Chapter 40
By the end of this section, you should be able to answer the following questions:
Another way of representing a surface $S$ in $\R^3$ is by a parametrisation.
This
is where the coordinate variables are functions of two parameters $u$ and $v$:
$$
x=x(u,v),\ \ y=y(u,v),\ \ z=z(u,v)
$$
and the vector
$$
\r(u,v) = x(u,v)~\i+y(u,v)~\j+z(u,v)~\k
$$
traces out the surface as $u,v$ vary over some region $D$ in the
"$uv$-plane".
So for every point $(u,v)$ in $D,$ there corresponds a point on
the surface $S$.
The following diagram shows the point $P$ on the surface $S$ which corresponds to the point $(u,v)$ in the region $D$ in the $uv$-plane. As $(u,v)$ moves around all points in $D,$ the point $P$ moves around in $S,$ tracing out the entire surface.
Note that a surface defined explicitly by $z=f(x,y)$ is equivalent to a parametrisation $$ \r(x,y) = x~\i+y~\j+f(x,y)~\k, $$ where we treat the coordinate variables $x$ and $y$ as the parameters. Note that we have not specified any bounds on the variables. Often the challenge is to not only find suitable functions for a parametrisation, but for a finite surface to determine bounds on the parameters.
A good motivation to use parametrisations is that sometimes surfaces cannot be the graphs of functions defined as
$z=f(x,y).$
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Another reason is given by the limitations of the computer considering the expression $z= f(x,y).$ For example if we try to plot
$x^2+y^2+z^2=4.$
We can use our knowledge of cylindrical and spherical coordinates to parametrise certain surfaces with which these coordinates are naturally associated.
Recall cylindrical coordinates: $$ x=r\cos\theta,\ \ y=r\sin\theta,\ \ z=z. $$ Setting exactly one of the cylindrical coordinates to a constant value necessarily gives a parametric surface.
% Define components as anonymous functions
fx = @(u,v) 1.4 * (exp(u/29) - 1).* cos(u) .* (cos(v/2)).^2;
fy = @(u,v) 1.4 * (1 - exp(u/29)) .* sin(u) .* (cos(v/2)).^2;
fz = @(u,v) .7 * (exp(u/29).* sin(v) - exp(u/16) - sin(v)+3);
% Plot surface
fsurf(fx,fy,fz,[0 6*pi 0 2*pi])
camlight % Fancy shading
title('Parametric surface')
xlabel('x');
ylabel('y');
zlabel('z');
box on % Add frame
fx = @(u,v) 1.4 * (exp(u/29) - 1).* cos(u) .* (cos(v/2)).^2;
fy = @(u,v) 1.4 * (1 - exp(u/29)) .* sin(u) .* (cos(v/2)).^2;
fz = @(u,v) .7 * (exp(u/29).* sin(v) - exp(u/16) - sin(v)+3);
fsurf(fx,fy,fz,[0 6*pi 0 2*pi])
Setting $z=2$ with $0\leq\theta\leq 2\pi,$ $0\leq r\leq 3$ describes a disc of radius 3, centred at the $z$ axis lying in the plane $z=2:$
Surface(r cos(θ), r sin(θ), 2, r, 0, 3, θ, 0, 2 π)
Setting $r=5$ with $0\leq\theta\leq 2\pi,$ $1\leq z\leq 3$ describes the surface of a cylinder of radius 5 and of height 2 between $z=1$ and $z=3:$
Surface(5 cos(θ), 5 sin(θ), z, z, 1, 3, θ, 0, 2 π)
Setting $\theta = \pi/2$ with $2\leq z\leq 4,$ $0\leq r\leq 1$ describes a rectangle lying in the $yz$-plane. Another description of the same surface would be $x=0, \ \{ (y,z)\ |\ 0\leq y\leq 1,\ 2\leq z\leq 4\}:$
Surface(r cos(Ï€/2), r sin(Ï€/2), z, r, 1, 3, z, 2, 4)
How can you do this?
Recall spherical coordinates: $$ x=r\cos\theta\sin\phi,\ \ y=r\sin\theta\sin\phi,\ \ z=r\cos\phi. $$
Setting exactly one of the spherical coordinates to a constant value necessarily gives a parametric surface.
Setting $r=2$ with $0\leq\theta\leq 2\pi,$ $0\leq\phi\leq \pi$ describes the surface of a sphere of radius 2 centred at the origin:
Surface(2 cos(θ) sin(ϕ), 2 sin(θ) sin(ϕ), 2 cos(ϕ), θ, 0, 2 π ,ϕ, 0, π)
Setting $\phi=\pi/3$ with $0\leq r\leq 2,$ $0\leq \theta\leq 2\pi$ describes the open cone with angle $\pi/3$ to the positive $z$-axis, the "mouth" of which lies on the sphere of radius 2 and with vertex located at the origin:
Surface(r cos(θ) sin(π/3), r sin(θ) sin(π/3), r cos(π/3), r, 0, 2, θ, 0, π)
Setting $\theta =0$ with $0\leq r\leq 3,$ $0\leq\phi\leq\pi$ describes the half disc of radius 3 lying in the $xz$-plane:
Surface(r cos(0) sin(ϕ), r sin(0) sin(ϕ), r cos(ϕ), r, 0, 2, ϕ, 0, π)
How can you do this?
See online demo here
Let $S$ be a surface parametrised by $$ \r(u,v) = x(u,v)~\i+y(u,v)~\j+z(u,v)~\k. $$
Here we find the tangent plane to $S$ at a point $P$ specified by $\r(a,b)$. There are two important families of curves on $S$. One where $u$ is a constant, the other where $v$ is a constant.
$\r(u,v) = x(u,v)~\i+y(u,v)~\j+z(u,v)~\k.$
Here we find the tangent plane to $S$ at a point $P$ specified by $\r(a,b)$. There are two important families of curves on $S$. One where $u$ is a constant, the other where $v$ is a constant.
The diagram below shows the relationship between horizontal and vertical lines in $D$ (in the $uv$-plane) and curves on $S$.
Setting $u=a$ defines a curve on $S$ parametrised by $\r(a,v)$, for all values of $v$ such that $(a,v)$ lies in $D$. A tangent vector to this curve at $P$ is
$\ds \r_v = \frac{\partial x}{\partial v}(a,b)~\i+\frac{\partial y}{\partial v}(a,b)~\j+\frac{\partial z}{\partial v}(a,b)~\k.$
Similarly setting $v=b$ defines another curve on $S$ parametrised by $\r(u,b)$. A tangent vector to this curve at $P$ is
$\ds \r_u = \frac{\partial x}{\partial u}(a,b)~\i+\frac{\partial y}{\partial u}(a,b)~\j+\frac{\partial z}{\partial u}(a,b)~\k.$
If $\r_u$ and $\r_v$ are continuous and $\r_u\times\r_v$ is never $\mathbf 0$ inside $D$ (we make an exception for points on the boundary of $D$), we call the surface smooth (it has no "kinks").
For a smooth surface, $\r_u\times\r_v$ is a normal vector at any point inside $D.$ This vector evaluated at $(u,v)=(a,b)$ is also normal to the tangent plane at the point $P=(x(a,b),y(a,b),z(a,b)).$
The equation of the tangent plane at $P$ is given by
$\ds \big(\r_u(a,b)\times\r_v(a,b)\big)\cdot \big((x~\i+y~\j+z~\k) - \r(a,b)\big)=0.$
$\r_u $ $=2u~\i + 0~\j + 1~\k,$ $\quad $ $\r_v $ $=0~\i + 2v~\j + 2~\k $
$\r_u\times\r_v$ $= \left| \begin{array}{ccc} \i & \j & \k\\ 2u & 0 & 1 \\ 0 & 2v & 2 \end{array} \right|$ $ =-2v~\i - 4u~\j + 4uv~\k$
Point $(1,1,3) $ corresponds to $u=1,v=1,$
since $u^2=1, ~v^2=1,~u+2v=3;$
and $\r_u\times \r_v\big|_{(1,1)} =-2~\i-4~\j+4~\k .$
$\r_u\times\r_v $ $ =-2v~\i - 4u~\j + 4uv~\k$
and $\r_u\times \r_v\big|_{(1,1)} =-2~\i-4~\j+4~\k .$
Using the equation of the tangent plane
$\ds \big(\r_u\times \r_v\big|_{(1,1)} \big)\cdot \big((x~\i+y~\j+z~\k) -( \i+\j+3~\k)\big)=0,$
we obtain
$\ds-2(x-1)-4(y-1)+4(z-3)=0.$