THE RETURN CIRCUIT. 45
easier path through the supplementary conductors. Hence
electrolytic action was practically obviated so far as the
cables were concerned.
A measurement of the current thus collected from the
telephone cables into a main ground wire from the station
showed over 500 amperes capable, if flowing continuously,
of eating away 37,500 lbs. of lead per year. And as this
current did not include that which found its way to water
and gas pipes, the real amount of current which left the
rails and wandered home through underground conductors
was considerably larger than the figure mentioned, prob-
ably several times as great. ‘The distribution of this cur-
rent is so irregular from place to place, as indicated on the
map, that it would be very hard indeed to estimate the total
proportion it bears to the whole current on the system.
So far as data are available however they indicate that we
would not be wide of the truth in saying that ten to twenty
per cent of the current on the system may follow other
paths than that through the rails and bonds. Even more
than this may appear in occasional instances. So while the
earth helps the return circuit directly but little, buried
conductors may help very materially, perhaps to their own
serious detriment. It should be remembered that the elec-
trolytic action is not necessarily proportional to the differ-
ences of potential such as are noted on the maps. The
places most injured depend on local conductivity and some
of the worst instances recorded have occurred where the
measured potential difference was only one or two volts.
Figs. 33 and 34 give a graphic idea of the kind of
damage that is done to pipes by electrolysis from stray
currents. Fig. 33 shows the effect of corrosion on an iron
gas pipe, and Fig. 34 that on a lead water pipe. Both are
from photographs of the ‘‘horrible examples.”’ As the
action tends to become concentrated in spots, a pipe may be
perforated in a rather short time. Iron water pipe has some-
times been riddled in five to eight months. That this is
easily possible may be readily seen, for suppose that con-
ditions are such as to get in a certain spot a flow of half