As I recall from a lecture in a physical electronics class and from more recent 
reading on the web, under the conditions prevalent in most electronic circuits, 
electrons essentially diffuse through a conductor.  Their major velocity is 
random in both magnitude and direction because of collisions with the atoms of 
the conductor.  An electric field causes them to shift average position a 
little, but not as much as you might think.  Only a rather small amount of net 
movement of electrons is needed to build up a countering field that balances 
the applied field.  If the applied field is in the direction of a complete 
circuit, then they will drift all the way through the circuit bumping their way 
madly past the conductor's atoms.  The net velocity through the conductor may 
be high, but under most conditions, it is still modelled as a kind of quantum 
mechnical diffusion.

Motion of a conductor through a magnetic field has nearly the same effect as an 
applied electric field.  If you search for the "Hall Effect" on the web, you 
will find discussions which include the countering electric field set up when 
the electrons shift.


Mark Holm
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