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There are 4 pillars that
make up the foundation
of Electricity &
Magnetism.
Gauss’Law(Electricity)
Gauss’Law(Magnetism)
Faraday’slawofinduction
Ampere’sLaw
Electricity & Magnetism
We’ll study each of
these in varying
degrees.
Maxwell’s
Equations
Karl Fredrick Gauss (1777-1855)
He was a contemporary of Charles Coulomb (1736-1806)
Instead of finding the field from a single charge, Gauss found the field
from a bunch of charges (charge distribution).
Why is Gauss’ Law important?
Specific
Coulomb’s Law finds a
field/charge from point charges.
+Q
General
Gauss’ Law finds a field/charge
from any charged object.
+Q
+Q
-Q
+Q
First Pillar: Gauss’ Law
The electric field coming through a certain area is
proportional to the charge enclosed.
Gaussian Surface
 An imaginary surface around a charge distribution
(group of charges) arbitrarily chosen for its symmetry (so
the Electric Field coming through the imaginary surface is
fairly constant through all areas of the surface).
Examples:
Point Charge Wire Strange Shape Parallel Plates
(Capacitor)
+Q
-Q -Q -Q -Q -Q +Q
+Q
-Q
+Q + + + + +
- - - - -
Sphere:
Surface Area = 4πr2
Cylinder:
Surface Area = 2πrh Strange Surface:
Calculus
Box:
Surface Area = L x W
What is Gauss’ Law?
Quick reminders on Electric Field Lines
1. More field lines = stronger field.
2. Field lines always come out of the surface perpendicularly.
3. Out of +, into ‒
(show the direction a + charge will move)
The electric field coming through a certain area is
proportional to the charge enclosed.
2
2. Electric Fields
3. Charge enclosed
The field is proportional to the charge inside the Gaussian Surface.
More Field Lines = Stronger Field = Stronger Charge Inside.
3
What is Gauss’ Law?
Gauss’ Law:
∫EdA α Q
The electric field coming through a certain area is
proportional to the charge enclosed.
How do we make this an equation? – Add a constant!
∫EdA = cQ
c = 1/εo  remember this?!?
Permitivity Constant
εo = 8.85x10-12
Nm2
/C  k = 1/4πεo = 8.99 x 109
Nm2
/C2
o
Q
EdA
ε
=∫
How much field through a certain area
Rename this to be Electric Flux (ΦE)  how much field comes through a
certain area.
The electric field coming through a certain area is
proportional to the charge enclosed.
o
E
Q
EdA
ε
==Φ ∫
And finally…
ΦE = Electric Flux (Field through an Area)
E = Electric Field
A = Area
q = charge in object (inside Gaussian surface)
εo = permittivity constant (8.85x 10-12
)
Gauss’ Law Summary
Sample Problem 1
A Van de Graaff machine with a radius of 0.25 m
has been charged up. What is the electric field
0.1 m away from the center of the sphere?
Hint: Where are all the charges? On the outside.
So how much charge is in the center? None.
0
0
===Φ
o
E EA
ε
Since all the charge is on the surface, it proves there is no field
inside a conducting surface!
Sample Problem 2
Find the electric field around a point charge,
Q.
Remember the area of a sphere (Gaussian
Surface in this case) is 4πr2
.
2
2
2
4
1
kforgettdon'
4
)4(
r
kQ
E
r
Q
E
Q
rE
Q
EA
oo
o
o
=
=→=
=
=
πεπε
ε
π
ε
What does this look like?
Coulomb’s electric field for point charges!
+Q
Sample Problem 3
A solid sphere of radius R = 40 cm has a total positive
charge of 26 μC uniformly distributed throughout its
volume. Calculate the magnitude of the electric field at
the following distances from the center of the sphere.
(a) 0 cm (b) 30 cm (c) 60 cm
0
0
===Φ
==Φ
o
E
o
E
EA
Q
EA
ε
ε
0
0
===Φ
==Φ
o
E
o
E
EA
Q
EA
ε
ε
Inside sphere Q = 0 Still inside sphere
∴Q still = 0
CNxE
x
x
E
Q
rE
Q
EA
o
o
E
/1049.6
1085.8
1026
)6.04(
)4(
5
12
6
2
2
=
=
=
==Φ
−
−
π
ε
π
ε
Sample Problem 3
A solid sphere of radius R = 40 cm has a total positive
charge of 26 μC uniformly distributed throughout its
volume. Calculate the magnitude of the electric field at
the following distances from the center of the sphere.
(a) 0 cm (b) 30 cm (c) 60 cm
0
0
===Φ
==Φ
o
E
o
E
EA
Q
EA
ε
ε
0
0
===Φ
==Φ
o
E
o
E
EA
Q
EA
ε
ε
Inside sphere Q = 0 Still inside sphere
∴Q still = 0
CNxE
x
x
E
Q
rE
Q
EA
o
o
E
/1049.6
1085.8
1026
)6.04(
)4(
5
12
6
2
2
=
=
=
==Φ
−
−
π
ε
π
ε

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Gausslaw 130128075041-phpapp02

  • 1. There are 4 pillars that make up the foundation of Electricity & Magnetism. Gauss’Law(Electricity) Gauss’Law(Magnetism) Faraday’slawofinduction Ampere’sLaw Electricity & Magnetism We’ll study each of these in varying degrees. Maxwell’s Equations
  • 2. Karl Fredrick Gauss (1777-1855) He was a contemporary of Charles Coulomb (1736-1806) Instead of finding the field from a single charge, Gauss found the field from a bunch of charges (charge distribution). Why is Gauss’ Law important? Specific Coulomb’s Law finds a field/charge from point charges. +Q General Gauss’ Law finds a field/charge from any charged object. +Q +Q -Q +Q First Pillar: Gauss’ Law
  • 3. The electric field coming through a certain area is proportional to the charge enclosed. Gaussian Surface  An imaginary surface around a charge distribution (group of charges) arbitrarily chosen for its symmetry (so the Electric Field coming through the imaginary surface is fairly constant through all areas of the surface). Examples: Point Charge Wire Strange Shape Parallel Plates (Capacitor) +Q -Q -Q -Q -Q -Q +Q +Q -Q +Q + + + + + - - - - - Sphere: Surface Area = 4πr2 Cylinder: Surface Area = 2πrh Strange Surface: Calculus Box: Surface Area = L x W What is Gauss’ Law?
  • 4. Quick reminders on Electric Field Lines 1. More field lines = stronger field. 2. Field lines always come out of the surface perpendicularly. 3. Out of +, into ‒ (show the direction a + charge will move) The electric field coming through a certain area is proportional to the charge enclosed. 2 2. Electric Fields 3. Charge enclosed The field is proportional to the charge inside the Gaussian Surface. More Field Lines = Stronger Field = Stronger Charge Inside. 3 What is Gauss’ Law?
  • 5. Gauss’ Law: ∫EdA α Q The electric field coming through a certain area is proportional to the charge enclosed. How do we make this an equation? – Add a constant! ∫EdA = cQ c = 1/εo  remember this?!? Permitivity Constant εo = 8.85x10-12 Nm2 /C  k = 1/4πεo = 8.99 x 109 Nm2 /C2 o Q EdA ε =∫ How much field through a certain area Rename this to be Electric Flux (ΦE)  how much field comes through a certain area.
  • 6. The electric field coming through a certain area is proportional to the charge enclosed. o E Q EdA ε ==Φ ∫ And finally… ΦE = Electric Flux (Field through an Area) E = Electric Field A = Area q = charge in object (inside Gaussian surface) εo = permittivity constant (8.85x 10-12 ) Gauss’ Law Summary
  • 7. Sample Problem 1 A Van de Graaff machine with a radius of 0.25 m has been charged up. What is the electric field 0.1 m away from the center of the sphere? Hint: Where are all the charges? On the outside. So how much charge is in the center? None. 0 0 ===Φ o E EA ε Since all the charge is on the surface, it proves there is no field inside a conducting surface!
  • 8. Sample Problem 2 Find the electric field around a point charge, Q. Remember the area of a sphere (Gaussian Surface in this case) is 4πr2 . 2 2 2 4 1 kforgettdon' 4 )4( r kQ E r Q E Q rE Q EA oo o o = =→= = = πεπε ε π ε What does this look like? Coulomb’s electric field for point charges! +Q
  • 9. Sample Problem 3 A solid sphere of radius R = 40 cm has a total positive charge of 26 μC uniformly distributed throughout its volume. Calculate the magnitude of the electric field at the following distances from the center of the sphere. (a) 0 cm (b) 30 cm (c) 60 cm 0 0 ===Φ ==Φ o E o E EA Q EA ε ε 0 0 ===Φ ==Φ o E o E EA Q EA ε ε Inside sphere Q = 0 Still inside sphere ∴Q still = 0 CNxE x x E Q rE Q EA o o E /1049.6 1085.8 1026 )6.04( )4( 5 12 6 2 2 = = = ==Φ − − π ε π ε
  • 10. Sample Problem 3 A solid sphere of radius R = 40 cm has a total positive charge of 26 μC uniformly distributed throughout its volume. Calculate the magnitude of the electric field at the following distances from the center of the sphere. (a) 0 cm (b) 30 cm (c) 60 cm 0 0 ===Φ ==Φ o E o E EA Q EA ε ε 0 0 ===Φ ==Φ o E o E EA Q EA ε ε Inside sphere Q = 0 Still inside sphere ∴Q still = 0 CNxE x x E Q rE Q EA o o E /1049.6 1085.8 1026 )6.04( )4( 5 12 6 2 2 = = = ==Φ − − π ε π ε