Potential energy of electric dipole
*“ Potential energy of electric dipole”:
The energy possessed by the dipole due to its specific position in an uniform electric field is called potential energy. It is a scalar quantity. It is denoted by U.
*Measurement —The work done in turning a dipole from Standard position to any other position is stored in dipole in the form of potential energy.
Consider and electric dipole AB made up of two point charges -q and +q having a dipole moment P.
the dipole Axis making an angle Φ with direction of electric field
“standard position of dipole is the perpendicular position with respect to direction of electric field in which the potential energy of a dipole becomes zero”
let the work done against dipole torque τ = P·E sinθ in turning a dipole by small angle dθ is dw·
work done = dipole torque × angular displacement
dw = τ·dθ
dw = P·Esinθ taking integration of both side in the limit θ1 to θ2
∫w =∫θ1θ2
pEsinθdθ
W = - P·E [cosθ2 - cosθ1]
W = P·E [ cosθ1 - cosθ2]
If θ1 = π/2 and θ2 = θ
then W = P·E ( cosπ/2 - cosθ)
∴ W = P·E ( 0 - cosθ)
W = - P·E cosθ
This work done is stored in dipole
in the form of potential energy
∴ U = W
∴ U = -P·E cosθ
The energy possessed by the dipole due to its specific position in an uniform electric field is called potential energy. It is a scalar quantity. It is denoted by U.
*Measurement —The work done in turning a dipole from Standard position to any other position is stored in dipole in the form of potential energy.
Consider and electric dipole AB made up of two point charges -q and +q having a dipole moment P.
the dipole Axis making an angle Φ with direction of electric field
“standard position of dipole is the perpendicular position with respect to direction of electric field in which the potential energy of a dipole becomes zero”
let the work done against dipole torque τ = P·E sinθ in turning a dipole by small angle dθ is dw·
work done = dipole torque × angular displacement
dw = τ·dθ
dw = P·Esinθ taking integration of both side in the limit θ1 to θ2
∫w =∫θ1θ2
pEsinθdθ
W = - P·E [cosθ2 - cosθ1]
W = P·E [ cosθ1 - cosθ2]
If θ1 = π/2 and θ2 = θ
then W = P·E ( cosπ/2 - cosθ)
∴ W = P·E ( 0 - cosθ)
W = - P·E cosθ
This work done is stored in dipole
in the form of potential energy
∴ U = W
∴ U = -P·E cosθ
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