Electric Potential - Engineering Physics - Lecture Slides, Slides of Engineering Physics

This course is designed for engineers. This subject is compiled of physical applications and concepts. This lecture includes: Line of Charge, Semicircle of Charge, Electric Field Due to a Line of Charge, Entire Surface of Charge, Uniform Charge Density

Typology: Slides

2012/2013

Uploaded on 09/27/2013

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Today’s agenda:
Electric potential of a charge distribution.
You must be able to calculate the electric potential for a charge distribution.
Equipotentials.
You must be able to sketch and interpret equipotential plots.
Potential gradient.
You must be able to calculate the electric field if you are given the electric potential.
Potentials and fields near conductors.
You must be able to use what you have learned about electric fields, Gauss’ law, and
electric potential to understand and apply several useful facts about conductors in
electrostatic equilibrium.
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Today’s agenda:

Electric potential of a charge distribution. You must be able to calculate the electric potential for a charge distribution.

Equipotentials. You must be able to sketch and interpret equipotential plots.

Potential gradient. You must be able to calculate the electric field if you are given the electric potential.

Potentials and fields near conductors. You must be able to use what you have learned about electric fields, Gauss’ law, and electric potential to understand and apply several useful facts about conductors in electrostatic equilibrium.

Electric Potential of a Charge Distribution

Example 1: potential and electric field between two parallel

conducting plates.

Assume V 0 <V 1 (so I have a direction to draw the electric field).

Also assume the plates are large compared to their separation,

so the electric field is constant and perpendicular to the plates.

V 0 V 1

Also, let the plates be separated E

by a distance d.

d

V Ed

Important note: the derivation of

did not require rectangular plates, or any plates at all. It works

as long as E is uniform and parallel or antiparallel to d.

In general, E should be replaced by the component of along

the displacement vector.

E

d V^ ^ E d

Example 2: A rod of length L located along the x-axis has a total

charge Q uniformly distributed along the rod. Find the electric

potential at a point P along the y-axis a distance d from the

origin.

y

x

P

d

L

dq

x dx

r

=Q/L

dq=dx

2 2

dq dx dV k k r (^) x d

L

0

V  dV 

What are we assuming when we use this equation?

Example 3: Find the electric potential due to a uniformly

charged ring of radius R and total charge Q at a point P on the

axis of the ring.

P

R

dQ

r

x

x

Every dQ of charge on the

ring is the same distance

from the point P.

2 2

dq dq dV k k r (^) x R

ring ring^2

dq V dV k

x R

 

P

R

dQ

r

x

x

(^2 2) ring

k V dq

x R

2 2

kQ V

x R

Could you use this expression for V to calculate E? Would you

get the same result as I got in Lecture 3?

You must derive an equation for the potential at the center of a ring if you need it for homework! In lecture I will show you how easy the derivation is.

Include the sign of Q to get the correct sign for V.

Homework hint: derive this equation in tomorrow’s homework!

P

r

dQ

x x R

R

ring ring 2 2 0 2 2 0 0

1 2 rdr rdr V dV (^4) x r 2 x r

R 2 2 2 2 2 2 2 0 0 0 0

Q

V x r x R x x R x

2 2 2 R

2

Q

R

2 2 2 0

Q

V x R x 2 R

P

r

dQ

x x R

Could you use this expression for V to calculate E? Would you

get the same result as I got in Lecture 3?

See your text for other examples of potentials calculated from

charge distributions, as well as an alternate discussion of the

electric field between charged parallel plates.

Remember: worked examples in the text are “testable.”

Make sure you know what Vab means, and how it relates to

V.

Vif = Vf – Vi so Vif = -Vif

Special Dispensation

For tomorrow’s homework only: you may use the equation for the

electric field of a long straight wire without first proving it:

line 0

E.

2 r

Of course, this is relevant only if a homework problem requires you

to know the electric field of a long straight wire.

You can also use this equation for the electric field outside a long

cylinder that carries charge.

Homework Hints!

In energy problems involving potentials, you may know the

potential but not details of the charge distribution that

produced it (or the charge distribution may be complex). In

that case, you don’t want to attempt to calculate potential

energy using. Instead, use U  q V.

If the electric field is zero everywhere in some region, what

can you say about the potential in that region? Why?

1 2

12

q q

U k

r

PRACTICAL APPLICATION

For some reason you think practical applications are important.

Well, I found one!

Today’s agenda:

Electric potential of a charge distribution. You must be able to calculate the electric potential for a charge distribution.

Equipotentials. You must be able to sketch and interpret equipotential plots.

Potential gradient. You must be able to calculate the electric field if you are given the electric potential.

Potentials and fields near conductors. You must be able to use what you have learned about electric fields, Gauss’ law, and electric potential to understand and apply several useful facts about conductors in electrostatic equilibrium.

Equipotentials

Equipotentials are contour maps of the electric potential.

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