Physics Notes Chapter 17 Electric Forces and Fields

Similar documents
HW Chapter 16 Q 6,8,10,18,19,21 P 1,2,3,4. Chapter 16. Part 1: Electric Forces and Electric Fields. Dr. Armen Kocharian

Electrostatics. Electrical properties generated by static charges. Introduction

Chapter 15. Electric Forces and Electric Fields

Chapter Electric Forces and Electric Fields. Prof. Armen Kocharian

Chapter 15. Electric Forces and Electric Fields

CHAPTER 15 PRE-TEST: ELECTRIC FORCE AND FIELDS

History. The word electricity comes from the Greek elektron which means amber. The amber effect is what we call static electricity.

Ch 16 practice. Multiple Choice Identify the choice that best completes the statement or answers the question.

General Physics (PHY 2140)

Chapter Assignment Solutions

Greeks noticed when they rubbed things against amber an invisible force of attraction occurred.

ELECTROSTATICS. the study of electric charges, forces and fields Static Electricity is Stationary Electricity or Accumulation of charge

electric charge Multiple Choice Identify the choice that best completes the statement or answers the question.

Conceptual Physics Electrostatics and Static Electricity Notes and Worksheets

Electrostatics. Do Now: Describe the Concept of charge

Electric Charge and Static Electricity

Electrostatics. Electrostatics the study of electrical charges that can be collected and held in one place. Also referred to as Static Electricity

ELECTROSTATICS 3. P.Ravindran, PHY041: Electricity & Magnetism 15 January 2013: Electrostatics 3

PHYSICS - Electrostatics

SPH 4U: Unit 3 - Electric and Magnetic Fields

Electrostatics and Electric Potential - Outline

Chapter 23. Electric Fields

Electrostatics. Electrostatics - the study of electrical charges that can be collected and held in one place - charges at rest.

Lab 6 Electrostatic Charge and Faraday s Ice Pail

Electric Force and Field Chapter Questions

Electric Charge. Positive and Negative Charge

Electrostatics. The Nature of Electric Charge

Electric Force and Charges. Conceptual Physics 11 th Edition. Electric Force and Charges

Chapter 20 & 21: Electrostatics

Chapter 16. Properties of Electric Charge. electric charge is + or -. like charges repel unlike charges attract

Electric Force and Electric Field Practice Problems PSI AP Physics 1

20.1 Electric Charge and Static Electricity. Electric charge is responsible for clothes that stick together when they are removed from a dryer.

PHYSICS - CLUTCH CH 22: ELECTRIC FORCE & FIELD; GAUSS' LAW

CHAPTER 15 ELECTRIC FORCE & FIELDS

Static Electricity Electrostatics

Chapter 20. Static Electricity

Quiz. Chapter 15. Electrical Field. Quiz. Electric Field. Electric Field, cont. 8/29/2011. q r. Electric Forces and Electric Fields

Electric Charge. Demo Lab. Return to Table of Contents. abp_electric charge force presentation_ notebook. March 21, 2017

Chapter 17 & 18. Electric Field and Electric Potential

Concept Summary. Adapted from Batesville High School Physics

Electric Charge & Force Problems - 1 v Goodman & Zavorotniy

Section 1: Electric Charge and Force

Section 12. Please pick-up section 12 packet and worksheet

Conceptual Questions. Fig.8.51 EXERCISES. 8. Why can t electric field lines cross? 9. In which direction do charges always move in an electric field?

33 Electric Fields and Potential. An electric field is a storehouse of energy.

To start off. The atom is made up of protons, neutrons, and electrons. Electrons have a negative (-) charge. Nucleus stays still only electrons move

Chapter 23. Electric Fields

ELECTRICITY. Chapter ELECTRIC CHARGE & FORCE

Today: Finish Chapter 20 (Sound) Chapter 22 (Electrostatics)

INTRODUCTION TO BIOPHYSICS. II semester, week /2015

Ch 16: Electric Charge and Electric Field. Opposites attract by Paula Abdul

- Like charges repel Induced Charge. or by induction. Electric charge is conserved

Applied Physics. Faisal Haider

Electric Charge & Force Problems - 1 v Goodman & Zavorotniy

Learning Outcomes from Last Time. Class 3. Learning Outcomes. What Causes Forces -Two Experiments. What Causes Forces -Two Experiments

Electrostatics. Physics 10. Atomic Structure

Chapter 20 Review Questions

Electrostatic and Electromagnetic Exam Wednesday

c. They have electric charges that move freely d. Electrons are added to the rod a. charges are of unlike signs b. charges are of like signs

HIGH SCHOOL SCIENCE. Physical Science 7: Electricity & Magnetism

PHYSICS 30 ELECTRIC FIELDS ASSIGNMENT 1 55 MARKS

Chapter 21. Electric Charge

Physics 122 Unit 3 S1 Electrostatics Weebly.notebook. Unit 3. Section 1 Electrostatics

Electric Charge and Force

Algebra Based Physics

Chapter 16. Properties of Electric Charge. Electric Charge. The Milikan Experiment. Properties of Electric Charge, continued

Note on Posted Slides

Electric Forces and Electric Fields

People experience static electricity everyday.

A negatively charged object has more electrons than protons. A negatively charged object has more electrons than protons

Quest Chapter 32. Think Is this any different than the electrons flying around a nucleus?

Welcome to PHYS2002!

SECTION 1: SHADE IN THE LETTER OF THE BEST ANSWER ON THE BUBBLE SHEET. (60%)

10th week Lectures March Chapter 12

Chapters 21 and 22: Giancoli, 4 th Edition Electrostatics

Electric Charge & Force - 1 v Goodman & Zavorotniy

Electric Charge. Physics 4B. Atomic Structure

3/9/2016. Chapter 25 Electric Charges and Forces. Chapter 25 Preview. Chapter 25 Preview

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons. Particle Mass Electric Charge. m e = 9.

PES 1120 Spring 2014, Spendier Lecture 2/Page 1

PHYSICS. Chapter 22 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Ch.7 Electric Charges & Electric Fields. 7.1 Properties of Electric Charge

L 24 Electricity & Magnetism [2]

Electric Charge and Electric Field AP Physics 4 Lecture Notes

Unit 3 Lesson 1 Electric Charge and Static Electricity. Copyright Houghton Mifflin Harcourt Publishing Company

Chapter 18 Electrostatics Electric Forces and Fields

Electric Charge. Labs, Activities & Demonstrations: Notes: Unit: Electricity & Magnetism NGSS Standards: N/A

Physics Worksheet Electrostatics, Electric Fields and Potential Section: Name: Electric Charges

Chapter 21 Electric Charge and Electric Field

Lecture 13. PHYC 161 Fall 2016

General Physics II. Electric Charge, Forces & Fields

Electric Charges & Electric Forces Chapter 20 Structure of atom

STATIC ELECTRICITY & CAPACITANCE: Solutions to higher level questions

UNIT V: Electricity and Magnetism Chapters 32-37

Intro Video: n What is charge? n v=dvlpasdwxpy

Electric Fields Practice Multiple Choice

Chapter 18 Electric Force and Electric Fields. Sections

PE q. F E = q. = kq 1q 2 d 2. Q = ne F e

Chapter 23. Electric Charge and Electric Field

SOWETO/DIEPKLOOF P.O.BOX BOOYSENS 2016!!! " /7 #

Transcription:

Physics Notes Chapter 17 Electric Forces and Fields I. Basic rules and ideas related to electricity a. electricity is about charges or charged objects where they are and how they move electrostatics is about charges that are not continuously moving. b. charges come in two kinds only they are: positive (due to Protons) and negative (due to electrons) c. Charge on a proton exactly equals the magnitude of the charge of an electron the type (or sign) of their charge is opposite. e = elementary charge (magnitude of the charge of a proton or electron) e = 1.60 X 10-19 C C = coulomb; SI unit for charge the charge on one electron is -1.6 X 10-19 Coulombs the charge on one proton is +1.6 X 10-19 Coulombs d. Charges exert forces on other charges over a distance (without contact being necessary) LIKE charges repel each other and UNLIKE or OPPOSITE charges attract. (link to three video clips: like charges and unlike charges interacting in combinations) http://paer.rutgers.edu/pt3/experimentindex.php?topicid=10&cycleid=56 e. Electrons and Protons are charged electrically - we call them charged particles, BUT when an atom, or any object, has equal numbers of electrons and protons and carries zero net charge it is said to be electrically neutral. f. Charge is quantized ; - charge on a proton or electron, e, is the smallest amount of free charge that has been discovered; any charge greater than e will be of some distinct whole number multiple of e ; Robert Millikan first demonstrated this in his famous oil drop experiment g. Conservation of Electric charge- electric charge is always conserved never created or destroyed only transferred from one object to another. h. ELECTRICITY is NOT the same thing as MAGNETISM and electricity does NOT involve North or South Poles!!!! BUT electricity and magnetism are related to each other a relationship which we will investigate in Ch. 22. II. Facts to remember about Matter or substances a. Matter is made up of atoms and atoms contain equal numbers of protons and electrons. With equal numbers of positive protons and negative electrons atoms are neutral so matter is neutral in most circumstances. b. Matter can become charged if it loses or gains some electrons. An atom that has become charged is called an ion. If an atom gains an electron it becomes negatively charged and if it loses an electron it becomes positive. NOTICE: ONLY THE ELECTRONS CAN BE LOST OR GAINED. Protons do not move from one atom to another unless it involves a nuclear reaction. III. Charging an object by contact and by induction 3 general ways that matter can become charged: 1. contact or conduction- touching a charged conductor to a neutral one 2. friction rubbing electrons from one originally neutral object onto another (both objects become charged) 3. induction holding a charged object near another object while providing a ground to the second object. Page 1 of 8

First some definitions: Conductors materials in which electric charges move freely; metals Insulators materials in which electric charges do not move freely; glass, rubber, wood A surface charge can be induced on insulators by charge polarization as shown here -> Semiconductors conduct a moderately small amount of electricity (useful in electrical devices since their properties can be changed by adding small amounts of other atoms); silicon, germanium. In pure form they are actually insulators, but made to conduct by adding impurities (this is called doping ) Charging by contact - 1. Friction - by rubbing two different neutral materials together, you can transfer some electrons from one surface to another. Ex: shoes on carpet electrons move from the carpet to the shoes. The two objects receive an opposite charge. 2. Conduction - an already charged object can be brought into contact with something else and transfer electrons to or from the new object. The two objects end up the same charge. This example is for an electroscope being charged by conduction. Charging by Induction - an induced charge can be produced in a neutral object by bringing a charged object nearby but not touching the neutral one. You then attach a wire (or touch it with a finger) providing a path for electrons to move onto or off of the once neutral object. This is called grounding the object. The newly charged object will be the opposite charge of the original. Page 2 of 8

(link to five video clips: demos and questions on charging an electroscope) http://paer.rutgers.edu/pt3/experimentindex.php?topicid=10&cycleid=50 IV. Coulomb s law - pronounced cool ahmz law and electrostatic force (force between charged objects) a. Coulomb s Law states that the force between 2 charged objects or particles is directly proportional to the product of their charges and is inversely proportional to the distance between them SQUARED. b. The formula is: qq where q is the amount of charge in coulombs, d is the distance in meters between 1 2 F =k 2 them, and k is the electrical constant or Coulomb s constant and the value for d Coulomb s electrical constant is: k = 9.0 X 10 9 N. m 2 /C 2 The force produced on some charged object by two or more other charged objects must be found by summing the forces as vectors. Example #1: The figure below shows three point charges that lie along the x axis. Determine the magnitude and direction of the net electrostatic force on charge q 1. -4.0 x 10-6 C +6.0 x 10-6 C -7.0 x 10-6 C q 2 q 1 q 3 0.20m 0.15m Page 3 of 8

Gravitational forces Vs. Electrical Forces The electrostatic force is analogous to the gravitational force except that the electrostatic force can be either attractive or repulsive and it is MUCH stronger, while gravity only attracts (as far as we know) and it is comparatively weak. {Demo: charged balloon held above neutral pieces of paper (electric force overcomes gravity) and attraction of the neutral meter stick with charged rod.} Gravitational Forces Electrostatic Forces G = 6.67 x 10-11 Nm 2 /kg 2 is VERY small k = 9 x 10 9 Nm 2 /C 2 is VERY large gravity is a weak force electrostatic forces are strong inverse square force inverse square force attractive only attractive and repulsive Gravitational Field Electrostatic Field (+ charge) gravitational field strength, g electric field strength, E g's vector nature points towards the center of the planet E's vector nature points away from a positive charge or towards a negative charge each surface represents a unique value for g each surface represents a unique value for E g is measured in N/kg (or m/sec 2 ) E is measured in N/C {Do WS on Coulomb s Law Parts 1 & 2 here} V. Electric Force Fields a. A charged object has an area around it where it exerts a force on other charges that come into the field (a lot like a massive object exerts a force due to gravity on other objects that come near) Page 4 of 8

b. any force field can be represented by force field lines. Electric force field lines are useful in visualizing the electric field in a region of space. Wherever the lines are close together the field is stronger. The direction is shown (see above) as an arrow pointing away from a positive charge and toward a negative. This is different from a gravity field, because gravity only attracts so there is no force field away from in gravity. c. If a second charge is placed at some point in the field, the second charge interacts with the field at that point (this explanation does away with the idea of action at a distance because an interaction between particles separated by some distance is no longer required They are interacting with a force field with which they are in contact) The direction of E is the same as the direction of the electric force that would be exerted on a small positive test charge that could be placed in the field. This direction was decided arbitrarily in order to make electric forces, current, and electric fields easy to describe and calculate consistently. Electric field lines originate on a positive charge (or infinity) and terminate on a negative charge (or infinity) so if the charge (Q) is positive, the field would point outward from it, If negative the field would point toward it. Rules for drawing electric field lines: Lines begin at positive charge (or infinity) and terminate on negative charge (or infinity) (away from + and toward -) Number of lines drawn leaving a positive charge or approaching a negative charge is proportional to the magnitude of the charge present No two field lines can cross each other VI. Calculating the magnitude and direction of an electric force field kq E = r The magnitude is found using 2 E=Electric Field strength, r = distance between the charged object creating the force field and the point at which you are measuring the electric field strength Page 5 of 8

Example 2: Three charges are arranged as shown below. Calculate the magnitude and state the direction of the net electric field (E) at a point 3.0 cm to the right of the 5.00 µc charge. Then calculate the force that would act on a proton if it were placed at that point in the field and its acceleration once it was released from that position. 2.00 cm q 5.00 cm q q 1 2 3-1.00 µ C -3.00 µ C 5.00 µ C Do worksheet Coulomb s Law, Electrostatic Forces and Fields: Part 3 Characteristics of Conductors that are in electrostatic equilibrium (not grounded) - like the Van De Graaff generator (shown below) when charged up or an electroscope that is charged. Electric field is zero everywhere inside the conductor so you are safe inside (see the Faraday Cage pictures at bottom of page) Any excess charge resides entirely on its outer surface see diagram to right On irregular shaped objects, the excess charge accumulates where the radius of curvature is smallest (at sharp points). This is one of the reasons that lightning rods work to protect buildings. The charge accumulates at the somewhat sharp tip and then escapes into the atmosphere thereby discharging the building so the lightning will NOT strike. Lightning rods protect buildings in case the lightning still strikes because they ground the strike and take it into the ground. Page 6 of 8

Diagram of a classical Van de Graaff generator. 6) lower roller (metal) 1) hollow metallic sphere (with positive charges) 7) lower electrode (ground) 2) electrode connected to the sphere with a mesh or 8) spherical device with negative charges, used to discharge metal brushes in close proximity to the belt the main sphere 3) upper roller (made of plexi-glass) 9) spark produced by the difference of potentials (or Voltage) 4) side of the belt with positive charges 5) opposite side of the belt with negative charges Be able to describe these processes (Van De Graff, Lightning, lightning rods, Faraday cages) as shown here and discussed in class: Formation of Lightning! Lightning rods and how they work! Safety techniques: protection inside a Faraday Cage (see below), Car, or metal building and Body position for safety. (Demos of Van De Graff generator- Relate to Lightning and lightning rods and Faraday cages.) The person is protected from shock inside the conductor due to the charge all positioned on the outside of the metal cage! The electric force field (E) is zero inside the conducting cage, but is very powerful on the outer surface and extends outward from that surface. Page 7 of 8

Left - Notice the person inside touching the inner surface of the Faraday Cage! Right - A person-shaped Faraday Cage shielding him! Homework problems p. 654-656 # s 1-16, 19, 20, 28-30, 35-38 and 43. Page 8 of 8