2 scalar and vector field

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Scalar and Vector Fields Scalar Field : A scalar quantity, smoothly assigned to each point of a certain region of space is called a scalar field Examples : i)Temperature and pressure distribution in the atmosphere ii) Gravitational potential around the earth

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brief description of scalar and vector fields required for mathematical analysis

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Page 1: 2 Scalar and Vector Field

Scalar and Vector FieldsScalar Field :

A scalar quantity, smoothly assigned to each point of a certain region of space is called a scalar fieldExamples :i) Temperature and pressure

distribution in the atmosphereii) Gravitational potential around the

earth

Page 2: 2 Scalar and Vector Field

iii) Assignment to each point, its distance from a fixed point

222 zyxr

O

Page 3: 2 Scalar and Vector Field

O

),,( zyx

),,( zyxf

x

z

y

Once a coordinate system is set up, a scalar field is mathematically represented by a function : )(),,( rfzyxf

is the value of the scalar assigned to the point (x,y,z)

),,( zyxf

Page 4: 2 Scalar and Vector Field

A smooth scalar field implies that the function , is a smooth or differentiable function of its arguments, x,y,z.

),,( zyxf

Page 5: 2 Scalar and Vector Field

Since the scalar field has a definite value at each point, we must have

),,(),,( zyxfzyxf

O),,( zyxf

Consider two coordinate systems.

x

y

z

O’

z

y

x

),,( zyxf

Page 6: 2 Scalar and Vector Field

Vector Fields :

A vector quantity, smoothly assigned to each point in a certain region of space is called a vector field

Examples :

i) Electric field around a charged bodyii) Velocity variation within a steady flow of fluid

Page 7: 2 Scalar and Vector Field

iii) Position vector assigned to each point

Or

Page 8: 2 Scalar and Vector Field

Once a coordinate system is fixed, a vector field is mathematically represented by a vector function of position coordinates : )(),,( rForzyxF

O

)(rF

r

Page 9: 2 Scalar and Vector Field

Resolving the vector at each point into its three components, the vector field can be written as :

kzyxFjzyxFizyxFzyxF zyxˆ),,(ˆ),,(ˆ),,(),,(

A smooth vector field implies that the three functions, , are smooth or differentiable functions of the three coordinates x,y,z.

zyx FFF &,

Page 10: 2 Scalar and Vector Field

),(sin),(cos),( yxFyxFyxF yxx

),(cos),(sin),( yxFyxFyxF yxy

x

yF

x

y

How Are the Component Functions in Two Frames Related to One another?

Page 11: 2 Scalar and Vector Field

In Three Dimensions :

zyxx FRFRFRF 131211

zyxy FRFRFRF 232221

zyxz FRFRFRF 333231

MatrixRotationRRRRRRRRR

R

333231

232221

131211

Page 12: 2 Scalar and Vector Field

Gradient of a Scalar Field

dzzfdy

yfdx

xfrfrdrfdf

)()(

O

r rdr

rd

kdzjdyidxkzfj

yfi

xf ˆˆˆˆˆˆ

Page 13: 2 Scalar and Vector Field

rdf

Where, we have the shorthand notation :

fkzfj

yfi

xf

ˆˆˆ

Since is a vector assigned to each point

f

it defines a vector field. This vector field is called the gradient of the scalar field

f

Page 14: 2 Scalar and Vector Field

We have

df )ˆ(ˆ ndsrddsnfrdf

nfdsdf

n

ˆˆ

That is, the rate of change of a scalar field in any direction at a point, is the component of the gradient of the field in the given direction, at that point.

Page 15: 2 Scalar and Vector Field

Thus, gradient of a scalar field at any point may be defined as a vector, whose direction is the direction in which the scalar increases most rapidly, and whose magnitude is the maximum rate of change

fdsdfnf

dsdf

n

maxˆ

ˆ

And the maximum value occurs when is in the same direction as

n̂f

Page 16: 2 Scalar and Vector Field

Ex. 1.3Find the gradient of the scalar field :

222)( zyxrrf

and show that it has the properties as stated.

Page 17: 2 Scalar and Vector Field

Prob. 1.12The height of a certain hill (in feet) is given by :

)122818432(10),( 22 yxyxxyyxh

where x & y are distances (in miles) measured along two mutually perpendicular directions from a certain point. (c) How steep is the hill at the place (1 mi,

1 mi)(d) In which direction, must one move at this point so that the slope is 220 ft/mi

Page 18: 2 Scalar and Vector Field

x

y

),( yxh

Page 19: 2 Scalar and Vector Field

x

y

),( yxh

Page 20: 2 Scalar and Vector Field

Further Examples :

)()( rFrf b)

Let Then )()() rrFrrfi

)()() rrFrrfii

gdgdfrgfa

))(()

Page 21: 2 Scalar and Vector Field

Prob. 1.13

Let r be the separation vector from a fixed point to the point and let r be its length. Find :

),,( zyx ),,( zyx

a) (r2)

b) (1/r)

c) (rn)

Page 22: 2 Scalar and Vector Field

The ‘Del’ Operator

The gradient of a scalar field can be thought of as the result of the vector differential operator :

zk

yj

xi

ˆˆˆ

acting on the scalar field :f

zk

yj

xif

ˆˆˆ

Page 23: 2 Scalar and Vector Field

The gradient (2-dim) will be a vector field, if, at every point in space, we have :

yf

xf

xf

sincos

yf

xf

yf

cossin

Is the Gradient of a Scalar Field a Vector Field?

Prob. 1.14

Page 24: 2 Scalar and Vector Field

Important Properties of the Gradient1. The line integral of the gradient of a scalar field from one point to another, is independent of the path of integration (it depends only on the two points)

)()( 12

21

PfPfldfldfCC

1C2C

1P

2P

Page 25: 2 Scalar and Vector Field

2. Line integral of the gradient around a closed path is zero

0ldf

3. If the line integral of a vector field from one point to another is independent of the path joining them, then that vector field must be the gradient of a scalar field.

Page 26: 2 Scalar and Vector Field

),,( zyx

:),,( zyxffieldscalartheConstruct

),,(

)0,0,0(

),,(zyx

ldFzyxf

),,(int zyxpothetoorigintheconnectingpatharbitraryanyispaththewhere

Proof :Let be a vector field whose line integral is path independent.

F

Page 27: 2 Scalar and Vector Field

x y z

zyx zdzyxFydyxFxdxFzyxf0 0 0

),,()0,,()0,0,(),,(

),,( zyx

)0,0,(x)0,,( yx

Choosing the path as above

To show : Ff

Page 28: 2 Scalar and Vector Field

),,( zyxFzf

z

Similarly, choosing the paths as below,

),,( zyx

)0,0,(x

),0,( zx ),,( zyx

),,0( zy),0,0( z

xy FxfF

yf

&

Page 29: 2 Scalar and Vector Field

fF

),,( zyx

),,( 000 zyx

),,(

),,( 000

),,(zyx

zyx

ldFzyxg

However, the scalar field, whose gradient is the vector field , is not unique.

F

Page 30: 2 Scalar and Vector Field

We still have : gF

),,(

)0,0,0(

000

),,(),,(zyx

ldFzyxgzyxf

Czyxg ),,(

However,

That is, the two scalar fields, which give us the same vector field as their gradient, differ from each other by a constant.

Page 31: 2 Scalar and Vector Field

If the scalar field is constructed as :

),,(

),,( 000

),,(zyx

zyx

ldFzyxf

then :0),,( 000 zyxf

Since are arbitrary, the zero of the scalar field is arbitrary.

000 &, zyx

Page 32: 2 Scalar and Vector Field

Level or constant surfaces of a scalar field

Given a scalar field , the locus of all points which

satisfy the condition :

),,( zyxf

Czyxf ),,(

defines a surface, known as the level or constant surface

of the field

Czyxf ),,(

Page 33: 2 Scalar and Vector Field

1C2C

3C

Page 34: 2 Scalar and Vector Field

),,(),,( 000 zyxfzyxf

Through every point in space, one can draw a level surface of :

),,( 000 zyxf

Page 35: 2 Scalar and Vector Field

Level surfaces of the scalar field :222),,( zyxzyxf

Page 36: 2 Scalar and Vector Field

4. The gradient of a scalar field, at each point in space, is perpendicular to the level surface (constant surface) of the scalar field, passing through that point

.),,( Constzyxf

Pf

P

Page 37: 2 Scalar and Vector Field

Ex.: Find the unit normal to the surface :

22 yxz

Page 38: 2 Scalar and Vector Field

Given the three components of a vector field, , one can construct nine first derivatives :

zyx FFF &,

zF

yF

xF zxx

.,..........,,

What scalar and vector fields can be constructed out of these nine first derivatives?

Divergence and Curl of a Vector Field

Page 39: 2 Scalar and Vector Field

Correction!

x

y

'x

'y

),( 00 yx

Coordinate Transformation Equations

;)(sin)(cos 00 yyxxx

)(cos)(sin 00 yyxxy

;sincos 0xyxx 0cossin yyxy

Page 40: 2 Scalar and Vector Field

It turns out that only one scalar field and one vector field can be constructed out of these nine first derivatives :Divergence :

zF

yF

xFF zyx

Curl :

kyF

xF

jxF

zFi

zF

yFF xyzxyz ˆˆˆ

Page 41: 2 Scalar and Vector Field

kFjFiFz

ky

jx

iF zyxˆˆˆˆˆˆ

kFjFiFz

ky

jx

iF zyxˆˆˆˆˆˆ

zyx FFFzyx

kji

ˆˆˆ

Page 42: 2 Scalar and Vector Field

Example :

Let the vector field be : rrF

)(

3 F

0

F

Page 43: 2 Scalar and Vector Field

Surface Integral of a Vector Field

F

ad

S

S

adF

Page 44: 2 Scalar and Vector Field

i) Gauss’ Divergence Theorem :

S V

dFadF

VS

Here, is any vector field and , any closed surface

F

S

Two Important Theorems

ad

Page 45: 2 Scalar and Vector Field

A Simple Application of Divergence Theorem

General Proof of Archimedes’ Principle

S S

b adPFdF

xy

zFd dah )()( zhgzP

Page 46: 2 Scalar and Vector Field

ii) Stokes’ Curl Theorem

ld

ad

C S

adFldF )(

Here, C is any closed loop (planar or otherwise), and S is any surface bounded by the loop.

Page 47: 2 Scalar and Vector Field

Second DerivativesfieldVectorf

2

2

2

2

2

2

)(zf

yf

xff

i) f2

Where is a second derivative operator, known as the Laplacian.

2

2

2

2

2

22

zyx

ii) 0

f

Page 48: 2 Scalar and Vector Field

fieldscalarAF

F

a legitimate vector field, which is not much used.

Page 49: 2 Scalar and Vector Field

fieldvectorAF

0) Fi

FFFii

2)

Page 50: 2 Scalar and Vector Field

Certain Product Rules

)()()(.1 fggffg

)()()(.2 ABBABA

ABBA)()(

)()()(.3 fFFfFf

)()()(.4 BAABBA

Page 51: 2 Scalar and Vector Field

Prob. 1.60Show that

V S

adTdTa

)()(

Hence show that :0

S

adaProb. 1.61b :

Prob. 1.61c : a is the same for all surfaces sharing the same boundary.

Page 52: 2 Scalar and Vector Field

Prob. 1.61a : Find the vector area of a hemispherical bowlBack to Prob. 1.60

V S

adFdFb )()(

V S

adTUUTdTUUTd

)()()( 22

Page 53: 2 Scalar and Vector Field

Prob. 1.61d

Show that : ldra

21

Proof :

C S

adrAldrA )]([)(

Use the product rule :BAABBA)()()(

)()( ABBA

Page 54: 2 Scalar and Vector Field

Two Important Results

i) If the Curl of a vector field vanishes, then that vector field must be the gradient of a scalar field :

fFtsfF

..0

We have seen : 0)0) Fiifi

The converse results are also true.

Page 55: 2 Scalar and Vector Field

ii) If the Divergence of a vector field vanishes, then the vector field must be the Curl of a scalar field :

GFtsGF

..,0

Page 56: 2 Scalar and Vector Field

Theorem I : The following statements are equivalent.(A) Vector field is such that its line integral around any closed path is zero

F

(C) Vector field is the gradient of a scalar field

F

(B) Vector field is such that its line integral from one point to another is independent of the path joining the two.

F

Page 57: 2 Scalar and Vector Field

)()()()( DCBA Or

)()()()()( ADCBA

(D) Vector field is such that it has a vanishing curl

F