Lesson 31: Surface integrals - I \(17.6\)
Warmup: What is a surface?
stack lines stack curves
eg: plane, sphere, cone, paraboloid
Accessible transcription generated on 4/6/2026
Warmup: What is a surface?
stack lines stack curves
eg: plane, sphere, cone, paraboloid
Representations of a curve:
Function: \(z = f(x,y) = x^2 - y\)
Level set: \(z = 0 \implies y = x^2\), which is a parabola.
Representation: \(\vec{r}(t)\)
Representations of a surface:
Function: \(w = f(x,y,z) = x^2 + y^2 - z\)
Level set: \(w = 0 \implies z = x^2 + y^2\), which is a paraboloid.
Representation: \(\vec{r}(u,v)\)
\(u, v\) lie in \(R\) in \(\mathbb{R}^2\)
\[\vec{r}(u,v) = \langle \cos u, \sin u, 2v \rangle, \quad 0 \le u \le \frac{3\pi}{2}, \quad 0 \le v \le 1.\]
\(v=0, \ 0 \le u \le \frac{3\pi}{2}\)
\(\vec{r}(u,0) = \langle \cos u, \sin u, 0 \rangle\)
\(v=1, \ 0 \le u \le \frac{3\pi}{2}\)
\(\vec{r}(u,1) = \langle \cos u, \sin u, 2 \rangle\)
fix \(v: 0 \le v \le 1\)
\(\vec{r}(u, "v") = \langle \cos u, \sin u, "2v" \rangle\)
stack \(\frac{3}{4}\)th circles of radius 1 from \(z=0\) to \(z=2\)
\[\downarrow\]
\(\frac{3}{4}\)th cylinder of radius 1 height 2
Consider the surface defined by the equation:
\[z = x^2 + y^2\]Parametrization:
We can parameterize this surface using \(u\) and \(v\) as follows:
\[x = u, \quad y = v, \quad z = u^2 + v^2\]This gives the vector-valued function:
\[\vec{r}(u,v) = \langle u, v, u^2 + v^2 \rangle\]Bounds:
\[-\infty < u < \infty\] \[-\infty < v < \infty\]What if we are only interested in the part of the surface between \(1 \le z \le 9\)?
Substituting our parametrization for \(z\), we get the condition:
\[1 \le z = u^2 + v^2 \le 9\]Consider the equation of a plane: \[4x + 3y + z = 12\] We can solve for \(z\) to get: \[z = 12 - 4x - 3y\] The parameterization is then defined by: \[\vec{r}(u,v) = \langle u, v, 12 - 4u - 3v \rangle\]
For the entire plane, the bounds are: \[-\infty < u < \infty\] \[-\infty < v < \infty\]
What if we want only the part of the plane in the 1st Octant?
In the first octant, the coordinates must satisfy: \[x \ge 0, \quad y \ge 0, \quad z \ge 0\] Translating these conditions into our parameters \(u\) and \(v\), we get: \[u \ge 0, \quad v \ge 0, \quad 12 - 4u - 3v \ge 0\]
Example: Parametrize a sphere of radius 2, centered at the origin.
The Cartesian equation for a sphere of radius 2 is:
\[x^2 + y^2 + z^2 = 4\]Solving for \(z\), we can describe the surface in two parts:
Alternatively, this surface is much simpler in spherical coordinates, where the radius \(\rho\) is constant:
\[\rho = 2\]The standard equations for converting from spherical to Cartesian coordinates are:
\[x = \rho \sin \phi \cos \theta\] \[y = \rho \sin \phi \sin \theta\] \[z = \rho \cos \phi\]By substituting \(\rho = 2\), we obtain the vector parametrization of the sphere:
\[\mathbf{r}(\phi, \theta) = \langle 2 \sin \phi \cos \theta, 2 \sin \phi \sin \theta, 2 \cos \phi \rangle\]The bounds for the parameters to cover the entire sphere are:
\[0 \le \theta \le 2\pi\] \[0 \le \phi \le \pi\]The following notes describe the formulation of surface integrals, using the analogy of line integrals for context.
For a line integral over a curve \(C\):
\[ \int_C f \, ds \]The infinitesimal arc length \(ds\) is defined as:
\[ ds = |\vec{r}'(t)| \, dt \]The integral over the curve is evaluated over the interval \([a, b]\) as:
\[ \int_C f \, ds = \int_a^b f(\vec{r}(t)) |\vec{r}'(t)| \, dt \]In the case where the function \(f = 1\), the integral yields the total length of the curve:
\[ \int_C 1 \, ds = \text{Arc length} \]The surface integral of a function \(f\) over a surface \(S\) is expressed as:
\[ \iint_S f \, dS \]In this expression, \(dS\) represents the infinitesimal area element, which is calculated using the magnitude of the cross product of the partial derivatives of the parameterization \(\vec{r}(u,v)\):
\[ dS = |\vec{r}_u \times \vec{r}_v| \, dA \]General Formula: The formula for evaluating the surface integral over the parameter region \(R\) is:
\[ \iint_S f \, dS = \iint_R f(\vec{r}(u,v)) |\vec{r}_u \times \vec{r}_v| \, dA \]When the function \(f = 1\), the integral represents the total area of the surface \(S\):
\[ \iint_S 1 \, dS = \text{Surface Area} \]Find the area of the part of the plane \(4x + 3y + z = 12\) in the \(1^{\text{st}}\) octant.
Solution:
\[\vec{r}(u, v) = \langle u, v, 12 - 4u - 3v \rangle\]where \(u, v\) are in \(R\).
Calculating the partial derivatives and their cross product:
\[\vec{r}_u = \langle 1, 0, -4 \rangle\] \[\vec{r}_v = \langle 0, 1, -3 \rangle\] \[\vec{r}_u \times \vec{r}_v = \langle 4, 3, 1 \rangle, \quad |\vec{r}_u \times \vec{r}_v| = \sqrt{26}\]The integral becomes:
\[\text{Area} = \iint_R \sqrt{26} \, dA = \sqrt{26} \iint_R 1 \, dA\] \[\text{Area} = \sqrt{26} \times \text{Area of } R = 6\sqrt{26}.\]eg: find area of surface parametrized by \[ \vec{r}(u,v) = \langle \cos u, \sin u, 2v \rangle, \quad 0 \le u \le \frac{3\pi}{2}, \quad 0 \le v \le 1 \]