Quick viewing(Text Mode)

The Del Operator & Field Operations

The Del Operator & Field Operations

10/6/2020

Electromagnetics: Electromagnetic Theory The & Field Operations

Outline

vs. Vector Fields • The Del Operator ∇ • of a ∇𝑉 • of a ∇ · 𝐴⃗ • of a Vector Field ∇𝐴⃗ • Laplacian Operation ∇

Slide 2

1 10/6/2020

Scalar vs. Vector Fields

Slide 3

Scalar Field Vs. Vector Field (2D)

Scalar Field 𝑓 𝑥, 𝑦, 𝑧 Vector Field 𝐹⃗ 𝑥, 𝑦, 𝑧

• Magnitude only • Magnitude • Direction Slide 4

2 10/6/2020

Scalar Field Vs. Vector Field (3D)

Scalar Field 𝑓 𝑥, 𝑦, 𝑧 Vector Field 𝐹⃗ 𝑥, 𝑦, 𝑧

• Magnitude only • Magnitude • Direction Slide 5

Isocontour Lines

Isocontour lines the paths of equal value. Closely isocontours conveys that the is varying rapidly.

Slide 6

3 10/6/2020

The Del Operator

Slide 7

The Del Operator ∇

The del operator  is the vector . It is sort of a 3D . Even though  is a Coordinate Del Operator vector, it is never System written as ∇.  Cartesian aaaˆˆˆ   x x yzyz 1 Cylindrical aaaˆˆˆ   z z Derived from the Cartesian using coordinate 11  Spherical aaˆˆ   a ˆtransformation. rrr   rsin 

Slide 8

4 10/6/2020

Summary of Vector Operations

Operation Input Output

Vector Addition & Subtraction Vectors Vector UV  Dot ProductUV Vectors Scalar  Cross ProductUV Vectors Vector Gradientf Scalar Function Vector Function  DivergenceU Vector Function Scalar Function  CurlU Vector Function Vector Function Scalar Laplacian2V Scalar Function Scalar Function  Vector Laplacian2U Vector Function Vector Function

Slide 9

Gradient of a Scalar Field

Slide 10

5 10/6/2020

Gradient of a Scalar Field (1 of 3)

Start with a scalar field 𝑓 𝑥, 𝑦 .

Slide 11

Gradient of a Scalar Field (2 of 3) Plot the gradient ∇𝑓 𝑥, 𝑦, 𝑧 on top of 𝑓 𝑥, 𝑦, 𝑧 . The background color is the original scalar field 𝑓 𝑥, 𝑦, 𝑧 .

Slide 12

6 10/6/2020

Gradient of a Scalar Field (3 of 3)

The gradient will always be perpendicular to the isocontour lines.

Slide 13

The Gradient ∇𝑉

The gradient calculates how rapidly, and in what direction, a scalar function is increasing.

Coordinate Gradient Operator System VVV Cartesian Vaˆˆˆ  a  a x x yzyz VVV1 Cylindrical Vaˆˆˆ  a  a z z VV11  V Spherical Vaˆˆ  a  a ˆ rrr   rsin 

Slide 14

7 10/6/2020

Algebra Rules for the Gradient

UV U V Sum/Difference Rule

UV U V V U Rule

UVUUV  2 VV

VnVVnn1 

Slide 15

Properties of the Gradient 1. The gradient of a scalar function is a vector function. 2. The magnitude of V is the local maximum rate of change in V. 3. V points in the direction of maximum rate of change in V. 4. V at any is perpendicular to the constant V surface that passes through that point. 5. V points toward increasing numbers in V.

Slide 16

8 10/6/2020

Divergence of a Vector Field

Slide 17

Divergence of a Vector Field (1 of 2)

Start with the following vector field 𝐹⃗ 𝑥, 𝑦 .

Observe how the field seems to be converging to point in the upper left and diverging from a point in the low right.

Slide 18

9 10/6/2020

Divergence of a Vector Field (2 of 2)

The divergence is ∇ · 𝐹⃗ 𝑥, 𝑦 .

Divergence measures the tendency of a vector field to diverge from a point or converge to a point.

Divergence is a scalar quantity and is shown as the colored regions. Blue indicates negative divergence (convergence) and red indicates positive divergence.

Slide 19

Divergence of a Vector Field (2D)

Vector Field 𝐴⃗ 𝑥, 𝑦 Divergence ∇ · 𝐴⃗ 𝑥, 𝑦

Slide 20

10 10/6/2020

Divergence ∇ · 𝐴⃗

The divergence of a vector field is a scalar field that measures the tendency of a vector field to diverge from a point or converge to a point.

Coordinate Gradient Operation System

 A Ay A Cartesian A x   z xyz

 11  A  A A Cylindrical A    z   z  2 11 rAr   A sin 1A Spherical A    rrr2 sin  r sin

Slide 21

Algebra Rules for Divergence

  A BAB   Distributive Rule

Slide 22

11 10/6/2020

Properties of Divergence ∇ · 𝐴⃗

1. The divergence of a vector function is a scalar function. 2. The divergence of a scalar field does not make sense. 3. The original vector field will point form larger to smaller numbers in the scalar field.

Slide 23

Curl of a Vector Field

Slide 24

12 10/6/2020

Curl of a Vector Field (1 of 2)

Start with the following vector field 𝐹⃗ 𝑥, 𝑦 .

Observe how the field seems to be rotating around two different axes.

Slide 25

Curl of a Vector Field (1 of 2)

The curl is ∇𝐹⃗ 𝑥, 𝑦 .

Curl measures the tendency of the vector field to circulate around an axis.

Curl is a vector quantity and is shown as the blue arrows. The magnitude of the curl conveys the strength of the circulation. The direction of the curl is the axis of the circulation.

Slide 26

13 10/6/2020

Curl of a Vector Field (2D)

Vector Field 𝐴⃗ 𝑥, 𝑦 Curl ∇𝐴⃗ 𝑥, 𝑦

y

x z

y

x z

Slide 27

Curl

The curl of a vector function is a vector function that quantifies the tendency of the vector field to circulate around an axis. The magnitude of the curl conveys the strength of the circulation. The direction of the curl is the axis of the circulation.

Coordinate Curl Operation System

 AA AAzzyyAAxx  A  aaaˆˆˆxyz      Cartesian yz  zx   xy

  11AAAA  A  A  A zz aaˆˆ     a ˆ Cylindrical z zz       

  1111ArAsin A AA  rA A   aaaˆˆˆ rr    Spherical r  r rrrrrsin  sin    

Slide 28

14 10/6/2020

Algebra Rules for Curl

  A BAB   Distributive Rule

     A B  A  BB   A  B  AA   B

Slide 29

Properties of Curl

1. The curl of a vector function is a vector function. 2. The curl of a scalar field does not make sense.  3. Curl follows the right‐hand rule. A 4. The divergence of the curl of a vector field is always zero. ∇ · ∇𝐴⃗ 0 5. The curl of the gradient of a scalar field is always zero. ∇ ∇𝑉 0 6. Note that ∇ · 𝐴⃗ 𝐴⃗ · ∇. ∇ · 𝐴⃗ calculates the ⃗ ⃗  derivative of 𝐴, whereas 𝐴 · ∇ sets up A a derivative operation that is scaled by 𝐴⃗.

Slide 30

15 10/6/2020

Laplacian Operation

Slide 31

Scalar Laplacian ∇𝑉

The scalar Laplacian is defined as the divergence of the gradient. It is 2 sort of a measure of the tendency of the scalar function to form bowls. VV 

Coordinate Scalar Laplacian Operation System 222VVV 2V   Cartesian x222yz

22 2 11VVV   Cylindrical V  22  2      z

2 2211VVV     1  Spherical Vr22  sin   222 rr r rsin     r sin  

Slide 32

16 10/6/2020

Visualization of Scalar Laplacian ∇𝑉

2  Vx, y Vx , y

Slide 33

Vector Laplacian ∇𝐴⃗

The vector Laplacian is defined as the   2 AA    A gradient of the divergence minus the curl. 

Coordinate Scalar Laplacian Operation System  22 2 2 Cartesian A Aax ˆˆˆxyyzz Aa  Aa

 22 2 2 Cylindrical A Aaˆˆˆ  Aa  Aaz z

 22 2 2 Spherical A Aarrˆˆˆ Aa   Aa

Slide 34

17 10/6/2020

Visualization of Vector Laplacian ∇𝐴⃗

 Axy,  2 Axy,

Slide 35

Properties of the Laplacian

1. The Laplacian of a scalar function is a scalar function. 2. The scalar Laplacian arises when dealing with . 3. The Laplacian of a vector function is a vector function. 4. The vector Laplacian arises in the equation.

Slide 36

18 10/6/2020

Classification of Vector Fields

Slide 37

Irrotational  A vector field is irrotational if A 0

Examples of Irrotational Fields Gravity Electric potential

Irrotational Rotational

Consequences: 1. Irrotational fields must flow in essentially straight lines.   2. If A 0, then  Ad 0 and the field is said to be conservative. L

Slide 38

19 10/6/2020

Solenoidal (Divergenceless)  A vector field is solenoidal if A 0

Examples of Solenoidal Fields Fluid flows Magnetic fields

Consequences: 1. If the vector function does not diverge from any points, it must form loops.    2. If A 0, then  Ads0 and the field will have zero net flux. S

Slide 39

Laplacian Vector Fields

A vector field is Laplacian if it is both irrotational and solenoidal   A 0 A 0

Slide 40

20