Chapter 20 Electric Forces and Fields: Coulomb’s...
Transcript of Chapter 20 Electric Forces and Fields: Coulomb’s...
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Chapter 20
Electric Forces and Fields: Coulomb’s Law
Reading: Chapter 20
1
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Electric Charges
There are two kinds of electric charges- Called positive and negative
Negative charges are the type possessed byNegative charges are the type possessed by electrons
Positive charges are the type possessed by protons
Charges of the same sign repel one another and charges with opposite signs attract one another
El i h i l d i i l dElectric charge is always conserved in isolated system
Neutral – equal number of positive and negative chargesand negative charges
P iti l h d
2
Positively charged
![Page 3: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/3.jpg)
Electric Charges: Conductors and Isolators
Electrical conductors are materials in which some of the electrons are free electrons
fThese electrons can move relatively freely through the material
Examples of good conductors include copper, aluminum and silver
Electrical insulators are materials in which all of the electrons are bound to atoms
These electrons can not move relatively freely through the materialthrough the material
Examples of good insulators include glass, rubber and wood
3Semiconductors are somewhere between
insulators and conductors
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Electric Charges
![Page 5: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/5.jpg)
Electric Charges
![Page 6: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/6.jpg)
Electric Charges
![Page 7: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/7.jpg)
Electric Charges
![Page 8: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/8.jpg)
Electric Charges
![Page 9: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/9.jpg)
Electric Charges
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Electric Charges
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Electric Charges
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Electric Charges
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Electric Charges
![Page 14: Chapter 20 Electric Forces and Fields: Coulomb’s Lawphysics.gsu.edu/apalkov/lecture1112_3.pdfCoulomb’s Law • Mathematically, the force between two electric charges: = 12 qq Fk](https://reader033.fdocuments.net/reader033/viewer/2022051508/5aa32f7b7f8b9aa0108e3ca9/html5/thumbnails/14.jpg)
Electric Charges
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Electric Charges
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Coulomb’s Law
• Mathematically, the force between two electric charges:
= 1 2q qF k
• The SI unit of charge is the coulomb (C)
=12 2eF kr
• ke is called the Coulomb constant– ke = 8.9875 x 109 N.m2/C2 = 1/(4πeo)
e is the permittivity of free space– eo is the permittivity of free space– eo = 8.8542 x 10-12 C2 / N.m2
Electric charge:Electric charge:electron e = -1.6 x 10-19 Cproton e = 1.6 x 10-19 C
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Coulomb’s Law
1 212 21 2
| || |e
q qF F kr
= =
21++
21
21F 12FDirection depends on the sign of the product
1 2q q 1 2 0q q >
21 12F F= − opposite directions, the same magnitude
−
1 2
1 2 0q q >−
21F 12F
1 2 0q q >
−+
1 2
0q q21F 12F
1 2 0q q <
The force is attractive if the charges are of opposite signThe force is repulsive if the charges are of like sign
17
The force is repulsive if the charges are of like sign
Magnitude: 1 212 21 2
| || |e
q qF F kr
= =
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Coulomb’s Law: Superposition Principle
• The force exerted by q1 on q3 is F13
• The force exerted by q2 on q3 is F23y q2 q3 23
• The resultant force exerted on q3 is the vector sum of F and Fsum of F13 and F23
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Coulomb’s Law
q q 5 6= 1 2
21 2eq qF kr
++
1 2 13F−
23F 33 21 31F F F= +
1 1q мC= 2 2q мC= −
5m 6m Resultant force:
3F1 1q мC 2 2q мC
3 3q мC=Magnitude:
6 6| || | 2 10 3 10
13F
23F
6 6| || | 10 3 10q q − −
6 69 43 2
23 2 2
| || | 2 10 3 108.9875 10 15 106e
q qF k N Nr
− −−⋅ ⋅ ⋅
= = ⋅ = ⋅
6 69 43 1
13 2 2
| || | 10 3 108.9875 10 2.2 1011e
q qF k N Nr
−⋅ ⋅= = ⋅ = ⋅
4 4 4(15 10 2 2 10 ) 12 8 10F F F N N− − −4 4 43 23 13 (15 10 2.2 10 ) 12.8 10F F F N N= − = ⋅ − ⋅ = ⋅
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Coulomb’s Law
q q 5 61 221 212
€e
q qF k rr
= ++
1 2 32F−
12F 32 12 32F F F= +
F1 1q мC= 2 2q мC= −
5m 6m
F
Resultant force:
2F1 1q мC 2 2q мC
3 3q мC=Magnitude:
6 6| || | 2 10 3 10
32F
12F
6 6| || | 10 2 10q q − −
6 69 43 2
32 2 2
| || | 2 10 3 108.9875 10 15 106e
q qF k N Nr
− −−⋅ ⋅ ⋅
= = ⋅ = ⋅
6 69 41 2
12 2 2
| || | 10 2 108.9875 10 7.2 105e
q qF k N Nr
−⋅ ⋅= = ⋅ = ⋅
4 4 4(15 10 7 2 10 ) 7 8 10F F F N N− − −4 4 42 32 12 (15 10 7.2 10 ) 7.8 10F F F N N= − = ⋅ − ⋅ = ⋅
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Coulomb’s Law
q q 5 61 221 212
€e
q qF k rr
= ++
1 221F−
31F 31 21 31F F F= +
F1 1q мC= 2 2q мC= −
5m 6m
F
Resultant force:
1F1 1q мC 2 2q мC
3 3q мC=Magnitude: 21F
31F
6 6| || | 10 3 10
6 6| || | 10 2 10q q − −
6 69 43 1
31 2 2
| || | 10 3 108.9875 10 2.2 1011e
q qF k N Nr
− −−⋅ ⋅
= = ⋅ = ⋅
6 69 41 2
21 2 2
| || | 10 2 108.9875 10 7.2 105e
q qF k N Nr
−⋅ ⋅= = ⋅ = ⋅
4 4 4(7 2 10 2 2 10 ) 5 10F F F N N− − −4 4 41 21 31 (7.2 10 2.2 10 ) 5 10F F F N N= − = ⋅ − ⋅ = ⋅
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Coulomb’s Law
q q= 1 2
21 2eq qF kr +
131F
21F1 21 31F F F= +
F F1 1q мC= 2 2q мC= −5m 6m
Resultant force:
+
2−
3
31F 21F
1F
1 1q мC 2 2q мC
3 3q мC= 7mMagnitude:ag tude
6 69 41 2
21 2 2
| || | 10 2 108.9875 10 5 106e
q qF k N Nr
− −−⋅ ⋅
= = ⋅ = ⋅
6 69 33 1
31 2 2
| || | 10 3 108.9875 10 1.1 105e
q qF k N Nr
− −−⋅ ⋅
= = ⋅ = ⋅
13F+
1
F
5m 6m
+
112F
5m6m
13F
23F3F
12F1F
32F
22
+
213F −
23F3 7m+
232F−
3 7m
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Conservation of Charge Electric charge is always conserved in isolated system
1 1q мC= 2q мC
g y yTwo identical sphere
1 1q мC2 2q мC= −
Th t d b d ti i Wh t i th l t iThey are connected by conducting wire. What is the electric charge of each sphere?
The same charge q. Then the g qconservation of charge means that :
1 2 1 2 0.52 2
q qq мC мC+ −= = = −1 22q q q= +
2 2
For three spheres: 1 1q мC= 2 2q мC= − 3 3q мC=
23
1 2 33q q q q= + +
1 2 3 1 2 3 13 3
q q qq мC мC+ + − += = =
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Chapter 20
El i Fi ldElectric Field
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Electric Field
An electric field is said to exist in the region of space around a charged object
This charged object is the source chargeThis charged object is the source chargeWhen another charged object, the test charge, enters this electric
field, an electric force acts on it.The electric field is defined as the electric force on the test charge
per unit chargeFE =
If you know the electric field you can find the force
0
Eq
=
If you know the electric field you can find the force
If i iti F d E i th di ti
F qE=
25
If q is positive, F and E are in the same directionIf q is negative, F and E are in opposite directions
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Electric Field
The direction of E is that of the force on a positive test chargeThe SI units of E are N/C
0
FEq
=
= 02e
qqF kr
Coulomb’s Law:
20
eF qE kq r
= =
Then
0q r
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Electric Field
q is positive, F is directed away from qfrom q
The direction of E is also away from the positive source chargep g
q is negative, F is directed toward qE is also toward the negative
source charge
= 02e
qqF kr 2
0e
F qE kq r
= =
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Electric Field: Superposition Principle
• At any point P, the total electric field due to a group of source charges equals the vector sum of electric g qfields of all the charges
= ∑ ii
E Ei
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Electric Field
5 6+
1 2 1E−
2E
Electric Field:
1 2E E E= +
1 1q мC= 2 2q мC= −
5m 6m2eqE kr
=
E E1 1q мC 2 2q мC
Magnitude:6| | 2 10
2E
1E E
6| | 10q −
69 22
2 2 2
| | 2 108.9875 10 / 5 10 /6e
qE k N C N Cr
−⋅= = ⋅ = ⋅
69 21
1 2 2
| | 108.9875 10 / 0.7 10 /11e
qE k N C N Cr
= = ⋅ = ⋅
2 2 22 2 22 1 (5 10 0.7 10 ) / 4.3 10 /E E E N C N C= − = ⋅ − ⋅ = ⋅
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Electric Field
1E
2E
Electric field
1 1q мC= 2 2q мC= −5m 6m
1 2E E E= +
EE
2eqE kr
=
+
1 2−
1 1q мC 2 2q мC
7m
2E1E
E
Magnitude:
69 22| | 2 108 9875 10 / 5 10 /qE k N C N C
−⋅
69 21| | 108 9875 10 / 0 37 10 /qE k N C N C
−
= = ⋅ = ⋅
9 222 2 2
| | 8.9875 10 / 5 10 /6e
qE k N C N Cr
= = ⋅ = ⋅
1 2 28.9875 10 / 0.37 10 /5eE k N C N C
r= = ⋅ = ⋅
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Electric Field
1 10q мC= 2 10q мC=
2eqE kr
= z
1 10q мC 2 10q мC
E Direction of electric field?
5m ϕ
+ +
5m5m
ϕ
1 26m
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Electric Field
Electric field
1 10q мC= 2 10q мC=1 2E E E= +
2eqE kr
=E
2E
ϕ1E2E
1 10q мC 2 10q мC
ϕ
ϕ
+ +
5m5m
ϕ
+
1 2+
6mMagnitude:
6| | 10 10q −69 32
2 1 2 2
| | 10 108.9875 10 / 3.6 10 /5e
qE E k N C N Cr
⋅= = = ⋅ = ⋅
2E E −2 25 3 4 8
32
= 12 cosφE E −= =
5 3 4cosφ5 5 1
85
E E=
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Example
1 10q мC= 2 10q мC=1l m=
2ϕ1l m=
T1ϕ
+
1 2+
EF Electric field
1 10q мC 2 10q мC
r1 2m m m= =
0ET mg F+ + =mg
g
1 22E e
q qF k
r=
T iT F2cosT mgϕ = 2sin ET Fϕ =
1 21 2tan E
eF q q
kmg r mg
ϕ = =1 22 2tan E
eF q q
kϕ = =
33
mg r mg2 2emg r mgϕ
2 1ϕ ϕ=
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0planeE
eσ=2πk σ=
2εplaneE
0Q >
σ>0
planeE
02ε
Q=σAplaneE
σ<0planeE= e
0
|σ|2πk |σ|=2εplaneE
< 0Q
σ<0
planeE Q=σA
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Fi d l t i fi ld
Important Example
Find electric field σ>0
+ + + + ++ + + + +
+
-σ<0− − − − −
− − − − −−
σ>0E−E+
−σ<0
+ =σ
2εE
E+ E−− =
σ2ε
E
35
02ε 02ε
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Fi d l t i fi ld
Important Example
σ>0+ + + + +Find electric field σ>0
−σ<0
+ + + + ++ + + + +
+
− − − − −+ =σ
2E − =
σ2
E σ<0− − − − − −
+02ε 02ε
E E E= +
σ>0E−E+
E E E+ −= +
0E E E+ −= − =
−σ<0E−E+ + −= + =
0
σε
E E E
E+E−
0E E E+ −= − =
36
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Important Example
0у >+ + + + + 0у >
0у− <
+ + + + ++ + + + +
+
− − − − − 0у <− − − − − −
σ>00E =
E= =0 0
σε ε
QEA
−σ<00E =
37
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Electric field due to a thin uniformly charged spherical shell
• When r < a, electric field is ZERO: E = 0
1A∆ 1 1q Aσ∆ = ∆ 2 2q Aσ∆ = ∆
2A∆ ∆Ω 2A∆ ∆Ω1r
the same
21 1A r∆ = ∆Ω 2
2 2A r∆ = ∆Ω
2E∆ 21 1 1
1 2 2 2e e e eq A r
E k k k kr r r
σ σσ
∆ ∆ ∆Ω∆ = = = = ∆Ωthe same
solid angle1E∆
1 1 1r r r
22 2 2
2 2 2 2e e e eq A r
E k k k kr r r
σ σσ
∆ ∆ ∆Ω∆ = = = = ∆Ω
2r2 2 2r r r
1 2E E∆ = ∆
1 2 0E E∆ + ∆ =
382A∆ 2
1Er
∝Only because in Coulomb law
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M i f Ch d P i lMotion of Charged Particle
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Motion of Charged Particle
• When a charged particle is placed in an electric field, it experiences an electrical force
• If this is the only force on the particle it must be the net force• If this is the only force on the particle, it must be the net force• The net force will cause the particle to accelerate according to
Newton’s second law
F qE= - Coulomb’s law
F ma= - Newton’s second law
qa Em
=
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Motion of Charged Particle
What is the final velocity?
F qE= - Coulomb’s lawq
F ma= - Newton’s second law
| |q fv| |y
qa Em
= −
vMotion in x with constant velocity
l
Motion in x – with constant acceleration 0v | |
yqa Em
= −Motion in x – with constant velocity
0
ltv
= - travel time
After time t the velocity in y direction becomes0xv v=
41| |
y yqv a t Etm
= = −fvyvthen
220f
qv v Etm
= +
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Chapter 20
C d t i El t i Fi ldConductors in Electric Field
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Electric Charges: Conductors and Isolators
Electrical conductors are materials in which some of the electrons are free electrons
fThese electrons can move relatively freely through the material
Examples of good conductors include copper, aluminum and silver
Electrical insulators are materials in which all of the electrons are bound to atoms
These electrons can not move relatively freely through the materialthrough the material
Examples of good insulators include glass, rubber and wood
43Semiconductors are somewhere between
insulators and conductors
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Electrostatic Equilibrium
Definition:when there is no net motion of charges within a conductor, the conductor is said to be in electrostatic equilibrium
Because the electrons can move freely through the material F qE
no motion means that there are no electric forcesno electric forces means that the electric field
inside the conductor is 0
F qE=
inside the conductor is 0
If electric field inside the conductor is not 0, then0E ≠
44
If electric field inside the conductor is not 0, then there is an electric force and, from the second Newton’s law, there is a motion of free electrons.
0E ≠F qE=
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Conductor in Electrostatic Equilibrium
• The electric field is zero everywhere inside the conductor
• Before the external field is applied, free electrons are distributedfree electrons are distributed throughout the conductor
• When the external field is applied, the l t di t ib t til thelectrons redistribute until the
magnitude of the internal field equals the magnitude of the external field
• There is a net field of zero inside the conductor
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Conductor in Electrostatic Equilibrium
• If an isolated conductor carries a charge, the charge resides on its surface
0E =
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