Parametric Surfaces

A parametric surface is a surface traced out by a vector function of two parameters, r(u, v) = ⟨x(u, v), y(u, v), z(u, v)⟩, as (u, v) moves over a region D. Its tangent vectors r_u and r_v give a normal vector r_u × r_v, and its surface area is the double integral of |r_u × r_v| over D.

Before this lesson: Vector Functions and Space Curves, Partial Derivatives, Cross Product and Double Integrals in Polar Coordinates

What a parametric surface is

A curve in space needs one parameter: r(t) traces a path as t changes. A surface needs two. Each point (u, v) in a flat region D is sent to a point r(u, v) in space, so the whole region D bends into a surface.

Hold v fixed and let u change, and r traces a u-curve on the surface. Hold u fixed instead and you get a v-curve. Together these curves form a curved grid, like lines of latitude and longitude on a globe.

Left: a square region D in the uv-plane divided into a 4 by 4 grid, with one small cell of width Δu and height Δv shaded orange. An arrow labeled r(u, v) points to the right panel. Right: a curved, saddle-shaped surface in space with the matching grid of u-curves and v-curves in gray; the image of the small cell is a curved patch shaded orange. From the corner of the patch, a blue arrow r_u points along a u-curve, a green arrow r_v points along a v-curve, and a navy arrow r_u × r_v points out of the surface, perpendicular to both. A label says the patch area is about |r_u × r_v| Δu Δv.
Each small cell of D maps to a curved patch. The tangent vectors r_u and r_v span the patch, and their cross product is normal to the surface.

Tangent vectors, normal vector and surface area formula

The partial derivatives r_u and r_v are tangent to the u-curve and the v-curve through a point. Both lie in the tangent plane, so their cross product is a normal vector.

\mathbf{r}_u = \left\langle \dfrac{\partial x}{\partial u}, \dfrac{\partial y}{\partial u}, \dfrac{\partial z}{\partial u} \right\rangle, \qquad \mathbf{r}_v = \left\langle \dfrac{\partial x}{\partial v}, \dfrac{\partial y}{\partial v}, \dfrac{\partial z}{\partial v} \right\rangle, \qquad \mathbf{n} = \mathbf{r}_u \times \mathbf{r}_v

A small Δu by Δv cell of D maps to a patch that is almost a parallelogram with sides r_u Δu and r_v Δv. Its area is about |r_u × r_v| Δu Δv. Adding up the patches gives the surface area. The surface should be smooth, meaning r_u × r_v ≠ 0 inside D.

A(S) = \iint_D \left| \mathbf{r}_u \times \mathbf{r}_v \right| \, dA

Common parametrizations

Surfacer(u, v)|r_u × r_v|
Graph z = f(x, y)⟨x, y, f(x, y)⟩√(1 + f_x² + f_y²)
Cylinder x² + y² = a²⟨a cos θ, a sin θ, z⟩a
Sphere x² + y² + z² = a²⟨a sin φ cos θ, a sin φ sin θ, a cos φ⟩a² sin φ
Cone z = √(x² + y²)⟨r cos θ, r sin θ, r⟩r√2
Plane through P₀ with direction vectors a and bP₀ + u a + v b|a × b|

The sphere uses the angles of spherical coordinates with ρ = a fixed, and the cylinder uses cylindrical coordinates with r = a fixed. For a graph, the formula matches the one in applications of double integrals.

Parametric surface examples

Example 1: Identify a parametric surface

Describe the surface r(u, v) = ⟨2 cos u, 2 sin u, v⟩ for 0 ≤ u ≤ 2π and 0 ≤ v ≤ 5.

x^2 + y^2 = (2\cos u)^2 + (2\sin u)^2

Square x and y and add.

= 4\cos^2 u + 4\sin^2 u

Square each term.

= 4(\cos^2 u + \sin^2 u)

Factor out 4.

= 4

Use cos² u + sin² u = 1 (see fundamental trig identities).

z = v, \quad 0 \le v \le 5

The height z runs from 0 to 5.

Answer: every point satisfies x² + y² = 4, so the surface is the circular cylinder of radius 2 around the z-axis, from z = 0 to z = 5. The u-curves are circles and the v-curves are vertical lines.

Example 2: Tangent plane to a parametric surface

Find the tangent plane to r(u, v) = ⟨u², v², u + 2v⟩ at the point where u = 1 and v = 1.

\mathbf{r}(1, 1) = \langle 1, 1, 3 \rangle

Find the point: x = 1², y = 1², z = 1 + 2(1).

\mathbf{r}_u = \langle 2u, 0, 1 \rangle = \langle 2, 0, 1 \rangle

Differentiate each component with respect to u, then set u = 1.

\mathbf{r}_v = \langle 0, 2v, 2 \rangle = \langle 0, 2, 2 \rangle

Differentiate with respect to v, then set v = 1.

\mathbf{n} = \langle 0 \cdot 2 - 1 \cdot 2,\; 1 \cdot 0 - 2 \cdot 2,\; 2 \cdot 2 - 0 \cdot 0 \rangle

Take r_u × r_v (see cross product).

= \langle -2, -4, 4 \rangle

Simplify each component.

-2(x - 1) - 4(y - 1) + 4(z - 3) = 0

Write the plane through (1, 1, 3) with this normal (see equation of a plane).

(x - 1) + 2(y - 1) - 2(z - 3) = 0

Divide both sides by −2.

x - 1 + 2y - 2 - 2z + 6 = 0

Distribute.

x + 2y - 2z + 3 = 0

Combine the constants: −1 − 2 + 6 = 3.

Answer: x + 2y − 2z + 3 = 0. Check: 1 + 2(1) − 2(3) + 3 = 0, so the point is on the plane.

Example 3: Area of a spherical cap

Find the area of the part of the sphere x² + y² + z² = 16 that lies above the plane z = 2.

\mathbf{r}(\varphi, \theta) = \langle 4\sin\varphi\cos\theta, 4\sin\varphi\sin\theta, 4\cos\varphi \rangle

Parametrize the sphere of radius 4.

4\cos\varphi = 2 \Rightarrow \cos\varphi = \tfrac{1}{2} \Rightarrow \varphi = \tfrac{\pi}{3}

Find where the sphere meets z = 2. The cap is 0 ≤ φ ≤ π/3 and 0 ≤ θ ≤ 2π.

\mathbf{r}_\varphi = \langle 4\cos\varphi\cos\theta, 4\cos\varphi\sin\theta, -4\sin\varphi \rangle

Differentiate with respect to φ.

\mathbf{r}_\theta = \langle -4\sin\varphi\sin\theta, 4\sin\varphi\cos\theta, 0 \rangle

Differentiate with respect to θ.

\mathbf{r}_\varphi \times \mathbf{r}_\theta = \langle 16\sin^2\varphi\cos\theta, 16\sin^2\varphi\sin\theta, 16\sin\varphi\cos\varphi \rangle

Take the cross product. The third component is 16 sin φ cos φ (cos² θ + sin² θ).

|\mathbf{r}_\varphi \times \mathbf{r}_\theta| = \sqrt{256\sin^4\varphi + 256\sin^2\varphi\cos^2\varphi}

Take the length. The first two components give 256 sin⁴ φ (cos² θ + sin² θ).

= 16\sin\varphi\sqrt{\sin^2\varphi + \cos^2\varphi} = 16\sin\varphi

Factor out 256 sin² φ. Here sin φ ≥ 0 because 0 ≤ φ ≤ π.

A = \int_0^{2\pi} \int_0^{\pi/3} 16\sin\varphi \, d\varphi \, d\theta

Set up the area integral.

\int_0^{\pi/3} 16\sin\varphi \, d\varphi = \big[-16\cos\varphi\big]_0^{\pi/3} = -8 + 16 = 8

Inner integral.

A = \int_0^{2\pi} 8 \, d\theta = 16\pi

Outer integral.

Answer: 16π ≈ 50.27 square units. Check: a cap of height h on a sphere of radius R has area 2πRh = 2π(4)(2) = 16π.

Example 4: Area of part of a paraboloid

Find the area of the part of the paraboloid z = x² + y² that lies below the plane z = 4.

\mathbf{r}(r, \theta) = \langle r\cos\theta, r\sin\theta, r^2 \rangle, \quad 0 \le r \le 2,\; 0 \le \theta \le 2\pi

Use polar parameters. The condition z = r² ≤ 4 means r ≤ 2.

\mathbf{r}_r = \langle \cos\theta, \sin\theta, 2r \rangle, \quad \mathbf{r}_\theta = \langle -r\sin\theta, r\cos\theta, 0 \rangle

Take the partial derivatives.

\mathbf{r}_r \times \mathbf{r}_\theta = \langle -2r^2\cos\theta, -2r^2\sin\theta, r \rangle

Take the cross product. The third component is r cos² θ + r sin² θ = r.

|\mathbf{r}_r \times \mathbf{r}_\theta| = \sqrt{4r^4 + r^2} = r\sqrt{4r^2 + 1}

Take the length and factor out r² (r ≥ 0).

A = \int_0^{2\pi} \int_0^2 r\sqrt{4r^2 + 1} \, dr \, d\theta

Set up the area integral.

\int_0^2 r\sqrt{4r^2 + 1} \, dr = \dfrac{1}{8}\int_1^{17} \sqrt{w} \, dw

Substitute w = 4r² + 1, so dw = 8r dr; r = 0 gives w = 1 and r = 2 gives w = 17 (see u-substitution with definite integrals).

= \dfrac{1}{8} \cdot \dfrac{2}{3} \big[w^{3/2}\big]_1^{17} = \dfrac{17\sqrt{17} - 1}{12}

Integrate the power w^(1/2) and evaluate.

A = 2\pi \cdot \dfrac{17\sqrt{17} - 1}{12} = \dfrac{\pi(17\sqrt{17} - 1)}{6}

Outer integral. The integrand does not depend on θ.

Answer: π(17√17 − 1)/6 ≈ 36.18 square units.

Example 5: Sheet metal for a funnel

A funnel is shaped like the part of the cone z = √(x² + y²) between z = 1 and z = 3, with lengths in inches. How much sheet metal covers its side?

\mathbf{r}(r, \theta) = \langle r\cos\theta, r\sin\theta, r \rangle, \quad 1 \le r \le 3,\; 0 \le \theta \le 2\pi

On the cone z = r, so 1 ≤ z ≤ 3 means 1 ≤ r ≤ 3.

\mathbf{r}_r = \langle \cos\theta, \sin\theta, 1 \rangle, \quad \mathbf{r}_\theta = \langle -r\sin\theta, r\cos\theta, 0 \rangle

Take the partial derivatives.

\mathbf{r}_r \times \mathbf{r}_\theta = \langle -r\cos\theta, -r\sin\theta, r \rangle

Take the cross product.

|\mathbf{r}_r \times \mathbf{r}_\theta| = \sqrt{r^2\cos^2\theta + r^2\sin^2\theta + r^2} = r\sqrt{2}

Take the length: r² + r² = 2r².

A = \int_0^{2\pi} \int_1^3 \sqrt{2}\, r \, dr \, d\theta

Set up the area integral.

\int_1^3 \sqrt{2}\, r \, dr = \sqrt{2} \cdot \dfrac{9 - 1}{2} = 4\sqrt{2}

Inner integral: r²/2 from 1 to 3.

A = 2\pi \cdot 4\sqrt{2} = 8\sqrt{2}\,\pi \approx 35.54

Outer integral.

Answer: about 35.5 square inches of sheet metal. Check: the frustum formula π(r₁ + r₂)s with slant height s = √(2² + 2²) = 2√2 gives π(4)(2√2) = 8√2 π.

Common mistakes

MistakeExample of the errorFix
Leaving out the area factorWriting the cap area in Example 3 as the integral of 1 dφ dθThe area element is |r_u × r_v| dA, here 16 sin φ dφ dθ.
Using the wrong parameter limitsTaking 0 ≤ r ≤ 4 for z = x² + y² below z = 4Translate the condition: z = r² ≤ 4 gives r ≤ 2.
Covering part of the surface twiceLetting φ run from 0 to 2π on a sphereUse 0 ≤ φ ≤ π and 0 ≤ θ ≤ 2π, so each point is traced once.
Using a dot product for the normalComputing ⟨2, 0, 1⟩ · ⟨0, 2, 2⟩ = 2 as the normalA normal vector needs the cross product r_u × r_v, which is a vector.
Integrating the vector instead of its lengthIntegrating ⟨−r cos θ, −r sin θ, r⟩ for the cone’s areaSurface area needs the scalar |r_u × r_v| = r√2.

Related methods

Surfaces of revolution

Rotating y = f(x), a ≤ x ≤ b, about the x-axis gives r(x, θ) = ⟨x, f(x) cos θ, f(x) sin θ⟩. Then |r_x × r_θ| = f(x)√(1 + f′(x)²) when f(x) ≥ 0, and the area formula becomes the one from surface area of revolution.

Surface integrals and flux

The same area element |r_u × r_v| dA is used to integrate a function over a surface, and the normal r_u × r_v is used to find the flux of a vector field through it. That is the next lesson, on surface integrals.

Practice problems

  1. Describe the surface r(u, v) = ⟨u, v, 4 − u − v⟩.
  2. Describe the surface r(u, v) = ⟨3 cos v, u, 3 sin v⟩.
  3. Write a parametrization of the plane through (1, 2, 0) with direction vectors ⟨1, 0, 2⟩ and ⟨0, 1, −1⟩.
  4. For r(u, v) = ⟨u, v, uv⟩, find r_u, r_v and r_u × r_v at (u, v) = (1, 2).
  5. Find the tangent plane to r(u, v) = ⟨u + v, u − v, u²⟩ at the point where u = 1 and v = 0.
  6. Find the area of the part of the plane z = 1 + 2x + 2y above the rectangle 0 ≤ x ≤ 1, 0 ≤ y ≤ 2.
  7. Use r(θ, z) = ⟨2 cos θ, 2 sin θ, z⟩ to find the area of the cylinder x² + y² = 4 for 0 ≤ z ≤ 6.
  8. Use the sphere parametrization to show that a sphere of radius 3 has area 36π.
  9. Find the area of the helicoid r(u, v) = ⟨u cos v, u sin v, v⟩ for 0 ≤ u ≤ 1 and 0 ≤ v ≤ 2π.
  10. A dome is the part of the sphere x² + y² + z² = 100 above the plane z = 6, with lengths in meters. How much area needs paint?
Show answers

1.

x + y + z = u + v + (4 - u - v)

Add the three components.

= 4

The u and v terms cancel.

Answer: the plane x + y + z = 4.

2.

x^2 + z^2 = 9\cos^2 v + 9\sin^2 v

Square x and z and add.

= 9

Factor out 9 and use cos² v + sin² v = 1.

Answer: the circular cylinder x² + z² = 9 of radius 3 around the y-axis (y = u can be any number).

3.

\mathbf{r}(u, v) = \langle 1, 2, 0 \rangle + u\langle 1, 0, 2 \rangle + v\langle 0, 1, -1 \rangle

Start at the point and add multiples of each direction vector.

= \langle 1 + u, 2 + v, 2u - v \rangle

Add the components.

Answer: r(u, v) = ⟨1 + u, 2 + v, 2u − v⟩

4.

\mathbf{r}_u = \langle 1, 0, v \rangle = \langle 1, 0, 2 \rangle

Differentiate with respect to u, then set v = 2.

\mathbf{r}_v = \langle 0, 1, u \rangle = \langle 0, 1, 1 \rangle

Differentiate with respect to v, then set u = 1.

\mathbf{r}_u \times \mathbf{r}_v = \langle 0 \cdot 1 - 2 \cdot 1,\; 2 \cdot 0 - 1 \cdot 1,\; 1 \cdot 1 - 0 \cdot 0 \rangle = \langle -2, -1, 1 \rangle

Take the cross product.

Answer: r_u = ⟨1, 0, 2⟩, r_v = ⟨0, 1, 1⟩ and r_u × r_v = ⟨−2, −1, 1⟩

5.

\mathbf{r}(1, 0) = \langle 1, 1, 1 \rangle

Find the point.

\mathbf{r}_u = \langle 1, 1, 2u \rangle = \langle 1, 1, 2 \rangle, \quad \mathbf{r}_v = \langle 1, -1, 0 \rangle

Take the partial derivatives at u = 1.

\mathbf{n} = \langle 1 \cdot 0 - 2(-1),\; 2 \cdot 1 - 1 \cdot 0,\; 1(-1) - 1 \cdot 1 \rangle = \langle 2, 2, -2 \rangle

Take the cross product.

2(x - 1) + 2(y - 1) - 2(z - 1) = 0

Write the plane through (1, 1, 1).

(x - 1) + (y - 1) - (z - 1) = 0

Divide both sides by 2.

x + y - z = 1

Distribute and move the constant: −1 − 1 + 1 = −1.

Answer: x + y − z = 1

6.

\sqrt{1 + f_x^2 + f_y^2} = \sqrt{1 + 2^2 + 2^2} = \sqrt{9} = 3

Use the graph formula with f_x = 2 and f_y = 2.

A = \int_0^2 \int_0^1 3 \, dx \, dy = 3 \cdot 1 \cdot 2 = 6

The integrand is constant, so multiply by the area of the rectangle.

Answer: 6 square units

7.

\mathbf{r}_\theta \times \mathbf{r}_z = \langle 2\cos\theta, 2\sin\theta, 0 \rangle

Use r_θ = ⟨−2 sin θ, 2 cos θ, 0⟩ and r_z = ⟨0, 0, 1⟩.

|\mathbf{r}_\theta \times \mathbf{r}_z| = \sqrt{4\cos^2\theta + 4\sin^2\theta} = 2

Take the length.

A = \int_0^6 \int_0^{2\pi} 2 \, d\theta \, dz = 2 \cdot 2\pi \cdot 6 = 24\pi

Integrate the constant over the parameter rectangle.

Answer: 24π ≈ 75.40 square units, the same as circumference times height.

8.

|\mathbf{r}_\varphi \times \mathbf{r}_\theta| = 9\sin\varphi

Same steps as Example 3 with radius 3: the length is a² sin φ.

A = \int_0^{2\pi} \int_0^{\pi} 9\sin\varphi \, d\varphi \, d\theta

The whole sphere has 0 ≤ φ ≤ π.

\int_0^{\pi} 9\sin\varphi \, d\varphi = \big[-9\cos\varphi\big]_0^{\pi} = 9 + 9 = 18

Inner integral.

A = 18 \cdot 2\pi = 36\pi

Outer integral.

Answer: 36π, which matches 4πa² with a = 3.

9.

\mathbf{r}_u = \langle \cos v, \sin v, 0 \rangle, \quad \mathbf{r}_v = \langle -u\sin v, u\cos v, 1 \rangle

Take the partial derivatives.

\mathbf{r}_u \times \mathbf{r}_v = \langle \sin v, -\cos v, u \rangle

Take the cross product. The third component is u cos² v + u sin² v = u.

|\mathbf{r}_u \times \mathbf{r}_v| = \sqrt{\sin^2 v + \cos^2 v + u^2} = \sqrt{1 + u^2}

Take the length.

A = \int_0^{2\pi} \int_0^1 \sqrt{1 + u^2} \, du \, dv

Set up the area integral.

\int_0^1 \sqrt{1 + u^2} \, du = \tfrac{1}{2}\Big[u\sqrt{1 + u^2} + \ln\big(u + \sqrt{1 + u^2}\big)\Big]_0^1

Use the antiderivative from the substitution u = tan t (see trigonometric substitution).

= \tfrac{1}{2}\big(\sqrt{2} + \ln(1 + \sqrt{2})\big)

Evaluate. The lower limit gives 0.

A = \pi\big(\sqrt{2} + \ln(1 + \sqrt{2})\big) \approx 7.21

Multiply by 2π for the outer integral.

Answer: π(√2 + ln(1 + √2)) ≈ 7.21 square units

10.

\cos\varphi_0 = \dfrac{6}{10} = 0.6

The sphere meets z = 6 where 10 cos φ = 6.

A = \int_0^{2\pi} \int_0^{\varphi_0} 100\sin\varphi \, d\varphi \, d\theta

On a sphere of radius 10 the area element is 100 sin φ.

\int_0^{\varphi_0} 100\sin\varphi \, d\varphi = 100(1 - \cos\varphi_0) = 100(0.4) = 40

Inner integral: −100 cos φ from 0 to φ₀.

A = 40 \cdot 2\pi = 80\pi \approx 251.3

Outer integral.

Answer: 80π ≈ 251 square meters.

Parametric surfaces FAQ

What is a parametric surface?

It is a surface given by a vector function r(u, v) of two parameters. As (u, v) moves over a region D in the plane, the point r(u, v) traces out the surface in space.

How do you find the surface area of a parametric surface?

Find r_u and r_v, take the length of their cross product, and integrate it over the parameter region: A = ∬ |r_u × r_v| dA over D.

How do you find a normal vector to a parametric surface?

The cross product r_u × r_v at a point is normal to the surface there. Use it with the point r(u₀, v₀) to write the tangent plane.

How do you parametrize a sphere?

Use spherical angles with a fixed radius a: r(φ, θ) = ⟨a sin φ cos θ, a sin φ sin θ, a cos φ⟩ for 0 ≤ φ ≤ π and 0 ≤ θ ≤ 2π. Then |r_φ × r_θ| = a² sin φ.

Summary

  • A parametric surface is r(u, v) = ⟨x(u, v), y(u, v), z(u, v)⟩ for (u, v) in a region D.
  • r_u and r_v are tangent vectors, and r_u × r_v is a normal vector.
  • Surface area: A = ∬ |r_u × r_v| dA over D.
  • For a graph z = f(x, y), |r_x × r_y| = √(1 + f_x² + f_y²).
  • Sphere: a² sin φ. Cylinder: a. Cone z = √(x² + y²): r√2.

Previous lesson: Curl and Divergence

Next lesson: Surface Integrals

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