Question
Question: An electric dipole moment of dipole is \(\vec{p}=\left( -\hat{i}-3\hat{j}+2\hat{k} \right)\times {{1...
An electric dipole moment of dipole is p=(−i^−3j^+2k^)×10−29C.m is at the origin (0,0,0). The electric field due to this dipole at r^=(i^+3j^+5k^) (note that r⋅p=0) parallel is to:
A. (−i^+3j^−2k^)
B. (−i^−3j^+3k^)
C. (i^+3j^−2k^)
D. (i^−3j^−2k^)
Solution
The electric dipole moment is the product of the magnitude of the charge and the distance between the two charges. This is a useful concept for the study of dielectrics and other solid applications. The electric field of a dipole is always in the opposite direction (antiparallel) to that of the dipole moment.
As per the given data,
The electric dipole moment at origin is p=(−i^−3j^+2k^)×10−29C.m
The position vector is given as r^=(i^+3j^+5k^)
The dot product of electric dipole moment and position vector is zero (r⋅p=0)
Complete answer:
When two charges are kept parted by a certain distance it is known as a dipole. The product of the magnitude of the charge and the distance between the two charges is termed as an electric dipole moment.
Mathematically,
p=qd
Where,
q is the magnitude of the charge
d is the distance between two charges
The dot product is used to find the magnitude of the resultant quantity. Mathematically it is calculated as,
a⋅b=∣a∣∣b∣cosθ
As it is mentioned in the question that the dot product of the electric dipole moment and the position vector is zero (r⋅p=0).
So this can be written as,
r⋅p=∣r∣∣p∣cosθ=0⇒cosθ=0⇒θ=2π
So here we can say that the electric field and position vector are perpendicular to each other.
The electric field of a dipole is given as,
E=−λp
Here the minus sign represents that the electric field is in the opposite (anti-parallel) direction to that of the electric dipole moment.
For the situation mention in the question the electric field of the dipole can be given as,
E=−p⇒E=−(−i^−3j^+2k^)∴E=(i^+j^−2k^)
Thus, from the above discussion, the correct option which satisfies the given question is Option C.
Note:
The concept of electric dipole moment is also useful in atoms and molecules where the effects of charge separation can be measured easily. We can also find the potential of a dipole at a distance point using the superposing the point charge potentials. The potential at the point decreases with an increase in the distance between the point and the dipole.