We've already made a few definitions of operations that
we can do with vectors.
We've defined addition in the context of vectors
and you've seen that.
If you just have two vectors, say a1, a2, all the
way down to a n.
We defined the addition of this vector and let's say some
other vector, b1, b2, all the way down to
bn as a third vector.
If you add these two, we defined the addition operation
to be a third-- you will result in a third vector where
each of its components are just the sum of the
corresponding components of the two vectors you're adding.
So it's going to be a1 plus b1, a2 plus b2, all the way
down to a n plus bn.
We knew this and we've done multiple videos where we use
this definition of vector addition.
We also know about scalar multiplication.
Maybe we should just call it scaling multiplication.
And that's the case of look, if I have some real number c
and I multiply it times some vector, a1, a2, all the way
down to a n, we defined scalar multiplication of a vector to
be-- some scalar times its vector will result in
essentially, this vector were each of its components are
multiplied by the scalar.
ca1, ca2, all the way down to c a n.
And so after seeing these two operations, you might be
tempted to say, gee, wouldn't it be nice if there was some
way to multiply two vectors.
This is just a scalar times a vector, just scaling it up.
And that's actually the actual effect of what it's doing if
you visualize it in three dimensions or less.
It's actually scaling the size of the vector.
And we haven't defined size, very precisely just yet.
But you understand at least this operation.
For multiplying vectors or taking the product, there's
actually two ways.
And I'm going to define one of them in this video.
And that's the dot product.
And you signify the dot product by saying a dot b.
So they borrowed one of the types of multiplication
notations that you saw, but you can't write across here.
That'll be actually a different type of vector
multiplication.
So the dot product is-- it's almost fun to take because
it's mathematically pretty straightforward, unlike the
cross product.
But it's fun to take and it's interesting because it
results-- so this is a1, a2, all the way down to a n.
That vector dot my b vector: b1, b2, all the way down to bn
is going to be equal to the product of each of their
corresponding components.
So a1 b1 added together plus a2 b2 plus a3 b3 plus all the
way to a n, bn.
So what is this?
Is this a vector?
Well no, this is just a number.
This is just going to be a real number.
You're just taking the product and adding together a bunch of
real numbers.
So this is just going to be a scalar, a real scalar.
So this is just going to be a scalar right there.
So in the dot product you multiply two vectors and you
end up with a scalar value.
Let me show you a couple of examples just in case this was
a little bit too abstract.
So let's say that we take the dot product of the vector 2, 5
and we're going to dot that with the vector 7, 1.
Well, this is just going to be equal to 2 times 7 plus 5
times 1 or 14 plus 6.
No, sorry.
14 plus 5, which is equal to 19.
So the dot product of this vector and this vector is 19.
Let me do one more example, although I think this is a
pretty straightforward idea.
Let me do it in mauve.
OK.
Say I had the vector 1, 2, 3 and I'm going to dot that with
the vector minus 2, 0, 5.
So it's 1 times minus 2 plus 2 times 0 plus 3 times 5.
So it's minus 2 plus 0 plus 15.
Minus 2 plus 15 is equal to 13.
That's the dot product by this definition.
Now, I'm going to make another definition.
I'm going to define the length of a vector.
And you might say, Sal, I know what the length
of something is.
I've been measuring things since I was a kid.
Why do I have to wait until a college level or hopefully
you're taking this before college maybe.
But what is now considered a college level course to have
length defined for me.
And the answer is because we're abstracting things to
well beyond just R3 or just three-dimensional space is
what you're used to.
We're abstracting that these vectors could have 50
components.
And our definition of length will satisfy, will work, even
for these 50 component vectors.
And so my definition of length-- but it's also going
to be consistent with what we know length to be.
So if I take the length of a and the notation we use is
just these double lines around the vector.
The length of my vector a is equal to-- and this is a
definition.
It equals the square root of each of the terms, each of my
components, squared.
Add it up.
Plus a2 squared plus all the way to plus a n squared.
And this is pretty straightforward.
If I wanted to take let's call this was vector b.
If I want to take the magnitude of vector b right
here, this would be what?
This would be the square root of 2 squared plus 5 squared,
which is equal to the square root of-- what is this?
This is 4 plus 25.
The square root of 29.
So that's the length of this vector.
And you might say look, I already knew that.
That's from the Pythagorean theroem.
If I were to draw my vector b-- let me draw it.
Those are my axes.
My vector b if I draw it in standard
form, looks like this.
I go to the right 2.
1, 2.
And I go up 5.
1, 2, 3, 4, 5.
So it looks like this.
My vector b looks like that.
And from the Pythagorean theorem you know look, if I
wanted to figure out the length of this vector in R2,
or if I'm drawing it in kind of two-dimensional space, I
take this side which is length 2, I take that side which is
length 5; this is going to be the square root from the
Pythagorean theorem of 2 squared plus 5 squared.
Which is exactly what we did here.
So this definition of length is completely consistent with
your idea of measuring things in one-, two- or
three-dimensional space.
But what's neat about it is that now we can start thinking
about the length of a vector that maybe has 50 components.
Which you know, really to visualize it in our
traditional way, makes no sense.
But we can still apply this notion of length and start to
maybe abstract beyond what we traditionally
associate length with.
Now, can we somehow relate length with the dot product?
Well what happens if I dot a with itself?
What is a dot a?
So that's equal to-- I'll just write it out again.
a1, all the way down to a n dotted with a1 all the way
down to a n.
Well that's equal to a1 times a1, which is a1 squared.
Plus a2 times a2.
a2 squared.
Plus all the way down, keep doing that all the way down to
a n times a n, which is a n squared.
But what's this?
This is the same thing as the thing you
see under the radical.
These two things are equivalent.
So we could write our definition of length, of
vector length, we can write it in terms of the dot product,
of our dot product definition.
It equals the square root of the vector dotted with itself.
Or, if we square both sides, we could say that our new
length definition squared is equal to the dot product of a
vector with itself.
And this is a pretty neat-- it's almost trivial to
actually prove it, but this is a pretty neat outcome and
we're going to use this in future videos.
So this is an introduction to what the dot product
is, what length is.
In the next video I'm going to show a bunch of
properties of it.
It will almost be mundane, but I want to get all those
properties out of the way, so we can use
them in future proofs.