# Parametric vector equations

You can find the vector equation of any straight line through 3D space, but suppose a mathematical model you were working on required the vector equation of a general curve through 3D space - such as a roller coaster, or trajectory of a satellite.
A parametric curve is defined by a function. The function can be given any real number, known as the parameter t (from a chosen segment of the real number line [a, b]) and returns a vector, the point on the line corresponding to t. That is, it is a mapping from the segment [a,b] -> R3 3D space.
A convenient way of writing this mapping is with three normal functions, each a mapping from [a,b] -> R:
x = f(t)
y = g(t)
z = h(t)
for each of the cartesian components of the vector returned by the earlier mapping. Here are some examples...

### Parametric equation of a circle

 From the diagram it can be seen that, if we choose t from the interval [0, 2p] and map t to the vector (cos t, sin t, 0) we get the unit circle. The separate functions are: x = cos t y = sin t z = 0

What curve is given by adding coefficients,
x = a cos t
y = b sin t
z = 0
for some real numbers a and b?

### Parametric equation of a cylindrical spiral

 The parameter, t, can be thought of as time, and the unit circle above is then traced out by a point which starts at (1,0,0) at t = 0 and follows the circular path counterclockwise (looking down the z axis towards -ve inf.) until it arrives back there at t = 2p. Now if the z function is changed from z = 0 to z = t, the point will rise steadily as the circular path is traversed, so creating the sprial shown.

Thinking of the curve as being traced out by a particle with the parameter t representing the time is used in Newtonian mechanics. The parametric functions above give the position of the particle at any time t, and if you have started calculus, differentiating each of the three equations (for x, y and z) with respect t, results in a new parametric curve - the positions of the points on this curve giving the velocity of the particle at any time t. Differentiating again give the acceleration at any time t.

### Parametric equation of a cardiod

 x = (cos t)(1 - sin t) y = (sin t)(1 - sin t) z = 0

### Parametric equation of Archimedes' spiral

 The spiral found by Archimedes, and also found in nature: x = t cos t y = t sin t z = 0

### Parametric equation of the Lissajous curves

 The curves of Lissajous are the set with equations: x = cos pt y = sin qt z = 0 for any p, q belonging to the integers. (the curve on the left has p = 3, q = 5)

### Some more complicated parametric equations

 The butterfly fly curve, discovered by Temple H. Fay, is generated by the equations x = (cos t)(ecos t - 2cos 4t - sin5(t/12)) y = (sin t)(ecos t - 2cos 4t - sin5(t/12)) z = 0 for t belonging to [0, 24p]

Just as a note, this form of equations isn't anything different to what was covered earlier. For example the vector equation of a line was written,
r(t) = a + t (b - a )
which is the same as,
x = a1(1 - t) + b1t
y = a2(1 - t) + b2t
z = a3(1 - t) + b3t

Contents
Parametric Applet