Examples of 'vector right' in a sentence

Meaning of "vector right"

vector right: This phrase is commonly used in mathematics or physics to describe a vector that is orthogonal or perpendicular to a given vector. It signifies the direction that is at a right angle to the original vector

How to use "vector right" in a sentence

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vector right
So this vector right here must be perpendicular to n.
Three man squad closing on my vector right now.
So this vector right here is the vector x plus y.
You could define sum vector right there.
That vector right there is r of b.
Av times this vector right here.
This vector right here is the magnitude of a sine theta.
This is the vector right there.
Well this is all of the linear combinations of this vector right here.
I get this vector right here.
I can represent this guy with this green vector plus this vector right here.
Closing on my vector right now.
And this vector right here is clearly a member of my null space.
I am just translating this vector right over here.
That vector right here.

See also

The point specified by this vector right here.
I have that vector right there along that line.
So let me make a big version of the vector right there.
This vector right there.
So lets break down this vector right over here.
This vector right here in green, and this vector in red.
So let me draw my vector right there.
So this vector right here is the rotation by an angle of theta counterclockwise of c, x.
So this is the normal vector right over here.
So this vector right here is a cosine theta ; the magnitude of a cosine theta.
It would put me little super small vector right there.
And then this vector right there would be the vector a minus b.
You can define some unit vector right here.
Just this vector right here would be an orthonormal basis for just the span of v1.
And let me translate that vector right over there.
I get this vector right here . So I already figured out what they are.
And so a gets mapped to the zero vector right there.
So the magnitude of that vector right there is the magnitude of b cosine of theta.
It equals the set of the zero vector right there.
You can not represent this vector right there with some combination of those two vectors.
And that essentially gets you a vector right there.
So A times this vector right here is indeed equal to b.
The sum of these two vectors is this vector right here.
So let us have a vector right here . That is vector a.
So when t is equal to a, we are at this vector right here.
You can define some unit vector right here . You could define sum vector right there.
It's going to be perpendicular to this vector right here.
So that vector right there is x2.
And then I have this vector right here.
Likewise, this vector right here has a 1 in the fourth position.
That's my next position vector right there.
Well if this vector right here is a cosine theta -- and you.
So the transformation of x2 is that vector right there.
This vector right here in r3 got mapped to this vector in r2 by our function.
And so r of a will be this vector right here that ends at that point.

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