Electric Charge and Electric Field

Slides:



Advertisements
Similar presentations
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Advertisements

Electric Forces and Fields
Unit 14: Electrostatics.
Chapter 21 Electric Charge and Electric Field
Day 2 Electrical Charging & Coulomb’s Law. Objectives Charging by Conduction Charging by Induction Electroscopes Coulomb’s Law.
Chapter 23 Electric Fields
Electric Charges and Electric Fields
Electric Forces and Electric Fields. Properties of Electric Charges Two types of charges exist They are called positive and negative Named by Benjamin.
Electric Charge and Electric Field Electric Charge and Electric Field
CHAPTER 23 : ELECTRIC FIELDS
Chapter 21, Electric Charge, and electric Field. Charles Allison © Electric Charge, q or Q Charge comes in two types 1e = 1.6x Coulombs.
Nadiah Alenazi 1 Chapter 23 Electric Fields 23.1 Properties of Electric Charges 23.3 Coulomb ’ s Law 23.4 The Electric Field 23.6 Electric Field Lines.
Chapter 23 Electric Fields Summer 1996, Near the University of Arizona.
1/10/ Lecture 31 PHY 184 Spring 2007 Lecture 3 Title: The Coulomb Force.
Dr. Jie ZouPHY Chapter 23 Electric fields (cont.)
Lecture 9 Coulomb’s law Electric field. 3.3 Coulomb’s Law Coulomb’s law gives the force between two point charges: The force is along the line connecting.
Chapter 23 Electric Charge and Electric Fields What is a field? Why have them? What causes fields? Field TypeCaused By gravitymass electriccharge magneticmoving.
Chapter 21 Electric Charge and Electric Fields
Chapter 23, part I 1. Electrical charge. 2. Coulomb’s Law about force between two point charges. 3. Application of Coulomb’s Law.
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 16 Electric Charge and Electric Field. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom.
Chapter 19 Electric Forces and Electric Fields Electric Charges There are two kinds of electric charges Called positive and negative Negative.
Electric Forces and Fields: Coulomb’s Law
Electric Forces and Fields Chapter 17. Section 17-1 Objectives Understand the basic properties of electric charge Understand the basic properties of electric.
Electric Charge and Electric Field
18.5 Coulomb's Law. The magnitude F of the electrostatic force exerted by one point charge on another point charge is directly proportional to the magnitudes.
1 Norah Ali Al-moneef king Saud unversity 23.1 Properties of Electric Charges 23.2 Charging Objects By Induction 23.3 Coulomb’s Law 23.4 The Electric Field.
Electric Field Physics Overview Properties of Electric Charges Charging Objects by Induction Coulomb’s Law The Electric Field Electric Field Lines.
Electric Charge and Coulomb’s Law
Electric Charge and Electric Field
Forces and Fields Lesson 4
Foundation year General Physics PHYS 101 Lecture 9: Coulomb’s law and Electric field Instructor: Sujood Alazzam 2015/
Section 23.3: Coulomb’s Law
Electric Charges Conduction: Transfer of a charge easily. Induction: Influence transfer of a charge. (polarization of a charge) Insulator: Does not transfer.
Chapter 16 Electric Charge and Electric Field. Units of Chapter 16 Static Electricity; Electric Charge and Its Conservation Electric Charge in the Atom.
Charles Allison © 2000 Chapter 21, Electric Charge, and electric Field.
Electric Charge and Electric Field
Norah Ali Al-moneef king Saud unversity
Physics 2102 Lecture 04: WED 03 SEP
Coulomb’s Law (electrical force between charged particles).
Electrostatics Getting a Charge Out of Physics
Electricity and Magnetism Electric Fields: Coulomb’s Law
COULOMB’S LAW Coulomb’s Law – charges exert forces on each other and have been shown to be directly proportional to the magnitude of the charge and inversely.
Electrostatics Forces and Fields
Lecture 01: Electric Fields & Forces
Phy2005 Applied Physics II Spring 2017 Announcements:
Electric Forces and Electric Fields
Electric Fields Chapter 14.1.
Chapter 21, Electric Charge, and electric Field
Chapter 21, Electric Charge, and electric Field
Coulomb’s Law.
Coulomb’s Law Pg
Electric Fields and Forces
PHYSICS 2415 Suggested strategies: Read text before lecture
Section 23.3: Coulomb’s Law
Electrical Charge There are only two types of charges: (+) and (-)
PHYS 1441 – Section 002 Lecture #3
Norah Ali Al-moneef king Saud unversity
Chapter 21, Electric Charge, and electric Field
Charge & Coulomb’s Law
PHYS 1441 – Section 002 Lecture #3
Structure of matter in the Universe
Textbook: 7.1, 7.2 Homework: pg # 2 – 6
Electrostatics AP Physics.
Electrical Charge and Coulomb’s Law of Electrostatic Force
Chapter 23: Electric Field
Chapter 7: Electric Field
Norah Ali Al-moneef king Saud unversity
Presentation transcript:

Electric Charge and Electric Field

Coulomb’s Law Experiment shows that the electric force between two charges is proportional to the product of the charges and inversely proportional to the distance between them.

Coulomb’s Law Experiment shows that the electric force between two charges is proportional to the product of the charges and inversely proportional to the distance between them. Figure 21-14. Coulomb’s law, Eq. 21–1, gives the force between two point charges, Q1 and Q2, a distance r apart. Coulomb’s law, Eq. 21–1, gives the force between two point charges, Q1 and Q2, a distance r apart.

Properties of electric force between two stationary charge particles: The electric force.. is inversely proportional to square of the separation between particles and directed along the line joining them is proportional to the product of the charges q1 and q2 on the two particles is attractive if charges are of opposite sign and repulsive if the charges are of the same sign Is a conservative force

Coulomb’s Law equation An equation giving the magnitude of electric force between two point charges (Point charges defined as a particle of zero size that carries an electric charge) Where ke is called the Coulomb constant and ke = 8.9875 x 109 Nm2C-2 (S.I units) or ke = 1/ 4πЄ0 and Є0 = permittivity of free space = 8.8542 x 10-12 C2N-1m-2

Coulomb’s Law Coulomb’s law: This equation gives the magnitude of the force between two charges.

Coulomb’s Law The force is along the line connecting the charges, and is attractive if the charges are opposite, and repulsive if they are the same. The direction of the static electric force one point charge exerts on another is always along the line joining the two charges, and depends on whether the charges have the same sign as in (a) and (b), or opposite signs (c).

Coulomb’s Law Unit of charge: coulomb, C The proportionality constant in Coulomb’s law is then: Charges produced by rubbing are typically around a microcoulomb:

Coulomb’s Law Electric charge is quantized in units of the electron charge.

Coulomb’s Law The proportionality constant k can also be written in terms of , the permittivity of free space: (16-2)

Electric Force is a vector Figure 23.7 Two point charges separated by a distance r exert a force on each other that is given by Coulomb’s law. The force F21 exerted by q2 on q1 is equal in magnitude and opposite in direction to the force F12 exerted by q1 on q2. (a) When the charges are of the same sign, the force is repulsive. Two point charges separated by a distance r exert a force on each other that is given by Coulomb’s law. The force F21 exerted by q2 on q1 is equal in magnitude and opposite in direction to the force F12 exerted by q1 on q2. When the charges are of the same sign, the force is repulsive.

When the charges are of opposite signs, the force is attractive. Figure 23.7 Two point charges separated by a distance r exert a force on each other that is given by Coulomb’s law. The force F21 exerted by q2 on q1 is equal in magnitude and opposite in direction to the force F12 exerted by q1 on q2. (b) When the charges are of opposite signs, the force is attractive. When the charges are of opposite signs, the force is attractive.

Where, is a unit vector directed from q1 to q2. Since the force obeys Newton’s third law, then F12 = - F21

Example: Question 1 The electron and proton of a hydrogen atom are separated by a distance of approximately 5.3 x 10-11 m. Find the magnitude of the electric force.

Example: Solution 1 Fe = 8.2 x 10-8 N

Coulomb’s Law Example 2: Three charges in a line. Three charged particles are arranged in a line, as shown. Calculate the net electrostatic force on particle 3 (the -4.0 μC on the right) due to the other two charges. Solution: Coulomb’s law gives the magnitude of the forces on particle 3 from particle 1 and from particle 2. The directions of the forces can be found from the geometrical arrangement of the charges (NOT by putting signs on the charges in Coulomb’s law, which is what the students will want to do). F = -1.5 N (to the left).

Exercise What is the magnitude of the force a +25 µC charge exerts on a +2.5 mC charge 28 cm away?

Exercise 2. Three point charges, Q1 = 3 µC, Q2 = -5 µC, and Q3 = 8 µC are placed on the x-axis as shown in Figure 1. Find the net force on the charge Q2 due to the charges Q1 and Q3. Q1 20 cm 30 cm Q2 Q3

Exercise 3. Particles of charge +75, +48 and -85 µC are placed in a line . The center one is 0.35 m from each of the others. Calculate the net force on each charge due to the other two.

Coulomb’s Law Example 3: Electric force using vector components. Calculate the net electrostatic force on charge Q3 shown in the figure due to the charges Q1 and Q2. Figure 21-18. Determining the forces for Example 21–3. (a) The directions of the individual forces are as shown because F32 is repulsive (the force on Q3 is in the direction away from Q2 because Q3 and Q2 are both positive) whereas F31 is attractive (Q3 and Q1 have opposite signs), so F31 points toward Q1. (b) Adding F32 to F31 to obtain the net force. Solution: The forces, components, and signs are as shown in the figure. Result: The magnitude of the force is 290 N, at an angle of 65° to the x axis.

Coulomb’s Law Approach We use Coulomb’s law to find the magnitude of the individual forces. The direction of each force will be along the line connecting Q3 to Q1 or Q2. The forces F31 and F32 have the directions shown in figure, Q1 exerts an attractive force on Q3 Q2 exerts a repulsive force on Q3 4. The forces F31 and F32 are not in the same line, so to find the resultant force on Q3, we resolve F31 and F32 into x and y components and perform vector addition.

Exercise Three charged particles are placed at the corners of an equilateral triangle of side 1.20 m . The charges are +7.0µC, -8.0µC and -6.0µC. Calculate the magnitude and direction of the net force on Q1 due to the other two.

Electrical Force with Other Forces, Example The spheres are in equilibrium. Since they are separated, they exert a repulsive force on each other. Charges are like charges Model each sphere as a particle in equilibrium. Proceed as usual with equilibrium problems, noting one force is an electrical force. Section 23.3

Electrical Force with Other Forces, Example cont. The force diagram includes the components of the tension, the electrical force, and the weight. Solve for |q| If the charge of the spheres is not given, you cannot determine the sign of q, only that they both have same sign. Section 23.3

Examples Two indentical small spheres, each having a mass of 3.00 x 10-2 kg, hang in equilibrium as shown in Figure. The length, L of each string is 0.150m and the θ= 5.000. Find the magnitude of the charge on each sphere.

Summary Two kinds of electric charge – positive and negative. Charge is conserved. Charge on electron: e = 1.602 x 10-19 C. Conductors: electrons free to move. Insulators: nonconductors.

Summary Charge is quantized in units of e. Objects can be charged by conduction or induction. Coulomb’s law: