2 square root
of 2 j plus 7 k.
And you could ignore
the d part there.
And the reason why
you can ignore that
is that will just
shift the plane,
but it won't fundamentally
change how the plane is tilted.
So a this normal vector, will
also be normal if this was e,
or if this was 100, it would be
normal to all of those planes,
because all those
planes are just shifted,
but they all have
the same inclination.
So they would all kind of
point the same direction.
And so the normal vectors would
point in the same direction.
So hopefully you found
that vaguely useful.
We'll now build on this
to find the distance
between any point in three
dimensions, and some plane.
The shortest distance that
we can get to that plane.