lecture 6-1 thin sheet of any charge distribution just to left of disk just to right of disk tiny...
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Lecture 6-Lecture 6-11
Thin sheet of any charge distribution
'R diskE E E ������������������������������������������
'L diskE E E ������������������������������������������
Just to left of disk
Just to right of disk
0 0
0
( ' )
( ' )
2 2
disk
disk
disk disk
E E E
E E
E E
n
n
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tiny disk
0nE
Lecture 6-Lecture 6-22
Charges and fields of a conductor
• In electrostatic equilibrium, charges inside a conductor do not move. Thus, E = 0 everywhere in the interior of a conductor.
• Since E = 0 inside, there are no net charges anywhere in the interior. Net charges can only be on the surface(s).
The electric field must be perpendicular to the surface just outside a conductor, since, otherwise, there would be currents flowing along the surface.
0
Lecture 6-Lecture 6-33Electrostatic Shielding (Continued)
+++
+
+
+
Add Q’ If you now add charge Q’ to the conductor and/or Q’’ on the outside of the conductor, the interior electric fields do not change.
Q’’
If you move charge q in the cavity, the exterior electric fields and the extreior charge distribution are not affected.
Conducting shell electrostatically shields its exterior from changes on the inside.
q
Conducting shell electrostatically shields its interior from changes on the outside, too.
Lecture 6-Lecture 6-44
READING QUIZ 1
IN WHAT DIRECTION CAN YOU MOVE A TEST CHARGE RELATIVE TO AN ELECTRIC FIELD SO THAT THE ELECTRIC POTENTIAL DOES NOT CHANGE?
A| Move in the direction of the electric field lines.
B| Move opposite to the direction of the electric field lines.
C| Move from point A in the electric field to point B in
in the electric field along an arbitrary path.
D| Move relative to the electric field along a path which is
everywhere perpendicular to the electric field.
Lecture 6-Lecture 6-55
Electric Potential Energy of a Charge in Electric Field
• Coulomb force is conservative => Work done by the Coulomb force is path independent.
• Can associate potential energy to charge q0 at any point r in space. ( )U r
It’s energy! A scalar measured in J (Joules)
d l
ldEqdW 0
ldEqdWdU 0
Lecture 6-Lecture 6-66Electric Potential Energy of a Charge (continued)
i is “the” reference point. Choice of reference point (or point of zero potential energy) is arbitrary.
0
d l
i is often chosen to be infinitely far ( )
ldEqdW 0
ldEqdWdU 0
0
( ) ( )r
i
U U r U i
q E dl
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r
ildEq0
Lecture 6-Lecture 6-77
Gravitational vs Electrostatic Potential Energy
( ) ( )b
a
U U b U a
dF l
a
b
qE��������������
mg��������������
Gravity Coulomb
mg l qE l
Work done by gravity or the Coulomb force decreases the potential energy.
(if g, E uniform)
b
aldF
Lecture 6-Lecture 6-88Potential Energy in the Field due to a Point Charge q
0
02
02
0 0
( )P
P
r
r
U r q E dl
q qk r dl
l
q qk dl
l
q q q qk k
l r
����������������������������
From ∞
This is also called the potential energy of the two-charge configuration of q and q0.
What is the work required to bring q0 in from infinity?
P
ldEq0
Lecture 6-Lecture 6-99Potential Energy of a Multiple-Charge Configuration
(a)
(b)
(c)
1 2 /kq q d
1 31 32 2
2
q q qq qk k k
dd
q
d
2 3
1 3 3 41 2 2 4
1 4
2 2
q q q qq q q qk k k k
d dq q q q
k k
d
d d
d
Lecture 6-Lecture 6-1010Physics 241 –Warm-up quiz
Three point charges carry the same charge -q. Which of the following statements is true? Select one of (a) – (e).
A. An electron would have a higher potential energy at point A than at point B
B. A proton would have a higher potential energy at point A than at point B
C. An electron would have a lower potential energy at point A than at point B
D. The potential energy is the same for an electron and a proton at point A.
E. The potential energy is the same for a proton at point A and point B.
A B-q-q
-q
Lecture 6-Lecture 6-1111Electric Potential
• So U(r)/q0 is independent of q0, allowing us to introduce electric potential V independent of q0.
0
( )( )
U rV r
q
• [Electric potential] = [energy]/[charge] SI units: J/C = V (volts)
• U(r) of a test charge q0 in electric field generated by other source charges is proportional to q0 .
0
( )( )
U rV r
q
taking the same
reference point
Potential energy difference when 1 C of charge is moved between points of potential difference 1 V1 J
Scalar!
Lecture 6-Lecture 6-1212
Potential at P due to a point charge q
0
0
( )( ) qU r
V rq
qk
r
From ∞
Lecture 6-Lecture 6-1313
Electron Volt
• V=U/q is measured in volts => 1 V (volt) = 1 J / 1 C
J N mV E m V
C CN V
EC m
19
1 1 1
1 | | 1 1.602 10 1
J C V
eV e V C V
• V depends on an arbitrary choice of the reference point.
• V is independent of a test charge with which to measure it.
(electron volt)
POTENTIAL DIFFERENCES V2 – V1
Lecture 6-Lecture 6-1414
DOCCAM 2
Lecture 6-Lecture 6-1515
Potential due to two (source) charges
1 2( )| | | |
q qV x k k
x x a
1 2 0q q
Lecture 6-Lecture 6-1616
Potential due to Multiple Source Charges: Example
1 2 3 4
( )
/ 2
V P
q q q qk
d
Dotted line is an equipotential when
q1=12nC, q2= -24nC, q3=31nC, q4=17nC
E from V
x
VE
x
y
VE
y
z
VE
z
Expressed as a vector, E is the negative gradient of V
VE
We can obtain the electric field E from the potential V by inverting the integral that computes V from E:
r
zyx
r
dzEdyEdxEldErV )()(
Lecture 6-Lecture 6-1818
Lightning
E = 3 x 106 N/C
at electrical breakdown of air
ΔV on the order of 109 V
http://micro.magnet.fsu.edu/electromag/java/lightning/index.html
Lecture 6-Lecture 6-1919
DOCCAM 2
Examples (only a Preview)
Point charge Q: ( )Q
V r kr
2
( )Q V
E r k r rr r
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Charged disk: ( ) ??V z 2 2
0
( ) (1 )2
V zE z z z
z z R
��������������
( )Q
V r kr
2( )
QE r k r
r
��������������
Uniformly charged sphere:
r > R
r < R2
20
1( ) 3
4 2
Q rV r
R R
30
1( )
4
QrE r r
R
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Charged sheet:0
( ) sgn( )2
E z z z
�������������� ( ) ??V z
Charged line: ( ) ??V z 0
( )2
E r rr
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Lecture 6-Lecture 6-2121Physics 241 – 10:30 Quiz 3
A spherical shell is uniformly charged with a positive charge density σ. Which of the following statements is (are) true? Select one of (a) – (e).
1. An electron would have a higher potential energy at point A than at point B
2. A proton would have a higher potential energy at point A than at point B
3. The electric potential is lower at A than at B 4. The electric potential is higher at A than at B
A B
a) 1 and 3 onlyb) 1 and 4 onlyc) 2 and 3 onlyd) 2 and 4 onlye) None of them
σ
Lecture 6-Lecture 6-2222Physics 241 – 11:30 Quiz 3
A sphere is uniformly charged with a negative surface charge density. Which of the following statements is (are) true? Select one of (a) – (e).
1. A proton would have a higher potential energy at point A than at point B
2. An electron would have a higher potential energy at point A than at point B
3. The electric potential is lower at A than at B 4. The electric potential is higher at A than at B
A B
a) 1 and 3 onlyb) 1 and 4 onlyc) 2 and 3 onlyd) 2 and 4 onlye) None of them
-σ