Magnitude and direction of electric field at point P

AI Thread Summary
The discussion focuses on calculating the electrostatic potential and electric field at point P due to an electric dipole. The total potential at point P is derived as Vtot = kq(1/(x+a) - 1/(x-a)), simplifying to Vtot = (2kqa)/(x^2). The magnitude and direction of the electric field E are determined by taking the gradient of the potential function, which points along the x-axis toward the nearest charge. For points along the x-axis, the electric field direction is toward (a, 0) for x > 0 and toward (-a, 0) for x < 0. The discussion emphasizes the importance of understanding the relationship between potential, electric field, and their respective directions in the context of dipoles.
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Homework Statement



An electric dipole is defined as two point charges separated by distance L.
Consider point P with coordinates (x,0).
A dipole along the x-axis is separated by distance a from the origin. q- is closer to point P
Find:

1) Electrostatic potential due to dipole at point P
2) Magnitude and direction of electric field E at point P in terms of dipole moment and distance x

Homework Equations



V = k\frac{q}{r}

The Attempt at a Solution



1) Vtot = V+q + V-q

= kq(\frac{1}{x+a} - \frac{1}{x-a})

=\frac{2kqa}{x^2}

2) I know that taking the divergence of \frac{2kqa}{x^2} will give a scalar. Is this divergence going to be \frac{d}{dx}? How do I go about getting the magnitude and direction from there?

Thank you
 
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The value of the gradient is the magnitude of the vector. Since both poles are on the x-axis and your given point is (x, 0), the vector will point along the x-axis to the nearest pole. That means that for x> 0 it points toward (a, 0) and for x< 0, it points toward (-a, 0).

More generally, if the point could be any point in the xy-plane, (x, y), rather than just (x, 0), the potential function would be
\phi(x,y)= \frac{kq}{\sqrt{(x-a)^2+ y^2}}+ \frac{kq}{\sqrt{(x+a)^2a+ y^2}}
and the force vector the gradient of that:
\frac{\partial \phi}{\partial x}\vec{i}+ \frac{\partial \phi}{\partial y}\vec{j}
 
Ah, I see. Thank you
 
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