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§1.5 Delta Function; Function Spaces
Christopher Crawford PHY 416
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Outline Example derivatives with singularities Electric field of a point charge – divergence singularity Magnetic field of a line current – curl singularity Delta singularity δ(x) Motivation – Newton’s law: yank = mass x jerk Definition – differential of step function dϑ = δ dx Important integral identities Calculating with delta functions Distributions – vs. functions Delta as an `undistribution’ Singularities and boundary conditions Building up higher dimensions: δ3(r) Linear function spaces – functions as vectors Delta as a basis function or identity operator Correspondence table between vectors and functions
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Example: magnetic field of a straight wire
This time: a singularity in the curl of magnetic intensity (flow)
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Example: Inverse Square Law
Force of a constant carrier flux emanating from a point source
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Newton’s law yank = mass x jerk force = mass x accel.
impulse = m x Δv singularities become more pronounced!
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Delta singularity δ(x)
Differential definition: dϑ(x) = δ(x) dx Heaviside step function ϑ(x) = { 1 if x>0, 0 if x <0 } Delta `function’ as a limit:
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Important integral identities
Note the different orders of derivative Offset delta function
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Calculations with δ(x)
Jacobian Higher dimension
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Delta `undistribution’
Something you can integrate (a density) The “distribution” of mass or charge in space The delta `function’ is not well defined as a function but it is perfectly meaningful as an integral Think of δ(x) as an “undistribution” The charge is clumped up into a singularity
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Boundary conditions 2-d version of a PDE on the boundary
Derived from PDE by integrating across the boundary RULES: Proof:
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δ(x) as a basis function
Each f(x) is a component for each x Write function as linear combination δ(x’) picks off component f(x) The Dirac δ(x) is the continuous version of Kröneker δij Represents a continuous type of “orthonormality” of basis functions It is the kernel (matrix elements) of the identity matrix
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