Scalar field: Temperatures The shown temperatures are samples of the field 77 82 83 68 55 66 83 75 80 90 91 75 71 80 72 84 73 82 88 92 77 88 73 64.

Slides:



Advertisements
Similar presentations
Electric Forces and Fields
Advertisements

Continuous Charge Distributions
Electric Charges and Electric Fields
Reading Quiz The voltage (or electric potential) of a battery determines how much work the battery can do on an electric charge. how much net electric.
Chapter 22 Electric Potential.
Topic 9.3 Electric Field, Potential, and Energy
Electric Field Physics Department, New York City College of Technology.
Chapter 23 Summer 1996, Near the University of Arizona Chapter 23 Electric Fields.
Electric Charge and Electric Field
Electric Forces and Electric Fields
From Chapter 23 – Coulomb’s Law
Electric Energy and Capacitance
Fall 2008Lecture 1-1Physics 231 Electric Charges, Forces, and Fields.
Physics Electrostatics: Electric Field Diagrams Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund.
The Electric Field. The electric field E at a point in space is defined as an electric force F, acting on a positive test charge q divided by the magnitude.
Chapter 22 Electric Field
Electric Field Lines - a “map” of the strength of the electric field. The electric field is force per unit charge, so the field lines are sometimes called.
Fig 24-CO, p.737 Chapter 24: Gauss’s Law قانون جاوس 1- Electric Flux 2- Gauss’s Law 3-Application of Gauss’s law 4- Conductors in Electrostatic Equilibrium.
Lecture 3 Electric Field Electric Field Lines Conductors in Electrostatic Equilibrium Millikan’s Oil-Drop Experiment Van de Graff Generator Electric Flux.
Chapter 21 Gauss’s Law. Electric Field Lines Electric field lines (convenient for visualizing electric field patterns) – lines pointing in the direction.
1 Electric Field – Continuous Charge Distribution As the average separation between source charges is smaller than the distance between the charges and.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electric energy (Electric Potential Energy) Electric potential Gravitation.
Electrostatics Properties of Electric Charges.
Chapter 16 Electric Forces and Electric Fields
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism (Electrostatics) a. Electric Charge, Electric Field & Gauss’ Law.
Electric Charge and Electric Field 16
Chapter 18 Electric Forces and Electric Fields The Origin of Electricity The electrical nature of matter is inherent in atomic structure. coulombs.
Electric Forces and Fields: Coulomb’s Law
Electric Charge and Electric Field
ELECTRICITY AND MAGNETISM Phy 220 Chapter1: ELECTRIC FIELDS.
Electric Field Physics Overview Properties of Electric Charges Charging Objects by Induction Coulomb’s Law The Electric Field Electric Field Lines.
General Physics II, Lec 3, By/ T.A. Eleyan 1 Lecture 3 The Electric Field.
A proton and an electron are held apart a distance of 1 m and then let go. Where would they meet? 1) in the middle 2) closer to the electron’s side 3)
Lecture 2 The Electric Field. Chapter 15.4  15.9 Outline The Concept of an Electric Field Electric Field Lines Electrostatic Equilibrium Electric Flux.
CHAPTER 24 : GAUSS’S LAW 24.1) ELECTRIC FLUX
S-113 Define these terms A.Charge B.Potential Difference (Voltage) C.Current (Amps) D.Resistance.
1 Physics 8.02T For now, please sit anywhere, 9 to a table.
Electric Charge, Forces, and Fields Electric charge is a property of many elementary particles. There is a basic unit of charge that apparently cannot.
Halliday/Resnick/Walker Fundamentals of Physics
Chapter 21 Electric Charge and Electric Field HW #4: Chapter 21: Pb.21,Pb.38, Pb.40, Pb.52, Pb.59, Pb.80 Due Friday, Feb 20.
The Electric Field The electric field is present in any region of space if there exists electric forces on charges. These electric forces can be detected.
Electrostatics.
Electric Charge and Electric Field
Physics 213 General Physics
Electric Fields Year 13. Electrostatic force Like charges repel, unlike charges attract How does this force act if charges are not in contact? –An electric.
Electric Field-Intro Electric force is a field force. Field forces can act through space, i.e. requires no physical contact. Faraday developed the concept.
Force Fields Objective: TSW understand and apply the concept of a force field by calculating the field, the force and motion of a particle in a field.
Electricity Field Lines/Pot Surf 1 TOC Definition of a Field Field Lines Electric Field Lines Definition of a Potential Surface Motion of Particles in.
Electric Field.
The Electric Field. The electric field E at a point in space is defined as an electric force F, acting on a positive test charge q divided by the magnitude.
Electric Charge (1) Evidence for electric charges is everywhere, e.g.
Chapter 25 Electric Potential. Electrical Potential Energy The electrostatic force is a conservative force, thus It is possible to define an electrical.
1.Electrostatics Electric Field. The Electric Field is defined as the force on a test charge (small positive charge), divided by the charge: EE F F Electric.
1) Electric Charge I 1) one is positive, the other is negative 2) both are positive 3) both are negative 4) both are positive or both are negative Two.
Chapter 18 Electric Forces and Electric Fields The Origin of Electricity The electrical nature of matter is inherent in atomic structure. coulombs.
Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.
Electric Fields… …and Gauss’ Law Chapter 18 The Concept of a Field A field is defined as a property of space in which a material object experiences a.
Electric Fields Due to Continuous Charge Distributions
Fig 24-CO, p.737 Chapter 24: Gauss’s Law قانون جاوس 1- Electric Flux 2- Gauss’s Law 3-Application of Gauss’s law 4- Conductors in Electrostatic Equilibrium.
Scalar.
Electric Force Holt: Chapter 17-2 Pages
Force between Two Point Charges
Tribal Challenge Review Question!
The Electric Field Figure Force exerted by charge Q on a small test charge, q, placed at points A, B, and C.
King Saud university Norah Ali Al-Moneef
Quiz 1 (lecture 2) * A positive and negative charge with equal magnitude are connected by a rigid rod, and placed near a large negative charge. What is.
Electrical Field 15.4 Maxwell developed an approach to discussing fields An electric field is said to exist in the region of space around a charged object.
16 – 3 Electric Field.
Phys102 Lecture 2 The Electric Field
Electric Force Holt: Chapter 17-2 Pages
Presentation transcript:

Scalar field: Temperatures The shown temperatures are samples of the field

Vector field: Winds

3. Electric field Coulomb’s low and electric field Q q - test charge Definition Units (Action at a distance?) If the electric force on a test charge q located at point P is F, then the electric field at point P is F/q. Because the force is always proportional to q, the electric field is independent of the test charge! P Charge Q creates an electric (electrostatic) field E. Charge q is used to find this electric field E.

Example: A negative charge, placed in the electric field between two charged plates, experiences an electric force as shown below. What is the direction of the electric field? A. LeftB. Right C. Upward D. Downward The negative charge is attracted by the positive plate and is repelled from the negative plate The electric field is directed from the positive to the negative charge! Example: Between the red and the blue charges, which of them experiences the greater electric field due to the green charge? dd same electric field same point in space Both charges feel the same electric field due to the green charge because they are at the same point in space!

Example (Electron in a uniform electric field): Describe the motion of an electron that enters a region with a uniform electric field having initial velocity perpendicular to the direction of the field Once the electric field is known, finding the force on a given charge is simple… Constant acceleration in the –y direction. Identical to projectile motion! F = –|q e |E parabola E v0v0 electron

Two most important questions: 1)How can one find force, F on the electric charge, q, exerted by field E? 2)How can electrostatic field E be created? Answers: 1) 2) Field E is due to other charges 2a) Field due to a single charge: 2b) Field due to a number of charges: Principle of superposition has been used in 2b)

Q1Q1 Q3Q3 Q4Q4 Q7Q7 Q2Q2 Q6Q6 Q5Q5 Q8Q8 q1q1 Charges Q 1, Q 2 … create electric field. This field is independent from the test charge q 1. If we will replace the charge q 1 with another charge q 2, then the force on the new charge will be different then, but the electric field is independent from q. test charge These charges create electric field Definition of electric field Principle of superposition

Example (Net electric field ): Which of the three vectors best represents the direction of the net electric field at the location of charge Q? Q q 1 < 0 q 2 > 0 C A B E1E1 E2E2 E net Example: Calculate the electric field at the center of a square 52.5 cm on a side if one corner is occupied by a charge +45μC and the other three are occupied by charges -27μC.

Electric field lines Definition: Electric field lines indicate the direction of the force due to the given field on a positive charge, i.e. electric force on a positive charge is tangent to these lines Number of these lines is proportional to the magnitude of the charge Properties: Electric field lines start on positive charges or came from infinity, they end on negative charges or end at infinity Density of these lines is proportional to the magnitude of the field +Q -Q - -2Q

Electric Field Lines Around Electric Charges A single positive charge (an electric monopole) A positive charge and a negative of equal magnitude (an electric dipole) Two equal positive charges

Example: A. E 1 = E 2 > E 3 B. E 1 > E 2 > E 3 C. E 1 > E 2 ; E 3 = 0 The electric field lines in a certain region of space are as shown below. Compare the magnitude of the electric field at points 1, 2 and 3. The magnitude of the electric field is proportional to the local density of lines. Being on the same line or being between the lines is totally irrelevant.

Electric field in conductors The electric field inside a conductor in equilibrium is always zero. The electric field right outside a conductor in equilibrium is perpendicular to the surface of the conductor. We cannot have a force parallel to the surface (would produce motion), but perpendicular to it is OK. E = 0

Example: A 4.7μC and a -3.5μC charge are placed 18.5 cm apart. Where can a third charge be placed so that it experiences no net force? x – d To experience no net force, the third charge Q must be closer to the smaller magnitude charge (the negative charge). The third charge cannot be between the charges, because it would experience a force from each charge in the same direction, and so the net force could not be zero. And the third charge must be on the line joining the other two charges, so that the two forces on the third charge are along the same line. Equate the magnitudes of the two forces on the third charge, and solve for x > 0.