X Coordinate

So that's going to be the x coordinate.

Our velocity vector as a function of time is going to be equal to the derivative of our x position as a function of time, or we could say the velocity in the x direction times the i unit vector, plus the velocity in the y direction times the j unit vector.

So the acceleration vector as a function of time is just going to be the second derivative of x with respect to t, or you'd say the acceleration in the x direction as a function as a function of time times i, plus the acceleration in the y direction.

For t is greater than or equal to 0, the derivative of x with respect to t is 4t 1 the derivative of y with respect to t is sin(t 2) and at time t 0, x(0) 0 and y(0) 4

And then y coordinate is going to be the y coordinate coordinate of B plus the y coordinate of the origin.

Y Coordinate

X axis

On the horizontal axis, we have Period.

That was our second coordinate.

That is the x axis.

Our first coordinate is going to be multiples of v1.

X position of main window

The X position of the main window.

X position of assistant window

The X position of the assistant window.

That's my x axis.

That is my x axis.

And maybe in the x direction they're constant, regardless of your level of x, the magnitude stays.

So that's why Period is on the horizontal axis.

Now, the second coordinate tells you increments of v2.

This is our x axis.

Next, remove the two X axis shipping blocks holding the ram in place in the X axis direction

The y coordinate of the origin is 0 divided by 2.

It's just B over 2 on the y coordinate.

So this is what its representation is in the B coordinate system.

Only this guy survives.

Now in our new system, what's our first coordinate?

And if I were to draw the x axis, the x axis would kind of pop out of the middle right there.

So that is our y axis, and this is our x axis.

Each circle represents an hourly measurement by a single telescope as a function of time (day of year on the abscissa) and the asymptotic longitude of the viewing direction (in degree on the ordinate).

This fairly simple example, all of the vectors point in the x direction.

Economies of scale gave rise to this sigmoidal behavior.

That is the x axis, and that is the y axis.

This will give me the coordinate of the midpoint between origin and B.

So the only term that's going to be non zero is the 2 times the 1.

Now we will check roll along the X axis

So I multiply x by c inverse then I get the b coordinates for x.

So that's going to be how it's changing in the x direction, and in the y direction we do something very similar.

Then we will check for roll along X axis travel

And the thing that's driving is on the horizontal, the thing that's being driven is on the vertical.

So you could almost view this as a traditional x and y.

You know, that would be the y axis there, and the x axis would pop out the middle.

This provides two values along the Y axis and along the X axis

And what a unit vector is, so the i hat vector goes in the positive x direction.