Hawkins Electrical Guide v. 03 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applicationsHawkins, N. (Nehemiah)
Science
Hawkins Electrical Guide v. 03 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applications
Hawkins, N. (Nehemiah)
Electrical engineering -- Handbooks, manuals, etc.
Fig. 617.--Diagram of Leeds and Northrup bridge for locating faults in
power circuits, showing arrangement of the connections including the lead
cables and galvanometer contacts. Make connections as shown. The clamps
must be so fastened at A and C that the contact resistances will be very
small. This contact resistance will figure as an error in the measurement.
If, for instance, the contact resistance were equal to .001 of an ohm,
and the wire were of such a size that .001 of an ohm were equal to the
resistance of 20 feet of the cable, there would be an error of 20 feet
in the location of the fault. For this reason all contact resistances
throughout the loop from A to C must be extremely small. The battery is
to be connected to the posts marked Ba., and the post marked Gr. is to
be grounded. It will very frequently happen that the ground is to the
cable sheath or some other conductor. In this case, the binding post Gr.
should be grounded to this conductor. Sufficient battery should be used
to give a readable deflection on the galvanometer for a small movement of
the contact on the bridge wire. The fault is located by the usual Murray
formula. If, for instance, the galvanometer show no deflection when the
contact is at 300 on the scale, it would indicate that the fault is at a
distance from A equal to .003 of the total length of the loop from A to C.
A testing current of five amperes may be used with this bridge. In cases
of necessity, this current may be increased to eight amperes, but when
this current is used it should not be allowed to pass through the bridge
for a longer time than is necessary. It frequently happens that small
faults which have a very high resistance develop in high pressure cables.
Such faults are likely to break down and result in damage and should be
located. It is usually impossible to locate these faults until they have
been partially carbonized. This must be done by applying a sufficiently
high voltage between the cable and the sheath (or whatever it is grounded
on) to break down the fault. In order to prevent the breaking down process
from resulting in a serious burn out a high resistance must be placed in
the circuit which will prevent an excessive current, or the circuit must
be carefully fused. The former procedure is the better.]
Location of Faults where the Loop is Composed of Cables of Different Cross
Sections.--Faults in loops of this character may be located with the same
degree of accuracy as those in loops of a uniform cross section, provided
the length and cross section of each length of cable are known. An example
will illustrate the method:
In the diagram, fig. 617, assume the length of the cable AE to be
550 yards of 25,000 cir. mil., EF, 500 yards of 40,000 cir. mil., and
FC, 1,050 yards of 30,000 cir. mil. These lengths must be reduced by
calculation to equivalent lengths of one size, and for this purpose it is
best to select the largest size. The results of this calculation are as
follows:
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