BRAIN M P
Applications =! uniformly
S
normalcharge
surface. an wire,
straight
charged
represents
Electric
Flux:
Electricfield
clectric
an of lines area.
this
fieldcrOSsing
clectric
surface density, to
number the duethin
Arca field sin. Totalclosed the fieldlong
times
inside
charge E=
an total external pE Theorem
: ininitely
Electric
over experiences = a 1/[,
over contained
the Torque
t
or
linear
flux
an i=pxEfluxisvacuum
in Gauss's
electric 1 A
is moment distance
to ofmagnitude
Dipole position)
on
(End = sheet,
dipole equal i.e. (Q) line
Axial
On gdensity, charged
uniformly
a
in 4nEGr to
charges, 3
due plane
Every
dipole the (2a).
p=qx
ismagnitude field
and charge thin E=
the the
awith of (9) between
:Dipole dipole
due
to
field
Electric Electric
charge
infinite
product field
Twolines cross
never
other.
each surface
associated
pwhose can On position)
line(Broad
on
Equatorial
Electric either
the 2i 4nEo shellpR
FIELDS
field loops.
form
Electrostatic E= spherical
Electric is
Electric
Field: characteristics
AND aat afromair not closed r4TE,
in
intensity
r q
Basic
do =I thin 4E
R* =0
distant
CHARGES charge 47tE unaffected
the p E= R,E
linesany two
between
Force of
charges.
other density, charged
point
fieldpoint i presence R, =
E
r<
> i.e.,
BLECTRIC is uniformly
ri.e., R,
and
charges
from
positive
start
lines
Field end
atnegative
Superposition charges
charge r= shell
charges. Principle the shell surface
charges
charges
unlike
for by the
Using
i
volume a the Inside
to the
like would
forces
of
sum
total! due outside On
Law
Coulomb's field
for vectorthe force.
i,
The
us Electricpoint
an of given system
time. give a
always
unit At
charge:
Quantization
of :charge '
4IE basicis with
isolated
is and unchangedtheintoall system. surface
Gaussian
bodya ne of
of eby t shcll
4NE,
r
Conservation
an taking
of
aon multiple=
denoted
q of charge:
of
Additivity
is signs)
system the E= E=0 spherical
by charge
charge remains sumproper in R
of integral
charge a (i.e. charges R charged
Properties
Basic Total Total of
Charges charge
sumwith uniformly
individual R
4TE,
account
algebraic
Total For
E=
Applications =! uniformly
S
normalcharge
surface. an wire,
straight
charged
represents
Electric
Flux:
Electricfield
clectric
an of lines area.
this
fieldcrOSsing
clectric
surface density, to
number the duethin
Arca field sin. Totalclosed the fieldlong
times
inside
charge E=
an total external pE Theorem
: ininitely
Electric
over experiences = a 1/[,
over contained
the Torque
t
or
linear
flux
an i=pxEfluxisvacuum
in Gauss's
electric 1 A
is moment distance
to ofmagnitude
Dipole position)
on
(End = sheet,
dipole equal i.e. (Q) line
Axial
On gdensity, charged
uniformly
a
in 4nEGr to
charges, 3
due plane
Every
dipole the (2a).
p=qx
ismagnitude field
and charge thin E=
the the
awith of (9) between
:Dipole dipole
due
to
field
Electric Electric
charge
infinite
product field
Twolines cross
never
other.
each surface
associated
pwhose can On position)
line(Broad
on
Equatorial
Electric either
the 2i 4nEo shellpR
FIELDS
field loops.
form
Electrostatic E= spherical
Electric is
Electric
Field: characteristics
AND aat afromair not closed r4TE,
in
intensity
r q
Basic
do =I thin 4E
R* =0
distant
CHARGES charge 47tE unaffected
the p E= R,E
linesany two
between
Force of
charges.
other density, charged
point
fieldpoint i presence R, =
E
r<
> i.e.,
BLECTRIC is uniformly
ri.e., R,
and
charges
from
positive
start
lines
Field end
atnegative
Superposition charges
charge r= shell
charges. Principle the shell surface
charges
charges
unlike
for by the
Using
i
volume a the Inside
to the
like would
forces
of
sum
total! due outside On
Law
Coulomb's field
for vectorthe force.
i,
The
us Electricpoint
an of given system
time. give a
always
unit At
charge:
Quantization
of :charge '
4IE basicis with
isolated
is and unchangedtheintoall system. surface
Gaussian
bodya ne of
of eby t shcll
4NE,
r
Conservation
an taking
of
aon multiple=
denoted
q of charge:
of
Additivity
is signs)
system the E= E=0 spherical
by charge
charge remains sumproper in R
of integral
charge a (i.e. charges R charged
Properties
Basic Total Total of
Charges charge
sumwith uniformly
individual R
4TE,
account
algebraic
Total For
E=
