← Math 21a: Multivariable Calculus

Unit 9: Curl, Divergence, and Parametrized Surfaces

A paddlewheel that spins or sits still, a point that sources or sinks fluid, and the surfaces that flux gets measured through.

9 topics · 28 questions

Each topic is a path, not a menu: work down it in order and every question builds on the one above. Click any of them to watch the answer draw itself.

9.1 The Curl of a Vector Field

  1. How it worksHow does the combination of partial derivatives Qx - Py measure the local spinning tendency of a two-dimensional vector field?
  2. Worked exampleFind the curl of the vector field F(x, y) = <-y, x>.
  3. Common mistakeWhy doesn't a vector field that visually curves and swirls have to have nonzero curl at every point?
Your turn1 of 2
Find the curl (Qx - Py) of the vector field F(x, y) = <4·x·y2, 4·x2·y>, as a function of x and y.

9.2 The Divergence of a Vector Field

  1. How it worksHow does adding up Px and Qy measure whether a vector field is expanding outward or collapsing inward at a point?
  2. Worked exampleFind the divergence of the vector field F(x, y) = <x, y> at the point (1, 1).
  3. Common mistakeWhy isn't a vector field with divergence zero automatically a field where nothing at all is happening?
  4. Going furtherWhat happens to the divergence at a point that is acting as a sink instead of a source?
Your turn1 of 2
Find the divergence (Px + Qy) of the vector field F(x, y) = <4·x3, 4·y3>, as a function of x and y.

9.3 Parametrized Surfaces

  1. How it worksHow do two parameter functions u and v sweep out a two-dimensional surface sitting inside three-dimensional space?
  2. Common mistakeWhy isn't a parametrized surface's equation the same thing as the level-surface equation you would write for the same shape?
  3. Worked exampleFind a parametrization for the sphere of radius 3 centered at the origin using spherical angles as parameters.
Your turn1 of 2
The sphere of radius 4 is parametrized by r(u, v) = <4·sin(u)·cos(v), 4·sin(u)·sin(v), 4·cos(u)>. Find its x-component, as a function of u and v.

9.4 The Normal Vector to a Parametrized Surface

  1. How it worksHow does taking the cross product of the two partial derivative vectors ru and rv produce a vector normal to the surface?
  2. Worked exampleFind the normal vector to the surface r(u, v) = <u, v, u2 + v2> at the point where u = 1, v = 0.
  3. Going furtherWhat happens to the surface's normal vector direction when the roles of the parameters u and v are swapped?
Your turn1 of 2
For r(u, v) = <u, v, 4·u2 + 4·v2>, find the x-component of the normal vector ru x rv, as a function of u.

9.5 Surface Area of a Parametrized Surface

  1. How it worksHow does the magnitude of ru cross rv measure the local area-stretching factor of a parametrized surface?
  2. Worked exampleFind the surface area of the parametrized surface r(u, v) = <u, v, u + v> for 0 ≤ u ≤ 1, 0 ≤ v ≤ 1.
  3. Ties togetherHow does this surface-area formula generalize the earlier surface-area formula built from ordinary partial derivatives fx and fy?
Your turn1 of 2
Find the surface area of the parametrized surface r(u, v) = <u, v, 4·u + 4·v> for 0 ≤ u ≤ 4, 0 ≤ v ≤ 2.

9.6 Flux Integrals Through a Surface

  1. How it worksHow does the dot product of a vector field with the surface's normal vector, integrated over the surface, add up total flux?
  2. Worked exampleFind the flux of F(x, y, z) = <0, 0, 1> through the parametrized surface r(u, v) = <u, v, 0> for 0 ≤ u ≤ 1, 0 ≤ v ≤ 1.
  3. Common mistakeWhy doesn't reversing a surface's chosen orientation leave a flux integral's value unchanged?
Your turn1 of 2
Find the flux of F(x, y, z) = <0, 0, 4> through the parametrized surface r(u, v) = <u, v, 0> for 0 ≤ u ≤ 3, 0 ≤ v ≤ 4.

9.7 Orientation of Surfaces and Curves

  1. How it worksHow does choosing a consistent normal vector direction across an entire surface define that surface's orientation?
  2. Common mistakeWhy isn't every surface in space guaranteed to have two separate, consistent sides to choose an orientation from?
  3. Worked exampleFind the outward-orientation normal vector for the sphere x2 + y2 + z2 = 1 at the point (0, 0, 1).
Your turn1 of 2
The unit sphere is parametrized by r(u, v) = <sin(u)·cos(v), sin(u)·sin(v), cos(u)>. Its outward unit normal at each point equals r(u,v) itself. Find its x-component, as a function of u and v.

9.8 Vector Fields in Fluid Flow: Sources, Sinks, and Rotation

  1. How it worksHow do curl and divergence, computed from the very same vector field, end up measuring two completely independent physical behaviors?
  2. Worked exampleFind both the curl and the divergence of the vector field F(x, y) = <x2, y2>, and describe the flow they predict.
  3. Ties togetherHow do curl and divergence together give a complete local picture of a fluid flow's rotation and expansion at every point?
Your turn1 of 2
Find the divergence of the vector field F(x, y) = <4·x2, 4·y2>, as a function of x and y.

9.9 Surfaces of Revolution as Parametrized Surfaces

  1. How it worksHow do a profile curve and a rotation angle combine into the two parameters that describe a surface of revolution?
  2. Worked exampleFind a parametrization for the surface obtained by revolving the curve z = y2 around the z-axis.
  3. Going furtherWhat happens to the parametrization when the profile curve is revolved only partway around the axis instead of a full circle?
Your turn1 of 2
Revolving the profile curve z = 4·s2 (s the distance from the axis) around the z-axis gives Z(s, theta) = 4·s2. Write it as a function of s.