Divergence of a Magnetic Field not equaling zero

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The discussion centers on the divergence of a magnetic field, specifically addressing the confusion around the divergence of B not equaling zero in cylindrical coordinates. The user highlights a contradiction when applying the divergence formula, leading to the result that Div(B) equals B_rho / rho. Clarification is sought on how constant vector components in Cartesian coordinates can yield nonzero partial derivatives in cylindrical coordinates. The conversation emphasizes the importance of understanding how the unit vectors in cylindrical coordinates can affect the divergence calculation. Overall, the thread seeks to resolve the apparent discrepancy in the divergence of magnetic fields in different coordinate systems.
Maliska
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I have a larger problem involving divergences and curls, but the correct answer requires ∇°B (divergence of B) = 0. I understand the proof of this in Griffiths, but the definition of divergence in cylindrical coordinates is:

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After using the product rule to split the first term, we get the divergence of B is B_rho / rho + 0 + 0 + 0, or simply Div(B)=B_rho / rho; however, this clearly contradicts what we know about the divergence of B being zero. Can someone please clarify this for me, I've been stuck at it for hours.

Thanks.

P.s. First post!
 
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How do you know that the partial derivatives you claim to be zero are zero? Do you have a specific field in mind? A field that's a constant vector in Cartesian can look rather different in polar.
 
Thank you haruspex for responding. The partial derivatives I said equal zero could be my mistake, but please explain how a vector with constant components in cartesian coordinates can have nonzero partial derivatives in cylindrical coordinates.
 
Aρ, for example, refers to the component of the vector in the ρ direction. If the vector is constant, its component in the ρ direction may yet depend on θ and z. It's not that the vector varies, but that the unit ρ-direction vector does.
 
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