Electrostatics II. Introduction

Similar documents
Electrostatics: Coulomb's Law

Preview of Period 10: Electric Charge and Force

Lab 1 Electrostatics 1

NORTHERN ILLINOIS UNIVERSITY PHYSICS DEPARTMENT. Physics 211 E&M and Quantum Physics Spring Lab #2: Electrostatics. qq k r

Static Electricity 2

Electric Charge & Force Problems - 1 v Goodman & Zavorotniy

Bell Ringer: Define to the best of your ability the definition of:

Department of Physics & Astronomy Undergraduate Labs. Measuring the Electric Force with the Milligram Balance

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

Electrostatics. Experiment NC. Objective. Introduction. Procedure

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

Question Sheet for Laboratory 3: E-1: Electrostatics

Chapter 20. Static Electricity

Electrostatics. Apparatus:

Electrostatics and Electric Potential - Outline

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

Lab 6 Electrostatic Charge and Faraday s Ice Pail

Note on Posted Slides

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

Name: Block: Date: NNHS Introductory Physics: MCAS Review Packet #4 Introductory Physics, High School Learning Standards for a Full First-Year Course

Conceptual Physics Electrostatics and Static Electricity Notes and Worksheets

Part I Electrostatics. 1: Charge and Coulomb s Law July 6, 2008

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

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

Review of Static Electricity

Electromagnetism. Electricity Electromagnetism Magnetism Optics. In this course we are going to discuss the fundamental concepts of electromagnetism:

Chapter 20 Review Questions

ELECTRIC FORCES AND ELECTRIC FIELDS

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

AP Physics-B ElectroStatics Electric Charges: Subatomic Particles and Electricity: atoms subatomic particles protons neutrons electrons nucleus

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?

Electrostatics x C.

PHY132 Introduction to Physics II Class 8 Outline:

7.2. Electric Force 7-2A. What Is the Attraction to Water? Words to Know. Find Out ACTIVITY. Materials. What Did You Find Out?

Two. ( ) :. ; J.. v ( -I ) f - ) N. 1 o f.., J e. ( b) Like c a.,,9"s ref" ti. iocl, c, Qi' (f) .. i:1: ti,: f. c; (. c\... '1 t e-' r

32 Electrostatics. Electrostatics involves electric charges, the forces between them, and their behavior in materials.

Electrostatics x C.

Pre-LAB 1 Preparation: Electric Charge & Electric Interactions

LAST NAME FIRST NAME DATE

Electric Force and Charges. Conceptual Physics 11 th Edition. What are Atoms Made of?

UNIT 2 COULOMB S LAW. Objectives. to understand Coulomb s Law qualitatively and quantitatively

Electric Charge and Static Electricity

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

Some differences: Some basic similarities: Charges. Electrons vs. Protons 3/25/12. Chapters 22-25: Electromagnetism!

Chapter Assignment Solutions

AP Physics 1 Electrostatics Practice Problems. Multiple Choice

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

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

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

Electric Charge & Force Problems - 1 v Goodman & Zavorotniy

Electric Force and Field Chapter Questions

Electric Charges & Electric Forces Chapter 20 Structure of atom

Physics 1520, Fall 2011 Quiz 3, Form: A

Electrostatics-Coulomb's Law

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

Phys1112: Electric Charge and Force

Applied Physics. Faisal Haider

PHYSICS - Electrostatics

ALABAMA SCHOOL OF FINE ART, 8 TH GRADE HONORS PHYSICS QUIZ : ELECTROSTATICS TIME: 90 MINUTES NAME

I. Origin of Electricity

Charge. Electrostatics Notes (614) Review: Atomic Structure 3/10/14! Charge!! 3 Basic Particles make up Atoms:

Physics Test Review Electrostatics, Electric Fields and Potential Session: Name:

Electric Charge and Force

Electric Force and Electric Field Practice Problems PSI AP Physics 1

Electrostatics Notes (614) (teacher)

Electric Charge and Static Electricity

Some differences: Some basic similarities: Charges. Electrons vs. Protons 4/3/15. Chapters 22-25: Electromagnetism!

Lab 1 ELECTROSTATICS

Chapter 20 Electric Fields and Forces

Physics 208 Spring 2008 Lab 3 (E-1): Electrostatics

General Physics II. Electric Charge, Forces & Fields

Electric Charges and Fields

Lab 3: Electric Charge and Force

LAB 1 - ELECTROSTATICS

C) D) Base your answers to questions 22 through 24 on the information below.

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

Young Physicists Program: January 2011 Lab 4: Shocking facts about electrostatics

TA guide Physics 208 Spring 2008 Lab 3 (E-1): Electrostatics

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

Chapter 19. Electric Charges, Forces and Electric Fields

Experiment 6. Coulomb s Law - PRELAB. Lab section: Partner's name(s): Grade: 0. Pre-lab Homework (2 points)

PHY205H1F Summer Physics of Everyday Life Class 7: Physics of Music, Electricity

Demonstration 1: Faraday Ice Pail and Charge Production

PHY 112L Activity 1 Electric Charges, Potentials, and Fields

Electrostatics 1 July 6. Name Date Partners ELECTROSTATICS

Chapter 12 Electrostatic Phenomena

CHAPTER 15 PRE-TEST: ELECTRIC FORCE AND FIELDS

7.9.4 Static Electricity

6 Three rods, X, Y. and Z are charged by friction. Rod X attracts rod Y, but repels rod Z. What are the signs of the charges on each of these rods?

Review of Static Electricity

What are some properties of interactions involving electrified objects?

Welcome to PHYS2002!

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

Electrostatics. Electrical properties generated by static charges. Introduction

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

Test Review FQ3eso_U5_3_Electric force

Section 1: Electric Charge and Force

Unit 2: Electrostatics

Chapter 1. Electrostatics. The Electric Charge

Electric Charge & Force - 1 v Goodman & Zavorotniy

Transcription:

Electrostatics II Objective: To learn how excess charge is created and transferred. To measure the electrostatic force between two objects as a function of their electrical charges and their separation distance. Apparatus: Copper sphere on rod (3, one with standing base), charging rod, capacitor, fake fur, scale, meter stick, ring stand, voltmeter, connectors and wires Introduction There are two types of electrical charge, positive and negative. Like charges (positive and positive, or negative and negative) repel each other, while unlike charges (positive and negative) attract each other. Materials through which charges are free to move, like most metals, are called conductors. Materials in which charges are not free to move, like most nonmetals, are called insulators. The charges that are mobile in conductors are negative charges the free electrons that are not bound to any particular atoms. The charges that are static are positive charges protons which are in the nuclei of the atoms that make up the material. Charge is neither created nor destroyed (conservation of charge). The appearance of excess charge on an object happens when charge is transferred from somewhere else. For instance, rubbing a piece of amber with a piece of fur results in the amber acquiring a net negative charge; however, the fur has acquired an equal amount of positive charge from the same interaction. In this experiment, you will produce excess charge by rubbing a plastic rod with (fake) fur. You will then transfer the charge from the rod to one of the conducting copper spheres. The spheres are connected to insulated rods so that they can be handled without the charge leaking out. Due to the electrostatic force, a scale on which one of the charged spheres is placed would then read

heavier or lighter in the presence of another charged sphere, compared to the weight reading if the sphere were electrically neutral. You will measure the distance between the spheres using a meter stick, and the charge on each sphere by discharging it into a capacitor, a device that stores a charge. Since the capacitor is connected to a voltmeter, you can then determine the charge that was on it from the equation: Q=CV where Q is the charge, C is the capacitance, and V is the voltage Coulomb's Law, which determines the electrostatic force between objects 1 and 2 based on their electrical charges and separation distance, is written as follows: Q Q F k r 1 2 2 The constant of proportionality k has the units Newton-Meter 2 /Coulomb 2 and has the value k 9x10 9 N m 2 C 2 As in gravitational forces, the electrostatic force lies along the line connecting the center of the spheres. The sign of the Coulomb force will either be positive, denoting repulsion or negative, denoting attraction. Note that if only one of the charges in the equation is negative, the force will be attractive. If both charges are negative or positive, the force will be repulsive. As mentioned before, like charges repel while unlike charges attract. How to charge objects You can produce excess charge on objects by two methods: 1. Charging by contact involves charging an object that is electrically neutral by touching it with an object that is already charged. In this experiment, you will rub the charging rod to give it excess charge, then transfer that charge to a copper sphere using the following technique: Pick up the charging rod the clear cylindrical rod that is unattached to any copper sphere. Hold it by one end. Pick up the (fake) fur in the other hand and wrap it around the rod, covering as much of it as you can. Rub the fake fur against the rod vigorously several times, along the length of the rod. You should hear crackling sounds as charges are being separated. Do not rub so hard that your hands sweat or the fur gets hot, since that could diminish the transfer of charge. (If you need to, you can use the hand dryer in the rest room to dry the fur.) You will then rub the length of the rod (rotating at the same time, since the charges on the rod are static) on the copper sphere with the rod, transferring the charge. You should again hear crackling sounds if you are indeed transferring charge from the rod to the sphere. See the photos on the next page.

Rubbing the fur against the rod Rubbing the surface area of the rod on the sphere 2. Charging by induction involves no contact, and relies on the fact that an object with, say, positive charge brought close to, but not touching, a conductor, will draw negative charges toward the side that is nearer to the positive object. Since the conductor was originally electrically neutral, positive charges will migrate to the opposite side, leading to a separation of charges. Such an object, which has its unlike charges separated but which remains electrically neutral, is electrically polarized. The next page shows an illustration of how to charge an object by induction.

Charging by Induction Charging by Induction In the illustration above, (A) a neutral sphere is brought close to a sphere with positive excess charge. (B) The positively charged sphere pulls the negative charges on the neutral sphere towards it. The positive charges on the neutral sphere are pushed away from it, leading to an electric polarization of the neutral sphere. (C) When one side of the electrically polarized sphere is touched, or grounded, charge from that side flows from where the sphere is touched and into the ground. (D) The previously neutral sphere now has excess negative charge. Note that the two spheres never physically touched. This polarization effect can also explain why a charged object can exert forces on insulators the electric force causes the positive and negative charges in the insulator to separate slightly, with the negative charges being pulled towards the positive (for example) rod and the positive charges being pushed away. Since Coulomb's law is distance-dependent, the two objects experience a net attractive force, since the unlike charges are closer than the like charges. Bear in mind that had a negatively charged rod been used, attraction would again result, because it would have drawn positive charges closer than the negative charges. Note that when a charged sphere touches an identical one that was previously neutral, charges flow from one to the other such that after the make contact, the initial charge Q is now shared equally between them, with each one having a charge Q/2. To make a sphere electrically neutral again, simply touch it with your finger the charges travel from the sphere through your body and down to the ground. While you are doing the experiment make sure that you do not accidentally touch any spheres that are charged this will render them uncharged.

Activities A. Qualitative Observations Find out what small objects (tiny pieces of paper, hair, etc.) a charged rod can attract and write these in hand-in sheet. Since you used the fur to charge the rod, then the fur should have excess charge of opposite sign. Can you pick up the same objects with the fur as well? B. Dependence of Coulomb Force on Signs of Charge Together with your lab partner(s), design and perform an experiment to qualitatively prove that charges of the same sign repel and charges of opposite sign attract. Before you do that, read the paragraph below regarding the detection of the Coulomb force. Remember, to start off with an electrically neutral sphere, you will have to touch it to ground it. Also, bear in mind that spheres too close to each other will exchange charges, while spheres too far from each other may not exert forces high enough for the scale to measure. Using the scale to measure the Coulomb Force of one sphere on another Turn on the scale by pressing the On button. If it reads ERR, try pressing the On button again and holding it down until you see CAL on the display. Let go and it should display a scale reading. Press the Mode button until the correct units are shown choose g for grams. Tare the scale by pressing the On button one more time. Now place the sphere (connected to the insulated rod and wooden base) on the scale. Record its mass. When you perform the experiment, any differences in the scale reading relative to this number will represent the electrostatic force (remember to properly convert between mass measured in grams to force measured in Newtons). Think about how the scale reading would indicate attraction or repulsion. Measuring force and distance between two charged spheres (NOTE: exact setup may differ slightly from illustration)

C. Dependence of Coulomb Force on Distance Design and perform an experiment to determine how the Coulomb force varies with distance. Here are a few things to remember when measuring the force while changing the sphere separation: -Loosen the clamp on the ring stand to adjust the height, then re-tighten. Make sure you are reading the distance after you have tightened the clamp, since a loose clamp will position the sphere lower than it should be. -You need to work quickly, since charge will slowly leak from the spheres. -Remember to convert the mass to kilograms and then multiply by g to obtain the force in Newtons. You may use the curve-fitting features of Graphical Analysis to find the F vs. d dependence. Include a description of your experiment, including a graph or your data, and any additional observations in the hand-in sheet. D. Dependence of Coulomb Force on Charge Design and perform an experiment to determine how the Coulomb force varies with charge, without having to directly measure the charge (as you will later do with a capacitor and voltmeter). It will only be necessary to vary the charge on one of the spheres think of how you can halve the charge on sphere, and continually do so. Include a description of your experiment, including a graph of your data, and any additional observations in the hand-in sheet. E. Compare Theory to Experiment Using Measured Force, Distance and Charge Now you will measure the force between two charged spheres and compare it to the force as obtained from the Coulomb's Law equation. First, position the spheres at a distance of your choosing; record this distance. Now charge the spheres and measure the force using the scale reading. In order to calculate what the force should be using Coulomb s law, you will need to measure the charge on each sphere, as described below. Turn on the multimeter and set it to measure voltage the multimeter acts as a voltmeter in this setting. In a moment you will use the voltmeter to measure the charge on each sphere. Before doing so, however, connect the voltmeter s black and red leads to each other this discharges the capacitor, ensuring that it does not contain any residual charge and is ready to measure the true charge on the spheres. Next touch the black lead to something that is grounded; you can use your body to ground the black lead by simply holding the metal plug of the black lead with your fingers. Now touch the red lead to one sphere and pull it away. You should hear the discharge pop resulting from the charge leaving the sphere and charging up the capacitor; record the voltage. Connect the black and red leads again to discharge the capacitor, then repeat this procedure using the other sphere. Calculate the charge on each sphere using your voltage measurements.

Based on the charges and the distance between each sphere, calculate what the force should be using Coulomb s law. Recharge the spheres and repeat this procedure two more times (three total). Record all of your measurements in the hand-in sheet.