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2
3
4
By:
Aakanksha
Simran
Sejal
Class: XII
 It states that the force of attraction or repulsion between
any two stationary point charges is directly proportional to
the product of their magnitudes of the two charges and
inversely proportional to the square of the distance
between them.
Electrostatic Induction
Electric fields
E
+ + + + + + + + + +
+ + + + + + + + +
Earth
p=qL = the electric dipole moment
The dipole moment p is defined as a vector
directed
from -ve to +ve.
22
θ−=+ cosE2EE x2x1
iˆcosE2E,So net θ−=

2
a
kq
E =
a2
L
a
cos 2
L
==θ
iˆ
a2
L
a
kq
2E,So 2net −=

r
Enet = −
kqL
a3
ˆi
2
2
2
L
ra 




+=
( )( )
2
3
2
3 2
r2
L32
2
L2
net
)(1(
1
r
p
k
r
p
kE 







+
=
+
=

qLp =
r
Enet
;
kp
r3
Electric Dipole
a
a
E
1
E1x
θ
θ
ˆi
ˆj
y
For large r
E1x = −E cosθ and E1x = E2x
E2
23
A uniform external electric field exerts no net force on a dipole, but it
does exert torque that tends to rotate the dipole in the direction of the
field (align with )p

extE

1F

2F

x
Torque about the com = τ
= FLsinθ
= qELsinθ = pEsinθ =
r
p ×
r
E
Ep

×=τSo,
When the dipole rotates through θ, the electric field does work:
24
Potential Energy
Ans. The energy is minimum when aligns with
EpcospEU

⋅−=θ−==
Integrating
,
So, U=-

p⋅

E
p

E

dW=−τdθ=−pEsinθdθWork done equals
The minus sign arises because the torque opposes any increase in θ.
Setting the negative of this work equal to the change in the potential
energy, we have
θθ+=−= dsinpEdWdU
0UcospEdsinpEdWdUU +θ−=θθ−=−== ∫ ∫ ∫
°=θ= 90when0UchooseWe
 The electric flux through a given area held
inside an electric field is the measure of the
total number of electric lines of force
passing normally through that area
 ΔΦ=E Δs cosθ
It is a scalar quantity and it’s SI unit is
(Nm*m)/c
It has direction which is normal to the plane.
States the total electric flux
through a closed surface
(surface integral of electric
field over a closed surface)
is equal to 1/εo times the
total charge enclosed by the
surface.
Mathematically
( )enclosed
s
qSdE∫ =
0
1
.
ε

Electrostatics123
Electrostatics123
Electrostatics123
Electrostatics123
Electrostatics123
Electrostatics123
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Electrostatics123

  • 1.
  • 2. 2
  • 3. 3
  • 4. 4
  • 6.
  • 7.
  • 8.
  • 9.
  • 10.
  • 11.  It states that the force of attraction or repulsion between any two stationary point charges is directly proportional to the product of their magnitudes of the two charges and inversely proportional to the square of the distance between them.
  • 12.
  • 15. E + + + + + + + + + + + + + + + + + + + Earth
  • 16.
  • 17.
  • 18.
  • 19.
  • 20.
  • 21. p=qL = the electric dipole moment The dipole moment p is defined as a vector directed from -ve to +ve.
  • 22. 22 θ−=+ cosE2EE x2x1 iˆcosE2E,So net θ−=  2 a kq E = a2 L a cos 2 L ==θ iˆ a2 L a kq 2E,So 2net −=  r Enet = − kqL a3 ˆi 2 2 2 L ra      += ( )( ) 2 3 2 3 2 r2 L32 2 L2 net )(1( 1 r p k r p kE         + = + =  qLp = r Enet ; kp r3 Electric Dipole a a E 1 E1x θ θ ˆi ˆj y For large r E1x = −E cosθ and E1x = E2x E2
  • 23. 23 A uniform external electric field exerts no net force on a dipole, but it does exert torque that tends to rotate the dipole in the direction of the field (align with )p  extE  1F  2F  x Torque about the com = τ = FLsinθ = qELsinθ = pEsinθ = r p × r E Ep  ×=τSo, When the dipole rotates through θ, the electric field does work:
  • 24. 24 Potential Energy Ans. The energy is minimum when aligns with EpcospEU  ⋅−=θ−== Integrating , So, U=-  p⋅  E p  E  dW=−τdθ=−pEsinθdθWork done equals The minus sign arises because the torque opposes any increase in θ. Setting the negative of this work equal to the change in the potential energy, we have θθ+=−= dsinpEdWdU 0UcospEdsinpEdWdUU +θ−=θθ−=−== ∫ ∫ ∫ °=θ= 90when0UchooseWe
  • 25.  The electric flux through a given area held inside an electric field is the measure of the total number of electric lines of force passing normally through that area  ΔΦ=E Δs cosθ It is a scalar quantity and it’s SI unit is (Nm*m)/c It has direction which is normal to the plane.
  • 26. States the total electric flux through a closed surface (surface integral of electric field over a closed surface) is equal to 1/εo times the total charge enclosed by the surface. Mathematically ( )enclosed s qSdE∫ = 0 1 . ε 