Coulombs Law Two point Charges (equivalent to a weight of something with a mass of 10 -5 kg = 10 -2 gm or 10 mg - long strand of hair) 1 nC 1 cm q2q2 q1q1.

Slides:



Advertisements
Similar presentations
Coulomb’s Law and the Electric Field
Advertisements

Chapter 21 Electric Fields.
Unit 14: Electrostatics.
Relative to the effort it would take to thoroughly read the chapter once, how much effort did you put into doing the reading assignment? a) 0-20% b) 20-50%
CHAPTER 23 : ELECTRIC FIELDS
22-4 Coulomb’s Law q1 Unit q2 Only apply to point charges r
EEE340Lecture 081 Example 3-1 Determine the electric field intensity at P (-0.2, 0, -2.3) due to a point charge of +5 (nC) at Q (0.2,0.1,-2.5) Solution.
Electric Charge, Force, and Field
General Physics II, Lec 11, Discussion, By/ T.A. Eleyan 1 Review (Electrostatic)
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. What are the x and y components of the force on a particle with positive charge.
From long view of the history of mankind – seen from, say, ten thousand years from now – there can be little doubt that the most significant event.
1/10/ Lecture 31 PHY 184 Spring 2007 Lecture 3 Title: The Coulomb Force.
 like charges repel  unlike charges attract  charges can move but charge is conserved Law of conservation of charge: the net amount of electric charge.
Dr. Jie ZouPHY Chapter 23 Electric fields (cont.)
From long view of the history of mankind – seen from, say, ten thousand years from now – there can be little doubt that the most significant event of.
Lecture 1 agenda: Electric Charge. Just a reminder of some things you learned back in grade school. Coulomb’s Law (electrical force between charged particles).
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. What are the x and y components of the force on a particle with positive charge.
Group of fixed charges exert a force F, given by Coulomb’s law, on a test charge q test at position r. The Electric Field The electric field E (at a given.
Example Problem Solution:
A charged particle with positive charge q 1 is fixed at the point x=a, y=b. y x q1q1 q2q2 a c d b What are the x and y components of the force on a particle.
Electric Field. Force at a Distance  Electric charges act on each other at a distance. Empty space between charges Net force on a charge  Force has.
Fall 2008Lecture 1-1Physics 231 Electric Charges, Forces, and Fields.
Electric Fields and Forces
WHY?. = Electromagnetism I Lecture 2 Coulomb’s Law and the Concept of Electric Field.
Chapter 23 Electric Charge and Electric Fields What is a field? Why have them? What causes fields? Field TypeCaused By gravitymass electriccharge magneticmoving.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Chapter 21 Electric Charge and Electric Fields
1. Electrostatics Electric Force. First review the gravitational force… Any two masses are attracted by equal and opposite gravitational forces: m1m1.
R 2R2R a a Today… More on Electric Field: –Continuous Charge Distributions Electric Flux: –Definition –How to think about flux.
Electric Charge and Electric Field 16
Electric Forces and Electric Fields
AP Physics C. “Charge” is a property of subatomic particles. Facts about charge:  There are basically 2 types: positive (protons) and negative (electrons)
Chapter 16 Section 2 Electric force. Objectives  Calculate electric force using Coulomb’s law.  Compare electric force with gravitational force.  Apply.
ELEC 3105 Lecture 1 Coulomb. 4. Electrostatics Applied EM by Ulaby, Michielssen and Ravaioli.
General Physics II, Lec 3, By/ T.A. Eleyan 1 Lecture 3 The Electric Field.
Review You have two neutral pieces of tape stuck together. You rip them apart and notice that each one is charged (because each one is attracted to your.
PHYSICS 632 SUMMER 2006 Orientation 8:30 – 10:30 Room 203 Electricity & Magnetism Richard A. Lindgren, Office Room 302 Your Goals: Get a degree, crossover.
Q20. Electric Charge Force and Field
Consider a force like gravitation which varies as but 1) billion-billion-billion-billion times stronger; 2) there are two kinds of “matter”: positive.
Chapter 21 Electric Charge and Electric Field
Physics 213 General Physics
Electric Charge and Electric Field
Ch. 21 Electric Forces & Fields
Phy 2049: Physics II Syllabus, grades and exams
Electricity. Electrostatic The Electric Field Electric charge. Conductors and Insulators Coulomb´s Law The Electric field. Electric Field Lines Calculating.
Coulomb’s Law Pg
1. 2 PHYSICS 632 SUMMER :00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302/22 Text: Halliday, Resnick, and.
Objectives: The students will be able to: 1.Demonstrate that charged objects exert forces, both attractive and repulsive. 2.Explain that charging is the.
Chapter 22 Electric Fields The Electric Field: The Electric Field is a vector field. The electric field, E, consists of a distribution of vectors,
A penny carrying a small amount of positive charge Q p exerts an electric force F on a nickel carrying a large amount of positive charge Q n that is a.
Fall 2010 Prof. Yong Chen Prof. Michael Manfra Lecture 2 Slide PHYS 272:
Charles Allison © 2000 Chapter 21, Electric Charge, and electric Field.
Key Ideas in Chapter 14: Electric Field  A charged particle makes an electric field at every location in space (except its own location).  The electric.
How strong are Coulomb forces? Electron and proton in a hydrogen atom Compare electric and gravitational forces electron and proton m e = 9.11x kg,
P202c22: 1 Chapter 22: Electric Charge and Electric Field Electric Charge Ancient Greeks ~ 600 BC Static electicity: electric charge via friction (Attempted)
Coulomb’s Law (electrical force between charged particles).
Electric Forces and Fields
The Experimental Law of Coulomb
Which graphical representation of electric field of a point charge
Coulomb’s Law Pg
Electric Fields Electric Flux
Section 23.3: Coulomb’s Law
Coulomb’s Law and the Electric Field
Electricity and Magnetism
Electric Charge and Electric Field
Coulomb’s Law and the Electric Field
Chapter 21, Electric Charge, and electric Field
Electric Charge.
Physics 014 Electric fields 1.
Structure of matter in the Universe
Presentation transcript:

Coulombs Law Two point Charges (equivalent to a weight of something with a mass of kg = gm or 10 mg - long strand of hair) 1 nC 1 cm q2q2 q1q1 r What is the force between two positive charges each 1 nanoCoulomb 1cm apart in a typical demo? Repulsion

Coulombs Law Two Pennies The force is What is the force between two 3 gm pennies one meter apart if we remove all the electrons from the copper atoms? (Modeling) What is their acceleration as they separate? The atom Cu has 29 protons and a 3 gm penny has = The total charge is

Principle of Superposition Three Charges in a Line In the previous example we tacitly assumed that the forces between nuclei simply added and did not interfere with each other. That is the force between two nuclei in each penny is the same as if all the others were not there. This idea is correct and is referred to as the Principle of Superposition. Example of charges in a line –Three charges lie on the x axis: q 1 =+25 nC at the origin, q 2 = -12 nC at x =2m, q 3 =+18 nC at x=3 m. What is the net force on q 1 ? We simply add the two forces keeping track of their directions. Let a positive force be one in the + x direction. 1 2 x 3

Find charge Q on two pith balls separated by distance d. Approximate Solution Change to proper units:m,kg,s,N,C Suppose d =2 cm, L=20 cm, and m = 0.20 g, Find Q in nanoCoulombs. Two hanging equally charged pith balls

Exact Solution

Force on a charge due to an infinitely long wire. Charge Q is uniformly distributed on the infinite wire with charge density  We choose the Y-axis through the line charge and the X-axis through the point charge. Now, because the line charge is infinite and straight (on Y-axis), we can assume the X-axis is the mid-point of the infinite wire. Then by Coulomb’s law for the small line segment dy Resolving the forces into its components: As it is can be seen that the y-component of the force exerted by the top half of the infinite wire will cancel the y-component force exerted by the bottom half of the infinite wire. +L -L 0 x y r

Force on a charge due to an infinitely long wire cont. You can also use polar coordinates for this integration. -L 0 x y r +L