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Published byIlmari Kähkönen Modified over 6 years ago
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§1.3.2 The fundamental theorem of differentials [FTD]
Christopher Crawford PHY 416
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Outline Regions – what you integrate over Boundary operator : boundaries vs. cycles Boundary of a boundary and converse Geometric representation of fields – flux and flow Derivatives as boundaries – coboundary Duality – two different ways of looking at things Poincaré lemma – analog of : exact vs. closed Vector identities stemming from and converse Generalized Stokes’ theorem – a geometric duality [next class] Pictures of FTVC, Stokes’ Gauss’ theorems, proof by induction
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Regions and boundaries
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Flux/flow representation of fields
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Differential as a boundary
Small change in [source of] potential / flow / flux equals equipotential / flux / subst. at the boundary One higher dimension (extra `d’) d2=0 (boundary of a boundary) What about the converse?
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Fundamental Theorem of Differentials
Given a star-like [spherical] coordinate system,
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Poincaré lemma and converse
Differentials = everything after the integral sign – type of vector Pictoral representation of vector/scalar fields – integration by eye Exact sequence – mathematical structure
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