Surfaces for Surface Integrals

Một phần của tài liệu Advanced engineering mathematics 10th edition (Trang 465 - 469)

Case III. Complex conjugate roots are of minor practical importance, and we discuss the derivation of real solutions from complex ones just in terms of a typical example

10.5 Surfaces for Surface Integrals

Whereas, with line integrals, we integrate over curves in space (Secs. 10.1, 10.2), with surface integrals we integrate over surfaces in space. Each curve in space is represented by a parametric equation (Secs. 9.5, 10.1). This suggests that we should also find parametric representations for the surfaces in space. This is indeed one of the goals of this section. The surfaces considered are cylinders, spheres, cones, and others. The second goal is to learn about surface normals. Both goals prepare us for Sec. 10.6 on surface integrals. Note that for simplicity, we shall say “surface” also for a portion of a surface.

Representation of Surfaces

Representations of a surface Sin xyz-space are (1)

For example, or represents a

hemisphere of radius aand center 0.

Now for curves Cin line integrals, it was more practical and gave greater flexibility to use a parametric representation where This is a mapping of the interval located on the t-axis, onto the curve C (actually a portion of it) in xyz-space. It maps every t in that interval onto the point of C with position vector See Fig. 241A.

Similarly, for surfaces Sin surface integrals, it will often be more practical to use a parametricrepresentation. Surfaces are two-dimensional. Hence we need twoparameters, r(t).

atb,

atb.

rr(t),

x2⫹y2⫹z2⫺a2⫽0 (z⭌0) z⫽ ⫹2a2⫺x2⫺y2

zf(x, y) or g(x, y, z)⫽0.

z x y

r(t) r(u,v)

Curve C in space

z x y

a b

t

(t-axis)

v

u

R

(uv-plane) Surface S in space

(A) Curve (B) Surface

Fig. 241. Parametric representations of a curve and a surface

which we call uand v. Thus a parametric representationof a surface Sin space is of the form

(2)

where (u, v) varies in some region Rof the uv-plane. This mapping (2) maps every point (u, v) in Ronto the point of Swith position vector r(u, v). See Fig. 241B.

E X A M P L E 1 Parametric Representation of a Cylinder

The circular cylinder has radius a, height 2, and the z-axis as axis. A parametric representation is

(Fig. 242).

The components of rare The parameters u, vvary in the rectangle in the uv-plane. The curves are vertical straight lines. The curves are parallel circles. The point Pin Fig. 242 corresponds to u⫽p>3⫽60°, v⫽0.7. 䊏

v⫽const u⫽const

2p, ⫺1⬉v⬉1

R: 0⬉uxa cos u, ya sin u, zv.

r(u, v)⫽[a cos u, a sin u, v]⫽a cos uia sin ujvk x2⫹y2⫽a2, ⫺1⬉z⬉1,

r(u, v)⫽[x(u, v), y(u, v), z(u, v)]⫽x(u, v)iy(u, v)jz(u, v)k

(v = 1)

(v = 0)

(v = –1) v

u P

x y z

u v

P z

x y

Fig. 242. Parametric representation Fig. 243. Parametric representation

of a cylinder of a sphere

E X A M P L E 2 Parametric Representation of a Sphere

A sphere can be represented in the form (3)

where the parameters u, v vary in the rectangle Rin the uv-plane given by the inequalities The components of rare

The curves and are the “meridians” and “parallels” on S(see Fig. 243). This representation is used ingeographyfor measuring the latitude and longitude of points on the globe.

Another parametric representation of the sphere also used in mathematics is (3*)

where 0⬉u⬉2p, 0⬉v⬉p. 䊏

r(u, v)⫽a cos u sin via sin u sin vja cos vk v⫽const

u⫽const

xa cos v cos u, ya cos v sin u, za sin v.

⫺p>2⬉v⬉p>2.

0⬉u⬉2p, r(u, v)⫽a cos v cos uia cos v sin uja sin vk

x2⫹y2⫹z2⫽a2

E X A M P L E 3 Parametric Representation of a Cone

A circular cone can be represented by

in components The parameters vary in the rectangle Check that as it should be. What are the curves and ?

Tangent Plane and Surface Normal

Recall from Sec. 9.7 that the tangent vectors of all the curves on a surface Sthrough a point Pof Sform a plane, called the tangent planeof Sat P(Fig. 244). Exceptions are points where Shas an edge or a cusp (like a cone), so that Scannot have a tangent plane at such a point.

Furthermore, a vector perpendicular to the tangent plane is called a normal vectorof Sat P.

Now since Scan be given by in (2), the new idea is that we get a curve C on Sby taking a pair of differentiable functions

whose derivatives and are continuous. Then C has the position vector . By differentiation and the use of the chain rule (Sec. 9.6) we obtain a tangent vector of Con S

Hence the partial derivatives and at P are tangential to S at P.We assume that they are linearly independent, which geometrically means that the curves and on Sintersect at Pat a nonzero angle. Then and span the tangent plane of Sat P. Hence their cross product gives a normal vector Nof Sat P.

(4)

The corresponding unit normal vector nof Sat Pis (Fig. 244)

(5) n1

ƒNƒ

N1 ƒrurvƒ

rurv. Nrurv0.

rv

ru v⫽const

u⫽const rv

ru

~rr(t)⫽ dr

~ dt ⫽ 0r

0u ur⫹ 0r

0v vr.

~(t)rr(u(t), v(t))

vr⫽dv>dt

ur ⫽du>dt

uu(t), vv(t) rr(u, v)

v⫽const u⫽const

x2⫹y2⫽z2,

R: 0⬉uH, 0⬉v⬉2p. xu cos v, yu sin v, zu.

r(u, v)⫽[u cos v, u sin v, u]⫽u cos viu sin vjuk, z⫽2x2⫹y2, 0⬉tH

n

rv ru

P

S

Fig. 244. Tangent plane and normal vector

Also, if Sis represented by then, by Theorem 2 in Sec. 9.7, (5*)

A surface Sis called a smooth surfaceif its surface normal depends continuously on the points of S.

Sis called piecewise smoothif it consists of finitely many smooth portions.

For instance, a sphere is smooth, and the surface of a cube is piecewise smooth (explain!). We can now summarize our discussion as follows.

T H E O R E M 1 Tangent Plane and Surface Normal

If a surface S is given by(2) with continuous and satisfying (4) at every point of S, then S has, at every point P, a unique tangent plane passing through P and spanned by and and a unique normal whose direction depends continuously on the points of S. A normal vector is given by(4) and the corresponding unit normal vector by(5). (See Fig. 244.)

E X A M P L E 4 Unit Normal Vector of a Sphere

From we find that the sphere has the unit normal vector

We see that nhas the direction of the position vector [x, y, z] of the corresponding point. Is it obvious that this must be the case?

E X A M P L E 5 Unit Normal Vector of a Cone

At the apex of the cone in Example 3, the unit normal vector nbecomes undetermined because from we get

We are now ready to discuss surface integrals and their applications, beginning in the next section.

n⫽c x

22(x2⫹y2) ,

y 22(x2⫹y2)

, ⫺1 12d ⫽ 1

12a x 2x2⫹y2

iy

2x2⫹y2 jkb. (5*)

g(x, y, z)⫽ ⫺z⫹2x2⫹y2⫽0

n(x, y, z)⫽cx a, y

a, z ad ⫽x

a iy a jz

a k.

g(x, y, z)⫽x2⫹y2⫹z2⫺a2⫽0 (5*)

rv, ru

rv⫽ 0r>0v ru⫽ 0r>0u

n1 ƒgrad gƒ

grad g.

g(x, y, z)⫽0,

1–8 PARAMETRIC SURFACE REPRESENTATION Familiarize yourself with parametric representations of important surfaces by deriving a representation (1), by finding the parameter curves (curves and

) of the surface and a normal vector of the surface. Show the details of your work.

1. xy-plane (thus similarly in

Probs. 2–8).

2. xy-plane in polar coordinates (thus ur, v⫽u)

u sin v]

r(u, v)⫽[u cos v, uivj;

r(u, v)⫽(u, v)

Nrurv

v⫽const

u⫽const

3. Cone

4. Elliptic cylinder 5. Paraboloid of revolution

6. Helicoid Explain the

name.

7. Ellipsoid

8. Hyperbolic paraboloid u2] v, bu sinh

r(u, v)⫽[au cosh v, c sin v]

b cos v sin u, r(u, v)⫽[a cos v cos u,

r(u, v)⫽[u cos v, u sin v, v].

u2]

r(u, v)⫽[u cos v, u sin v, r(u, v)⫽[a cos v, b sin v, u]

r(u, v)⫽[u cos v, u sin v, cu]

P R O B L E M S E T 1 0 . 5

9. CAS EXPERIMENT. Graphing Surfaces, Depen- dence on a,b,c.Graph the surfaces in Probs. 3–8. In Prob. 6 generalize the surface by introducing parame- ters a, b. Then find out in Probs. 4 and 6–8 how the shape of the surfaces depends on a, b, c.

10. Orthogonal parameter curves and on occur if and only if

Give examples. Prove it.

11. Satisfying (4). Represent the paraboloid in Prob. 5 so

that and show

12. Condition (4). Find the points in Probs. 1–8 at which (4) does not hold. Indicate whether this results from the shape of the surface or from the choice of the representation.

13. Representation Show that or

can be written etc.)

(6) and

N⫽grad g⫽[⫺fu, ⫺fv, 1].

r(u, v)⫽[u, v, f(u, v)]

( fu⫽0f>0u, gzf(x, y)⫽0

zf(x, y) zf(x, y).

N0

N~ . N~

(0, 0)⫽0

rurv⫽0.

r(u, v) v⫽const

u⫽const

14–19 DERIVE A PARAMETRIC REPRESENTATION

Find a normal vector. The answer gives onerepresentation;

there are many. Sketch the surface and parameter curves.

14. Plane

15. Cylinder of revolution 16. Ellipsoid

17. Sphere 18. Elliptic cone 19. Hyperbolic cylinder

20. PROJECT. Tangent Planes T(P) will be less important in our work, but you should know how to represent them.

(a) If then

(a scalar triple product) or

(b) If then

(c) If then

Interpret (a)⫺(c) geometrically. Give two examples for (a), two for (b), and two for (c).

T(P): z*⫺z⫽(x*⫺x)fx(P)⫹(y*⫺y)fy(P).

S: zf(x, y),

T(P): (r*⫺r(P))ⴢⵜg⫽0.

S: g(x, y, z)⫽0,

r*(p, q)⫽r(P)⫹pru(P)⫹qrv(P).

T(P): (r*⫺r ru rv)⫽0 S: r(u, v),

x2⫺y2⫽1 z⫽ 2x2⫹4y2

x2⫹(y⫹2.8)2⫹(z⫺3.2)2⫽2.25 x2⫹y2⫹19 z2⫽1

(x⫺2)2⫹(y⫹1)2⫽25 4x⫹3y⫹2z⫽12

Một phần của tài liệu Advanced engineering mathematics 10th edition (Trang 465 - 469)

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