Vector Fields: Intro, Div, Curl
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1 Vector Fields: Intro, Div, Curl Calculus III Josh Engwer TTU 07 November 2014 Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
2 The Function Landscape FUNCTION TYPE PROTOTYPE MAPPING (Scalar) Function y = f (x) f maps scalar scalar 2D Vector Function F(t) = f 1 (t), f 2 (t) F maps scalar 2D vector 3D Vector Function F(t) = f 1 (t), f 2 (t), f 3 (t) F maps scalar 3D vector Function of 2 Variables z = f (x, y) f maps 2D point scalar Function of 3 Variables w = f (x, y, z) f maps 3D point scalar 2D Vector Field 3D Vector Field F(x, y) = M(x, y), N(x, y) F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z) F maps 2D point to 2D vector F maps 3D point to 3D vector REMARK: Going forward, multivariable functions f (x, y), g(x, y, z) may be referred to as scalar fields. Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
3 The Function Landscape FUNCTION TYPE PROTOTYPE MAPPING (Scalar) Function y = f (x) f : R R 2D Vector Function F(t) = f 1 (t), f 2 (t) F : R R 2 3D Vector Function F(t) = f 1 (t), f 2 (t), f 3 (t) F : R R 3 Function of 2 Variables z = f (x, y) f : R 2 R Function of 3 Variables w = f (x, y, z) f : R 3 R 2D Vector Field F(x, y) = M(x, y), N(x, y) F : R 2 R 2 3D Vector Field F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z) F : R 3 R 3 R := The set of all scalars on the real line R 2 := The set of all ordered pairs (x, y) on the xy-plane R 2 := The set of all 2D vectors v 1, v 2 on the xy-plane R 3 := The set of all ordered triples (x, y, z) in xyz-space R 3 := The set of all 3D vectors v 1, v 2, v 3 in xyz-space ( ) say R Two ( ) say R Three Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
4 Vector Fields in R 2 Definition A 2D vector field is a function F(x, y) that assigns a vector to each point in its domain and has the form F(x, y) = M(x, y), N(x, y) = M(x, y)î + N(x, y)ĵ where the components of F are (scalar) functions of two variables. Proposition Let D R 2 be a region on the xy-plane. Let F(x, y) = M(x, y), N(x, y) be a 2D vector field. Dom(F) := Dom(M) Dom(N) Then: F(x, y) is continuous on region D its components are continous: F(x, y) C(D) M(x, y), N(x, y) C(D) F(x, y) C (1,1) (D) M(x, y), N(x, y) C (1,1) (D) F(x, y) C (2,2) (D) M(x, y), N(x, y) C (2,2) (D) Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
5 Vector Fields in R 3 Definition A 3D vector field is a function F(x, y, z) that assigns a vector to each point in its domain and has the form F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z) = M(x, y, z)î + N(x, y, z)ĵ + P(x, y, z) k where the components of F are (scalar) functions of three variables. Proposition Let E R 3 be a solid in xyz-space. Let F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z) be a 3D vector field. Dom(F) := Dom(M) Dom(N) Dom(P) Then: F(x, y, z) is continuous on solid E its components are continous: F(x, y, z) C(E) M(x, y, z), N(x, y, z), P(x, y, z) C(E) F(x, y, z) C (1,1,1) (E) M(x, y, z), N(x, y, z), P(x, y, z) C (1,1,1) (E) F(x, y, z) C (2,2,2) (E) M(x, y, z), N(x, y, z), P(x, y, z) C (2,2,2) (E) Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
6 Vector Fields in R 2 (Plot) Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
7 Vector Fields in R 3 (Plot) Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
8 Examples of Vector Fields Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
9 Examples of Vector Fields Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
10 Examples of Vector Fields Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
11 Examples of Vector Fields Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
12 Vector Fields are Vectors with Variable Components WEX : Let F(x, y, z) = xy, yz, xz and G(x, y, z) = x, 2y, 3z. Compute: (a) F + G (b) F G (c) F G (d) F G (a) F + G = xy, yz, xz + x, 2y, 3z = xy + x, yz + 2y, xz + 3z (b) F G = xy, yz, xz x, 2y, 3z = xy x, yz 2y, xz 3z (c) F G = xy, yz, xz x, 2y, 3z = (xy)(x) + (yz)(2y) + (xz)(3z) = x 2 y + 2y 2 z + 3xz 2 (d) F G = xy, yz, xz x, 2y, 3z î ĵ k = xy yz xz x 2y 3z = yz xz 2y 3z î xy xz x 3z ĵ + xy yz x 2y k = [(yz)(3z) (xz)(2y)] î [(xy)(3z) (xz)(x)] ĵ + [(xy)(2y) (yz)(x)] k = 3yz 2 2xyz, x 2 3xyz, 2xy 2 xyz Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
13 The Del Operator Definition The del operator in R 2 is defined by Definition := x, y The del operator in R 3 is defined by := x, y, z i.e., is the vector with the partial derivative operators as components. REMARK: The del operator is useful in simplifying notation & remembering certain vector field operations. Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
14 Divergence of a Vector Field Definition Let 2D vector field F(x, y) C (1,1) s.t. F(x, y) = M(x, y), N(x, y). Then the divergence of F(x, y) is div F F = x, M, N := M y x + N y = M x + N y Definition Let 3D vector field F(x, y, z) C (1,1,1) s.t. F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z). Then the divergence of F(x, y, z) is div F F = x, y, M, N, P := M z x + N y + P z = M x + N y + P z REMARK: The divergence of a vector field is a scalar field. Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
15 Positive Divergence (Geometric Interpretation) F(x, y) = 10x, 10y F = x [ ] 10x + [ ] 10y = = 20 > 0 y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
16 Negative Divergence (Geometric Interpretation) F(x, y) = 10x, 10y F = x [ ] 10x + [ ] 10y = = 20 < 0 y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
17 Zero Divergence (Geometric Interpretation) F(x, y) = 3, 2 F = x [ ] 3 + [ ] 2 = = 0 y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
18 Zero Divergence (Geometric Interpretation) F(x, y) = y, x F = x [ ] y + [ ] x = = 0 y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
19 Zero Divergence (Geometric Interpretation) F(x, y) = cos y, sin ( x 2) F = x [ ] cos y + [ sin ( x 2) ] = = 0 y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
20 Curl of a Vector Field Definition Let 3D vector field F(x, y, z) C (1,1,1) s.t. F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z). Then the curl of F(x, y, z) is î ĵ k curl F F := x y M N P z = REMARK: The curl of a vector field is a vector field. P y N z, M z P x, N x M y REMARK: Treat 2D vector fields as 3D vector fields with 3 rd component zero: extends to F(x, y) = M(x, y), N(x, y) F(x, y, z) = M(x, y), N(x, y), 0 Then, curl F = curl F = 0, 0, N x M ( N = y x M ) k y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
21 Curl (Geometric Interpretation) F(x, y) = y, x F = 0, 0, [ ] x [ y] = 0, 0, 1 ( 1) = 0, 0, 2 x y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
22 Curl (Geometric Interpretation) F(x, y) = y, x F = 0, 0, [ ] x [ y] = 0, 0, 1 1 = 0, 0, 2 x y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
23 Curl (Geometric Interpretation) F(x, y) = 3, 2 F = 0, 0, [ ] 2 [ 3] = 0, 0, 0 0 = 0, 0, 0 = x y 0 Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
24 Curl (Geometric Interpretation) F(x, y) = y, x F = 0, 0, [ ] x [ y] = 0, 0, 1 1 = 0, 0, 0 = x y 0 Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
25 Curl (Geometric Interpretation) F(x, y) = 12 y2, 12 x2 F = 0, 0, [ 1 ] x 2 x2 [ 1 ] y 2 y2 = 0, 0, x ( y) = 0, 0, x + y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
26 Laplacian of a Scalar Field Definition Let f (x, y) C (2,2). 2 f := div Then the Laplacian of f is ( ) grad f f = 2 f x f y 2 = f xx + f yy Definition Let f (x, y, z) C (2,2,2). 2 f := div Then the Laplacian of f is ( ) grad f f = 2 f x f y f z 2 = f xx + f yy + f zz WEX : Compute the Laplacian of f (x, y) = x 4 + y 3. f x = 4x 3 f y = 3y 2 f xx = 12x 2 f yy = 6y 2 f = f xx + f yy = 12x 2 + 6y Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
27 Harmonic Functions Definition Let D R 2 be a region on the xy-plane. Let function f (x, y) C (2,2) (D). Then f is harmonic in D f Har(D) 2 f = 0 2 f x f y 2 = 0 Definition Let E R 3 be a solid in xyz-space. Let function f (x, y, z) C (2,2,2) (E). Then f is harmonic in E f Har(E) 2 f = 0 2 f x f y f z 2 = 0 WEX : Is f (x, y) = x 2 y 2 harmonic in R 2? (Justify answer) f x = 2x f y = 2y f xx = 2 f yy = 2 = 2 f = f xx + f yy = 2 + ( 2) = 0 (x, y) R 2 Since 2 f = 0, f is harmonic in R 2 Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
28 Summary of Operations on Vector Fields OPERATION DEL OPERATOR NOTATION ALTERNATIVE NOTATION Gradient f grad f Divergence F div F Curl F curl ( F ) Laplacian 2 f div grad f Vector Field, Scalar kf Vector Field 2 Vector Fields F + G Vector Field 2 Vector Fields F G Vector Field 2 Vector Fields F G Scalar Field 2 Vector Fields F G Vector Field Vector Field, Scalar Field f F Vector Field Scalar Field f Vector Field Scalar Field 2 f Scalar Field Vector Field F Scalar Field Vector Field F Vector Field Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
29 Div & Curl (Properties & Identities) (k R f, g : R 3 R F, G : R 3 R 3 ) div(kf) = k div F curl(kf) = k curl F div(f ± G) = div F ± div G curl(f ± G) = curl F ± curl G div(f F) = f div F + ( f F) curl(f F) = f curl F + ( f F) div(curl F) = 0 curl( f ) = 0 div(f g) = f div ( g) + f g div(f G) = curl F G F curl G 2 (fg) = f 2 g + 2 f g + g 2 f Vector Calculus Identities NOT to be considered: (F G) curl(f G) curl(curl F) Any Identity involving terms of the forms (G )F or (G )f Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
30 Div & Curl (Properties & Identities) (k R f, g : R 3 R F, G : R 3 R 3 ) (kf) = k F (kf) = k F (F ± G) = F ± G (F ± G) = F ± G (f F) = f ( F) + ( f F) (f F) = f ( F) + ( f F) ( F) = 0 ( f ) = 0 (f g) = f ( g) + f g (F G) = ( F) G F ( G) 2 (fg) = f 2 g + 2 f g + g 2 f Vector Calculus Identities NOT to be considered: (F G) (F G) ( F) Any Identity involving terms of the forms (G )F or (G )f Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
31 Proof that ( F) = 0 Let vector field F C (2,2,2) s.t. F(x, y, z) = M(x, y, z), N(x, y, z), P(x, y, z). Prove: ( F) = 0 PROOF: ( F) = QED = x = = x, y, P z y N z, M z P x, N x M y [ P y N ] + [ M z y z P ] + [ N x z x M ] y ( 2 ) ( P x y 2 N 2 ) ( M + x z y z 2 P 2 ) N + y x z x 2 M z y ( 2 ) ( P x y 2 P 2 ) ( N + y x z x 2 N 2 ) M + x z y z 2 M z y = = 0 [ ] Since F C (2,2,2), mixed 2 nd partials are equal Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
32 Proof that ( f ) = 0 Let scalar field f C (2,2,2). Prove: ( f ) = 0 PROOF: ( f ) = QED = = x, y, f z x, f y, f = z y f y z f z î x f x z f z ĵ + x f x î ĵ k x f x y f y y f y k 2 f y z 2 f z y, 2 f z x 2 f x z, 2 f x y 2 f y x = 0, 0, 0 = 0 z f z [ ] Since f C (2,2,2), mixed 2 nd partials are equal Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
33 Not every expression involving div, grad, curl makes sense! WEX : Explain why ( x 2 + yz ) makes no sense. x 2 + yz is a scalar field, but the curl of a scalar field is not defined. WEX : Let F be a vector field. Explain why ( F) makes no sense. F yields a scalar field, but the divergence of a scalar field is not defined. WEX : Let f be a scalar field & F be a vector field. Explain why ( f ) ( F) makes no sense. f yields a vector field, F yields a scalar field, but the cross product of a scalar field and a vector field is not defined. Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
34 Fin Fin. Josh Engwer (TTU) Vector Fields: Intro, Div, Curl 07 November / 34
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