Longview,
Really strange things are happening at that website, too.
I have no idea why. Maybe some web-bot is interfering with these sites.
However, it seems if you get to that website (or some other) thru the Google search:
Feynman "two kinds of momentum"
- then the link to the pdf works.
The basic idea, though, is that a linear current flow generates a magnetic vector
potential depending on the current and its extent. At any point, this vector potential
is a vector pointing in the same direction as the current. It represents the coupling
between the charged particles.
The value of this vector potential is proportional to how much momentum
a charged particle in the current flow acquires in a collision -i.e., the more forcefully
it is impeded by an obstacle, the more momentum it draws from this momentum field
to push into the obstacle (say another charged particle), an continue on its path.
When two oppositely charged particles collide in an intense current, say a idealized
collision where both have equal and opposite momenta, then both will draw the
same momentum (but in opposite directions) from the vector potential. If the current
is intense, this momentum will be large, and light particles, like electrons, will acquire
a large gain in momentum, giving them very large effective masses in collisions.
It think this is sort of analogous to how the atom at the tip of an speeding arrow borrows
momentum from the arrow body when it hits a target, or how the lead car of long
train will impact an obstacle with much greater momentum than its own, by its
coupling to the rest of the train.