Proof of Divergence Formula in Spherical Coordinates

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SUMMARY

The discussion focuses on deriving the divergence formula in spherical coordinates, specifically addressing the formula: DIV(F) = ∇·F = (1/r²)(∂/∂r)(r²Fₗ) + (1/(rsinφ))(∂/∂φ)(sinφFₗ) + (1/(rsinφ))(∂Fₜ/∂θ). The user encounters difficulties in setting up limits for the surface integrals as the volume approaches zero and questions the necessity of multiplying by sinθ. The distinction between polar angle φ and azimuthal angle θ is clarified, with φ being the angle in the plane and θ the angle out of the plane.

PREREQUISITES
  • Understanding of vector calculus, specifically divergence
  • Familiarity with spherical coordinates and their notation
  • Knowledge of surface integrals and volume elements in calculus
  • Basic concepts of trigonometric functions, particularly sine
NEXT STEPS
  • Study the derivation of divergence in cylindrical coordinates for comparison
  • Learn about surface integrals in vector calculus
  • Explore the application of divergence in physics, particularly in fluid dynamics
  • Review trigonometric identities and their applications in calculus
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Mathematicians, physicists, and engineering students who are studying vector calculus and need to understand the application of divergence in spherical coordinates.

eliasds
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Hello - I'm supposed to derive the divergence formula for spherical coordinates by carrying out the surface integrals of the surface of the volume in the figure (the figure is a piece of a sphere similar to a box but with curves). The radial coord is r. The polar angle is \varphi and the azimuthal angle is \theta.The divergence formula is easy enought to look up: DIV(F) = \nabla\bulletF =

\frac{1}{r^{2}}\frac{\partial}{\partial r}r^{2}F_{r}+\frac{1}{rsin\varphi}\frac{\partial}{\partial \varphi}\left( sin\varphi F_{\varphi}\right) + \frac{1}{rsin\varphi}\frac{\partial F_{\theta}}{\partial\theta}

And the volume of the little piece of a sphere is easy enough:
r^{2}sin\varphi \Delta r \Delta\varphi\Delta\theta

But when I try to set up the limits for each side as the volume goes to zero I never end up with the first and second sin\varphi in the equation. Supposedly I'm supposed to multiply by a sin\theta but I don't see why.

What I end up with is:
\frac{\partial}{\partial r}F_{r}+\frac{1}{r}\frac{\partial}{\partial \varphi}\left( F_{\varphi}\right) + \frac{1}{rsin\varphi}\frac{\partial F_{\theta}}{\partial\theta}
 
Last edited:
Physics news on Phys.org
How is polar angle different from azimuth angle?
 
Phi is the angle in the page, and the theta is the angle out of the page.
 

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