lecture 3-1 electric field define electric field, which is independent of the test charge, q, and...
TRANSCRIPT
![Page 1: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/1.jpg)
Lecture 3-1
Electric Field
Define electric field, which is independent of the test charge, q, and depends only on position in space:
FE
q��������������
��������������
dipole
• One is > 0, the other < 0
-q q
electric dipole of dipole moment:
p q d����������������������������
d��������������
- +
![Page 2: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/2.jpg)
Lecture 3-2
Dipole in uniform electric fields
• No net force. The electrostatic forces on the constituent point charges are of the same magnitude but along opposite directions. So, there is no net force on the dipole and thus its center of mass should not accelerate.
• Net torque! There is clearly a net torque acting on the dipole with respect to its center of mass, since the forces are not aligned.
http://qbx6.ltu.edu/s_schneider/physlets/main/dipole_torque.shtml
Ep
![Page 3: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/3.jpg)
Lecture 3-3
Electric Field from Coulomb’s Law
20
1ˆ
4i
ii i
qE r
r
++
+ +
+
--
-+-
-
Bunch of Charges
dV
dq dA
dL
(volume charge)
(surface charge)
(line charge)
Continuous Charge Distribution
dq2
0
1ˆ
4
dqE r d E
r
��������������P
r
Summation over discrete charges
Integral over continuous charge distribution
Pir
iq
k
http://www.falstad.com/vector3de/
![Page 4: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/4.jpg)
Lecture 3-4
Reading Quiz 1
Which one of the following statements is incorrect ?
• A) Electric fields leave positive charges and end on negative charges
• B) Electric field lines can intersect at some points in space.
• C) Electric field field lines from a dipole fall off faster than 1/r2.
• D) Electric fields describe a conservative force field.
![Page 5: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/5.jpg)
Lecture 3-5
SUMMARY: FIND THE ELECTRIC FIELD
GIVEN THE CHARGES
1) GEOMETRY FOR qi or dqi
2) DISCRETE CHARGES q i
3) CONTINUOUS CHARGES dqi
line charge density λ (x)
surface charge density σ (x.y)
volume charge density ρ (x,y,z)
Geometry may suggest other coordinate systems, R,θ,Φ or R,θ,Z
![Page 6: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/6.jpg)
Lecture 3-6
Continuous Charge Distribution 1 Charged Line
At a point P on axis:
Q
L
/ 2px LEx = k λ (1/r1 – 1/r2 ) ( Eqn 22-2a)
Ex = k λ (1/( XP – L/2 ) - 1/( XP + L/2 )
Ex = k ( Q/L) L [ XP2 – (L/2)2 ] -1
For XP2 >> (L/2)2 Ex = k Q / XP
2
For XP = 0 Ex = 0
![Page 7: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/7.jpg)
Lecture 3-7
Again: Continuous Charge Distribution 1: Charged Line
At a point P on perpendicular axis:
/ 2
2 2/ 2
/ 2
2 2 3/ 2/ 2
2 2
2 2 2 3/ 2
cos
tan( )
sec
( tan )
cos (2sin )
/ 2 2 /
L
y L
L
L
dxE E k
x y
yk dx x y
x y
yk d
y y
k
L and E k y
kd
y y
1 2
x
2 2
1 1
2
1
2 2 2 3/ 2
2
2 12 3/ 2
cos( )
secsin sin tan
(tan 1)
x x
y x x
dx yE k k dx
r x y
k kd x y
y y
![Page 8: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/8.jpg)
Lecture 3-8Physics 241 –Warm-up quiz 2
The rod is uniformly charged with a positive charge density . What is the direction of the electric field at a point P on a line perpendicular to the rod? Note that the line and the rod are in the same plane.
a) to the right b) to the leftc upd) downe) lower right
p
![Page 9: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/9.jpg)
Lecture 3-9General location of P: Charged Line
2 2
1 1
2
1
2 2 2 3/ 2
2 12 2 1/ 2
2 1
sin( )
1 cos cos
( )
cos cos
x x
x x x
x
x
dx xE k k dx
r x y
k kx y y y
k
y
2 2
1 1
2
1
2 2 2 3/ 2
2
2 12 3/ 2
cos( )
secsin sin tan
(tan 1)
x x
y x x
dx yE k k dx
r x y
k kd x y
y y
At a point P off axis:
![Page 10: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/10.jpg)
Lecture 3-10
Continuous Charge Distribution 2: Charged Ring
Use symmetry!
2
3(
)
( )
(
/ )
/
kQ
kQ x x a
a x x a
2
Q
R
At point P on axis of ring:
ds
2 2
2 2 3/ 2
2 2 3/ 2
cos
( )
( )
x
dsE E k
x ax
k dsx a
xk Q
x a
Ex = k Q x ( x2 + a2 )-3
![Page 11: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/11.jpg)
Lecture 3-11Continuous Charge Distribution 3: Charged Disk
2 2 3/ 2
2 2 3/ 20
2 2 3/ 20
2 2 1 2
2
0
/
0
( )
2( )
2( )
2 ( )
12 1 0
1 ( / )
/ 2
x x
R
R
R
R whole plane and
xE E dE k dq
x a
xk ada
x a
akx da
x a
E
kx x a
k xR x
<= Independent of x
Superposition of rings!
At a point P on axis:Use the ring with radius a EX value
2dq a da
0
2
2 2
22
( )
k x R
Ek R kQ
x Rx x
dEx = k dq x ( x2 + a2 ) -3
Integrate rings from 0 to R
Ex = -2πσkx ( 1/( x2 + R2 )1/2 – 1/x )
E = σ/2εo
![Page 12: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/12.jpg)
Lecture 3-12
Continuous Charge Distribution 4: Charged Sheets
( ) ( ) E=const in each region Superposition!
Capacitor geometry
![Page 13: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/13.jpg)
Lecture 3-13
MULTIPLE CHARGE SHEET EXAMPLE
DOCCAM 2
![Page 14: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/14.jpg)
Lecture 3-14
Gauss’s Law: Qualitative Statement
Form any closed surface around charges
Count the number of electric field lines coming through the surface, those outward as positive and inward as negative.
Then the net number of lines is proportional to the net charges enclosed in the surface.
![Page 15: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/15.jpg)
Lecture 3-15 Electric flux
N E A E An ����������������������������
# of field lines N= density of field lines x “area”
where “area” = A2 x cos
General definition of electric flux: E
S
E n dA ��������������
(must specify sense, i.e., which way)
To state Gauss’s Law in a quantitative form, we first need to define Electric Flux.
E An��������������
Sum over surface
![Page 16: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/16.jpg)
Lecture 3-16
Electric Flux through Closed SurfaceE
• The integral is over a CLOSED surface.E n
• Since is a scalar product, the electric flux is a
SCALAR quantity
E nS S
E n dA E dA ��������������
• The integration element is a vector normal to the surface and points OUTWARD from the surface. Out is +, In is -
n
E proportional to # field lines coming through outward
![Page 17: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/17.jpg)
Lecture 3-17
Why are we interested in electric flux?
E is closely related to the charge(s) which cause it.
2
22
0
4
E
rE ndA kq ndA
rkQ Q
rr
��������������
Consider Point charge Q
If we now turn to our previous discussion and use the analogy to the number of field lines, then the flux should be the same even when the surface is deformed. Thus should only depend on Q enclosed.
![Page 18: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/18.jpg)
Lecture 3-18
Gauss’s Law: Quantitative Statement
The net electric flux through any closed surface equals the net charge enclosed by that surface divided by 0.
How do we use this equation??The above equation is TRUE always but it doesn’t look easy to use.
BUT - It is very useful in finding E when the physical situation exhibits a lot of SYMMETRY.
0
enclosedE
QE ndA
![Page 19: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/19.jpg)
Lecture 3-19Physics 241 – 10:30 Quiz 3
The left half of a rod is uniformly charged with a positive charge density , whereas the right half is uniformly charged with a charge density of . What is the direction of the electric field at a point on the perpendicular bisector and above the rod as shown?
a) to the right b) to the leftc upd) downe) E is zero.
![Page 20: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/20.jpg)
Lecture 3-20Physics 241 – 11:30 Quiz 3
The upper half of a ring is uniformly charged with a positive charge density , whereas the lower half is uniformly charged with a charge density of . What is the direction of the electric field at a point on the perpendicular axis and to the left of the ring as shown?
a) to the right b) to the leftc upd) downe) E is zero.
![Page 21: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/21.jpg)
Lecture 3-21
1 22 2
1 2
cosA A
r r
![Page 22: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/22.jpg)
Lecture 3-22
Gauss’ Law - Examples
2
QE k
r
Shell Theorem
• Outside shell: E is as if Q at center
• Inside: E is zero
![Page 23: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/23.jpg)
Lecture 3-23
Proof of the Shell Theorem
• By symmetry, the electric fieldmust only depend on r and isalong a radial line everywhere.
• Apply Gauss’s law to the blue surface , we get
2
0
20
(4 )
1
4
QE r
QE
r
Electric Field Outside
![Page 24: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/24.jpg)
Lecture 3-24
Uniformly charged thin shell: Inside
• By symmetry, the electric fieldmust only depend on r and isalong a radial line everywhere.
• Apply Gauss’s law to the blue surface , we get E = 0.
E = 0 inside
Discontinuity in E
• Equal and opposite contributions from charges on diagonally opposite surface elements.
![Page 25: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/25.jpg)
Lecture 3-25
Electric Field of a Uniformly Charged Sphere
Apply Gauss’s Law directly or use superposition of the shell results
![Page 26: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/26.jpg)
Lecture 3-26Physics 241 –Quiz 2a
Two identical point charges are each placed inside a large cube. One is at the center while the other is close to the surface. Which statement about the net electric flux through the surface of the cube is true?
a) The flux is larger when the charge is at the center.b) The flux is the same (and not zero).c) The flux is larger when the charge is near the
surface.d) Not enough information to tell.e) The flux is zero in both cases.
+Q+Q
![Page 27: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/27.jpg)
Lecture 3-27Physics 241 –Quiz 2b
Two identical point charges are each placed inside a large sphere. One is at the center while the other is close to the surface. Which statement about the net electric flux through the surface of the sphere is true?
a) The flux is larger when the charge is at the center.b) The flux is larger when the charge is near the
surface.c) The magnitude of the flux is the same (and not zero).d) Not enough information to tell.e) The flux is zero in both cases.
+Q+Q
![Page 28: Lecture 3-1 Electric Field Define electric field, which is independent of the test charge, q, and depends only on position in space: dipole One is > 0,](https://reader035.vdocuments.mx/reader035/viewer/2022070414/5697c0141a28abf838ccd2bd/html5/thumbnails/28.jpg)
Lecture 3-28Physics 241 –Quiz 2c
Two identical point charges are placed, at the center of a large sphere in one case, and outside an identical sphere in the other case. Which statement about the net electric flux through the surface of the sphere is true?
a) The flux is larger when the charge is inside.b) The flux is larger when the charge is outside.c) The flux is the same (and not zero).d) Not enough information to tell.e) The flux is zero in both cases.
Q>0
Q>0