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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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A soul crushing technical manual written by a sadist that has served as the right of passage for physics PhDs since the dawn of time. Every single one of my professors studied this book, and every ... Read full review
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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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