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Divergence and Curl of Electrostatic Fields
rrE ˆ4
1)(
20 r
q
Field of a point charge
arrows field lines:E lines/area ofnumber
of direction E
Bits of thread in oil align with the field lines.
2222222222
)()(ˆˆ2
yxaryxarr
y
r
y
r
xa
r
xaBA
BABAo
yxE
Construction principle:Field lines start at +q and end at –q.The number of lines is proportional to q.If the total charge is different from 0, there will be linesgoing to or coming from infinity.Field lines never cross.The field lines point in radial direction near point charges.
Divergence of E (Gauss’s Law)
charge. theencloses , :chargepoint SS o
qd
aE
VS
dQQ
d enco
enc , :form integral aE
o
E :form aldifferenti
Application of Gauss’s law (integral form):
1. Spherical symmetry:
3. Plane symmetry:
The direction of the field is known, and it is constant on the Gaussian surface
2. Cylindrical symmetry:
Example 2.2What is the field outside the uniformly charged sphere?
Example 2.3Field inside a long cylinder with charge density ks
Example 2.4Infinite plate with uniform surface charge density
Example 2.5
Field Lines and Flux
gpenetratin lines field ofnumber S.S
aE dE
Flux through a surface:
Streamlines of a fluid flowing around a cylinder.
.0 fluid ibleincompress an offlow Stationary
:analogon icHydrodynam
v
Conservation of flux:
00 aEE d
Flux tube:
The flux (number of field/stream lines) through the different cross sections of the flux tube is constant.
Curl of E
rE ˆ4
1 :chargepoint
20
r
q
0aE d0 E
i
iEEfor trueremain
General properties
Laws of electrostatics
0aE d
0 E
o
E :form aldifferenti
VS
dQQ
d enco
enc , :form integral aE