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Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator: charges relatively fixed Charge is conserved in an isolated system – you can transfer charge, but not create or destroy charge The MKS unit of charge is 1 Coulomb Charge is quantized: e = 1.6 x 10 -19 Coulombs. Typically there are around 10 13 excess or deficient charges on a body – 10 13 /10 23 or 1 part in 10 10 23.1 Properties of Electric Charges
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Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Dec 20, 2015

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Page 1: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Chapter 23 Electric Fields

• Two kinds + and –• Charge is a scalar• Like charges repel and unlike attract• Conductor: charges relatively free to move• Insulator: charges relatively fixed• Charge is conserved in an isolated system – you can

transfer charge, but not create or destroy charge• The MKS unit of charge is 1 Coulomb• Charge is quantized: e = 1.6 x 10-19 Coulombs.

Typically there are around 1013 excess or deficient charges on a body – 1013/1023 or 1 part in 1010

23.1 Properties of Electric Charges

Page 2: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

23.2 Induced Charges

Page 3: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

CT1: Two uniformly charged spheres are firmly fastened to and electrically insulated from frictionless pucks on an air table. The charge on sphere 2 is three times the charge on sphere 1. Which force diagram correctly shows the magnitude and direction of the electrostatic forces:

A.

B.

C.

D.

E.

F.

G. None of these.

Page 4: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

23.3 Coulomb’s Law

F12 = keq1q2/r2 r

ke = 8.99 x 109 Nm2/C2

^

Page 5: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

CT2: P23.5 A hydrogen atom is composed of a nucleuscontaining a single proton, about which asingle electron orbits. The electric force between the two particles is 2.3 x 1039 greater than the gravitational force! If we can adjust the distance between the two particles, can we find a separation at which the electric and gravitational forces are equal?

A. Yes, we must move the particles farther apart.

B. Yes, we must move the particles closer together.

C. No, not at any distance

Page 6: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Chapter 23 Electric Fields

Superposition

The effect of several electrical forces acting on a charge due to several other charges is the vector sum of the individual forces from each charge as if the remaining charges weren’t present.

F1 = F21 + F31 + F41 + F51 + F61 + F71 + …..

23.3 Coulomb’s Law

Page 7: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

P23.5 (p.666)

P23.8 (p.667)

Page 8: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

CT3: P23.8 Which statement is true?A. The charged bead is in stable

equilibrium only if the charge is positive.

B. The charged bead is in stable equilibrium only if the charge is negative.

C. The charged bead is in stable equilibrium if the charge is either positive or negative.

D. The charged bead is in never in stable equilibrium.

Page 9: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

I. Definition

Coulomb Force:

Electric Field:

E = lim F/q0 q0 is a positive

q0 0 test charge

Ch23.4 The Electric Field

Chapter 23: Electric Fields

charge1 charge2

charge1 charge2electric

field

Page 10: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

II. Calculation of E

A. Point Charge

B. Discrete Distribution of Point Charges

Discrete sum – superposition (P 23.17 and P23.18)

Note: E depends only on the source charge(s)

Ch23.4 The Electric Field

Chapter 23: Electric Fields

Page 11: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

CT4: P23.18For very large x

A. The dipole field is stronger than the monopole (single charge) field.

B. The dipole field is weaker than the monopole field.

C. The dipole field is equal to the monopole field.

Page 12: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Continuous Distribution (P23.27)

∫Uniform volume charge density = q/V and dq = dV

Uniform surface charge density = q/A and dq = dA

Uniform linear charge density = q/l and dq = dl

Note: E depends only on the source charge distribution

Ch23.5 Electric Field of a Continuous Charge Distribution

Page 13: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

dl = rd

dq = dl

r

dEx

dE

Ch23.27

Page 14: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Ch23.6 Electric

Field Lines

• Electric field lines give a visualization of the electric force field

• The field points along the line in the direction of the arrow

• Field lines leave + charges and end on – charges

• The number of lines is proportional to the source charge, so the density of lines is proportional to field strength

Page 15: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Isolated Positive Point Charge

Ch23.6 Electric Field Lines

Page 16: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Isolated Negative Point Charge

Page 17: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Isolated Positive and

Negative Point Charges Compared

Page 18: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Two Isolated and Separated Equal Positive Point Charges

Page 19: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Isolated and Separated Equal Positive and Negative

Point Charges – Electric Dipole

Page 20: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Two Parallel Oppositely, but Equally, Charged Plates - Capacitor

Page 21: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Electric Field Lines – Two Isolated Separated Charges of Opposite Sign and Different Magnitudes

Page 22: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

P23.40 a) What is the ratio q2/q1? b) Signs of q1 and q2?

CT23.5

• 1

• 2

• 3

• 4

CT23.6

A. +,+

B. +,-

C. -,+

D.-,-

Page 23: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:
Page 24: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

Ch23.7 Motion of Charged Particles in a Uniform Electric Field

Squeak Demo

Do P23.41

Page 25: Chapter 23 Electric Fields Two kinds + and – Charge is a scalar Like charges repel and unlike attract Conductor: charges relatively free to move Insulator:

The coin doesn’t have to be charged for the cup to attract the coin. The charged cup can induce a polarization of the charge which results in an attraction. Common misconceptions - Charged objects only interact with other charged objects. Charged objects do not interact with uncharged (neutral) objects. Uncharged (neutral) is considered to be a third type of charge. Charged and uncharged objects attract each other because they are opposites. Correct answer