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Physics 2220 Chapter 24 Gausss Law

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... field on the axis of an annulus of radius R and infinitesimal thickness dR is. dEz = 2pske z RdR [z2 R2 ] 3/2 where s is the surface charge density, show ... – PowerPoint PPT presentation

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Title: Physics 2220 Chapter 24 Gausss Law


1
Physics 2220Chapter 24 Gausss Law
  • Quiz Given that the contribution to the
    electric field on the axis of an annulus of
    radius R and infinitesimal thickness dR is dEz
    2pske z RdR z2 R2 3/2 where s is the
    surface charge density, show that the electric
    field a distance z above an infinite plane of
    charge is Ez s/2eo, where ke 1/4peo.

2
Physics 2220Chapter 24 Gausss Law
  • Geometry

dEz 2pskezRdR z2 R2 3/2
dEz
z
dA 2pRdR
r z2 R2 1/2
R
s
3
Physics 2220Chapter 24 Gausss Law
  • Calculus

dEz 2pskezRdR z2 R2 3/2
dEz
Ez s/2eo
z
s
Ez ?08 2pskezRdR z2 R2 3/2
Ez 2pskez (-1)z2 R2 1/208
Ez 2pskez1/z - 0 2pske
Ez 2ps/4peo s/2eo
4
Physics 2220 Chapter 24 Gausss Law
  • 1' Lesson
  • The Electric Flux is defined to be the inner
    product (dot product) of the surface element and
    the electric field passing through a surface.
  • Gausss Law states that the integrated flux
    through a closed surface is equal to the enclosed
    charge divided by the permittivity of free
    space.
  • Gausss Law is a powerful tool in determining
    the electric field for many different charge
    distributions.

5
Physics 2220Chapter 24 Gausss Law
  • Electric Flux
  • A useful abstraction FE

dA
dFE E?dA
dFE E cos ? dA
E
6
Physics 2220Chapter 24 Gausss Law
  • Gausss Law
  • The total flux through a closed Gaussian
    surface is equal to the charge enclosed divided
    by the permittivity of free space.

FE ?S E?dA
dA
E
Gausss Law
q
? E?dA q/eo
7
Physics 2220Chapter 24 Gausss Law
  • Karl Friedrich Gauss
  • (1777-1855)
  • One of all-time greatest mathematicians
  • German child prodigy
  • Proved Fundamental Theorem of Algebra
  • Contributed to E-M

8
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • An infinite sheet of charge

E
dA
dFE 2Ez dA
dq s dA
2Ez dA s dA/ eo
Ez s / 2eo
s
9
Physics 2220Chapter 24 Gausss Law
  • Electric Field inside a Conductor

e
e
Equilibrium E 0
10
Physics 2220Chapter 24 Gausss Law
  • Electric Field inside a Conductor

E
dA
s
E 0
Ez dA sdA/ eo
Ez s/ eo
s
11
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • An infinite sheet of charge

E
dA
dFE 2Ez dA
dq s dA
2Ez dA s dA/ eo
Ez s / 2eo
s
12
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • Calculate the electric field at a distance R
    from an infinite line of charge with a uniform
    charge density ?.

R
?
13
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • Calculate the electric field at a distance R
    from an infinite line of charge with a uniform
    charge density ?.

ER (2pR) L ? L/eo
L
ER ?/(2peo R)
R
?
ER
dA
14
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • A spherically symmetric charge density ?

ER (4pR2 ) (1/eo )?? dV
?
ER 1/(4 peoR2 )?? dV
ER
R
dA
15
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • A spherically symmetric charge density ?

ER (4pR2 ) (1/eo )?? dV
?
ER 1/(4 peoR2 )?? dV
R
ER q/(4 peoR2 ) Rgta
16
Physics 2220Chapter 24 Gausss Law
  • Why does Gausss Law work?

Solid angle ?O ?A?r / R2 O 4pR2/R2 4p For
point charge ?FE ?A?rER ?O ER R2 But ER
q/4peoR2 FE O ER R2 4p (q/4peoR2 )R2
q/eo
17
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • What is the electric field inside a uniformly
    charged spherical shell of charge?

ER (4pR2 ) (1/eo )?? dV
ER 1/(4 peoR2 )?? dV
ER
R
dA
18
Physics 2220Chapter 24 Gausss Law
  • Applications of Gausss Law
  • What is the charge distribution if the electric
    field inside a conductor is zero?

ER (4pR2 ) (1/eo )?? dV
ER 1/(4 peoR2 )?? dV
ER
R
dA
19
Physics 2220Chapter 24 Gausss Law
  • Summary
  • FE ?S E?dA Electric Flux
  • ? E?dA q/eo Gausss Law
  • Ez s / eo E outside conducting plate E 0
    inside conductor
  • Ez s / 2eo E for infinite sheet of s
  • ER q/(4 peoR2 ) E outside spherical q
  • ER ?/(2peo R) E for line charge of ?
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