How Is Mutual Energy Calculated Between Non-Parallel Dipoles?

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The mutual energy between two non-parallel dipoles, p1 and p2, is expressed as U = -\frac{p_1\cdot p_2}{|r|^3} - 3\frac{(p_1\cdot r)(p_2\cdot r)}{|r|^5}, where r is the vector from p1 to p2. The discussion explores various approaches to derive this equation, including using potential energy integrals and the electric field generated by dipoles. There is a distinction made between electric dipoles (denoted by p) and magnetic dipoles (denoted by m), with a focus on the electric case. The relationship U = -p.E is highlighted, emphasizing the need to derive the electric field for an electric dipole. The conversation concludes with a reminder that potential energy can also be derived from the integral of force.
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i need to show that the mutual energy between two dioples p1 and p2 (not necessarily parallel to each other) is U=-\frac{p_1\cdot p_2}{|r|^3}-3\frac{(p_1\cdot r)(p_2\cdot r)}{|r|^5}
where r is the vector from p_1 to p_2. (the p's are moments of diople).

i tried using this equation: U=\int dV \rho_2 * \phi_1
and also this :\phi=\frac{p\cdot r}{|r|^3}
(phi is the potential and rho is the density).
\rho_2=-1/4\pi\nabla^2\phi_2=-1/4\pi[\frac{1}{|r|^2}@/@r(r^2@\phi/@r)+\frac{1}{|r|^2*sin(\theta)}@/@\theta(sin(\theta)@\phi/@\theta)]
where @ stands for peratial derivative, but i didnt get to the desired answer.
any pointers?
 
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What about

U=-{m\cdot B}

where m is the vector for one of the dipoles in field B from the other dipole.
 
you'll have to dig the equation for the field (B) of dipole, too, I reckon.
 
by B, you mean the magnetic field, well i haven't learned it yet (i mean we haven't touched it in class as of yet, i myself read it form purcell), i pretty much sure i don't need here to use B, perhaps something else?
 
So these are electric dipoles then? I guess p usually denotes electric dipole and m is for magnetic dipole.
 
anyway, same equation, just:

U = -p.E

instead of -m.B

and dig up the E field for an electric dipole
 
well for E i found already, shouldn't i prove that it equals p.E? or in other words how to derive it?
 
loop quantum gravity said:
well for E i found already, shouldn't i prove that it equals p.E? or in other words how to derive it?


If you want to find a derivation for U = -p.E, you might also remember that potential Energy is

the integral of F.dl

and the Force from a dipole is

F = (p.grad)E
 
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