

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
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.
Typology: Study notes
1 / 2
This page cannot be seen from the preview
Don't miss anything!


PHY 101 Lecture #7 Electrical circuits 1
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
PHY 101 Lecture #7 Electrical circuits 3
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
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
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
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.
ε
PHY 101 Lecture #7 Electrical circuits 7
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
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 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’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
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
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.