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### Course: Physics archive > Unit 13

Lesson 1: Magnets and Magnetic Force# Cross product 2

A little more intuition on the cross product. Created by Sal Khan.

## Want to join the conversation?

- in cross product why we use Sine, but not Cosine(31 votes)
- The primary purpose of "cross product" is to calculate areas. If you have two vectors, u⃗ and v⃗ , the area of the parallelogram having those two vectors as two sides is, of course, "base times height". The "base" is the length of one of the vector, |u⃗ |, say. To Find the "height", draw a line from the tip of v⃗ perpendicular to u⃗ . That gives a right triangle having |v⃗ | as hypotenuse. The "height" is the length of the "opposite side" which is given by |v⃗ |sin(θ) where θ is the angle between the vectors. That is, the area of the parallelogram formed by vectors u⃗ and v⃗ is |u⃗ ||v⃗ |sin(θ).

A primary use of the dot product, on the other hand, is to find the projection of one vector on the other. Again, draw a line from the tip of u⃗ perpedicular to v⃗ . The projection of u⃗ onto v⃗ is now the near side of the right triangle produced. Its length is |u|cos(θ). To find the actual vector projection, multiply that length by a unit vector in the direction of v⃗ which is v⃗ /|v⃗ . That is, the vector projection of u⃗ on v⃗ is given by |u⃗ |cos(θ)[v⃗ /|v⃗ |] which we can simplify by multiplying both numerator and denominator by |v⃗ |:

|u⃗ ||u⃗ |cos(θ)|v⃗ |2v⃗

The numerator of that fraction is u⃗ ⋅v⃗ .

I have done the vectors and other math symbols by using "LaTeX" which is implemented on this board To see the code used, click on the formula or click on "quote". There are several tutorials on the internet.(13 votes)

- This isn't intuitive at all for me. If at2:57you do exactly what he said (index finger points in the direction of b and middle finger for a) with your right hand, i still get my thumb going into the screen, the same result as in the last video. How is he flexing his thumb to get it to point out of the page? I'm really confused.(23 votes)
- I struggled with this too, but I think if you keep you index finger straight (as in fully extended and in line with your arm), then you should be able to figure it out.(7 votes)

- if we multiply the vectors as a cross product, why do we get another different vector, not the area?

I really don't get the intuition... :S(6 votes)- This is how I answered another similar question, hope it helps you as well...

We're not really finding an area when we are multiplying 2 vectors. You may get that idea because when we usually multiply two lengths in basic maths, we get the area that those two lengths form between them. However, those two lengths are scalars, and not vectors (which have directions). So when you multiply vectors, not only are you multiplying the magnitudes, you are also multiplying the directions. It may not be intuitive, but that's how multiplying vectors work. The "getting an area from two values" idea only applies to multiplying two scalars. Hope this helps.(3 votes)

- I asked this to my teacher in school, but i didn't get a convincing answer. If the multiplying 2 vectors with cross product leads you to the third dimension, what happens when you multiply 3 vectors with cross product? a fellow student said out of the bloom that it would lead back to the plane, which i found very convincing, but my teacher didn't agree and kept saying other stuff uncomprehensively (that's why i love khan academy).. what is the right answer?(4 votes)
- so you agree that it's always gonna rotate between the 3 axes(planes)?

but in your example i noticed that the degree between angles was 90.. an interesting idea i thought about: if for example we have a and b as vectors. and the degree between them is 45. a being on the x axis, and b between x and y axes. "a x b" would result with c wich would be parallel/on to the z axis. Now if you multiply "c x a" you'd return to the y axis which is perpendicular to both because one is parallel to x-axis and the other to z-axis. however if you multiply "c x b" the plane that both lie on in the same time is the a new plane with axis with (mathematically speaking) x=y is the axis and the result would probably give us a new axis which is (if you put the ordinary plane of x, y in front of you) of degree 135,,, and you could go on circuling in each direction, and you'd probably get 8 vectors on each plane... :\

just a thought(2 votes)

- why do we use the right hand rule? i mean, im sure a guy didn't just say oh, the direction of the third vector can be found with our right hand, without having an reasoning to support it(3 votes)
- The point is that the three fingers of your right hand form the three axes of a 3D Cartesian system. Any two vectors lie on a single plane. The cross product finds a vector that is perpendicular to the plane, or perpendicular to both the vectors you're finding the cross product of. Your fingers just give you a visual representation. There are actually two vectors that are perpendicular, the one at 180 degrees to the one you find, which you'd get if you used the left hand. So, why the right hand? Just convention, it's got to be one of them... Why drive on the left or right side of the road? Neither is correct, it's just important everyone does the same.(6 votes)

- Can I get an example of why knowing the direction (in vs out) of the cross-product vector is important. Also, I am sorry to say that I don't think that I understand Sal's explanation of the right hand rule at all. I'll need to see a video of someone using their actually hand before I can understand it.(2 votes)
- Hi! It's ok if you don't understand some aspects of it, there's no one who get's a concept right in one go!

I'm not sure about the first part of your question, i.e., the necessity of the direction, but I think it's because a vector can't point in two directions.

Well, here's a link showing a pictorial representation of the right hand thumb rule. Hope it's clear?

https://en.wikipedia.org/wiki/Right-hand_rule#/media/File:Right_hand_rule_cross_product.svg

PLEASE CORRECT ME IF I'M WRONG :)(1 vote)

- is it always true that pointing up (out of page), and pointing down (into the page)? i am confused as to how Sal can tell it is into or out of page, when is is pointing up or down.(2 votes)
- At6:57|a|opp/|A| is confusing .|A| is a vector not a scalar.So how can you just convert a vector into scalar?(2 votes)
- When we take the absolute value of a vector it give us just the magnitude of the vector. That's intuitive; think what we mean when we're taking absolute values of pure numbers: We're figuring out the distance that our number is from our origin; it doesn't matter the direction (negative or positive). In a vector, we have infinite possibilities for direction. When we take the absolute value, we ignore the direction and take only the distance from the origin. When we're talking about vectors, that distance is what we mean when we say "magnitude". And magnitude is a scalar. So lAl is just another way of saying "the magnitude of A".(0 votes)

- How can you use this if the vectors are given in ijk form and there is no angle given(0 votes)
- I think if you do this graphically using a matrix, it's much easier to remember. I'll try to create one here. So you need to find the determinant of a 3x3 matrix. Let's say vector A=<Ax,Ay,Az> and vector B=<Bx,By,Bz>. Unit direction i, j, and k correspond to x, y, and z.

In this matrix, the first row is supposed to have a ^ on top of i,j, and k. I'm not sure if the formatting will come through.

| i^ j^ k^ |

| Ax Ay Az |

| Bx By Bz |

To find the determinant, you need to use sub-determinants. For example, starting with i^, you cross out the row and the column that contains i^ and multiply it by the 2x2 determinant left in this case:

|Ay Az|

|By Bz|

Same idea for j^, but there IS A NEGATIVE SIGN in front of j^ and you cross out the row and column that contain j^. You can find k^ the same way as i^, but crossing out the row and column that contain k^. The determinant of the 2x2 matrix gives you the magnitude and the unit vectors give the components of the vector.(1 vote)

- why dont we use right hand screw rule as it is more easier to understand for students who come across this topic for first time, and I am confused between right hand rule and left hand rule for what is it used for?; thank you for helping me!(1 vote)
- Right hand screw rule is the exact same thing as right hand thumb rule.

Fleming's left hand rule is used to relate the direction of force(F), magnetic field (B) and current(I) in a conductor.

The right hand thumb rule is used to find the direction of magnetic field propagated by a current carrying wire.(2 votes)

## Video transcript

Let's see if we can get a little
bit more practice and intuition of what cross products
are all about. So in the last example,
we took a cross b. Let's see what happens when
we take b cross a. So let me erase some of this. I don't want to erase all of it
because it might be useful to give us some intuition
to compare. I'm going to keep that. Actually, I can erase
this, I think. So the things I have drawn
here, this was a cross b. Let me cordon it off so you
don't get confused. So that was me using the right
hand rule when I tried to do a cross b, and then we saw that
the magnitude of this was 25, and n, the direction,
pointed downwards. Or when I drew it here, it would
point into the page. So let's see what happens with
b cross a, so I'm just switching the order. b cross a. Well, the magnitude is going to
be the same thing, right? Because I'm still going to take
the magnitude of b times the magnitude of a times the
sine of the angle between them, which was pi over 6
radians and then times some unit vector n. But this is going
to be the same. When I multiply scalar
quantities, it doesn't matter what order I multiply
them in, right? So this is still going to be
25, whatever my units might have been, times
some vector n. And we still know that that
vector n has to be perpendicular to both a and b,
and now we have to figure out, well, is it, in being
perpendicular, it can either kind of point into the page here
or it could pop out of the page, or point
out of the page. So which one is it? And then we take our right hand
out, and we try it again. So what we do is we take
our right hand. I'm actually using my right hand
right now, although you can't see it, just to make sure
I draw the right thing. So in this example, if I take
my right hand, I take the index finger in the
direction of b. I take my middle finger in the
direction of a, so my middle figure is going to look
something like that, right? And then I have two leftover
fingers there. Then the thumb goes in the
direction of the cross product, right? Because your thumb has a right
angle right there. That's the right angle
of your thumb. So in this example, that's the
direction of a, this is the direction of b, and we're
doing b cross a. That's why b gets your
index finger. The index finger gets the first
term, your middle finger gets the second term, and the
thumb gets the direction of the cross product. So in this example, the
direction of the cross product is upwards. Or when we're drawing it in two
dimensions right here, the cross product would actually
pop out of the page for b cross a. So I'll draw it over. It would be the circle
with the dot. Or if I were to draw it
analogous to this, so this right here, that
was a cross b. And then b cross a is the exact
same magnitude, but it goes in the other direction. That's b cross a. It just flips in the
opposite direction. And that's why you have to use
your right hand, because you might know that, oh, something's
going to pop in or out of the page, et cetera, et
cetera, but you need to know your right hand to know
whether it goes in or out of the page. Anyway, let's see if we can
get a little bit more intuition of what this is all
about because this is all about intuition. And frankly, I'll tell you, the
cross product comes into use in a lot of concepts that
frankly we don't have a lot of real-life intuition, with
electrons flying through a magnetic field or magnetic
fields through a coil. A lot of things in our everyday
life experience, maybe if we were metal filings
living in a magnetic field-- well, we do live in
a magnetic field. In a strong magnetic field,
maybe we would get an intuition, but it's hard to have
as deep of an intuition as we do for, say, falling
objects, or friction, or forces, or fluid dynamics even,
because we've all played with water. But anyway, let's get a little
bit more intuition. And let's think about why is
there that sine of theta? Why not just multiply the
magnitudes times each other and use the right hand rule and
figure out a direction? What is that sine of
theta all about? I think I need to clear this up
a little bit just so this could be useful. So why is that sine
of theta there? Let me redraw some vectors. I'll draw them a
little fatter. So let's say that's a,
that's a, this is b. b doesn't always have
to be longer than a. So this is a and this is b. Now, we can think of
it a little bit. We could say, well, this is the
same thing as a sine theta times b, or we could say this
is b sine theta times a. I hope I'm not confusing-- all
I'm saying is you could interpret this as--
because these are just magnitudes, right? So it doesn't matter what order
you multiply them in. You could say this is a sine
theta times the magnitude of b, all of that in the direction
of the normal vector, or you could put the
sine theta the other way. But let's think about what
this would mean. a sine theta, if
this is theta. What is a sine theta? Sine is opposite over
hypotenuse, right? So opposite over hypotenuse. So this would be the
magnitude of a. Let me draw something. Let me draw a line here and
make it a real line. Let me draw a line there,
so I have a right angle. So what's a sine theta? This is the opposite side. So a sine theta is a, and sine
of theta is opposite over hypotenuse. The hypotenuse is the magnitude
of a, right? So sine of theta is equal to
this side, which I call o for opposite, over the
magnitude of a. So it's opposite over
the magnitude of a. So this term a sine theta is
actually just the magnitude of this line right here. Another way you could--
let me redraw it. It doesn't matter where the
vectors start from. All you care about is this
magnitude and direction, so you could shift vectors
around. So this vector right here, and
you could call it this opposite vector, that's the
same thing as this vector. That's the same thing as this. I just shifted it away. And so another way to think
about it is, it is the component of vector a, right? We're used to taking a vector
and splitting it up into x- and y-components, but now we're
taking a vector a, and we're splitting it up into--
you can think of it as a component that's parallel to
vector b and a component that is perpendicular to vector b. So a sine theta is the magnitude
of the component of vector a that is perpendicular
to b. So when you're taking the cross
product of two numbers, you're saying, well, I don't
care about the entire magnitude of vector a in this
example, I care about the magnitude of vector a that is
perpendicular to vector b, and those are the two numbers that
I want to multiply and then give it that direction
as specified by the right hand rule. And I'll show you some
applications. This is especially important--
well, we'll use it in torque and we'll also use it in
magnetic fields, but it's important in both of those
applications to figure out the components of the vector that
are perpendicular to either a force or a radius in question. So that's why this cross product
has the sine theta because we're taking-- so in
this, if you view it as magnitude of a sine theta
times b, this is kind of saying this is the magnitude
of the component of a perpendicular to b, or
you could interpret it the other way. You could interpret it as a
times b sine theta, right? Put a parentheses here. And then you could view
it the other way. You could say, well, b sine
theta is the component of b that is perpendicular to a. Let me draw that, just to
hit the point home. So that's my a, that's my b. This is a, this is b. So b has some component of it
that is perpendicular to a, and that is going to look
something like-- well, I've run out of space. Let me draw it here. If that's a, that's b, the
component of b that is perpendicular to a is going
to look like this. It's going to be perpendicular
to a, and it's going to go that far, right? And then you could go back to
SOH CAH TOA and you could prove to yourself that the
magnitude of this vector is b sine theta. So that is where the sine
theta comes from. It makes sure that we're not
just multiplying the vectors. It makes sure we're multiplying
the components of the vectors that are
perpendicular to each other to get a third vector that is
perpendicular to both of them. And then the people who invented
the cross product said, well, it's still ambiguous
because it doesn't tell us-- there's always two
vectors that are perpendicular to these two. One goes in, one goes out. They're in opposite
directions. And that's where the right
hand rule comes in. They'll say, OK, well, we're
just going to say a convention that you use your right hand,
point it like a gun, make all your fingers perpendicular,
and then you know what direction that vector
points in. Anyway, hopefully, you're
not confused. Now I want you to watch
the next video. This is actually going to be
some physics on electricity, magnetism and torque, and
that's essentially the applications of the cross
product, and it'll give you a little bit more intuition
of how to use it. See you soon.