Electric field at a point on the axis of a dipole derivation
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By using the formula for electric field due to point charge,
Electric field due to +q =
+1
4πε0
q
(r - l)2
The distance between (P and +q) = (r-l)
Electric field due to -q =
-1
4πε0
q
(r + l)2
The distance between (P and -q) = (r + l)
(Electric field due to +q will be positive and electric field due to- q will be negative)
Since electric field is a vector quantity so, the net electric field will be the vector addition of the two.
So, the net electric field E = E1 + E2
E =
1
4πε0
q
(r - l)2
-
1
4πε0
q
(r + l)2
E =
q
4πε0
[
1
(r - l)2
-
1
(r + l)2
]
On solving the equation we get −
E =
q
4πε0
[
(r + l)2 - (r - l)2
(r - l)2(r + l)2
]
E =
q
4πε0
4rl
(r2 - l2)2
......(1)
We know that the dipole moment or effectiveness of dipole (P) is given by −
P = 2ql
Therefore, putting this value in eq(1), we get
E =
1
4πε0
2Pr
(r2 - l2)2
......(2)
Certain assumptions are made based on this equation −
Since, the dipole is very small so ‘l’ is also very small as compared to the distance ‘r’.
So, on neglecting ‘r’ with respect to ‘l’ we get −
E =
1
4πε0
2Pr
r4
(from eq(2))
⇒ E =
1
4πε0
2P
r2
E =
1
4πε0
2P
r2
Electric field due to +q =
+1
4πε0
q
(r - l)2
The distance between (P and +q) = (r-l)
Electric field due to -q =
-1
4πε0
q
(r + l)2
The distance between (P and -q) = (r + l)
(Electric field due to +q will be positive and electric field due to- q will be negative)
Since electric field is a vector quantity so, the net electric field will be the vector addition of the two.
So, the net electric field E = E1 + E2
E =
1
4πε0
q
(r - l)2
-
1
4πε0
q
(r + l)2
E =
q
4πε0
[
1
(r - l)2
-
1
(r + l)2
]
On solving the equation we get −
E =
q
4πε0
[
(r + l)2 - (r - l)2
(r - l)2(r + l)2
]
E =
q
4πε0
4rl
(r2 - l2)2
......(1)
We know that the dipole moment or effectiveness of dipole (P) is given by −
P = 2ql
Therefore, putting this value in eq(1), we get
E =
1
4πε0
2Pr
(r2 - l2)2
......(2)
Certain assumptions are made based on this equation −
Since, the dipole is very small so ‘l’ is also very small as compared to the distance ‘r’.
So, on neglecting ‘r’ with respect to ‘l’ we get −
E =
1
4πε0
2Pr
r4
(from eq(2))
⇒ E =
1
4πε0
2P
r2
E =
1
4πε0
2P
r2
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