- #1
MatinSAR
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Then it is equal to ##Pr^{-3}##, Am I right?!kuruman said:Just expand the dot product and ##\vec r## then take derivatives.$$(\vec p\cdot \vec{\nabla})\vec r = \left(p_x\frac{\partial}{\partial x}+p_y\frac{\partial}{\partial y}+p_z\frac{\partial}{\partial z}\right)(x~\hat x+y~\hat y+z~\hat z)$$
kuruman said:Show me the math.
Yes. What is your final answer when you put it all together?MatinSAR said:I have used:
##p_x\frac{\partial}{\partial x}y=0##
##p_x\frac{\partial}{\partial x}z=0##
##p_y\frac{\partial}{\partial y}x=0##
##p_y\frac{\partial}{\partial y}z=0##
##p_z\frac{\partial}{\partial z}x=0##
##p_z\frac{\partial}{\partial z}y=0##
##p_x\frac{\partial}{\partial x}x=p_x##
##p_y\frac{\partial}{\partial y}y=p_y##
##p_z\frac{\partial}{\partial z}z=p_z##
##\vec P## , I guess.kuruman said:Yes. What is your final answer when you put it all together?
I am trying to solve ... I will send the work.kuruman said:Sorry, not that. I meant putting together the final expression ##\vec E=-\vec{\nabla}\psi=?##
Thanks a lot! Have a good day.kuruman said:That's it. Good job!
An electric dipole consists of two equal and opposite charges separated by a small distance. It is characterized by a dipole moment, which is a vector quantity pointing from the negative charge to the positive charge.
The electric field due to a dipole at a point on the axial line (along the line connecting the two charges) is given by \( E = \frac{1}{4\pi\epsilon_0} \cdot \frac{2p}{r^3} \), where \( p \) is the dipole moment and \( r \) is the distance from the dipole to the point where the field is being calculated.
The electric field due to a dipole at a point on the equatorial line (perpendicular bisector of the line connecting the two charges) is given by \( E = \frac{1}{4\pi\epsilon_0} \cdot \frac{p}{r^3} \), where \( p \) is the dipole moment and \( r \) is the distance from the dipole to the point where the field is being calculated.
The direction of the electric field due to an electric dipole at the origin depends on the position of the point where the field is being calculated. Along the axial line, the field points away from the dipole if the point is on the positive charge side, and towards the dipole if the point is on the negative charge side. Along the equatorial line, the field is perpendicular to the dipole moment and points away from the dipole axis.
The electric field strength due to an electric dipole decreases with the cube of the distance from the dipole. Specifically, the field strength is inversely proportional to \( r^3 \), where \( r \) is the distance from the dipole to the point where the field is being calculated.