Coverage: Comprehensive — all course material (Lessons 1–37)

Exam Date: Tuesday, May 05, 2026

Time: 1:00 PM - 3:00 PM

Location: Announced on Brightspace

Stokes' Theorem [Lessons 34–35] (§17.7)

Stokes' Theorem

Let \(S\) be an oriented, piecewise-smooth surface bounded by a simple closed curve \(C = \partial S\). Let \(\vec{F} = \langle P, Q, R \rangle\) have continuous partial derivatives on an open region containing \(S\). Then:

\[\oint_C \vec{F}\cdot d\vec{r} = \iint_S \operatorname{curl}(\vec{F})\cdot d\vec{S}\]

Equivalently, using \(d\vec{S} = \hat{n}\,dS\):

\[\oint_C \vec{F}\cdot d\vec{r} = \iint_S \operatorname{curl}(\vec{F})\cdot\hat{n}\,dS\]

Orientation Convention

The boundary curve \(C\) is positively oriented relative to \(S\) when, walking along \(C\) with the surface on your left, \(\hat{n}\) points away from your head. Equivalently: \(\hat{n}\) and the direction of traversal of \(C\) satisfy the right-hand rule.

Curl Formula

For \(\vec{F} = \langle P, Q, R \rangle\):

\[\operatorname{curl}(\vec{F}) = \nabla \times \vec{F} = \begin{vmatrix}\vec{i} & \vec{j} & \vec{k} \\ \partial_x & \partial_y & \partial_z \\ P & Q & R\end{vmatrix} = \langle R_y - Q_z,\; P_z - R_x,\; Q_x - P_y \rangle\]

Computing the Surface Integral Side

For surface \(z = g(x,y)\) with upward normal over region \(D\):

\[\iint_S \operatorname{curl}(\vec{F})\cdot d\vec{S} = \iint_D \left[-(R_y-Q_z)\,g_x - (P_z-R_x)\,g_y + (Q_x-P_y)\right]dA\]

Key: Stokes' theorem converts a line integral into a surface integral (or vice versa). It generalizes Green's Theorem: when \(S\) is flat in the \(xy\)-plane, Stokes' theorem reduces exactly to Green's theorem.

Connection to Green's Theorem

Green's Theorem is the special case of Stokes' Theorem where \(S\) lies in the \(xy\)-plane (\(z=0\), \(\hat{n}=\vec{k}\)):

\[\oint_C P\,dx + Q\,dy = \iint_D (Q_x - P_y)\,dA\]

Consequences

Practice Problems

Divergence Theorem [Lessons 36–37] (§17.9)

Divergence Theorem (Gauss's Theorem)

Let \(E\) be a simple solid region with outward-oriented boundary surface \(S = \partial E\). Let \(\vec{F} = \langle P, Q, R \rangle\) have continuous partial derivatives on an open region containing \(E\). Then:

\[\iint_S \vec{F}\cdot d\vec{S} = \iiint_E \operatorname{div}(\vec{F})\,dV\]

Divergence Formula

\[\operatorname{div}(\vec{F}) = \nabla\cdot\vec{F} = \frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} + \frac{\partial R}{\partial z}\]

Orientation Convention

The boundary surface \(S = \partial E\) must be oriented with the outward normal (pointing away from the interior of \(E\)). If the surface is given with inward normal, multiply the result by \(-1\).

Key: The Divergence Theorem converts a flux surface integral into a triple integral over the enclosed volume — often much easier to evaluate. It is especially useful when the surface consists of multiple pieces.

Physical Interpretation

The Divergence Theorem states that the net flux of \(\vec{F}\) out of a closed surface equals the total divergence (source/sink density) integrated over the enclosed volume. If \(\operatorname{div}(\vec{F}) = 0\) everywhere in \(E\), then the net flux through \(\partial E\) is zero.

Strategy: Replacing a Hard Surface

If \(S\) is an open surface (not closed), close it by adding a cap \(S_{\text{cap}}\), apply the Divergence Theorem to the closed surface \(S \cup S_{\text{cap}}\), then subtract the cap's contribution:

\[\iint_S \vec{F}\cdot d\vec{S} = \iiint_E \operatorname{div}(\vec{F})\,dV - \iint_{S_{\text{cap}}} \vec{F}\cdot d\vec{S}\]

Key Identities

Practice Problems