Chapter 21 Electric Charge and Electric Field

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Chapter 21 Electric Charge and Electric Field Electric charge Conductors and insulators Coulomb s Law Electric Fields Phys 2435: Chap 21, Pg 1

Electric Charge There are two kinds of charge: positive (+) and negative ( ) like charges repel unlike charges attract Charge is conserved The net amount of electric charge produced in any process is zero. Charge can be transferred from one place to another. Charge comes in packages (quantized) discrete amounts of smallest charge: electron Phys 2435: Chap 21, Pg 2

Electric Charge is Quantized Elementary charge: e = 1.602 x 10-19 C Any charge is an integer multiple of e. Q (proton) = e Q (electron) = -e Q (typical) has about 10 +12 of e. (seems continuous) Objects that carry a positive charge has a deficit of electrons Objects that carry a negative charge has an excess f electrons Most atoms and molecules are charge neutral. Q (lithium atom) = 0 Q (water molecule) = 0 Charged-atoms or molecules are called Ions. Unit: 1 Coulomb = 6.24 x 10 +18 e. Typical charge is µc = 10-6 C. Phys 2435: Chap 21, Pg 3

Types of Materials Insulators: charges cannot move freely glass, rubber, plastic Conductors: charges can move freely metals Semiconductors: : impurities alter electrical properties silicon, germanium Superconductors: : infinite conductivity at low temp. Material Conductivity silver 10 8 iron 10 7 germanium 10 0 silicon 10-3 rubber 10-13 Phys 2435: Chap 21, Pg 4

Charging by contact direct transfer Methods of Charging Charging by induction no contact Can happen to both conductors and insulators separation of charge is called polarization Phys 2435: Chap 21, Pg 5

ConcepTest 21.1(post) Electric Charge From the two separate tests, (1) have opposite charges what can you conclude about the charges? (2) have the same charge (3) all have the same charge (4) one ball must be neutral (no charge) Phys 2435: Chap 21, Pg 6

Coulomb s s Law New Topic Phys 2435: Chap 21, Pg 7

Coulomb s s Law Electric force is a field force (acts at a distance) F = k Q Q 1 r 2 2 k = 9 x 10 9 N m 2 /C 2 The unit for charge is Coulomb (C) The smallest charge: e = 1.6 x 10-19 C. Two 1-C charges separated by 1 m has Coulomb force of 9x10 9 N! Note similarity in form to gravitational force: Phys 2435: Chap 21, Pg 8

Coulomb s s Law: multiple charges If there are several charges, the net force on any one of them is the vector sum of the individual forces due to all the others. Superposition principle -q +q 1 +q 2 Phys 2435: Chap 21, Pg 9

ConcepTest 21.2(post) Coulomb s s Law Two balls with charges +Q and +4Q are fixed at a separation distance of 3R.. Is it possible to place another charged ball Q 0 on the line between the two charges such that the net force on Q 0 will be zero? (1) yes, but only if Q 0 is positive (2) yes, but only if Q 0 is negative (3) yes, independent of the sign (or value) of Q 0 (4) no, the net force can never be zero +Q +4Q 3R Phys 2435: Chap 21, Pg 10

ConcepTest 21.3(Post) Coulomb s s Law 1 2 3 Which of the arrows best represents the direction of the net force on charge +Q due to the other two charges? +2Q d +Q d 4 5 +4Q Phys 2435: Chap 21, Pg 11

Electric Field New Topic Phys 2435: Chap 21, Pg 12

The Concept of Electric Field Move around a small test charge and see what electric force it feels! Definition of the Electric Field: E = Since F is a vector, E is a vector field direction = direction of force on a small positive test charge F q 0 Phys 2435: Chap 21, Pg 13

Field Lines: visualizing E fields Lines start on positive charges and end on negative charges Number of lines leaving/entering amount of charge Tangent of line direction of E Density of lines magnitude of E Field lines never cross. Otherwise, there would be multiple field values at a given point, which is not physical. Phys 2435: Chap 21, Pg 14

Electric field of a point charge Coulomb s law: F = k Qq r 0 2 Q q 0 Electric field: E = k Q r 2 What about direction? +Q -Q Example: What is the electric field at a point which is 30 cm away from a point charge q=+3µc? Phys 2435: Chap 21, Pg 15

What about multiple point charges? Superposition principle The field at a given point is a vector sum of the electric field caused by each charge individually. E = E1 + E 2 + E 3 +L Example: electric dipole Point charges q 1 =+12nC and q 2 =-12nC are placed 10 cm apart. This combination of two charges with equal magnitude and opposite sign is called an electric dipole. Compute the electric field at points a, b, and c. Phys 2435: Chap 21, Pg 16

ConcepTest 21.4(post) Electric Fields Four equal charges sit at the for corners of a square. What is the electric field at the center of the square? 5) E = 0-2 C -2 C 2 1-2 C 3 4-2 C Phys 2435: Chap 21, Pg 17

ConcepTest 21.5.5(post) Electric Fields Two charges are fixed along the x-axis. They produce an electric field E directed along the negative y-axis at the indicated point. Which of the following is true? (1) charges are equal and positive (2) charges are equal and negative (3) charges are equal and opposite (4) charges are equal, but sign is undetermined (5) charges cannot be equal y E Q 1 Q 2 x Phys 2435: Chap 21, Pg 18