230 POWER DISTRIBUTION FOR ELECTRIC RAILROADS.
each, running at-a speed of twenty-five to thirty-five miles
per hour, including stops.
In the present state of the art, this is not a serious
matter. The only material difficulties that have been met
in practice are those connected with the delivery of the
necessary current to the moving car, and these are not
now of much moment.
The actual amount of power used for such service is
easy to compute. Taking for a unit a train composed of
one long motor car and one trail car, capable together of
accommodating nearly two hundred people, we can derive
the necessary power. The weight of the two cars complete
would be about fifty tons of which about thirty tons
would belong to the motor car and twenty to the trailer.
Allowing for ten tons live load the total weight of the
loaded train is sixty tons.
The tractive power per ton may be taken direct from
railway practice since the roadbed and rails are, or always
should be, the same ordinarily used in steam railroading.
For such track and speed the tractive coefficient should
never be more than 12 lbs. to 15 lbs. per ton. Taking the
latter figure as covering all ordinary contingencies of curves,
etc., the horizontal effort becomes goo 1bs.; to this must be
added the air resistance, and whatever resistance may be
due to grades. At thirty miles per hour the air resistance
is between 3 1bs. and 4 1bs. per square foot of surface normal
to the direction of motion.
Allowing 200 1bs. for this factor of the resistance we
have a horizontal tractive effort of r1oo lbs. and there
would be required at thirty miles per hour the expenditure
of eighty-eight mechanical horse power.
Maintaining this speed of thirty miles per hour on
grades, the additional horse power required would be
ninety-six for each per cent of grade, or dropping the
speed to twenty miles per hour on the grades, sixty-four
horse power for each per cent of grade.
Allowing about eighty per cent net efficiency from
the motor terminals to the wheels it appears that the elec-
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