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Vector Differentiation: Lecture #3

The document discusses vector differentiation and the gradient, divergence, and curl operators. 1. It defines the gradient of a scalar function as the vector of its partial derivatives, and explains that the gradient points in the direction of maximum increase of the function. 2. It provides the definitions of divergence and curl for vector fields in Cartesian, cylindrical, and spherical coordinate systems. Divergence measures how a vector field spreads out from a point, while curl measures swirling or rotation. 3. It discusses the geometric interpretations of gradient, divergence, and curl and gives examples to illustrate their meanings. Product rules involving these operators are also presented.

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Yash Kala
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0% found this document useful (0 votes)
84 views21 pages

Vector Differentiation: Lecture #3

The document discusses vector differentiation and the gradient, divergence, and curl operators. 1. It defines the gradient of a scalar function as the vector of its partial derivatives, and explains that the gradient points in the direction of maximum increase of the function. 2. It provides the definitions of divergence and curl for vector fields in Cartesian, cylindrical, and spherical coordinate systems. Divergence measures how a vector field spreads out from a point, while curl measures swirling or rotation. 3. It discusses the geometric interpretations of gradient, divergence, and curl and gives examples to illustrate their meanings. Product rules involving these operators are also presented.

Uploaded by

Yash Kala
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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Vector Differentiation

Lecture #3
Gradient
For a function f (x), what does df / dx imply? d f 
d f   d x
 dx 
f f
For a small change in x, how fast does f change ?
Consider a scalar function T (x, y, z)
x x
T T T
dT  dx dy dz
x y z

dl  xˆ d x  yˆ d y  zˆ d z
 T T T  ˆ
 xˆ  yˆ  zˆ  .  x d x  yˆ d y  zˆ d z   d T Geometric interpretation of Gradient:
 x y z 
For a given (dl) mag , dT is max when 
     = 0   T lies along which dT is max
T  grad T   xˆ  yˆ  zˆ 
 x y z 
Consider a constant temperature surface:

Let 
 n̂ PQ = d l
T Q (x + x, y + y, z + z)  xˆ d x  yˆ d y  zˆ d z
P (x, y, z)

dT  ?
 
T . d l 
Constant
temperature
Constant
surface
temperature
 
T l cos   2 = 0
surface
In cylindrical coordinates T (s, , z): T T T
dT  ds  d  dz
s  z

dl  ds  sˆ  sd ˆ  dz  zˆ
 
 dT  T . d l
where  T 1 T ˆ T
T  s
ˆ  zˆ
cyl s s  z
In spherical coordinates (r, , ):
T T T
dT  dr  d  d
r  

dl  dr  rˆ  rd ˆ  r sin  d ˆ
 
 dT  T . d l
 T 1 T ˆ 1 T ˆ
T  rˆ   
sph r r  r sin  
   
  xˆ  yˆ  zˆ
x y z


Vector ? T : Is this a product of del and T ?

 : A vector operator

An ordinary vector can multiply in 3 different ways

Three different ways it can act on:



1. T on a scalar (via the gradient)
 
2.  . v on a vector function (via the divergence)
 
3.   v on a vector function (via the curl)
Curl operation + Fundamental
Theorems of Vector Calculus
      vx  v y  vz
.v   xˆ  yˆ  zˆ  . v x xˆ  v y yˆ  v z zˆ  
Recap:
 
 x y z  x  y z
What would be div of a scalar? Meaningless! A scalar
Geometrical interpretation: Measure of how much v spreads out from the point P


P
P
P
P P

Positive divergence Negative divergence Zero divergence


A vector whose divergence is zero is also
A sphere embedded in a referred as solenoidal
3D-divergent vector field Example of a saw dust sprinkling at the
edge of a pond

.v in cylindrical coordinates:

 1  1 v v z
.v  svs   
s s s  z
In spherical coordinates
 1  2  1 v
.v  2
r r
r vr   1

r sin  
sin  v  
r sin  
 
Curl of a vector:   v
xˆ yˆ zˆ
    
 zˆ   v x xˆ  v y yˆ  v z zˆ 
    
 xˆ  yˆ v  a vector
 z y z  x y z
vx vy vz
Geometrical interpretation:
 
  v is a measure of how much v curls/swirls around the point in question
For div v: z
z
P

y y

What will be its curl? x x

What will be the direction of the curl?


Example: drop a paddlewheel on the edge of a pond

y
x
Consider flow of water in a river and if we
wish to determine if it has a curl, then we put Calculate curls of
a paddle wheel into the water and see if it
turns i) va  xyˆ

ii) vb   yxˆ  xyˆ


i)
xˆ yˆ zˆ ii) xˆ yˆ zˆ
         
v  v 
x y z x y z
0 x 0 y x 0

For a finite curl it will turn/spin  ẑ  2 ẑ


otherwise it will not spin
In cylindrical coordinates (s,, z) :

   1 v z v   vs v z  1  vs 


  v     sˆ        sv  
ˆ
 zˆ
 s  z   z s  s  s  

In spherical coordinates (r, , ):


    v  1  1 vr  ˆ
v 
1
 sin  v    rˆ    rv  
r sin 
    r  sin   r 
1  vr  ˆ
  r v    
r  r  
Product rules:
  
  f g   f g  g f
  
        
      
     
Involving gradient:
 A. B  A    B  B    A  A. B  B . A

Involving divergence:

     
    
 . f A  f  . A  A . f

    
        
 . A  B  B .   A  A.   B 

Involving curl:

     
    
  f A  f   A  A  f

  A  B   B .   A  A .   B  A  . B   B  . A
              

T ?
        T T T   2T  2T  2T

. T   ˆ
x  ˆ
y  ˆ
z 
 . 
 ˆ
x  ˆ
y  ˆ
z 
      2
T
 x y z   x y z  x  y z
2 2 2

Laplacian of
In cylindrical coordinates: a scalar T
1   T  1  T  T
2 2
T
2
s  2  2
s s  s  s  2
z
In spherical coordinates:

1  2 T  1   T  1   2T 
 T  2 r  2  sin   2 2  2 
2

r  r  r sin      r sin    
 
 
 T  0

 
  
.   v  0

   
      2
   v    . v   v
Line, surface, and volume integrals:
y
 
b
Line integral:

a
v . dl
Path
dl b

a z

x
Physical example:
 

Work done by a force: W  F . d l

If the Path forms a closed loop i.e. for b = a


 
 v . d l
For a special class of vector functions, line integral is independent of the Path
True for conservative forces
Surface integral:
  z da
 v .d a
S
y
 
 v .d a
For a closed surface:
(e.g. forming a balloon) x

If the vector function represents flow of a fluid, the surface integral will represent
total mass/time passing through the surface

Volume integral:
 T d
v
a scalar
If T represents density of a substance, which may vary from point to point, then the
volume integral will represent total mass
Fundamental theorem for gradients:
Consider a scalar function T (x, y, z)
y
Starting at a as one moves a short distance dl1 change in
b T will be  
d T  T . d l1
dl1
a z  Total change in T as one moves from a to b along a
specified path:

 
x b   b 
Path
a
T . d l   dT  T (b)  T (a )
a
  v .dl  0

This is the algebraic form of the fundamental theorem for gradients

Line integral of the derivative of a function is given by the value of the function at the
boundaries
Example: measuring height of Eiffel Tower
 
b   b
Path
a
T . d l   dT  T (b)  T (a )
a

1. Measure each step and add  LHS

2. Difference between two


readings of an altimeter  RHS

• Height: 1063 ft (324 m)


• Steps: 1710

 
b  
Corollary 1: T . d l is independent of the path from a to b
a
 Line integral of gradient is path independent

 
 
 T b   T b   0
Corollary 2:
T . d l  0
 
Fundamental theorem for divergences :    
. v d   v . d a
V
S
Also known as
Gauss’s theorem or Green’s theorem or divergence theorem
Integral of the divergence of a vector function over a region
equals the value of the function at the boundary i. e. surface that bounds the volume

Geometrical interpretation:
If v: flow of an incompressible liquid then the R.H.S would represent total
amount of liquid passing out/time through the surface

Divergence means spreading out e.g. Tap pouring out water

For a bunch of taps assuming each pours out equal amount of


incompressible fluid, one can determine total amount by using the
divergence theorem
(taps within the volume) =  (flow of fluid out through the surface)
 
Fundamental theorem for curls:     
  v . da   v . d l
S P

Integral of a derivative of a function over a region equals value of the function at its boundary

Curl Perimeter

Geometrical interpretation:
Twist of v 

 
    
  v . da
S
 v .dl
P

 
  
Corollary 1:   v . d a Depends only on the boundary line and not on the surface

   v . d a  0
  
Corollary 2: For a close surface e.g. mouth of a balloon

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