PHY 101 Lecture #7: Electric Field, Potential, and Intro to Circuits, Study notes of Physics

A lecture note from physics 101 at syracuse university, covering the topics of electric fields, electric potential energy and voltage, and a simple electrical circuit. The professor, peter r. Saulson, explains the concept of electric fields and their relation to electric forces, the electric field for a point charge, and the electric field from two charged metal plates. He also discusses the concept of electrical potential energy and voltage, and how they are related to electric fields. The lecture concludes with an introduction to a simple electrical circuit, explaining the role of a resistor in allowing current to flow.

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Uploaded on 08/09/2009

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PHY 101 Lecture #7 Electrical circuits 1
PHY 101 Lecture #7:
Electric Field, Electric Potential,
and Intro to Electrical Circuits
Prof. Peter R. Saulson
http://physics.syr.edu/courses/PHY101/
Off. Hrs: Tue 9:30 –11:00, Physics 263-4
Prof. Schwarz’s Problem Sessions:
Mon and Tues, 5:15 – 6:15, Physics 202/204
PHY 101 Lecture #7 Electrical circuits 2
Outline
1. Electric fields
2. Electric potential energy and voltage
3. A simple circuit
PHY 101 Lecture #7 Electrical circuits 3
Recall from last Thursday:
Electrical forces
Electrical phenomena recognized by electrical
forces.
Force between two charges q1and q2given by
Coulomb’s Law:
where charges are in coulombs, distance r in
meters, and ke= 8.99*109 N m2/C2. Force
comes out in newtons.
,
221
r
qqk
Fe
elec =
PHY 101 Lecture #7 Electrical circuits 4
1. Electric fields
It is useful to represent the effect of charges on
each other with the concept of the electric field.
When you have more than two charges,
Coulomb’s Law
would have to be applied for each pair of
charges, then summed.
Instead, you can write Fe=qE.
The electric field Erepresents the effect of all other
charges on the charge q.
,
221
r
qqk
Fe
elec =
PHY 101 Lecture #7 Electrical circuits 5
Electric field for a point charge
The electric force on a charge qdue to another
point charge Qis
Or, we can say that the electric field due to the
charge Qis
and then recall F= qE.
,
2
r
kQ
E=
,
2
r
qQk
Fe
elec =
PHY 101 Lecture #7 Electrical circuits 6
Electric field from
two charged metal plates
The field from a point charge is radial, and falls
off with distance.
Complicated
We can make a uniform electric field by putting
equal and opposite charges Qon two parallel
metal plates.
Field has strength
where Ais the area of the plates, and
ε
0= 8.85 * 10-12 C2/N m2.
,
0A
Q
E
ε
=
pf2

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PHY 101 Lecture #7 Electrical circuits 1

PHY 101 Lecture #7:

Electric Field, Electric Potential,

and Intro to Electrical Circuits

Prof. Peter R. Saulson [email protected] http://physics.syr.edu/courses/PHY101/ Off. Hrs: Tue 9:30 –11:00, Physics 263- Prof. Schwarz’s Problem Sessions: Mon and Tues, 5:15 – 6:15, Physics 202/

PHY 101 Lecture #7 Electrical circuits 2

Outline

  1. Electric fields
  2. Electric potential energy and voltage
  3. A simple circuit

PHY 101 Lecture #7 Electrical circuits 3

Recall from last Thursday:

Electrical forces

Electrical phenomena recognized by electrical forces.

Force between two charges q 1 and q 2 given by Coulomb’s Law:

where charges are in coulombs, distance r in meters, and k (^) e = 8.99*10^9 N m^2 /C^2. Force comes out in newtons.

r

kq q Felec = e

PHY 101 Lecture #7 Electrical circuits 4

1. Electric fields

It is useful to represent the effect of charges on each other with the concept of the electric field. When you have more than two charges, Coulomb’s Law

would have to be applied for each pair of charges, then summed. Instead, you can write F e = q E. The electric field E represents the effect of all other charges on the charge q.

212 , r

kq q F (^) elec = e

PHY 101 Lecture #7 Electrical circuits 5

Electric field for a point charge

The electric force on a charge q due to another point charge Q is

Or, we can say that the electric field due to the charge Q is

and then recall F = q E.

2 , r E =^ kQ

r

k qQ Felec = e

PHY 101 Lecture #7 Electrical circuits 6

Electric field from

two charged metal plates

The field from a point charge is radial, and falls off with distance. Complicated We can make a uniform electric field by putting equal and opposite charges Q on two parallel metal plates. Field has strength

where A is the area of the plates, and ε 0 = 8.85 * 10 -12^ C^2 /N m 2.

0 A

Q

E

ε

PHY 101 Lecture #7 Electrical circuits 7

Motion of charge in

a uniform electric field

In a uniform field, a charge feels a constant force. Like a mass in Earth’s gravitational field. So motion is accelerated in the same way. Use this to control the motion of beams of electrons, in a cathode ray tube. Television, computer monitor, etc.

PHY 101 Lecture #7 Electrical circuits 8

2. Electrical potential energy

Electrical force means you have to do work to move an electric charge from one position to another. If you have to do work to move the charge, then you store electrical potential energy in the system. The units of electrical PE are joules.

PHY 101 Lecture #7 Electrical circuits 9

Voltage

Voltage at some location is defined as the electrical potential energy that would be stored in moving 1 C of charge from a reference point to that location.

SI unit of voltage is the joule/coulomb, also known as the volt.

PHY 101 Lecture #7 Electrical circuits 10

Voltage in real life

Voltage’s definition may sound awkward, but it is easy to measure with a voltmeter.

Voltage between two points is easy to set, using a battery, which maintains a fixed voltage between its two terminals. Many kinds of battery available, with voltages between 1 and 24 volts. Later, we will study the chemistry that makes them work.

PHY 101 Lecture #7 Electrical circuits 11

3. A simple circuit

battery (^) component

A single component completes the circuit from one battery terminal to the other.

Here, the component is a resistor. A resistor lets current flow, but not freely as a wire would.

PHY 101 Lecture #7 Electrical circuits 12

Intuition about voltage

Voltage is sometimes called “electromotive force”. It makes circuits “go.” A ball falls down because of gravitational force (or equivalently, because it can give up GPE.) Currents flow in a circuit because they are given a path from high voltage to low voltage.