Results 1-3 of 86
Then the expansion of an arbitrary function f($, m) is f(k, n) = 2 2 a.m.U.(5)\,(m) (
2.44) where a--s assantov-oso (2.45) If the interval (a, b) becomes infinite, the set
of orthogonal functions U,(5) may become a continuum of functions, rather than a
55 ) becomes = 9 : ( xi x v . ) ( 5 . 62 ) 20 T The vector product ( x ; * v : ) is
proportional to the ith particle ' s orbital angular momentum , L ; = M ; ( xi x v . ) .
Thus ( 5 . 62 ) becomes m = s _ qi L ( 5 . 63 ) 2Mic If all the particles in motion
have the ...
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 .
What people are saying - Write a review
LibraryThing ReviewUser Review - barriboy - LibraryThing
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
LibraryThing ReviewUser Review - aproustian - LibraryThing
"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
References and suggested reading
Multipoles Electrostatics of Macroscopic Media
10 other sections not shown