Determine torque on a dipole and quadrupole (in external E-Field)

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SUMMARY

This discussion focuses on calculating the torque on dipoles and quadrupoles in an external electric field. The dipole moment is defined using the integral of charge density multiplied by the position vector crossed with the electric field, represented by the equation M = ∫ρ(r) r × E(r) d³r. For quadrupoles, the torque is calculated using M_i = ∫ρ(r) ε_ijk x_j E_k(r) d³r, where E_k(r) is expanded around the origin. The participants seek methods to simplify these equations further.

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  • Familiarity with vector calculus and integral equations
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Physicists, electrical engineers, and students studying electromagnetism who are interested in advanced calculations involving dipoles and quadrupoles in electric fields.

LeoJakob
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Homework Statement
Determine the torque on a dipole ## \vec{M}_{d} ## and on a quadrupole ## \vec{M}_{q} ## in an external electric field.
Hint 1: Develope Taylor series of the electric field ## \vec{E}(\vec{r}) ## around ## \vec{r}=0 ## up to and including the first order, using that in
Hint 2: ##\operatorname{rot} \vec{E}=0 ##
Relevant Equations
$$
\vec{M} = \int \rho(\vec{r}) \vec{r} \times \vec{E}(\vec{r}) d^{3} \vec r .
$$
For the dipole moment I calculated

$$\begin{aligned}
M &= \int \rho(\mathbf{r}) \mathbf{r} \times \mathbf{E}(\mathbf{r}) d^{3} \mathbf{r} \\
\mathbf{E}(\mathbf{r}) &\approx \mathbf{E}(\mathbf{0}) + \sum_{i=1}^{3} \nabla E_{i}(\mathbf{0}) \cdot \mathbf{r} \\
\mathbf{M}_{D} &= \mathbf{p} \times \mathbf{E} \\
&= \left( \int \rho(\mathbf{r}) \mathbf{r} d^{3} \mathbf{r} \right) \times \mathbf{E}(\mathbf{r}) \\
&= \int \rho(\mathbf{r}) \mathbf{r} \times \left[ \mathbf{E}(\mathbf{0}) + \sum_{i=1}^{3} \left( \nabla E_{i}(\mathbf{0}) \cdot \mathbf{r} \right) \mathbf{e}_i \right] d^{3} \mathbf{r} \\
&= \int \rho(\mathbf{r}) \left( \mathbf{r} \times \mathbf{E}(\mathbf{0}) + \sum_{i=1}^{3} \mathbf{r} \times \left[ \left( \nabla E_{i}(\mathbf{0}) \cdot \mathbf{r} \right) \mathbf{e}_i \right] \right) d^{3} \mathbf{r}
\end{aligned}$$

I don't know how to simplify this equation any further. Are there ways to simplify this equation?

How do I calculate the torque on the quadrupole?
 
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Try looking at the components, e.g.$$M_i = \int \rho(\mathbf{r}) \epsilon_{ijk} x_j E_k (\mathbf{r}) d^3 \mathbf{r}$$Then expand the field$$E_k (\mathbf{r}) = \left[ E_k (\mathbf{r}') + x_l \frac{\partial}{\partial x_l'} E_k(\mathbf{r}') + \dots \right]_{\mathbf{r}' = \mathbf{0}}$$You will be able to identify the dipole moment ##p_i = \int \rho(\mathbf{r}) x_i d^3 \mathbf{r}##.
 

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