Equipotential Lines and Electric Fields Plotting the Electric Field

Total Page:16

File Type:pdf, Size:1020Kb

Equipotential Lines and Electric Fields Plotting the Electric Field Physics Equipotential Lines and Electric Fields Plotting the Electric Field MATERIALS AND RESOURCES ABOUT THIS LESSON EACH GROUP TEACHER he electrical field produces a force that acts S E 5 alligator clip leads wire cutter between two charges in the same way that G the gravitational field force acts between A 2 batteries, 9 V wire, copper, T P two masses. In this activity students will measure #16 gauge 2 binder clips, large potentials that exist between charged regions, then plot R computer electric fields which are implied by these differences E H ® in potential. LabQuest C A multimeter, OBJECTIVES E seven-function T picture frame, Students will: plastic box-style, • Investigate the space between a pair of electrodes 8.5 in. × 11 in. that are connected to a source of direct current sensor, voltage probe • Plot and examine the plot in terms of the implied ruler, clear metric electric field tape, masking LEVEL 2 pieces wires, copper, #16 gauge, Physics approx. 20 cm Copyright © 2013 National Math + Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. i Physics – Equipotential Lines and Electric Fields COMMON CORE STATE STANDARDS (MATH) A-CED.2 (LITERACY) W.3 Create equations in two or more variables to Write narratives to develop real or imagined represent relationships between quantities; graph experiences or events using effective technique, equations on coordinate axes with labels and scales. well-chosen details, and well-structured event sequences. (MATH) S-ID.6B Represent data on two quantitative variables on (MATH) A-CED.4 a scatter plot, and describe how the variables are Rearrange formulas to highlight a quantity of related. Informally assess the fit of a function by interest, using the same reasoning as in solving plotting and analyzing residuals. equations. For example, rearrange Ohm’s law V = IR to highlight resistance R. (LITERACY) RST.9-10.3 Follow precisely a multistep procedure when (MATH) F-LE.2 carrying out experiments, taking measurements, or Construct linear and exponential functions, including performing technical tasks, attending to special cases arithmetic and geometric sequences, given a graph, or exceptions defined in the text. a description of a relationship, or two input-output pairs (include reading these from a table). S (LITERACY) RST.9-10.7 E (MATH) F-LE.5 Translate quantitative or technical information G expressed in words in a text into visual form (e.g., Interpret expressions for functions in terms of the A P a table or chart) and translate information expressed situation they model. Interpret the parameters in a visually or mathematically (e.g., in an equation) into linear or exponential function in terms of a context. R words. E (MATH) N-Q.1 H (LITERACY) RST.9-10.10 Use units as a way to understand problems and to C guide the solution of multi-step problems; choose A By the end of grade 10, read and comprehend E science/technical texts in the grades 9-10 text and interpret units consistently in formulas; choose T complexity band independently and proficiently. and interpret the scale and the origin in graphs and data displays. (LITERACY) W.1 Write arguments to support claims in an analysis of (MATH) S-ID.6A substantive topics or texts, using valid reasoning and Represent data on two quantitative variables on relevant and sufficient evidence. a scatter plot, and describe how the variables are related. Fit a function to the data; use functions fitted (LITERACY) W.4 to data to solve problems in the context of the data. Produce clear and coherent writing in which the Use given functions or choose a function suggested development, organization, and style are appropriate by the context. Emphasize linear, quadratic, and to task, purpose, and audience. exponential models. v. 2.0, 2.0 Copyright © 2013 National Math + Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. ii Physics – Equipotential Lines and Electric Fields ASSESSMENTS NEXT GENERATION SCIENCE STANDARDS The following types of formative assessments are embedded in this lesson: • Assessment of prior knowledge i i • Guided questions DEVELOPING AND ANALYZING AND OBTAINING/EVALUATING • Assessments of Process Skills USING MODELS INTERPRETING DATA COMMUNICATING The following additional assessments are located on our website: • Physics Assessment: Electrostatics • 2010 Physics Posttest, Free Response CAUSE AND EFFECT ENERGY AND MATTER PATTERNS Question 2; 2008 Physics Posttest, Free Response Question 3; Physics Posttest, Free Response Question 2. ACKNOWLEDGEMENTS PS2: FORCES PS3: ENERGY PS4: WAVES S AND INTERACTION Microsoft® product screenshots reprinted with E G ® permission from Microsoft Corporation. Microsoft , A Windows®, and Excel® are either registered P trademarks or trademarks of Microsoft Corporation R in the United States and/or other countries. E H ® ® EasyData™, Graphical Analysis , LabPro , C LabQuest™, and Logger Pro 3® used with A permission, Vernier Software & Technology. E T Copyright © 2013 National Math + Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. iii Physics – Equipotential Lines and Electric Fields TEACHING SUGGESTIONS he concept of electric fields was introduced When the circuit is connected, chemical reactions by Michael Faraday. The electric field is will also start that will corrode the tips of the copper Tthe region where the force on one charge wire and will change the resistance, and thus will is caused by the presence of another charge. The also distort the shape of the field if left too long. electric field is a vector quantity and by convention, After each period, the copper wires should be electric fields emanate from positive charges and cleaned with sandpaper or scraped clean. The plastic terminate on negative charges (Figure A). frames should be cleaned after each class period to avoid a build-up of copper compounds. The most likely chemical reactions are • Cu → Cu+2 + 2e− − −2 • H2O + 2e → H2 + O −2 −2 • CO2 + O → CO3 +2 −2 • Cu + CO3 → CuCO3 • H2O (s), a light blue precipitate S Figure A. Electric field There is also a science literacy piece that E accompanies this lesson which requires students to G Plastic picture frames are available from retail stores A interpret the soundness of articles written about the P in either 8 in. × 10 in. or 8.5 in. × 11 in. sizes. These dangers of electromagnetic fields. frames consist of a plastic box with a cardboard R E back for holding pictures. The box makes a good H flat container for holding a thin film of water. The C picture frames should be kept as level as possible so A that the electric field does not appear distorted. The E T water level should be kept shallow, just covering the bottom of the frame completely. Copyright © 2013 National Math + Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. iv DATA AND OBSERVATIONS ANSWER KEY Copyright ©2013 National Math +Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. Figure A. Equipotential lines,pointprobe Physics – Equipotential LinesandElectricFields –Equipotential Physics v T E A C H E R P A G E S ANSWER KEY (CONTINUED) Copyright ©2013 National Math +Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. Figure B. Equipotential lines,parallelline probe Physics – Equipotential LinesandElectricFields –Equipotential Physics vi T E A C H E R P A G E S Physics – Equipotential Lines and Electric Fields ANSWER KEY (CONTINUED) ANALYSIS 1. The electric field is constant on the straight 2. For example, choose two equipotential lines, line between the two charges. The electric field one at 10 V and 0.04 m from the positive is not constant along the curved electric field terminal and one at 2 V and 0.06 m from the lines. positive terminal. The electric field between them can be approximated as Electric field lines Equipotential V 10V− 2V lines E == =400 V/m = 400 N/C d 0.06m− 0.04m Notice that the units V/m are equivalent to force per unit of charge, newtons per coulomb (N/C). Figure C. Equipotential and electric field lines, point source S Table 1. Calculating Electric Field Strength E G Line Contact Points Voltage (V) Distance (m) Electric Field (V/m) A 1 A to C 8 − 4 = 4 0.039 100 P R 2 B to D 6 − 2 = 4 0.046 90 E H C 3 C to D 4 − 2 = 2 0.021 100 A E 4 A to G 8 − (−4) = 12 0.107 110 T 5 C to I 4 − (−8) = 12 0.127 90 3. The electric field between the point charges _ varies depending on the distance from + each charged point, becoming weaker with increasing distance. The electric field between the parallel lines is relatively constant. Figure D. Equipotential and electric field lines, parallel lines Copyright © 2013 National Math + Science Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. vii Physics – Equipotential Lines and Electric Fields ANSWER KEY (CONTINUED) CONCLUSION QUESTIONS 1. An electric field is a region in space where one 4. a. The work along an electric field line depends charge experiences a force from another charge. on the magnitude of the charge and the Electric potential is the amount of energy potential difference through which the charge stored in an electric charge due to its position is moved. in an electric field. The strength of an electric b. No work is required to move a charge along field is directly related to the magnitude of the an equipotential line because no force is electric charge producing the field. required, and there is no change in potential. 2. Electric field lines begin on positive charges 5.
Recommended publications
  • Particle Motion
    Physics of fusion power Lecture 5: particle motion Gyro motion The Lorentz force leads to a gyration of the particles around the magnetic field We will write the motion as The Lorentz force leads to a gyration of the charged particles Parallel and rapid gyro-motion around the field line Typical values For 10 keV and B = 5T. The Larmor radius of the Deuterium ions is around 4 mm for the electrons around 0.07 mm Note that the alpha particles have an energy of 3.5 MeV and consequently a Larmor radius of 5.4 cm Typical values of the cyclotron frequency are 80 MHz for Hydrogen and 130 GHz for the electrons Often the frequency is much larger than that of the physics processes of interest. One can average over time One can not however neglect the finite Larmor radius since it lead to specific effects (although it is small) Additional Force F Consider now a finite additional force F For the parallel motion this leads to a trivial acceleration Perpendicular motion: The equation above is a linear ordinary differential equation for the velocity. The gyro-motion is the homogeneous solution. The inhomogeneous solution Drift velocity Inhomogeneous solution Solution of the equation Physical picture of the drift The force accelerates the particle leading to a higher velocity The higher velocity however means a larger Larmor radius The circular orbit no longer closes on itself A drift results. Physics picture behind the drift velocity FxB Electric field Using the formula And the force due to the electric field One directly obtains the so-called ExB velocity Note this drift is independent of the charge as well as the mass of the particles Electric field that depends on time If the electric field depends on time, an additional drift appears Polarization drift.
    [Show full text]
  • 19-8 Magnetic Field from Loops and Coils
    Answer to Essential Question 19.7: To get a net magnetic field of zero, the two fields must point in opposite directions. This happens only along the straight line that passes through the wires, in between the wires. The current in wire 1 is three times larger than that in wire 2, so the point where the net magnetic field is zero is three times farther from wire 1 than from wire 2. This point is 30 cm to the right of wire 1 and 10 cm to the left of wire 2. 19-8 Magnetic Field from Loops and Coils The Magnetic Field from a Current Loop Let’s take a straight current-carrying wire and bend it into a complete circle. As shown in Figure 19.27, the field lines pass through the loop in one direction and wrap around outside the loop so the lines are continuous. The field is strongest near the wire. For a loop of radius R and current I, the magnetic field in the exact center of the loop has a magnitude of . (Equation 19.11: The magnetic field at the center of a current loop) The direction of the loop’s magnetic field can be found by the same right-hand rule we used for the long straight wire. Point the thumb of your right hand in the direction of the current flow along a particular segment of the loop. When you curl your fingers, they curl the way the magnetic field lines curl near that segment. The roles of the fingers and thumb can be reversed: if you curl the fingers on Figure 19.27: (a) A side view of the magnetic field your right hand in the way the current goes around from a current loop.
    [Show full text]
  • Experiment 1: Equipotential Lines and Electric Fields
    MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2006 Experiment 1: Equipotential Lines and Electric Fields OBJECTIVES 1. To develop an understanding of electric potential and electric fields 2. To better understand the relationship between equipotentials and electric fields 3. To become familiar with the effect of conductors on equipotentials and E fields PRE-LAB READING INTRODUCTION Thus far in class we have talked about fields, both gravitational and electric, and how we can use them to understand how objects can interact at a distance. A charge, for example, creates an electric field around it, which can then exert a force on a second charge which enters that field. In this lab we will study another way of thinking about this interaction through electric potentials. The Details: Electric Potential (Voltage) Before discussing electric potential, it is useful to recall the more intuitive concept of potential energy, in particular gravitational potential energy. This energy is associated with a mass’s position in a gravitational field (its height). The potential energy difference between being at two points is defined as the amount of work that must be done to move between them. This then sets the relationship between potential energy and force (and hence field): B G G dU ∆=UU−U=−Fs⋅d ⇒ ()in 1D F=− (1) BA∫ A dz We earlier defined fields by breaking a two particle interaction, force, into two single particle interactions, the creation of a field and the “feeling” of that field. In the same way, we can define a potential which is created by a particle (gravitational potential is created by mass, electric potential by charge) and which then gives to other particles a potential energy.
    [Show full text]
  • Principle and Characteristic of Lorentz Force Propeller
    J. Electromagnetic Analysis & Applications, 2009, 1: 229-235 229 doi:10.4236/jemaa.2009.14034 Published Online December 2009 (http://www.SciRP.org/journal/jemaa) Principle and Characteristic of Lorentz Force Propeller Jing ZHU Northwest Polytechnical University, Xi’an, Shaanxi, China. Email: [email protected] Received August 4th, 2009; revised September 1st, 2009; accepted September 9th, 2009. ABSTRACT This paper analyzes two methods that a magnetic field can be generated, and classifies them under two types: 1) Self-field: a magnetic field can be generated by electrically charged particles move, and its characteristic is that it can’t be independent of the electrically charged particles. 2) Radiation field: a magnetic field can be generated by electric field change, and its characteristic is that it independently exists. Lorentz Force Propeller (ab. LFP) utilize the charac- teristic that radiation magnetic field independently exists. The carrier of the moving electrically charged particles and the device generating the changing electric field are fixed together to form a system. When the moving electrically charged particles under the action of the Lorentz force in the radiation magnetic field, the system achieves propulsion. Same as rocket engine, the LFP achieves propulsion in vacuum. LFP can generate propulsive force only by electric energy and no propellant is required. The main disadvantage of LFP is that the ratio of propulsive force to weight is small. Keywords: Electric Field, Magnetic Field, Self-Field, Radiation Field, the Lorentz Force 1. Introduction also due to the changes in observation angle.) “If the electric quantity carried by the particles is certain, the The magnetic field generated by a changing electric field magnetic field generated by the particles is entirely de- is a kind of radiation field and it independently exists.
    [Show full text]
  • Physics 2102 Lecture 2
    Physics 2102 Jonathan Dowling PPhhyyssicicss 22110022 LLeeccttuurree 22 Charles-Augustin de Coulomb EElleeccttrriicc FFiieellddss (1736-1806) January 17, 07 Version: 1/17/07 WWhhaatt aarree wwee ggooiinngg ttoo lleeaarrnn?? AA rrooaadd mmaapp • Electric charge Electric force on other electric charges Electric field, and electric potential • Moving electric charges : current • Electronic circuit components: batteries, resistors, capacitors • Electric currents Magnetic field Magnetic force on moving charges • Time-varying magnetic field Electric Field • More circuit components: inductors. • Electromagnetic waves light waves • Geometrical Optics (light rays). • Physical optics (light waves) CoulombCoulomb’’ss lawlaw +q1 F12 F21 !q2 r12 For charges in a k | q || q | VACUUM | F | 1 2 12 = 2 2 N m r k = 8.99 !109 12 C 2 Often, we write k as: 2 1 !12 C k = with #0 = 8.85"10 2 4$#0 N m EEleleccttrricic FFieieldldss • Electric field E at some point in space is defined as the force experienced by an imaginary point charge of +1 C, divided by Electric field of a point charge 1 C. • Note that E is a VECTOR. +1 C • Since E is the force per unit q charge, it is measured in units of E N/C. • We measure the electric field R using very small “test charges”, and dividing the measured force k | q | by the magnitude of the charge. | E |= R2 SSuuppeerrppoossititioionn • Question: How do we figure out the field due to several point charges? • Answer: consider one charge at a time, calculate the field (a vector!) produced by each charge, and then add all the vectors! (“superposition”) • Useful to look out for SYMMETRY to simplify calculations! Example Total electric field +q -2q • 4 charges are placed at the corners of a square as shown.
    [Show full text]
  • Structure of the Electron Diffusion Region in Magnetic Reconnection with Small Guide Fields
    Structure of the electron diffusion region in magnetic reconnection with small guide fields MASSA0HU- by Jonathan Ng JAN I Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Bachelor of Science in Physics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 2012 @ Jonathan Ng, MMXII. All rights reserved. The author hereby grants to MIT permission to reproduce and distribute publicly paper and electronic copies of this thesis document in whole or in part. Author ............ Department of Physics May 11, 2012 / / Certified by..... *2) Jan Egedal-Pedersen Associate Professor of Physics Thesis Supervisor Accepted by ...... .............. ........ ............. ... Nergis Mavalvala Senior Thesis Coordinator, Department of Physics 2 Structure of the electron diffusion region in magnetic reconnection with small guide fields by Jonathan Ng Submitted to the Department of Physics on May 11, 2012, in partial fulfillment of the requirements for the degree of Bachelor of Science in Physics Abstract Observations in the Earth's magnetotail and kinetic simulations of magnetic reconnec- tion have shown high electron pressure anisotropy in the inflow of electron diffusion regions. This anisotropy has been accurately accounted for in a new fluid closure for collisionless reconnection. By tracing electron orbits in the fields taken from particle-in-cell simulations, the electron distribution function in the diffusion region is reconstructed at enhanced resolutions. For antiparallel reconnection, this reveals its highly structured nature, with striations corresponding to the number of times an electron has been reflected within the region, and exposes the origin of gradients in the electron pressure tensor important for momentum balance. The addition of a guide field changes the nature of the electron distributions, and the differences are accounted for by studying the motion of single particles in the field geometry.
    [Show full text]
  • Field Line Motion in Classical Electromagnetism John W
    Field line motion in classical electromagnetism John W. Belchera) and Stanislaw Olbert Department of Physics and Center for Educational Computing Initiatives, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 ͑Received 15 June 2001; accepted 30 October 2002͒ We consider the concept of field line motion in classical electromagnetism for crossed electromagnetic fields and suggest definitions for this motion that are physically meaningful but not unique. Our choice has the attractive feature that the local motion of the field lines is in the direction of the Poynting vector. The animation of the field line motion using our approach reinforces Faraday’s insights into the connection between the shape of the electromagnetic field lines and their dynamical effects. We give examples of these animations, which are available on the Web. © 2003 American Association of Physics Teachers. ͓DOI: 10.1119/1.1531577͔ I. INTRODUCTION meaning.10,11 This skepticism is in part due to the fact that there is no unique way to define the motion of field lines. Classical electromagnetism is a difficult subject for begin- Nevertheless, the concept has become an accepted and useful ning students. This difficulty is due in part to the complexity one in space plasma physics.12–14 In this paper we focus on a of the underlying mathematics which obscures the physics.1 particular definition of the velocity of electric and magnetic The standard introductory approach also does little to con- field lines that is useful in quasi-static situations in which the nect the dynamics of electromagnetism to the everyday ex- E and B fields are mutually perpendicular.
    [Show full text]
  • Electromagnetic Fields and Energy
    MIT OpenCourseWare http://ocw.mit.edu Haus, Hermann A., and James R. Melcher. Electromagnetic Fields and Energy. Englewood Cliffs, NJ: Prentice-Hall, 1989. ISBN: 9780132490207. Please use the following citation format: Haus, Hermann A., and James R. Melcher, Electromagnetic Fields and Energy. (Massachusetts Institute of Technology: MIT OpenCourseWare). http://ocw.mit.edu (accessed [Date]). License: Creative Commons Attribution-NonCommercial-Share Alike. Also available from Prentice-Hall: Englewood Cliffs, NJ, 1989. ISBN: 9780132490207. Note: Please use the actual date you accessed this material in your citation. For more information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms 9 MAGNETIZATION 9.0 INTRODUCTION The sources of the magnetic fields considered in Chap. 8 were conduction currents associated with the motion of unpaired charge carriers through materials. Typically, the current was in a metal and the carriers were conduction electrons. In this chapter, we recognize that materials provide still other magnetic field sources. These account for the fields of permanent magnets and for the increase in inductance produced in a coil by insertion of a magnetizable material. Magnetization effects are due to the propensity of the atomic constituents of matter to behave as magnetic dipoles. It is natural to think of electrons circulating around a nucleus as comprising a circulating current, and hence giving rise to a magnetic moment similar to that for a current loop, as discussed in Example 8.3.2. More surprising is the magnetic dipole moment found for individual electrons. This moment, associated with the electronic property of spin, is defined as the Bohr magneton e 1 m = ± ¯h (1) e m 2 11 where e/m is the electronic charge­to­mass ratio, 1.76 × 10 coulomb/kg, and 2π¯h −34 2 is Planck’s constant, ¯h = 1.05 × 10 joule­sec so that me has the units A − m .
    [Show full text]
  • Field Lines Electric Flux Recall That We Defined the Electric Field to Be the Force Per Unit Charge at a Particular Point
    Gauss’ Law Field Lines Electric Flux Recall that we defined the electric field to be the force per unit charge at a particular point: P For a source point charge Q and a test charge q at point P q Q at P If Q is positive, then the field is directed radially away from the charge. + Note: direction of arrows Note: spacing of lines Note: straight lines If Q is negative, then the field is directed radially towards the charge. - Negative Q implies anti-parallel to Note: direction of arrows Note: spacing of lines Note: straight lines + + Field lines were introduced by Michael Faraday to help visualize the direction and magnitude of the electric field. The direction of the field at any point is given by the direction of the field line, while the magnitude of the field is given qualitatively by the density of field lines. In the above diagrams, the simplest examples are given where the field is spherically symmetric. The direction of the field is apparent in the figures. At a point charge, field lines converge so that their density is large - the density scales in proportion to the inverse of the distance squared, as does the field. As is apparent in the diagrams, field lines start on positive charges and end on negative charges. This is all convention, but it nonetheless useful to remember. - + This figure portrays several useful concepts. For example, near the point charges (that is, at a distance that is small compared to their separation), the field becomes spherically symmetric. This makes sense - near a charge, the field from that one charge certainly should dominate the net electric field since it is so large.
    [Show full text]
  • Magnetic Fields, Magnetic Forces, and Sources of Magnetic Fields
    Magnetic Fields, Magnetic Forces, and Sources of Magnetic Fields W07D2 1 Announcements Problem Set 6 Due Thursday at 9 pm .This problem set is an introduction to Experiment 1 and the two problems from W06D2. Week 8 LS1 due Mon at 8:30 am Week 8 LS2 due Mon at 8:30 am Week 8 LS3 due Wed at 8:30 am Week 8 LS4 due Wed at 8:30 am 2 Outline Magnetic Field Lorentz Force Law Magnetic Force on Current Carrying Wire Sources of Magnetic Fields Biot-Savart Law 3 Magnetic Field of the Earth North magnetic pole located in southern hemisphere http://www.youtube.com/watch?v=AtDAOxaJ4Ms 4 Magnetic Force on Moving Charges Force on ! ! positive charge B ! Fq = qvq × B vq B B q vq F F q q B q + B Force on negative charge Magnetic force is perpendicular to both velocity of the charge and magnetic field 5 CQ: Cross Product and Magnetic Force An electron is traveling up in a magnetic field that points to the right. What is the direction of the force on the electron? v 1. Up. q 2. Down. B 3. Left. q = e 4. Right. 5. Into plane of figure. 6. Out of plane of figure. 6 Group Problem: Cyclotron Motion A positively charged particle vq with charge +q and mass m is B moving with speed v in a + uniform magnetic field of + q magnitude B directed into the plane of figure will undergo circular motion. Find (1) the radius R of the orbit, (2) the period T of the motion, (3) the angular frequency ω.
    [Show full text]
  • Electric Potential Equipotentials and Energy
    Electric Potential Equipotentials and Energy Phys 122 Lecture 8 G. Rybka Your Thoughts • Nervousness about the midterm I would like to have a final review of all the concepts that we should know for the midterm. I'm having a lot of trouble with the homework and do not think those questions are very similar to what we do in class, so if that's what the midterm is like I think we need to do more mathematical examples in class. • Confusion about Potential I am really lost on all of this to be honest I'm having trouble understanding what Electric Potential actually is conceptually. • Some like the material! I love potential energy. I think it is These are yummy. fascinating. The world is amazing and physics is everything. A few answers Why does this even matter? Please go over in detail, it kinda didn't resonate with practical value. This is the first pre-lecture that really confused me. What was the deal with the hill thing? don't feel confident in my understanding of the relationship of E and V. Particularly calculating these. If we go into gradients of V, I will not be a happy camper... The Big Idea Electric potential ENERGY of charge q in an electric field: b ! ! b ! ! ΔU = −W = − F ⋅ dl = − qE ⋅ dl a→b a→b ∫ ∫ a a New quantity: Electric potential (property of the space) is the Potential ENERGY per unit of charge ΔU −W b ! ! ΔV ≡ a→b = a→b = − E ⋅ dl a→b ∫ q q a If we know E, we can get V The CheckPoint had an “easy” E field Suppose the electric field is zero in a certain region of space.
    [Show full text]
  • Lecture 2 Electric Fields Chp. 22 Ed. 7
    Lecture 2 Electric Fields Chp. 22 Ed. 7 • Cartoon - Analogous to gravitational field • Warm-up problems , Physlet • Topics – Electric field = Force per unit Charge – Electric Field Lines – Electric field from more than 1 charge – Electric Dipoles – Motion of point charges in an electric field – Examples of finding electric fields from continuous charges • List of Demos – Van de Graaff Generator, workings,lightning rod, electroscope, – Field lines using felt,oil, and 10 KV supply., • One point charge • Two same sign point charges • Two opposite point charges • Slab of charge – Smoke remover or electrostatic precipitator – Kelvin water drop generator – Electrophorus 1 2 Concept of the Electric Field • Definition of the electric field. Whenever charges are present and if I bring up another charge, it will feel a net Coulomb force from all the others. It is convenient to say that there is field there equal to the force per unit positive charge. E=F/q0. • The question is how does charge q0 know about 1charge q1 if it does not “touch it”? Even in a vacuum! We say there is a field produced by q1 that extends out in space everywhere. • The direction of the electric field is along r and points in the direction a positive test charge would move. This idea was proposed by Michael Faraday in the 1830’s. The idea of the field replaces the charges as defining the situation. Consider two point charges: r q1 q0 3 r q1 + q0 2 The Coulomb force is F= kq1q0/r The force per unit charge is E = F/q0 2 Then the electric field at r is E = kq1/r due to the point charge q1 .
    [Show full text]