Lab 6 Electrostatic Charge and Faraday s Ice Pail

Similar documents
Electrostatic Charge Distribution (Charge Sensor)

Electrostatics x C.

Electrostatics x C.

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

Physics Notes Chapter 17 Electric Forces and Fields

Question Sheet for Laboratory 3: E-1: Electrostatics

Electrostatics. Apparatus:

CHAPTER 15 ELECTRIC FORCE & FIELDS

LAB 01 Electrostatic Charge

Electrostatics II. Introduction

CHAPTER 15 PRE-TEST: ELECTRIC FORCE AND FIELDS

Chapter 23. Electric Fields

Electrostatics: Coulomb's Law

PHYSICS - Electrostatics

Chapter 16 Electric Charge and Electric Field

Chapter 20. Static Electricity

Electrostatics. Physics 10. Atomic Structure

Physics Electrostatics

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

Electric Field Around a Conductor

Lab 1: Electrostatics Edited 9/19/14 by Joe Skitka, Stephen Albright, DGH & NET

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

Electric Forces and Electric Fields

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

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

Chapter 15. Electric Forces and Electric Fields

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

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

Electric Charges & Electric Forces Chapter 20 Structure of atom

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

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

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

Chapter 15. Electric Forces and Electric Fields

Chapter Electric Forces and Electric Fields. Prof. Armen Kocharian

UNIT 1 EXPLORING THE NATURE OF ELECTROSTATIC FORCES

9. Which of the following is the correct relationship among power, current, and voltage?. a. P = I/V c. P = I x V b. V = P x I d.

Review of Static Electricity

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

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

PHYSICS 30 ELECTRIC FIELDS ASSIGNMENT 1 55 MARKS

Electric Charge and Static Electricity

Algebra Based Physics

Electrostatics Experiments Experiment 1: Faraday Ice Pail and Charge Production

Chapter 21. Electric Charge

Welcome to PHYS2002!

Lab 1 Electrostatics 1

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

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

LAST NAME FIRST NAME DATE

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

Electromagnetism Unit- Electrostatics Sub-Unit

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

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

Electric Charge. Physics 4B. Atomic Structure

Chapter 16 Electric Charge and Electric Field

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

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

Chapter 23. Electric Charge and Electric Field

General Physics II. Electric Charge, Forces & Fields

Preview of Period 10: Electric Charge and Force

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

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

LAB 1 - ELECTROSTATICS

Electrostatics 1 July 6. Name Date Partners ELECTROSTATICS

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

Lab 1 ELECTROSTATICS

1. Electrostatic Lab [1]

Magnets attract some metals but not others

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?

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

HIGH SCHOOL SCIENCE. Physical Science 7: Electricity & Magnetism

Chapter 23. Electric Fields

Chapter Assignment Solutions

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

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

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

Lab 3: Electric Charge and Force

Applied Physics. Faisal Haider

Chapter 18 Electrostatics Electric Forces and Fields

Electric Fields Practice Multiple Choice

ISLAMABAD ACADEMY PHYSICS FOR 10TH CLASS (UNIT # 15)

Charge Transfer Diagrams

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

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

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

Physics 1520, Fall 2011 Quiz 3, Form: A

Electric charges. Basics of Electricity

Section 1 Electric Charge and Force

1. A coulomb is the same as: A. an ampere/second B. half an ampere second 2 C. an ampere/meter 2 D. an ampere second E. a newton meter 2 ans:

Applied Physics. Faisal Haider

Electric Charge. Positive and Negative Charge

Chapter 20 Review Questions

Chapter 10. Electrostatics

Electricity MR. BANKS 8 TH GRADE SCIENCE

PHY222 Lab 2 - Electric Fields Mapping the Potential Curves and Field Lines of an Electric Dipole

Fundamentals of Circuits I: Current Models, Batteries & Bulbs

Chapter 12 Electrostatic Phenomena

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

Electricity and Electromagnetism SOL review Scan for a brief video. A. Law of electric charges.

Transcription:

Lab 6 Electrostatic Charge and Faraday s Ice Pail Learning Goals to investigate the nature of charging an object by contact as compared to charging an object by induction to determine the polarity of two charge producers to measure the amount of charge on a charge producer. to investigate the distribution of charge on conducting objects of different geometries Apparatus: Qty Instrument Instrumental Error Instrumental Resolution 1 PASCO Interface (for one sensor) ± 0.1% ± 0.005 volt 1 GLX with Charge Sensor ± 1% ± 0.005 volt (microcoulombs) 3 Plastic Charge Producers and Proof Planes 1 Faraday Ice Pail 1 Pair of parallel plates 1 Hollow Conductive sphere 1 Electrostatics Voltage Source Theory: Electrical Charge All matter is composed of atoms, and those atoms contain subatomic particles, namely neutrons, protons and electrons. These particles can be described in terms of the charge they carry. Charge is a fundamental quantity (like mass) that is responsible for electric forces between particles. Charge is to electric forces like mass is to gravitational forces. Protons and electrons are the ultimate sources of charge. Protons are said to have a positive (+) charge, electrons are said to have a negative (-) charge, and neutrons are said to be neutral (no charge). The fundamental unit of charge is called the Coulomb [C]. Protons and electrons, while having different types of charge, both have the same magnitude of charge e = 1.602 x 10-19 C. The relationship defining the electric force between charged particles is called Coulomb s Law: 2 [1] F e = Kq 1 q 2 / r where K electrostatic constant = 9 x 10 9 [Nm 2 /C 2 ] q1 charge on particle 1 q2 charge on particle 2 r distance between particles Page 1 of 8

This equation tells us that like charges repel and unlike charges attract. For instance, electrons (negative charge) are attracted to protons (positive charge). Electrons repel other electrons, and protons repel other protons (see diagram below). Many atoms in matter have an equal number of protons as they do electrons. When we add all the charges together (electrons, protons, and neutrons), these atoms are called electrically neutral, because there is no net charge on the object since the total positive charges and total negative charges are in balance. However, if an electron is removed, the atom becomes an ion, meaning the total net charge of the whole atom becomes positive (since there are now more protons than electrons). This also applies to macroscopic objects. By charging an object, you are creating a net charge on that object. You are unbalancing the number of positive and negative charges that object contains. By discharging an object, you are restoring the balance of positive and negative charges, thereby making the object electrically neutral once again (net charge = 0). Conductors and Insulators There are three main categories of objects which carry charge: conductors, semiconductors, and insulators. This lab will only focus on conductors and insulators. Conductors are materials that allow charged particles, like electrons, to flow through them easily. Metals such as copper, silver and aluminum are some examples. When a conductor has a net charge, the excess charges feel the Coulombic forces of equation [1] from the other charges, and they spread out evenly over the surface of conductor. Insulators are materials through which charges have a difficult time flowing. Plastic, rubber, and wood are insulators. In fact, net charges on an insulator do not spread out evenly, but generally stay in one locale. Charging by Contact If a charged object comes in contact with a neutral conductor, many of the excess charges will transfer to the surface of the conductor. When the initially charged object is removed it leaves behind some of its excess charge.the conductor is now considered charged. The diagram below shows a positively charged rod charging a neutral conductor (in this case, only the excess charges are labeled in the diagram). This process is charging through contact. Charging Through Induction A conductor can also be charged through induction. Consider two conductors joined together so that they can share their charges as if they were one large conductor (see diagram below). If a charged object is brought close the surface of the conductor, the charges will rearrange and the conductor will be come polarized as before. If the conductors are detached while they are polarized, and the charged rod removed, both separate conductors will now be charged. However, this charge was NOT produced through contact with a charged object, but was induced through polarization. Page 2 of 8

Polarization When a charged object is brought within close proximity of a neutral conductor, the surface charges of that conductor will shift and rearrange due to the Coulombic forces. This rearrangement is called polarization, which turns a neutral object into an electric dipole (with positive and negative electric poles). Notice in the diagram to the left how the conductor stays neutral, but becomes polarized by the negatively charged rod. This is because the charges are free to move and rearrange themselves on the conductor s surface in response to the charged rod Electroscope To experimentally investigate electrostatics, some charge-detecting or measuring device is needed. A common instrument for this purpose is the electroscope, a device with two thin gold leaves vertically suspended from a common point. When a charged object is brought near the electroscope, the gold leaves separate, roughly indicating the magnitude of the charge. Although there are many different versions of the electroscope, all such instruments depend upon the repulsion of like charges to produce an output or reading. Unfortunately, such devices are relatively insensitive (large amounts of charge are needed to make the gold leaves separate), and the device does not have a quantitative reading. The Charge Sensor is an electronic electroscope. In addition to providing a quantitative measurement, the Charge Sensor is more sensitive and indicates polarity directly. Faraday s Ice Pail This lab will use a conductor configuration known as Faraday s Ice Pail. This setup involves a metal can placed inside of a larger metal can, with an insulator placed between them (see diagram). Think of the cans as two neutral conductors. + + + + + + If the inner can has any excess charges on its outside surface and the outer can is connected to a ground wire, the voltage difference between the outer and inner can be measured with a voltmeter to represent the net charge on the inner can. This lab involves lowering a charged rod into the inner can and measuring the polarized charge, or charging the inner can and measuring contact charge or induced charge. When inducing the charge on the inner can, the bridge conductor can be replicated by using your finger. This is done by touching both inner and outer can simultaneously with the same finger, allowing inner and outer cans to share charges. This is called grounding the inner can. When measuring the voltage, the charge detector will automatically convert the voltage reading (in [Volts]) to a charge reading (in [Coulombs]). The white and blue charging rods are both insulators that can be charged by rubbing them together. After rubbing, one rod will be positively charged, the other will be negatively charged. You will discover which rod has which charge during the experiment. The magnitude and sign of the charge on these rods can also be measured using Faraday s Ice Pail. Page 3 of 8

Prelab: #1 Draw on the surface of the plastic sphere below an equal number of both positive and negative charges. #2 Draw on the surface of the plastic sphere below an unequal number of positive and negative charges to indicate the sphere is negatively charged. #3 Draw on the surfaces of the plastic spheres below an unequal number of positive and negative charges to indicate the sphere on the left is negatively charged and the sphere on the right is positively charged. Indicate with arrows that the spheres are attracting each other. #3 Draw on the surfaces of the plastic sticks below an unequal number of positive and negative charges to indicate the sticks were rubbed together, then separated-- resulting in the left being negatively charged and the right being positively charged. #4 Draw on the surfaces of the plastic sticks below the situation described in #3 after a wire was connected between the two sticks. Page 4 of 8

Part I Electrostatic Charging Procedure: 1. Set up the PASCO Interface and the computer and start DataStudio. Connect the Charge Sensor to the interface. Open the DataStudio file: 64 Charging.ds The file opens with a Graph display of voltage from the Charge Sensor and a Meter display. The sample rate is set at 10 Hz. 2. Connect the alligator clips of the sensor s cable assembly to the inner (using two cable alligator) and outer (using single cable alligator) baskets of the Faraday Ice Pail. 3. Before starting any experiment using the Faraday Ice Pail, the pail must be momentarily grounded. To ground the pail, touch the inner pail and the shield at the same time with the finger of one hand or simultaneously touch inner and outer pails with a connecting wire. 4. Determine the Polarity of the Charge Producers A. Ground the Ice Pail and press the ZERO button on the Charge Sensor to discharge the sensor. Click Start in DataStudio to start recording data. B. Briskly rub the blue and white surfaces of the Charge Producers together several times. Without touching the Ice Pail, lower the white Charge Producer into the Ice Pail. Watch the Meter and Graph displays. C. Remove the white Charge Producer and then lower the blue Charge Producer into the Ice Pail. Watch the results. D. Record observations in notebook using the questions in the Data below Page 4 of 7 5. Measure the Charge on the White Charge Producer. E. Ground the Ice Pail and press the ZERO button on the Charge Sensor to discharge the sensor. Start recording data. F. Briskly rub the blue and white surfaces of the charge Producers together several times. Lower the white Charge Producer into the Ice Pail. Rub the surface of the white Charge Producer against the inner pail and then remove the Charge Producer. Watch the Meter and Graph displays. G. Record observations in notebook using Questions in the Data below 6. Measure the Charge on the Blue Charge Producer H. Ground the Ice Pail and press the ZERO button on the Charge Sensor to discharge the sensor. Start recording data. I. Briskly rub the blue and white surfaces of the Charge Producers together several times. Lower the blue Charge Producer into the Ice Pail. Rub the surface of the blue Charge Producer against the inner pail and then remove the Charge Producer. Watch the Meter and Graph displays. J. Record observations in notebook using Questions in the Data below 7. K. Ground the Ice Pail and press the ZERO button on the Charge Sensor to discharge the Charge the Ice Pail by Induction sensor. Start recording data. L. Briskly rub the blue and white surfaces of the Charge Producers together several times. Page 5 of 8

Without touching the Ice Pail with the Charge Producer, lower the white Charge Producer into the Ice Pail. While the Charge Producer is still inside the inner pail, use the finger of one hand to momentarily ground the Ice Pail. Watch the results. M.. After grounding the Ice Pail, remove the hand and then remove the Charge Producer. N. Record observations in notebook using Questions in the Data below O. Ground the Ice Pail and zero the sensor and repeat the procedure using the blue Charge Producer. N. Record observations in notebook using Questions in the Data below Data: Answer the following questions using the observation recorded above (record in notebook): 1. When two charge producers with different surface materials are rubbed together to create a charge imbalance, how will the electric charge on one of the producers compare to the electric charge on the other? Ans.:. 2. What polarity is the white Charge Producer? What polarity is the blue Charge Producer? Ans.:. 3. What happens to the charge on the Ice Pail when you rub the inner pail with the white Charge Producer and then remove the Charge Producer? Ans.:. 4. What happens to the charge on the Ice Pail when you rub the inner pail with the blue Charge Producer and then remove the Charge Producer? Ans.:. 5. What happens to the charge on the Ice Pail when the white Charge Producer is lowered into the inner pail without touching the inner pail? Ans.:. Page 5 of 7 6. What happens to the charge on the Ice Pail when the Ice Pail is momentarily grounded while the Charge Producer is still inside the inner pail? Ans.:. 7. What happens to the charge on the Ice Pail after the Charge Producer is removed from the inner pail? Ans.:. 8. What steps and in what sequence are used to charge the ice pail by conduction? Ans.:. 9. What steps and in what sequence are used to charge the ice pail by induction? Ans.:. 10. How does the result of charging by contact differ from the result of charging by induction? Ans.:. Part II Electrostatic Charge Distribution Learning Goals: to investigate electric charge distribution on conductive specimens: a hollow sphere and parallel plates. to use a charge sensor, proof plane, Faraday Ice Pail, and the DataStudio software to record distribution of charge on the sphere and parallel conducting plates. the magnitude and plot the Background Like electric charges repel and unlike charges attract. The distribution of electric charge on the surface of an object illustrates this principle. If electric charge is transferred to an object that is electrically neutral, the transferred charge will tend to distribute itself evenly over the surface of the object IF the surface is conductive and allows the charges to move freely. The transferred electric charges repel each other and move as far from each other as possible. However, if the surface is non-conductive, the charges cannot move as freely and won t distribute evenly. The arrangement of charges in Page 6 of 8

a non-conductive surface tends to attract or hold the transferred charges to that part of the object where they were transferred. Procedure: 1. Set up the PASCO Interface and the computer and start DataStudio. Connect the Charge Sensor to the interface. Set the GAIN switch to 5. 2. Open the DataStudio file: 65 Distribution.ds The file opens with a Table display of Location on Specimen and Charge. It also has a graph display and a meter display. The sample rate is set at 10 Hz. 3. Connect the alligator clips of the sensor s cable assembly to the inner (using two cable alligator) and outer (using single cable alligator) baskets of the Faraday Ice Pail. Connect the Electrostatic Voltage Source to a conductive specimen. Attach the spade plug end of the cable to the sphere and put the banana plug end into the +1000 V jack on the voltage source. AVOID DANGEROUS ELECTRICAL SHOCK: FOLLOW DIRECTIONS page 6 of 7 4. Plug a second cable into the COM jack on the voltage source, but don t connect it to anything. Before starting any experiment using the Faraday Ice Pail, the pail must be momentarily grounded. To ground the pail, touch the inner pail and the shield at the same time with the finger of one hand or simultaneously touch inner and outer pails with a connecting wire. 5. Measure the Charge at Several Locations on the Hollow Conductive Sphere (NOTE: Have one person handle the apparatus and a second person handle the computer) A. Ground the Ice Pail and press the ZERO button on the Charge Sensor to discharge the sensor. B. Click Start in DataStudio to start recording data. C. Touch the top of the Conductive Sphere with the Proof Plane. Without touching the Ice Pail, lower the Proof Plane into the Ice Pail about halfway down. Watch the Table display. Record the charge for position 1 in the Data Table. D. Remove the Proof Plane and ground it by touching it to the end of the cable that is connected to COM on the voltage source. Ground the ice pail and press ZERO on the Charge Sensor. E. Touch one side of the conductive sphere with the Proof Plane and then lower the Proof Plane into the Ice Pail. Record the charge for position 2 in the Data table. F. Ground the Proof Plane, ground the ice pail and ZERO the Charge Sensor again. Touch the opposite side of the conductive sphere and again and record the charge on the Proof Plane in the Data table. G. Repeat the process for other places on the outside and inside of the conductive sphere to complete the study. H. Click Stop to end data recording. 6. Repeat Procedure 5. using two parallel plate conductors. 7. Repeat procedure 5. using two parallel plate conductors that are much closer together. Data (record in notebook) 11. For the outside of the conductive sphere Page 7 of 8

12. For the inside of the conductive sphere 13. Sketch the charge distribution on the inside and outside of the conductive sphere according to location. Was the charge distribution on it uniform or not?. 14. For the outside of the parallel plates 15. For the inside of the parallel plates 16. Sketch the charge distribution on the inside and outside of the parallel plates according to location. Was the charge distribution on it uniform or not?. 17. For the outside of the close parallel plates 18. For the inside of the close parallel plates Page 7 of 7 19. Sketch the charge distribution on the inside and outside of the close parallel plates according to location. Was the charge distribution on it uniform or not?. 21. How does a conductor become charged when connected to a source of charge such as the Electrostatic Voltage Source?. 22. How does the charge distribution determine the magnitude and direction of the electric field in the vicinity of the charged conductor?. Page 8 of 8