Section 17.1 - Gordon State College

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Transcript Section 17.1 - Gordon State College

Section 17.1

Vector Fields

VECTOR FIELDS

Definition:

Let

D

vector field on

  2 2 is a (vector-valued) function

F

assigns to each point (

x

,

y

) in

D

that a two-dimensional vector

F

(

x

,

y

).

Since

F

(

x

,

y

) is a two-dimensional vector, we can write it in terms of its

component functions

P

and

Q

as follows:

F

(

x

,

y

) 

P

(

x

,

y

)

i

Q

(

x

,

y

)

j

P

(

x

,

y

),

Q

(

x

,

y

)

F

P

i

Q

j

The functions

P

and

Q

are sometimes called

scalar functions

.

EXAMPLES

Sketch the following vector fields.

1.

F

(

x

,

y

) = − yi + xj 2.

F

(

x

,

y

) = 3 xi + yj

VECTOR FIELDS (CONCLUDED)

Definition:

Let

E

 3

vector field on

 3 is a function

F

that assigns to each point ( three-dimensional vector

F

(

x

,

y

,

z

).

x

,

y

,

z

) in

E

a We can express

F

in terms of its component functions

P

,

Q

, and

R

as

F

(

x

,

y

,

z

) =

P

(

x

,

y

,

z

)

i

+

Q

(

x

,

y

,

z

)

j

+

R

(

x

,

y

,

z

)

k

Three dimensional vector fields can be sketched in space. See Figures 9 through 12 on page 1094.

PHYSICAL EXAMPLES OF VECTOR FIELDS

• •

Velocity fields

describe the motions of systems of particles in the plane or space.

Gravitational fields

are described by

Newton’s Law of Gravitation

, which states that the force of attraction exerted on a particle of mass

m

located at

x

=

x

,

y

,

z

by a particle of mass

M

located at (0, 0, 0) is given by

F

(

x

)  

mMG

x

|

x

| 3 where

G

is the gravitational constant.

PHYSICAL EXAMPLES OF VECTOR FIELDS (CONTINUED)

Electric force fields

are defined by

Coulomb’s Law

, which states that the force exerted on a particle with electric charge

q

located at (

x

,

y

,

z

) by a particle of charge

Q

located at (0, 0, 0) is given by 

F

(

x

) 

qQ

x x

3 where

x

= xi + yj + zk and

ε

is a constant that depends on the units for |

x

|,

q

, and

Q

.

INVERSE SQUARE FIELDS

Let

x

(

t

) =

x

(

t

)

i

+

y

(

t

)

j

+

z

(

t

)

k

be the position vector. The vector field

F field

if is an

F

(

x

) 

k

|

x

| 3

x inverse square

where

k

is a real number.

Gravitational fields and electric force fields are two physical examples of inverse square fields.

GRADIENTS AND VECTOR FIELDS

Recall that the gradient of a function

f

(

x

,

y

,

z

) is a vector given by 

f

(

x

,

y

,

z

) 

f x

(

x

,

y

,

z

)

i

f y

(

x

,

y

,

z

)

j

f z

(

x

,

y

,

z

)

k

Thus, the gradient is an example of a vector field and is called a

gradient vector field

.

NOTE: There is an analogous gradient field for two dimensions.

CONSERVATIVE VECTOR FIELDS

Definition:

A vector field

F

is called a

conservative vector field

if it is the gradient of some scalar function

f

differentiable function , that is if there exists a

f

such that . The function

f

F

.

is called the

potential function

for

EXAMPLES

1. Show that

F

(

x

,

y

) = 2 xi + yj is conservative.

2. Show that any inverse square field is conservative.