Divergence in Polar Coordinates

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SUMMARY

The divergence of a vector field in polar coordinates is expressed as \nabla\cdot\vec{A}=\frac{1}{r}\frac{\partial}{\partial r}(rA_{r})+\frac{1}{r}\frac{\partial}{\partial \theta}(A_{\theta}). This formulation accounts for the fact that the unit vectors in polar coordinates, \hat{r} and \hat{\theta}, are functions of position. Consequently, the gradient operator \nabla must act on both the vector components and the unit vectors, leading to the necessity of the additional terms in the divergence equation.

PREREQUISITES
  • Understanding of vector calculus, specifically divergence and gradient operations.
  • Familiarity with polar coordinate systems and their unit vectors.
  • Knowledge of partial derivatives and their application in vector fields.
  • Basic concepts of cylindrical coordinates and their mathematical implications.
NEXT STEPS
  • Study the derivation of divergence in cylindrical coordinates.
  • Explore vector calculus identities and their applications in physics.
  • Learn about the implications of coordinate transformations on vector fields.
  • Investigate the role of unit vectors in different coordinate systems.
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Mathematicians, physicists, and engineering students focusing on vector calculus and its applications in fields such as fluid dynamics and electromagnetism.

neutrino2063
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Why is
\nabla\cdot\vec{A}=\frac{1}{r}\frac{\partial}{\partial r}(rA_{r})+\frac{1}{r}\frac{\partial}{\partial \theta}(A_{\theta})

Where
\vec{A}=A_{r}\hat{r}+A_{\theta}\hat{\theta}
And
\nabla=\hat{r}\frac{\partial}{\partial r}+\hat{\theta}\frac{1}{r}\frac{\partial}{\partial \theta}
Instead of just:

\nabla\cdot\vec{A}=\frac{\partial}{\partial r}(A_{r})+\frac{1}{r}\frac{\partial}{\partial \theta}(A_{\theta})
 
Last edited:
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Because the unit vectors are actually functions of position in cylindrical coordinates. This means all the derivative in the gradient operator act not only on the components of a particular vector, but also the unit vectors themselves.
 

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