Scientific American Supplement, No. 388, June 9, 1883Various
Science
Scientific American Supplement, No. 388, June 9, 1883
Various
Science -- Periodicals
From the dynamo the current is conveyed through the axle boxes to the
axles, thence to the tires of the wheels, and finally back by the
rails, which are uninsulated, to the generating machine. The conductor
is laid in lengths of about 21 feet, the lengths being connected by
fish plates and also by a double copper loop securely soldered to the
iron. It is also necessary that the rails of the permanent way should
be connected in a similar manner, as the ordinary fish plates give a
very uncertain electrical contact, and the earth for large currents is
altogether untrustworthy as a conductor, though no doubt materially
reducing the total resistance of the circuit.
The dynamo is placed in the center of the car, beneath the floor, and
through intermediate spur gear drives by a steel chain on to one axle
only. The reversing levers, and also the levers working the mechanical
brakes, are connected to both ends of the car, so that the driver can
always stand at the front and have uninterrupted view of the rails,
which is of course essential in the case of a line laid by the side of
the public road.
The cars are first and third class, some open and some covered, and
are constructed to hold twenty people, exclusive of the driver. At
present, only one is fitted with a dynamo, but four more machines are
now being constructed by Messrs. Siemens Bros., so that before the
beginning of the heavy summer traffic five cars will be ready; and
since two of these will be fitted with machines capable of drawing a
second car, there will be an available rolling stock of seven cars. It
is not intended at present to work electrically the portion of the
line in the town at Portrush, though this will probably be done
hereafter; and a portion, at least, of the mineral traffic will be
left for the two steam-tramway engines which were obtained for the
temporary working of the line pending the completion of the electrical
arrangements.
Let us now put in a form suitable for calculation the principles with
which Mr. Siemens has illustrated in a graphic form more convenient
for the purposes of explanation, and then show how these principles
have been applied in the present case.
Let L be the couple, measured in foot-pounds, which the dynamo must
exert in order to drive the car, and _w_ the necessary angular
velocity. Taking the tare of the car as 50 cwt., including the weight
of the machinery it carries, and a load of twenty people as 30 cwt.,
we have a gross weight of 4 tons. Assume that the maximum required is
that the car should carry this load at a speed of seven miles an hour,
on an incline of 1 in 40. The resistance due to gravity may be taken
as 56 lb. per ton, and the frictional resistance and that due to other
causes, say, 14 lb. per ton, giving a total resistance of 280 lb., at
a radius of 14 inches. The angular velocity of the axle corresponding
to a speed of seven miles an hour, is 84 revolutions per minute. Hence
L = 327 foot pounds, and _w_ = (2[pi] x 84) / 60.
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