Electric field and forces

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Electric field and forces. Let’s reconsider Coulomb interaction. We know already. We ask: How does particle B know that A is there to exert a force. and vice versa. Answer: The presence of charge A alters the empty space and charge B experiences this alteration we call electric field. - PowerPoint PPT Presentation

Transcript of Electric field and forces

Page 1: Electric field and forces

Do you have access to MasteringPhysics

A) Yes B) No C) No, but I am confident

to get it from the bookstore before Thursday January 23

Clicker question

Page 2: Electric field and forces

Electric field and forces

Let’s reconsider Coulomb interaction

We know already

20

00 4

1

r

qqF A

We ask:How does particle B know that A is there to exert a force

Answer:The presence of charge A alters the empty space and charge B experiences this alteration we call electric field

Point P

0

0

q

FE

and vice versa

Page 3: Electric field and forces

Point P

0

0

q

FE

EqF 00

The concept of probing the electric field by the force experienced by a test charge gives rise to the definition:

The electric field E at a given point is given by the force F0

experienced by the test charge q0 divided by q0

0

0

00

limq

FE

q

A test charge q0 at point P experiences the force

The limit makes sure that the test charge does not affect the surrounding charge distribution

Page 4: Electric field and forces

q0

q

Vector properties of E originate from vector properties of F 0

0

0

00

limq

FE

q From we realize that the electric field is a vector quantity

Let’s first have a closer look to the vector properties of the Coulomb force

x

y

z 1r2r

2 1r r r F 0 points in the direction of

2 1r r r

00 2

0

4

q qF r

r

When writing:

ˆ :r

rr

where and

is a unit vector pointingin direction of

rEverything is taken care of, including the various signs of both charges

Page 5: Electric field and forces

With the full vector information about the force F0 the test charge experiences in an electric field of a point charge q we can visualize the vector character of the E-field of a point charge

00 2

0

4

q qF r

r

+q

20

4

qE r

r

E-field of a positive point charge:

x

y

z

q0

q0

Page 6: Electric field and forces

-q

E-field of a negative point charge:

is mathematically speaking a vector field( )E r

-Remember: for a 1-dimensional function we assign to every x a value f(x) -for a vector field in 3d we assign to every point in 3d space a vector

( , , )r x y z( ( , , ), ( , , ), ( , , ))x y zE E x y z E x y z E x y z

If 0( )E r E independent of (x,y,z) we say the field is homogeneous A special case is the zero electric field inside a

conductor Electrostatic fields must be zero here because otherwise they would drive a current

Page 7: Electric field and forces

For the charge distribution shown in the figure indicate a region where a point exists at which the net electric field is zero

A) Region A

B) Region B

C) Point C

D) Region D

E) Region E

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