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# Introduction to vector components

Vectors are quantities that have a magnitude and a direction. In the two-dimensional plane, we can describe them in an equivalent way, by thinking about the changes in x and y from the vector's tail to its head. Created by Sal Khan.

## Want to join the conversation?

- Could I get a refresher on the 30-60-90 triangle rule?(4 votes)
- The ratio between them is 1:sqrt of 3:2 where 1 is the side opposite to 30 degree angle, sqrt of 3 is opposite to 60, and 2 to 90.(4 votes)

- What is the tail and head of a vector quantity?(3 votes)
**Tail of a vector**is the initial (starting) point of a vector.

While, head of the vector is its opposite.**Head of the vector**simply means the vector's final (end point) point.(4 votes)

- Why do many of the practice/quiz problems state the vectors as "from the __ (ex. southward) direction" but actually are headed in that direction? Shouldn't the vector then be pointed north if it comes from the south?(2 votes)
- In physics, vectors are typically defined by their magnitude (length) and direction. The direction of a vector is usually given relative to a specific reference frame, such as north, east, south, and west.

When we say a vector is "from the southward direction," we mean that its direction is southward. So, the vector is pointing in the southward direction, not northward. In this case, the vector is pointing in the direction from which it originates, which is southward.

It's important to remember that the direction of a vector is independent of its position in space. So, even if a vector is positioned at a particular point, it still has a direction that is defined relative to a reference frame.(2 votes)

- Are two vectors with the same Δx and Δy, but different head and tail coordinate values the same vector?(2 votes)
- Yes, two vectors with the same Δx and Δy but different head and tail coordinate values would always be the same vector. This is true because vectors are defined solely by their magnitude and direction, and if they have the same Δx and Δy, they will also have the same magnitude and direction, and thus will be the same exact vector.(1 vote)

- At2:12what part of trigonometry/geometry did Khan use to find Dx,Dy?(2 votes)
- In the second example, how would you solve it if a right triangle wasn't formed? What would an example of that look like?(1 vote)
- You can always form a right triangle with legs of any two lengths you want. Just put the segments at right angles to each other, and join the endpoints to draw the hypotenuse.(2 votes)

## Video transcript

- [Instructor] In other
videos, we have talked about how a vector can
be completely defined by a magnitude and a
direction, you need both. And here we have done that. We have said that the magnitude of vector a is equal to three units, these parallel lines here on both sides, it looks like a double absolute value. That means the magnitude of vector a. And you can also specify
that visually by making sure that the length of this vector
arrow is three units long. And we also have its direction. We see the direction of
vector a is 30 degrees counter-clockwise of due East. Now in this video, we're
gonna talk about other ways or another way to specify
or to define a vector. And that's by using components. And the way that we're gonna do it is, we're gonna think about the tail of this vector and the
head of this vector. And think about as we go
from the tail to the head, what is our change in x? And we could see our change in x would be that right over there. We're going from this x
value to this x value. And then what is going
to be our change in y. And if we're going from
down here to up here, our change in y, we can
also specify like that. So let me label these. This is my change in x, and
then this is my change in y. And if you think about it, if someone told you your
change in x and change in y, you could reconstruct this
vector right over here by starting here, having that change in x, then having the change in y
and then defining where the tip of the vector would be
relative to the tail. The notation for this is
we would say that vector a is equal to, and we'll have parenthesis, and we'll have our change
in x comma, change in y. And so if we wanted to get tangible for this particular
vector right over here, we know the length of
this vector is three. Its magnitude is three. We know that this is, since
this is going due horizontally and then this is going
straight up and down. This is a right triangle. And so we can use a little
bit of geometry from the past. Don't worry if you need a little
bit of a refresher on this, but we could use a little bit of geometry, or a little bit of
trigonometry to establish, if we know this angle,
if we know the length of this hypotenuse, that
this side that's opposite the 30 degree angle is gonna
be half the hypotenuse, so it's going to be 3/2. And that the change in x is going to be the square root of three times the 3/2. So it's going to be three,
square roots of three over two. And so up here, we would
write our x component is three times the square
root of three over two. And we would write that
the y component is 3/2. Now I know a lot of you might be thinking this looks a lot like coordinates
in the coordinate plane, where this would be the x coordinate and this would be the y coordinate. But when you're dealing with vectors, that's not exactly the interpretation. It is the case that if the vector's tail were at the origin right
over here, then its head would be at these coordinates
on the coordinate plane. But we know that a vector is not defined by its position, by the
position of the tail. I could shift this vector around wherever and it would still be the same vector. It can start wherever. So when you use this
notation in a vector context, these aren't x coordinates
and y coordinates. This is our change in x,
and this is our change in y. Let me do one more example to show that we can actually go the other way. So let's say I defined some vector b, and let's say that its x
component is square root of two. And let's say that its y
component is square root of two. So let's think about what
that vector would look like. So it would, if this is its tail, and its x component which is its change in x is square root of two. So it might look something like this. So that would be change in x
is equal to square root of two. And then its y component would
also be square root of two. So I could write our change in y over here is square root of two. And so the vector would
look something like this. It would start here and
then it would go over here, and we can use a little bit of geometry to figure out the magnitude and the direction of this vector. You can use the Pythagorean
theorem to establish that this squared plus this squared is gonna be equal to that squared. And if you do that,
you're going to get this having a length of two, which tells you that the magnitude of
vector b is equal to two. And if you wanted to figure
out this angle right over here, you could do a little bit of trigonometry or even a little bit
of geometry recognizing that this is going to be a
right angle right over here, and that this side and that
side have the same length. So these are gonna be the same angles which are gonna be 45 degree angles. And so just like that, you could
also specify the direction, 45 degrees counter-clockwise of due East. So hopefully you appreciate
that these are equivalent ways of representing a vector. You either can have a
magnitude and a direction, or you can have your components and you can go back and
forth between the two. And we'll get more practice
of that in future videos.