I Computing F with Nabla Identity

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The discussion focuses on the computation of the force vector F in electrodynamics using the Nabla identity. The initial formulation of F was corrected to include cross terms, leading to the expression F = ∑_i p_i ∂_i (∑_j E_j e_j). In a three-dimensional space, the force vector is expressed as F = (p_1 ∂_1 + p_2 ∂_2 + p_3 ∂_3) E, which breaks down into components for each basis vector. It is confirmed that if a Cartesian basis is used, the basis vectors remain constant, simplifying the calculations to f_i = p_j ∂_j E_i. This clarification enhances the understanding of vector calculus in electrodynamics.
rakso
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Nabla identity
Hi!

The topic is electrodynamic but it's a question about Nabla identity. Given $$ F = (p \cdot \nabla)E $$

How does one compute F? Is this correct?

$$ F = \sum_{i} p_i \partial_{i} E_{i} e_{i} $$
 
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Not quite. You missed the "cross" terms.
$$\vec F=\sum_i p_i \partial_i \left(\sum_j E_j \hat e_j\right).$$
 
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Ah, I see.

So for example, if we're in ## R^3 ##, ## \vec{F} ## would then be

## \vec{F} = (p_1 \partial_1 + p_2 \partial_2 + p_3 \partial_3) \vec{E} = (p_1 \partial_1 E_1 + p_2 \partial_2 E_1 + p_3 \partial_3 E_1)\hat{e}_1 + (p_1 \partial_1 E_2 + p_2 \partial_2 E_2 + p_3 \partial_3 E_2)\hat{e}_2 + (p_1 \partial_1 E_3 + p_2 \partial_2 E_3 + p_3 \partial_3 E_3)\hat{e}_3##

Assuming that the basis vectors are constant?
 
Sure, if you have a Cartesian basis, they are independent of position and thus in this case you simply have
$$f_i=p_j \partial_j E_i.$$
 
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