Coulomb’s Law Performing electric field calculations on charge distributions in an X-Y coordinate Plane.

Slides:



Advertisements
Similar presentations
R3-1 Physics I Review 3 Review Notes Exam 3. R3-2 Newton’s Law of Universal Gravitation.
Advertisements

Electric Forces and Electric Fields. Properties of Electric Charges Two types of charges exist They are called positive and negative Named by Benjamin.
Electric Charge and Electric Field Electric Charge and Electric Field
Reading Quiz The voltage (or electric potential) of a battery determines how much work the battery can do on an electric charge. how much net electric.
Electric Charge, Force, and Field
Chapter 22 Electric Potential.
Chapter 23 Summer 1996, Near the University of Arizona Chapter 23 Electric Fields.
Dr. Jie ZouPHY Chapter 23 Electric fields (cont.)
Chapter 21 & 22 Electric Charge Coulomb’s Law This force of repulsion or attraction due to the charge properties of objects is called an electrostatic.
Chapter 16 Electric Energy and Capacitance. Question I Three equal positive charges are placed on the x-axis, one at the origin, one at x = 2 m, and the.
Chapter 22 Electric Field
Chapter 25 Electric Potential Electrical Potential and Potential Difference When a test charge is placed in an electric field, it experiences a.
‾The Electric Field ‾Electric Field of a Continuous Charge Distribution ‾Electric Field Lines ‾Electric potential Phys 2180 Lecture (2) 1.
Electrostatics: Coulomb’s Law & Electric Fields. Electric Charges  There are two kinds of charges: positive (+) and negative (-), with the following.
+ - q b b a b s r  a z r  50 kV Dirty air Clean air.
Chapter 19 Electric Forces and Electric Fields Electric Charges There are two kinds of electric charges Called positive and negative Negative.
Physics for Bioscience (Part II) Electricity Magnetism Waves Sound Optics by Dr. Chittakorn polyon Department of Physics, Faculty of Science,
ELECTRIC POTENTIAL Summer, 2008 Chapter 24 Electric Potential In this chapter we will define the electric potential ( symbol V ) associated with the.
Physics 2112 Unit 5: Electric Potential Energy
Electric Charge and Electric Field
Electric Energy and Capacitance
110/29/2015 Physics Lecture 4  Electrostatics Electric flux and Gauss’s law Electrical energy potential difference and electric potential potential energy.
SACE Stage 1 Physics Electric Fields. Introduction Consider two charges, the force between the two charged bodies is inversely proportional to the square.
Coulomb’s Law Performing electric field calculations on charge distributions in an X-Y coordinate Plane.
Electric Potential & Electric Potential Energy. Electric Potential Energy The electrostatic force is a conservative (=“path independent”) force The electrostatic.
Electrical Energy And Capacitance
Electric Fields and Forces
Electric Field-Intro Electric force is a field force. Field forces can act through space, i.e. requires no physical contact. Faraday developed the concept.
ELECTRIC FIELD  Consider that body A is initially within the given empty space.  Because of the charge it carries, it somehow modifies the space surrounding.
Static Electricity, Electric Forces, Electric Fields
Electric Potential.
Chapter 25 Electric Potential. Electrical Potential Energy The electrostatic force is a conservative force, thus It is possible to define an electrical.
1 Electric Potential Reading: Chapter 29 Chapter 29.
Static Electricity, Electric Forces, Electric Fields.
Chapter 22 Electric Fields The Electric Field: The Electric Field is a vector field. The electric field, E, consists of a distribution of vectors,
Electrostatics experiments Helped to develop the model of the atom.
Charles Allison © 2000 Chapter 21, Electric Charge, and electric Field.
Chapter 23 Electric Fields.
Electric Forces and Fields AP Physics C. Electrostatic Forces (F) (measured in Newtons) q1q1 q2q2 k = 9 x 10 9 N*m 2 /C 2 This is known as “Coulomb’s.
There are only two charges, positive and negative.
ELECTRIC POTENTIAL ENERGY and the ELECTRIC POTENTIAL.
Coulomb’s Law (electrical force between charged particles).
Electric Force Holt: Chapter 17-2 Pages
Coulomb’s Law Like charges repel, and unlike charges attract
COULOMB’S LAW Coulomb’s Law – charges exert forces on each other and have been shown to be directly proportional to the magnitude of the charge and inversely.
Electrostatics Forces and Fields
Fields & Forces Coulomb’s law Q r q How does q “feel” effect of Q?
Electric Force Unit 7.3.
Electric Fields Chapter 14.1.
Chapter 22 Electric Fields.
Electric Fields AP Physics C.
Electric Fields AP Physics C.
Chapter 25 Electric Potential.
Electrical Field 15.4 Maxwell developed an approach to discussing fields An electric field is said to exist in the region of space around a charged object.
Shocking You charge a electroscope by grounding it and then bringing a positively charged insulator near the electroscope. Then you break the connection.
Going over Friday’s Quiz
Equipotential surfaces
Aim: What is an Electric Field
Electric Field.
Electrostatics.
Mechanical Energy Kinetic Energy, energy of motion,
Electric Charge and Electric Field
Chapter 29 Electric Potential Reading: Chapter 29.
Chapter 25 - Summary Electric Potential.
Electrostatics.
Static Electricity, Electric Forces, Electric Fields, Electric Potential Energy, Electric Potential, Capacitors.
Static Electricity, Electric Forces, Electric Fields, Electric Potential Energy, Electric Potential, Capacitors.
Electrostatics Seo Physics.
Electric Force Holt: Chapter 17-2 Pages
Electric Force Unit 11.2.
Presentation transcript:

Coulomb’s Law Performing electric field calculations on charge distributions in an X-Y coordinate Plane

Coulomb’s Law: Calculates the electrostatic force that exists between charged point charges. Where FES = Electrostatic Force (N) k = Coulomb’s Constant (9.0 * 109 Nm2/c2) Q1 & Q2 = charge of point charges (coulombs) r = distance between point charges (m) The force can be attractive or repulsive.

Electric Fields Regions in space that distort the normal behaviors of charged particles such that they will experience a given amount of force per unit charge present at the field point. The field exists because of the presence of given source points containing a net charge.

Electric Field Vector An electric field is a vector quantity but the field itself is actually an infinite number of vector quantities spread out over a plane. An electric field is defined as force per unit charge. E0 = electric field vector (N/c) F0 = electrostatic force on q0 (N) q0 = charge (C) at field point

Points in an Electric Field Source Point(s) – Point charges at a given location in a charge distribution that are contributing to the electric field at the field point. Field Point – The point at which the electric field vector is calculated in a charge distribution. If there is a charge contained at the field point it is typically not considered in calculating the field at that location.

The Superposition Principle The electric field caused by individual point charges can each be evaluated at a given field point and the result can be combined with that from other point charges using vector addition.

The Superposition Principle This can be applied to any number of source points. It can also be applied to deal with continuous charge distributions (continuous lines or rings of charge) by breaking them up into a large number of point charges spaced close together. This means a wide variety of fields can be modeled on a spreadsheet.

Energy and Potential in Electric Fields Electric potential energy comes from work done by electrostatic forces. It is calculated for a specific charge in a field. Electric potential is energy per UNIT charge and usually refers to a position in an electric field compared to a reference position (usually infinitely far away) It is calculated for a specific location in a field

For a single charge there is no PE For a single point charge the potential can be calculated at various locations around the charge but there is no potential energy present until there is another charge present. When there is a 2 charge system the potential can be calculated at any location surrounding the charges but the PE can only be calculated for either one of the charges.

Electric Potential Energy (2 Point charges) Like Charges very close together will tend to accelerate apart due to a large electrostatic repulsion Like charges far apart will tend to accelerate apart due to electrostatic repulsion but are already far separated so do not reach the same velocity.

Electric Potential Energy Opposite charges very close together will tend to accelerate together due to a large electrostatic attraction but over a small distance so little work is done. Opposite charges very far apart will tend to accelerate together due to electrostatic attraction but over a large distance so a lot of work is done.

Field Equations for a Single Point Charge Electric Field (vector) Electric Potential (scalar)

Objectives: Calculate the field (and force on the field point) produced by any number of point charges as well as the field created by a continuous charge distribution Calculate the potential of a location (or potential energy of a point charge) given a number of point charges

Tips/Troubleshooting The IF functions are present in order to prevent errors caused by dividing by zero. Electrostatic force and potential energy are calculated when a charge is located on the field point. This is not necessary for the field and potential. Look at the graph to be able to view the charge distribution to better understand the results.

The Superposition Principle Allows for using Coulomb’s Law multiple point charges to form an electric fields The spreadsheet can calculate the field created by 100+ individual charges which closely approximates a continuous charge distribution. This will help you realistically model charge distributed along a straight line. Follow the instructions on the document and good luck.