This section delves into the fundamental ways vector fields can be expressed as derivatives of other fields—either as the negative gradient of a scalar potential or the curl of a vector potential. It explores the inherent properties of such fields (curl-free for scalar potentials, divergence-free for vector potentials), their connection to conservative fields, methods for constructing these potentials, and the crucial concept of their non-uniqueness. Finally, it introduces the Helmholtz Decomposition Theorem, which states that any vector field can be uniquely decomposed into a curl-free and a divergence-free component, each derivable from a respective potential.
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The line integral result of a dot moving along a straight and a curved path between the points is independent of the pathThe gravitational potential is the scalar potential of the gravitational fieldThe work of a conservative force field is path-independenthow integration constants behave during partial integrationhow knowing one partial derivative allows us to find the form of the potential and how the other partial derivative is used to resolve the unknown function of integrationhow the method for deriving the electric potential from a constant electric field extends from two dimensions to an arbitrary number of dimensionshow a scalar potential generates a curl-free and conservative vector fieldhow a vector potential generates a divergence-free vector fieldwhy vector fields derived from scalar potentials are always curl-freedivergence free vector fields have vector potentialsthe non-uniqueness of the vector potential and the concept of gauge transformationany vector field that can be expressed as the curl of another vector field must necessarily be divergence-freehow the curl of different vector potentials can lead to the same resultvisualize the constant vector field and the two different vector potentialsAn incompressible fluid flow and the existence and non-uniqueness of its vector potentialhow a general vector field can be decomposed into its curl-free and divergence-free componentsgauge freedom for a divergence-free vector field showing how different vector potentials can describe the same physical fieldthe constant electric field's scalar potential as horizontal equipotential planes and how the negative gradient of these planes yields the original electric fieldhow vectors combine and interact in 3D space to produce scalar or vector resultsCheck the components of a vector can be found through the scalar product with the basis vectorsComputing magnitude and inner product and cross product and angles and The volume of the parallelepiped spanned of three vectorsComputing cross product of the vectors through symbolic componentshow intermediate vectors are formedthe cross product of two vectors is orthogonal to bothsequentially prove that the vectors are normalized and orthogonal and display the corresponding transformation coefficientsthe sum of the diagonal elements of the Kronecker delta tensor equals the dimensionality of the spaceThe Cross Product and the Right-Hand Rule