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Then the expansion of an arbitrary function f($, m) is f(;, n) = 2, 2 a.m.U.(5)W,(m) (
2.44) where b d x -k a--s assavow-oso (2.45) If the interval (a, b) becomes infinite,
the set of orthogonal functions U,($) may become a continuum of functions, ...
Then the magnetic moment (5.55) becomes 1 In = #X*. x vi) (5.62) The vector
product (x, x v.) is proportional to the ith particle's orbital angular momentum, Li =
M.(x, x v.). Thus (5.62) becomes Qi - L 5.63 m Žiš. i (5.63) If all the particles in ...
Then inertial effects enter and the conductivity becomes complex. Unfortunately
at these same frequencies the description of collisions in terms of a frictional
force tends to lose its validity. The whole process becomes more complicated.
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"Jackson E&M is about learning how to approximate reliably...the entire book, with few exceptions, is a mathematical discussion on how to solve [the same] 4 problems for different boundary conditions." Read full review
Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
References and suggested reading
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