1. Electric Charge and Electric Field

2. Static Electricity; Electric Charge and Its Conservation
Electric charge is conserved – the arithmetic sum of the total charge cannot change in any interaction.

3. Electric Charge in the Atom
Nucleus (small, massive, positive charge)
Electron cloud (large, very low density, negative charge)

5. Electrons, Protons and Neutrons
Basic ingredients of matter:
electrons
qe = × Coulombs (more later)
protons
qP = × Coulombs
neutrons
qN = 0
Sign of qe is
just a convention
- a bit unfortunate
for some later
formulas
|qe| = |qP| to one part in or else galaxies blow up!
|Charge is conserved: the net sum of charge
in any closed system is constant

6. Basic Properties of Electric Charges
Benjamin Franklin and others
Charge comes in two types, arbitrarily called “positive” and “negative”.
Ordinary matter is “full of charge” (electrons and protons), but has nearly the same amount of positive and negative charge – it is nearly “neutral” (having no net charge)

7. Static Electricity; Electric Charge and Its Conservation
Objects can be charged by friction

8. Electric Charge in the Atom
Atom is electrically neutral.
Rubbing charges objects by moving electrons from one to the other.

9.                                                                                                                                                       As
As mentioned, different materials have different affinities for electrons. By rubbing a variety of materials against each other and testing their resulting interaction with objects of known charge, the tested materials can be ordered according to their affinity for electrons. Such an ordering of substances is known as a triboelectric series. One such ordering for several materials is shown in the table at the right. Materials shown highest on the table tend to have a greater affinity for electrons than those below it. Subsequently, when any two materials in the table are rubbed together, the one that is higher can be expected to pull electrons from the material that is lower. As such, the materials highest on the table will have the greatest tendency to acquire the negative charge. Those below it would become positively charged.

10. Static Electricity; Electric Charge and Its Conservation
Charge comes in two types, positive and negative; like charges repel and opposite charges attract

11. Positively Charged Negatively Charged Uncharged
Charged versus Uncharged Particles
Positively Charged
Negatively Charged
Uncharged
Possesses more protons than electrons
Possesses more electrons than protons
Equal numbers of protons and electrons

12. Insulators and Conductors Some materials are semiconductors.
Charge flows freely
Metals
Insulator:
Almost no charge flows
Most other materials
Some materials are semiconductors.

13. Insulators: The electrons are bound to the atoms
Insulators: The electrons are bound to the atoms. The electrons cannot move.
Conductors: The electrons are free to
move within a conductor. In an isolated atom the electrons are bound to a nucleus. In a conductor the electrons form a fluid. At any interior point in the conductor, the charge density is zero.

14. Semi-Conductor: The electrons are bound until the electric field is strong enough to pull the electrons away. In a semiconductor, the electrons are loosely bound to the atoms. By adding impurities to a semiconductor it possible to make it act like a conductor or an insulator. In semi-conductors, the mobile charges may be positive!

15. Charge Distribution
Excess charge on the surface of a metal of uniform curvature spreads out.
Charge on insulating materials
doesn't move easily
Excess charge on a metal accumulates at points. Lightning, lightning rods.

16. The transfer of charge between objects occurs more readily if the second object is made of a conducting material. Conductors allow for charge transfer through the free movement of electrons

17. Induced Charge; the Electroscope
Metal objects can be charged by conduction:

18. Induced Charge; the Electroscope
They can also be charged by induction:

19. Nonconductors won’t become charged by conduction or induction, but will experience charge separation:

20. Polarization

21. positive or neutral
negative
positive
positive

22. Electric Charge in the Atom
Polar molecule: neutral overall, but charge not evenly distributed

25. attract b. repel c. not affect
Two objects are shown below. One is neutral and the other is negative. Object X will ____ object Y.
attract
b. repel
c. not affect

26. Induced Charge; the Electroscope
The electroscope can be used for detecting charge:

27. Induced Charge; the Electroscope
The electroscope can be charged either by conduction or by induction.

29. Induced Charge; the Electroscope
The charged electroscope can then be used to determine the sign of an unknown charge.

30. 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 square of the distance between them.

31. Coulomb’s Law Coulomb’s law:
This equation gives the magnitude of the force.

32. 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.

33. 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:

34. Coulomb’s Law Charge on the electron:
Electric charge is quantized in units of the electron charge.

35. Coulomb’s Law
The proportionality constant k can also be written in terms of , the permittivity of free space:

36. Charges A and B exert repulsive forces on each other. qA = 4qB
Charges A and B exert repulsive forces on each other. qA = 4qB. Which statement is true?
STT25.4
1. FA on B > FB on A
2. FA on B < FB on A
3. FA on B = FB on A

37. How many electrons make up a charge of
What is the repulsive electrical force
between two protons 5 fermi apart from
each other in an atomic nucleus?

38. Note, the form of the equation is similar to the Law of Universal Gravitation

39. Compare the electric force holding the electron in orbit around the proton nucleus of the hydrogen atom, with the gravitational force between the same electron and proton. What is the ratio of these two forces?

40. Coulomb’s Law Coulomb’s law strictly applies only to point charges.
Superposition: for multiple point charges, the forces on each charge from every other charge can be calculated and then added as vectors.

41. Solving Problems Involving Coulomb’s Law and Vectors
The net force on a charge is the vector sum of all the forces acting on it.

42. Solving Problems Involving Coulomb’s Law and Vectors
Vector addition review:

43. The Electric Field
The electric field is the force on a small charge, divided by the charge:

44. The Electric Field
For a point charge:

45. Charge Q from a source with charge acts as a point charge to create an electric field. Its strength, measured a distance of 30 cm away, is 40 N/C. What would be the electric field strength ...
a. 30 cm away 2Q?
b. 30 cm away from a source with charge 3Q?
c. 60 cm away from a source with charge 2Q?
a) 80 N/C
b) 120 N/C
c) 20 N/C

46. z -Q y x Q Opposite charges of equal magnitude Q, -Q are fixed on the
x-axis at x = +1 m and x = -1 m. A third charge q will
experience no net force due to these two charges if it is placed
1. anywhere on the x-axis between the two other charges
2. anywhere on the x-axis, not between the two other charges
3. only at the origin
4. anywhere on the plane x = 0
5. nowhere – there is no place where the force on q is zero z -Q y x Q

47. On the line in which region,  A, B, or C,
may a point be found at which the net force  on a positive test charge q would be zero?  F = kq1q2 / r2

48. The Electric Field Force on a point charge in an electric field:
Superposition principle for electric fields:

49. The Electric Field
Problem solving in electrostatics: electric forces and electric fields
Draw a diagram; show all charges, with signs, and electric fields and forces with directions
Calculate forces using Coulomb’s law
Add forces vectorially to get result

50. Field Lines
The electric field can be represented by field lines. These lines start on a positive charge and end on a negative charge.

51. Field Lines
The number of field lines starting (ending) on a positive (negative) charge is proportional to the magnitude of the charge.
The electric field is stronger where the field lines are closer together.

52. Example of a “Field”
The electric field is our first example of a vector field.
A vector field consists of an infinite set of vectors, one vector for every point in space.
We can only draw some of them, like this:

53. F = qE The electric field of a POSITIVE POINT CHARGE looks like this:
The large red dot at the center is the charge PRODUCING THE FIELD,
E = (keQ / r 2) r
The small dots are TEST CHARGES: POSITIVE test charge (upper left) feels force ALONG THE FIELD.
NEGATIVE test charge (lower left) feels force OPPOSITE THE FIELD.

54. F = qE The electric field of a NEGATIVE POINT CHARGE looks like this:
The large blue dot at the center is the charge PRODUCING THE FIELD,
E = (keQ / r 2) r
The small dots are TEST CHARGES: POSITIVE test charge (upper left) feels force ALONG THE FIELD.
NEGATIVE test charge (lower left) feels force OPPOSITE THE FIELD

56. Field Lines
Electric dipole: two equal charges, opposite in sign:

57. Suppose that there are two positive charges - charge A (QA) and charge B (QB) - in a given region of space. Each charge creates its own electric field.
Since electric field is a vector, the usual operations which apply to vectors can be applied to electric field. That is, they can be added in head-to-tail fashion to determine the resultant or net electric field vector at each location

61. F = qE
An electron is observed to travel in a circular orbit, in the plane of the page. This could be caused by
1. an electric field pointing out of the page
2. an electric field pointing into the page
3. an electric field that points towards the center of the orbit
4. an electric field that points away from the center of the orbit
5. no electric field could cause this

62. At the position of the black dot, the electric field points
1. Left.
2. Down.
3. Right.
4. Up.
5. The electric field is zero.
STT26.1

63. Field Lines
The electric field between two closely spaced, oppositely charged parallel plates is constant.

64. Field Lines Summary of field lines:
Field lines indicate the direction of the field; the field is tangent to the line.
The magnitude of the field is proportional to the density of the lines.
Field lines start on positive charges and end on negative charges; the number is proportional to the magnitude of the charge.

65. Rank in order, from largest to smallest, the electric field strengths E1 to E4 at points 1 to 4.
1. E2 > E4 > E1 > E3
2. E2 > E1 = E4 > E3
3. E2 > E1 > E4 > E3
4. E1 = E2 > E3 = E4
5. E1 > E2 > E3 > E4
STT25.6

66. 4. There’s not enough information to tell.
An electron is placed at the position marked by the dot. The force on the electron is
1. to the left.
2. to the right.
3. zero.
4. There’s not enough information to tell.
STT25.5

67. Electric Fields and Conductors
The static electric field inside a conductor is zero – if it were not, the charges would move.
The net charge on a conductor is on its surface.

68. Electric Fields and Conductors
The electric field is perpendicular to the surface of a conductor – again, if it were not, charges would move.

70. Flux of the Electric Field
If a uniform field E is perpendicular to the surface (area A), the flux through that surface is ΦE = EA
Flux is the number of
field lines penetrating
the surface
Note:
 Units are (N/C)m2 = N-m2/C

71. field lines penetrating
If E is not perpendicular to the surface,
ΦE = EA cosθ
where θ is the angle between E and the normal to the surface.
Flux is the number of
field lines penetrating
the surface

72. Gauss’s Law Electric flux:
Electric flux through an area is proportional to the total number of field lines crossing the area.

73. Gauss’s Law
Flux through a closed surface:

74. Gauss’s Law
The net number of field lines through the surface is proportional to the charge enclosed, and also to the flux, giving Gauss’s law:
This can be used to find the electric field in situations with a high degree of symmetry.

75. Gauss’s Law
The flux ΦE that comes out through any closed surface is related to the charge Q enclosed by the surface by
ΦE = Qenc/0 .
Any closed surface (real or imaginary) can be used.

76. Four different closed  three
dimensional surfaces are
indicated by broken lines.
Flux through S1 is positive.
Flux through S4 is negative.
What are the fluxes through
S2 and S3?

77. Gauss’s Law
A solid metal sphere of radius 3.00 m carries a total charge 3.5μC of What is the magnitude of the electric field at a distance from the sphere’s center of (a) 0.15 m, (b) 2.90 m, (c) 3.10 m, and (d) 6.00 m?

78. (a) Inside a solid metal sphere the electric field is 0.
(c,d) Outside a solid metal sphere the electric field is the same as if all the charge were concentrated at the center as a point charge.

79. A point charge is at the center of two concentric imaginary spheres, one of radius R and one of radius 2R. The ratio of electric flux ΦE through the larger sphere to that through the smaller sphere is
1. 1/4
2. 1/2
3. 1
4. 2
5. 4

80. 1. Φa > Φc > Φb > Φd > Φe 2. Φb = Φe > Φa = Φc = Φd
These are two-dimensional cross sections through three-dimensional closed spheres and a cube. Rank order, from largest to smallest, the electric fluxes a to e through surfaces a to e.
STT27.4
1. Φa > Φc > Φb > Φd > Φe
2. Φb = Φe > Φa = Φc = Φd
3. Φe > Φd > Φb > Φc > Φa
4. Φb > Φa > Φc > Φe > Φd
5. Φd = Φe > Φc > Φa = Φb

81. A point charge q is placed at the center of a cube. The flux 1. q/o
ΦE = Qenc/0
A point charge q is placed at the center of a cube. The flux
ΦE through the top face of the cube is
1. q/o
2. q/4πo
3. q/4o
4. q/6o
5. cannot be determined from information given
6. Not Brett.

82. A point is placed at the center of a spherical Gaussian surface..
The flux ΦE is changed
1. if the sphere is replaced by a cube of the same volume
2. if the sphere is replaced by a cube of one-tenth the volume
3. if the point charge is moved off center (but still inside the original sphere
4. if the point charge is moved to just outside the sphere
5. if a second point charge is placed just outside the sphere.

83. Electric Forces in Molecular Biology: DNA Structure and Replication
Molecular biology is the study of the structure and functioning of the living cell at the molecular level.
The DNA molecule is a double helix:

84. Electric Forces in Molecular Biology: DNA Structure and Replication
The A-T and G-C nucleotide bases attract each other through electrostatic forces.

85. Electric Forces in Molecular Biology: DNA Structure and Replication
Replication: DNA is in a “soup” of A, C, G, and T in the cell. During random collisions, A and T will be attracted to each other, as will G and C; other combinations will not.

87. Photocopy Machines and Computer Printers Use Electrostatics
drum is charged positively
image is focused on drum
only black areas stay charged and therefore attract toner particles
image is transferred to paper and sealed by heat

88. Photocopy Machines and Computer Printers Use Electrostatics

89. Photocopy Machines and Computer Printers Use Electrostatics
Laser printer is similar, except a computer controls the laser intensity to form the image on the drum

90. Summary of Chapter
Two kinds of electric charge – positive and negative
Charge is conserved
Charge on electron:
Conductors: electrons free to move
Insulators: nonconductors

91. Summary Charge is quantized in units of e
Objects can be charged by conduction or induction
Coulomb’s law:
Electric field is force per unit charge:

92. Summary Electric field of a point charge:
Electric field can be represented by electric field lines
Static electric field inside conductor is zero; surface field is perpendicular to surface
Electric flux:
Gauss’s law:

93. Internet Archive: Details: Physics B Lesson 30: Electric Charges and Coulomb's Law
Internet Archive: Details: Physics B Lesson 31: Electric Fields
Internet Archive: Details: Physics B Lesson 32: Electric Potential
Internet Archive: Details: Physics B Lesson 33: Electrostatics with Conductors