2 scalar and vector field
DESCRIPTION
brief description of scalar and vector fields required for mathematical analysisTRANSCRIPT
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
iii) Assignment to each point, its distance from a fixed point
222 zyxr
O
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
A smooth scalar field implies that the function , is a smooth or differentiable function of its arguments, x,y,z.
),,( zyxf
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
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
iii) Position vector assigned to each point
Or
Once a coordinate system is fixed, a vector field is mathematically represented by a vector function of position coordinates : )(),,( rForzyxF
O
)(rF
r
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 &,
),(sin),(cos),( yxFyxFyxF yxx
),(cos),(sin),( yxFyxFyxF yxy
x
yF
x
y
How Are the Component Functions in Two Frames Related to One another?
In Three Dimensions :
zyxx FRFRFRF 131211
zyxy FRFRFRF 232221
zyxz FRFRFRF 333231
MatrixRotationRRRRRRRRR
R
333231
232221
131211
Gradient of a Scalar Field
dzzfdy
yfdx
xfrfrdrfdf
)()(
O
r rdr
rd
kdzjdyidxkzfj
yfi
xf ˆˆˆˆˆˆ
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
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.
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
Ex. 1.3Find the gradient of the scalar field :
222)( zyxrrf
and show that it has the properties as stated.
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
x
y
),( yxh
x
y
),( yxh
Further Examples :
)()( rFrf b)
Let Then )()() rrFrrfi
)()() rrFrrfii
gdgdfrgfa
))(()
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)
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
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
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
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.
),,( zyx
:),,( zyxffieldscalartheConstruct
),,(
)0,0,0(
),,(zyx
ldFzyxf
),,(int zyxpothetoorigintheconnectingpatharbitraryanyispaththewhere
Proof :Let be a vector field whose line integral is path independent.
F
x y z
zyx zdzyxFydyxFxdxFzyxf0 0 0
),,()0,,()0,0,(),,(
),,( zyx
)0,0,(x)0,,( yx
Choosing the path as above
To show : Ff
),,( zyxFzf
z
Similarly, choosing the paths as below,
),,( zyx
)0,0,(x
),0,( zx ),,( zyx
),,0( zy),0,0( z
xy FxfF
yf
&
fF
),,( zyx
),,( 000 zyx
),,(
),,( 000
),,(zyx
zyx
ldFzyxg
However, the scalar field, whose gradient is the vector field , is not unique.
F
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.
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
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 ),,(
1C2C
3C
),,(),,( 000 zyxfzyxf
Through every point in space, one can draw a level surface of :
),,( 000 zyxf
Level surfaces of the scalar field :222),,( zyxzyxf
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
Ex.: Find the unit normal to the surface :
22 yxz
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
Correction!
x
y
'x
'y
),( 00 yx
Coordinate Transformation Equations
;)(sin)(cos 00 yyxxx
)(cos)(sin 00 yyxxy
;sincos 0xyxx 0cossin yyxy
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
kFjFiFz
ky
jx
iF zyxˆˆˆˆˆˆ
kFjFiFz
ky
jx
iF zyxˆˆˆˆˆˆ
zyx FFFzyx
kji
ˆˆˆ
Example :
Let the vector field be : rrF
)(
3 F
0
F
Surface Integral of a Vector Field
F
ad
S
S
adF
i) Gauss’ Divergence Theorem :
S V
dFadF
VS
Here, is any vector field and , any closed surface
F
S
Two Important Theorems
ad
A Simple Application of Divergence Theorem
General Proof of Archimedes’ Principle
S S
b adPFdF
xy
zFd dah )()( zhgzP
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.
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
fieldscalarAF
F
a legitimate vector field, which is not much used.
fieldvectorAF
0) Fi
FFFii
2)
Certain Product Rules
)()()(.1 fggffg
)()()(.2 ABBABA
ABBA)()(
)()()(.3 fFFfFf
)()()(.4 BAABBA
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.
Prob. 1.61a : Find the vector area of a hemispherical bowlBack to Prob. 1.60
V S
adFdFb )()(
V S
adTUUTdTUUTd
)()()( 22
Prob. 1.61d
Show that : ldra
21
Proof :
C S
adrAldrA )]([)(
Use the product rule :BAABBA)()()(
)()( ABBA
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.
ii) If the Divergence of a vector field vanishes, then the vector field must be the Curl of a scalar field :
GFtsGF
..,0
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
)()()()( DCBA Or
)()()()()( ADCBA
(D) Vector field is such that it has a vanishing curl
F