The Gradient Theorem: Understanding the Physical Interpretation and Intuition

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Discussion Overview

The discussion revolves around the physical interpretation and intuition behind the gradient theorem, specifically the equation \(\iiint\limits_V \nabla \psi dV=\iint\limits_S \psi \vec{dS}\). Participants seek to clarify the concept, comparing it to the divergence theorem and exploring its implications in higher dimensions.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses uncertainty about the appropriate forum category for their question and seeks a more complete understanding of the gradient theorem's physical interpretation.
  • Another participant acknowledges the relationship between the gradient theorem and the divergence theorem, noting that the latter describes the rate of expansion of a vector field in relation to its boundary.
  • A participant reflects on the difficulty of grasping the intuition behind the gradient theorem in higher dimensions, despite understanding the one-dimensional case.
  • One reply suggests that the gradient theorem is a form of the divergence theorem and relates it to the generalized Stokes' Theorem from differential geometry, proposing a topological perspective to aid understanding.
  • The same reply introduces visual aids to illustrate the concept of integration over chains in two dimensions, emphasizing the cancellation of contributions from interior arrows in tilings of a region.

Areas of Agreement / Disagreement

Participants generally express uncertainty and seek clarification, indicating that multiple views and interpretations exist regarding the gradient theorem and its relationship to other mathematical concepts. The discussion remains unresolved with no consensus reached.

Contextual Notes

Participants note the complexity of understanding the gradient theorem in higher dimensions compared to one-dimensional cases, highlighting potential limitations in their current grasp of the topic.

member 428835
i am not sure if this post should be under calculus or not, but i think i'll get a more "complete" answer here. at any rate, I'm wondering if anyone can clarify the intuition behind the gradient theorem: [tex]\iiint\limits_V \nabla \psi dV=\iint\limits_S \psi \vec{dS}[/tex] by intuition, i refer to a physical interpretation. for instance, i understand the divergence theorem states (rate of expansion of a vector field) = (rate the vector field leaks out of the edges). but this extended gradient theorem is more difficult. please help! i doubt i need to clarify this notation, but please let me know if I've been ambiguous.

thanks!
 
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joshmccraney said:
i am not sure if this post should be under calculus or not, but i think i'll get a more "complete" answer here. at any rate, I'm wondering if anyone can clarify the intuition behind the gradient theorem: [tex]\iiint\limits_V \nabla \psi dV=\iint\limits_S \psi \vec{dS}[/tex] by intuition, i refer to a physical interpretation. for instance, i understand the divergence theorem states (rate of expansion of a vector field) = (rate the vector field leaks out of the edges). but this extended gradient theorem is more difficult. please help! i doubt i need to clarify this notation, but please let me know if I've been ambiguous.

thanks!

This is just the 3D version of [itex]\int_a^b{\frac{df}{dx}dx}=f(b)-f(a)[/itex]
 
yes, i do realize this, but I am a little shakey on the intuition. the slope vectors added up make sense to check the difference of endpoints, but the 2 and 3 dimensions are not as obvious.
 
joshmccraney said:
i am not sure if this post should be under calculus or not, but i think i'll get a more "complete" answer here. at any rate, I'm wondering if anyone can clarify the intuition behind the gradient theorem: [tex]\iiint\limits_V \nabla \psi dV=\iint\limits_S \psi \vec{dS}[/tex] by intuition, i refer to a physical interpretation. for instance, i understand the divergence theorem states (rate of expansion of a vector field) = (rate the vector field leaks out of the edges). but this extended gradient theorem is more difficult. please help! i doubt i need to clarify this notation, but please let me know if I've been ambiguous.

thanks!
When you post in the differential geometry part of the forum, you get a differential geometry answer.

Note first, though, that your "gradient theorem" is actually just a form of the Divergence Theorem. It turns out that all these integral theorems that you learn from multivariate calculus are actually results of a single theorem called the generalized Stokes' Theorem from differential geometry.

The intuition for your problem can be seen in 2 dimensions. From a topological standpoint, we can integrate over chains, and in the two dimensional case we'll look at a 2-chain and its boundary and see what integration over the two might be like. Look at the pictures below (Ignore the rainbows. Life in mathland is just that happy).

The first shows the oriented boundary of a region in two dimensional space. The second shows finer and finer oriented tilings of the region. Note that the interior arrows of each tiling go in opposite directions from their neighbors, "cancelling" each other out. The integral over the 2-chain would be equal to, in a sense, the contribution of the boundary.

Does this help?
 

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