Use of curl of gradient of scalar

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Discussion Overview

The discussion revolves around the mathematical property of the curl of the gradient of a scalar function and its implications in physics. Participants explore whether this property is trivial and how it is applied in various contexts, including electrostatics and differential geometry.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that the curl of the gradient of a scalar function is always zero, suggesting it is a trivial result.
  • Others propose that while the curl of the gradient is zero, the Laplacian of a function is not necessarily zero, indicating that only certain functions (harmonic functions) satisfy this condition.
  • One participant mentions the application of the curl of the gradient in electrostatics, where the electric field is represented by a scalar potential field, thus being curl-free.
  • Another participant raises the question of how the curl of the gradient is used in its differential form, specifically referencing Stokes' theorem.
  • There is a discussion about the implications of Clairaut's Theorem, noting that the curl of a gradient may not be zero for functions that do not meet certain smoothness criteria.

Areas of Agreement / Disagreement

Participants generally agree that the curl of the gradient is zero, but there is disagreement regarding the implications and applications of this property, particularly in relation to the Laplacian and the conditions under which these statements hold true.

Contextual Notes

Limitations include the dependence on the smoothness of functions and the specific conditions under which the Laplacian is zero. The discussion does not resolve the nuances of these mathematical properties.

Mike2
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I'm wondering if physics ever uses a differential equation of the form of a curl of a gradient of a scalar function. Or is this too trivial?

Thanks.
 
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The curl of the gradient of a scalar function is always zero. So, yeah, it's pretty trivial.

- Warren
 
Originally posted by chroot
The curl of the gradient of a scalar function is always zero. So, yeah, it's pretty trivial.

- Warren

well yes, but then don't they use the fact that the Laplacian is zero?
 
Originally posted by Mike2
well yes, but then don't they use the fact that the Laplacian is zero?
I think I see what you're asking. How about electrostatics? The electric field can be represented by a scalar potential field. Therefore, the curl of the gradient of this field is zero -- the electric field is curl-free.

- Warren
 
Originally posted by Mike2
well yes, but then don't they use the fact that the Laplacian is zero?

as ambitwistor correctly points out: the laplacian is not zero.

the the curl of a gradient is zero.

physicists use both facts.
 
Originally posted by Ambitwistor
Yes, but the Laplacian of an arbitrary function isn't automatically zero, so only certain functions (the harmonic ones) satisfy the condition that their Laplacian is zero. Every function satisfies the condition that the curl of its gradient equals zero, so that equation is not too useful on its own.

In other words, you could never find a "unique" function that satisfies the conditions. For ALL functions satisfy the conditions, right? Thanks.
 
Originally posted by lethe

physicists use both facts.

Yes, but the question is HOW do they use the fact that the curl of the gradient of a scalar. Yes they use it in Stoke's theorem, but do they use it in its differential form?
 
Originally posted by Mike2
Yes, but the question is HOW do they use the fact that the curl of the gradient of a scalar. Yes they use it in Stoke's theorem, but do they use it in its differential form?

you bet they do. this fact is the basis of de Rham cohomology. it provides a powerful tool for topological classification of manifolds, which rests on Poincaré duality, which is really just an application of Stokes theorem.
 
Yeah I'm glad as physicists we never really run into those weird functions that don't obey Clairaut's Theorem. Because if we did then technically the curl of a gradient of a scalar function wouldn't necessarily be zero. Since the curl of a gradient gives us second order mixed partial derivatives of the function in question like Fxy - Fyx as the z component, this may or may not be zero for Every function out there, though is certainly true for smooth twice continuously differentiable functions at least. SO the statement should be not that every function has a zero curl gradient but that only continuous smooth functions do, because a piecewise continuous function is certainly a function whether its smooth or not.
 

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