8. Properties of Curves

a. Vector Functions, Position, Velocity and Plots

Not all vector functions are position vectors or parametric curves.

2. Vector Functions: Velocity and Force

Velocity

Three pages from now, we will define the velocity of a curve as the derivative of the position vector. \[ \vec{v}(t)=\langle v_1(t),v_2(t),v_3(t)\rangle =\dfrac{d\vec{r}}{dt} =\left\langle \dfrac{dx}{dt},\dfrac{dy}{dt},\dfrac{dz}{dt}\right\rangle \] We do not regard the velocity vectors as located at the origin. Rather, we regard the velocity vector \(\vec{v}(t)\) at time \(t\) to be located at the point \(\vec{r}(t)\), the tip of the position vector.

Plot the spiral \(\vec{r}(t)=(t\cos t,t\sin t)\), its position vector and its velocity vector \[ \vec{v}(t)=\langle \cos t-t\sin t,\sin t+t\cos t\rangle \] for \(\pi \le t \le 4\pi\). (You are not yet expected to be able to do all this yourself.)


The parametric curve is in blue.
Its position vector is in red.
Its velocity vector is in magenta.

The plot shows a spiral in blue with several radial arrows in red
    going from the origin to various points on the spiral, labeled by r.
    In addition, there are arrows tangent to the spiral at the tip of each
    radial arrow, in magenta, labeled by v.
The video shows a spiral being traced out with one radial arrow,
    in red, labeled r, from the origin to the current point on the spiral.
    In addition, there is a magenta arrow at the current point pointing in the
    direction of the curve. The position and velocity vectors grow in length
    at the same rate.

Before defining the velocity, we need to define a derivative and before we define a derivative we need to define a limit.

Force

A force is an example of a vector field which we defined in the chapter on Vectors. To plot the force vector we put the tail of each vector at the point where it is evaluated. If an object moves along a curve due to the action of a force, then the force must be evaluated at the position of the particle, and we only plot the force vectors at points on the curve.

A charged particle moves along the parabola \(y=16-(x-4)^2\) parametrized as \(\vec{r}(t)=\left\langle t,16-(t-4)^2\right\rangle\) under the action of an electric field \(\vec{F}(x,y)=\left\langle x,10-y\right\rangle\) which on the curve is \(\vec{F}(t)=\left\langle t,(t-4)^2-6\right\rangle\). Plot the curve and the vector field for \(-2 \le t \le 10\).

The first two graphics show the curve and the electric field separately. The third graphic contains both the curve and the electric field superimposed in the same plot, and the last graphic shows the electric field expressed along the curve at integers from \(x=-2\) to \(x=10\). (Note: All the vectors have been shortened by a factor of \(8\) so the arrows will not overlap.)

The plot shows a parabola opening down.
The curve.
The plot shows the electric field as a bunch of arrows pointing upward
    at the bottom of the plot and spreading out left (on the left) and right
    (on the right) as we move up in the plot.
The electric field at all points.
The plot shows the parabola and the vector field overlayed.
The curve in the electric field.
The plot shows the parabola and the vectors in the vector field that 
    originate on the parabola.
The electric field on the curve.

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Supported in part by NSF Grant #1123255

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