U.S. patent number 3,594,492 [Application Number 04/862,353] was granted by the patent office on 1971-07-20 for pipe-type cable systems with reduced ac losses.
This patent grant is currently assigned to General Cable Corporation. Invention is credited to George Bahder, Carlos Katz.
United States Patent |
3,594,492 |
Bahder , et al. |
July 20, 1971 |
**Please see images for:
( Certificate of Correction ) ** |
PIPE-TYPE CABLE SYSTEMS WITH REDUCED AC LOSSES
Abstract
A magnetic, low-loss liner in a metal pipe reduces the AC loss
of high-voltage electrical cable enclosed within the pipe; or the
cable in the pipe can be wrapped with a sheet or tapes of the
magnetic low-loss material. Tapes used for the purpose can be
plastic with suitable metal, such as ferromagnetic material of high
permeability distributed through the plastic. V
Inventors: |
Bahder; George (Edison, NJ),
Katz; Carlos (Bayonne, NJ) |
Assignee: |
General Cable Corporation (New
York, NY)
|
Family
ID: |
25338298 |
Appl.
No.: |
04/862,353 |
Filed: |
September 30, 1969 |
Current U.S.
Class: |
174/36; 174/113R;
174/26R; 174/108; 336/218 |
Current CPC
Class: |
H01B
7/26 (20130101); H01B 9/02 (20130101); H01B
9/0611 (20130101) |
Current International
Class: |
H01B
7/26 (20060101); H01B 9/00 (20060101); H01B
9/02 (20060101); H01B 9/06 (20060101); H01B
7/18 (20060101); H01b 009/02 () |
Field of
Search: |
;174/24,25,26,32,35,36,102,103,105,106,108,109,113,117.1
;336/218 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
|
|
|
|
|
|
|
870,953 |
|
Jun 1961 |
|
GB |
|
880,658 |
|
Apr 1943 |
|
FR |
|
Primary Examiner: Myers; Lewis H.
Assistant Examiner: Grimley; A. T.
Claims
We claim
1. An electrical cable system for transmitting alternating-current
when the cable is enclosed in a pipe, including a group of
individually insulated conductors extending side by side, and a
special magnetic shield surrounding at least three-quarters of the
circumference of the group, the shield being made of material
having high permeability and low loss, the magnetic shield having a
reluctance along its circumference lower than 5.times.10.sup.7 1/H
per foot of the cable system, an electrical resistance in the
direction of the length of the cable system higher than
10.sup..sup.-4 ohms per foot of the cable system, and an electrical
resistance in the direction of the radius of the cable system
greater than 1 ohm per foot of the cable system.
2. The electrical cable system described in claim 1 characterized
by the magnetic shield having a reluctance along its circumference
lower than 5.times.10.sup.7 1/H per foot of the cable system, an
electrical resistance in the direction of the length of the cable
system highe r than 10.sup..sup.-4 ohms per foot of the cable
system, and an electrical resistance in the direction of the radius
of the cable system greater than 1 ohm per foot of the cable
system.
3. The electrical cable system described in claim 1 characterized
by the special magnetic shield being wrapped around the outside of
the group of insulated conductors, and a skid wire over the outside
of the shield.
4. The electrical cable system described in claim 1 characterized
by the individual conductors being wrapped together by the special
magnetic shield.
5. The electrical cable system described in claim 1 characterized
by there being three conductors in the group and each of which has
a conductor shield, an insulating layer over the conductor shield,
an insulation shield covering the outside of the insulation,
moisture protection means outside of the insulation shield, the
special magnetic shield extending around the full circumference of
the group of conductors outside of the moisture protection means,
and a skid wire over the outside of the special magnetic
shield.
6. The electrical cable system described in claim 5 characterized
by the special magnetic shield comprising tapes made of plastic
material with metal distributed through the plastic, the metal
distribution including metal that is oriented so that the
projections thereof on the inner surface of the tape cover the
entire inner surface thereof.
7. The electrical cable system described in claim 4 characterized
by the special magnetic shield being a helically wound layer of
flexible tape made of plastic material having two rows of flexible
rods therein with the rods extending lengthwise of the tape and
with the rods of one row in staggered relation to the rods of the
other row, all of the rods being generally parallel to one another
and the rods of each row being spaced from one another transversely
of the tape, and the rods of one row being of a diameter greater
than the spacing of the rods of the other row.
8. The electrical cable system described in claim 4 characterized
by the special magnetic shield being a helically wound layer of
flexible tape made of plastic material having two rows of plates
therein with the plates extending lengthwise of the tape and with
the plates of one row in staggered relation to the plates of the
other row, all of the plates being generally parallel to one
another and the plates of each row being spaced from one another
transversely of the tape, the plates of one row being of a width
greater than the spacing of the plates of the other row.
9. The electrical cable system described in claim 4 characterized
by the special magnetic shield being a helically wound layer of
flexible tape made of plastic material having ferromagnetic
material dispersed throughout the plastic.
10. The electrical cable system described in claim 4 characterized
by the special magnetic shield being made of flexible magnetic
tape.
11. The electrical cable system described in claim 10 characterized
by the magnetic tape being intercalated with metal tape.
12. The electrical cable system described in claim 4 characterized
by the special magnetic shield being a helically wound layer of
flexible metal tape with the metal corrugated and the corrugations
extending transversely of the tape, and with layers of plastic
bonded to the surfaces of the corrugated metal.
13. The electrical cable system described in claim 4 characterized
by the special magnetic shield being made of flexible magnetic
tape, a metal pipe in which the cable is enclosed, and a continuous
strip of highly conductive metal connecting the shield to the pipe
in which the cable is enclosed.
14. The electrical cable system described in claim 1 characterized
by a metal pipe in which the cable is enclosed, the special
magnetic shield being a liner in the pipe in contact with the
inside surface of the pipe and extending around substantially the
entire circumferential extent of said surface.
15. An electrical cable system enclosure including a metal pipe,
and a liner in the pipe made of metal having higher permeability
and lower loss than the metal pipe the liner having a reluctance
along its circumference lower than 5.times.10.sup.7 1/H per foot of
the cable system, an electrical resistance in the direction of the
length of the cable system higher than 10.sup..sup.-4 ohms per foot
of the cable system, and an electrical resistance in the direction
of the radius of the cable system greater than 1 ohm per foot of
the cable system.
16. The electrical cable system enclosure described in claim 15
characterized by the liner being an inner pipe enclosed in the
first pipe.
Description
BACKGROUND AND SUMMARY OF THE INVENTION
This invention relates to high-pressure pipe-type cables installed
in metallic-type pipes, such as a steel pipe. These cables operate
at high pressure of oil or gas and are used for underground and
submarine transmission of electric power at high and extra high
voltages. In particular, the present invention relates to pipe-type
cable systems with reduced AC losses.
The use of steel pipes as an enclosure for the three-phase cable
system increases and distorts the magnetic field in the conductors,
causing a relatively large increase in the conductor's AC
resistance over the corresponding values for the cables placed in
air. In addition to the increase in conductor AC resistance, big
losses are originated in the pipe due to eddy currents and
hysteresis. For instance, in a three-phase, 345 kV, HPOF cable
system having segmental copper conductors with a 2000 MCM cross
section, the total losses in pipe, with the conductors arranged in
a triangular formation, are increased about 35 percent with respect
to the losses measured in air and with the conductors arranged in
cradle formation this increase is about 50 percent of the
corresponding values in air.
Several attempts have been made in the past to reduce the increase
in AC resistance due to the use of steel pipes in high-pressure
cable systems. The following methods were proposed to reduce the AC
losses in pipe-type cables:
1. The use of pipes made of a different material than steel.
2. The use of magnetic pipes provided with a section of nonmagnetic
material, or a section having longitudinal slits (U. S. Pat. No.
2,718,542 ) or provided with circumferential slits (U.S. Pat. No.
2,787,651).
3. The use of a pipe lined with a "magnetic field trap" (U.S. Pat.
No. 3,160,702).
Considerations made in the past indicated that losses at 60 Hz
could not be reduced over those attainable with steel pipes, by
using pipes made of any available nonmagnetic metal of reasonable
low price. Tests made using nonferrous materials such as Everdur
pipe (6.5 percent conductivity of copper) and aluminum pipe (61
percent conductivity of copper) and aluminum pipe (61 percent
conductivity of copper) gave AC resistance of the same order of
magnitude as obtained with steel pipes.
U. S. Pat. No. 2,718,542 "Electric Cable Systems", describes the
use of a magnetic pipe having a small longitudinal section of
nonmagnetic material and/or suggests the use of a pipe made of
magnetic material provided with numerous longitudinal slits. U.S.
Pat. No. 2,787,651, "Electric Cable Systems", suggests the use of a
pipe made of magnetic material provided with numerous
circumferential, or a helical slit. These methods provide only a
very slight reduction in the AC losses, much below the value which
might be interesting from the practical point of view. This is due
to the fact that the major portion of the losses are caused by eddy
currents and the proposed methods give only a small reduction of
these currents.
U.S. Pat. No. 3,160,702, "Alternating Current Pipe CAble System
with Magnetic Field Trap", discloses the use of a pipe lining
material made of a dielectric resin and having dispersed in it a
magnetic material. Such pipe lining creates an insulation layer
between the cables and the pipe and consequently the cable is
insulated from the pipe. The use of such a pipe appears to be
dangerous for the cable system in case of lightning, and switching
surges, and in case of ground faults which cause overvoltages.
Under overvoltage conditions the lining material may break through,
causing arcing which destroy the cable shield and subsequently, the
cable insulation.
With the invention described in this specification, the AC losses
in pipe-type cable systems can be substantially reduced without
increasing the susceptibility of the system to overvoltages. For
this purpose the cables installed in the pipe must be surrounded
with a layer of special magnetic material. The surrounding layer
should cover at least three-quarters, but preferably more, of the
cable assembly circumference and must have the following
properties:
1. The reluctance of the layer along the circumference should be
lower than 5.times.10.sup.7 1/H per foot of cable.
2. The 4 resistance in the longitudinal direction should be higher
than 10.sup..sup.-4 ohms per foot of cable.
3. The electrical resistance in the radial direction should be less
than 1 ohm per foot of cable.
With this invention at least 23 percent of the power loss, when
transmitting AC can be saved; or the line-current-carrying capacity
can be increased accordingly.
Other objects features and advantages of the invention will appear
or be pointed out as the description proceeds.
BRIEF DESCRIPTION OF DRAWING
In the drawing, forming a part hereof, in which like reference
characters indicate corresponding parts in all the views:
FIG. 1 is a diagrammatic view showing electric cables enclosed
within a pipe and provided with a special magnetic shield, in
accordance with this invention;
FIG. 2 is a modification of the construction shown in FIG. 1 with
the special magnetic shield made a part of the cable;
FIG. 3 is a diagrammatic view showing material from which the
special magnetic shield can be made;
FIG. 4 is a greatly enlarged sectional view of the line 4-4 of FIG.
3;
FIG. 5 is a view similar to FIG. 4 but showing a modified
construction of the special magnetic shield material;
FIG. 6 is a sectional view showing another form of material for the
special magnetic shield;
FIG. 7 is a sectional view taken on the line 7-7 of FIG. 6;
FIG. 8 is a view similar to FIG. 6 but showing still another
modification of the invention;
FIG. 9 is a sectional view taken on the line 9-9 of FIG. 8;
FIG. 10 is a sectional view similar to FIGS. 6 and 8 but showing
still another modification of the invention;
FIG. 11 is a sectional view taken on the line 11-11 of FIG. 10;
and
FIG. 12 is a graph showing one set of new results obtained with
this invention.
DESCRIPTION OF PREFERRED EMBODIMENTS
FIG. 1 shows electrical cables 10 of conventional construction and
each of which comprises a center conductor 12, a conductor shield
14, insulation 15, an insulation shield 16, overlying moisture
protection tapes 18 and skid wires 20. These cables 10 carry
three-phase power and they are enclosed in a metal pipe 22, usually
a steel pipe.
In order to reduce the alternating current power losses, the metal
pipe 22 has a special magnetic liner 24. This liner provides a
magnetic shield inside the pipe 22. The liner 24 is made of
material having high permeability and low loss. The magnetic shield
can be a metal alloy, as will be explained in connection with the
other figures.
When used as a liner for the pipe 22, the magnetic shield 24
preferably covers the entire inside surface of the pipe, but this
is not essential. For good results, however, the shield 24 should
extend around at least three-quarters of the circumference of the
pipe. The shield 24 reduces the magnetic flux in the pipe 22 and
thereby decreases the AC losses. On the other hand, the high
longitudinal resistivity of the shield 24 prevents high losses
within the shield.
In describing the special magnetic shields of this invention as
having high permeability and low loss, these terms are to be
understood as designating the relation between the magnetic flux
density at a point in a material to the magnetic intensity at the
same point, and the reluctance and resistance characteristics
described above. In describing the magnetic shield as being made of
a metal alloy, the term "alloy" is used in a special broad sense to
include not only true alloys of metals but also metal in powdered
form dispersed throughout a plastic matrix or metal encapsulated in
plastic tapes or sheets, as will be described in connection with
FIGS. 5--11.
With the construction shown in FIG. 1, this invention requires no
change in the design of the cables. In the construction which will
be described in connection with FIG. 2, special cable is used which
does not require the insertion of the liner 24 into the pipe
because the liner is made a part of the cable itself and is,
therefore, conveniently pulled into the pipe with the cable.
FIG. 3 shows a section of the metal sheet before it is inserted
into the pipe 22 of FIG. 1. The sheet is preferably a strip having
a width substantially equal to the inside circumference of the pipe
in which it is to be used. This particular sheet is a low-loss,
grain-oriented silicon steel, as indicated by the cross section
shown in FIG. 4.
The low-loss, high-permeability metal can also be manufactured into
a pipe with an outside diameter equivalent to the inside diameter
of the pipe 22 and factory installed in the pipe 22.
If the material used for the special magnetic shield is
sufficiently flexible it can be wrapped as a sheet around the group
of cables; but to make this more practical with cables that have to
be pulled into long lengths of pipe 22, a cable of special
construction is used.
FIG. 2 shows such a special cable. Corresponding parts are
indicated by the same reference characters as in FIG. 1 but with a
prime appended. The individual shielded and insulated conductors of
FIG. 2 are wrapped in a special magnetic shield 34 which is formed
by tapes wound helically, preferably with overlapping convolutions,
around the insulated and shielded conductors to form a composite
cable. Skid wires 36 are wound over the special magnetic shield
34.
If the resistivity of a tape 38 used for the magnetic shield 34
would otherwise be too high, it is intercalated with another tape
40 which may be nonmagnetic or magnetic material but which has good
electrical and thermal conduction properties. Copper or aluminum
are appropriate for the tape 40. With this intercalated
construction, fault currents or overvoltages can be easily
dissipated to ground.
If the special cable construction shown in FIG. 2 is not
commercially available, the wrapping of the tapes 38 and 40 and the
application of the skid wires 36 can be done in the field at the
time the cables are to be pulled into the pipe 22'.
FIGS. 1 and 2 show the conductors 12 and 12', respectively, in a
triangular configuration. The invention can be used with cables in
a cradle configuration or in any other configuration but because
the triangular configuration in a cable system has lower losses, it
is more efficient for use with this invention.
FIG. 5 shows a cross section of a tape made of plastic material
having ferromagnetic material dispersed through the plastic. The
ferromagnetic material can be metal or synthetic; and it should
have a very fine powdery appearance before being mixed. Magnetic
materials such as polycrystalline ceramics used in the manufacture
of ferrites, containing iron, oxygen and one or more of the
following metals: copper, nickel, zinc, cadmium, magnesium,
manganese, or others providing the characteristics of magnetic
ferrites, are appropriate for this invention.
FIGS. 6 and 7 show a special construction in which a low-loss
magnetic material in the form of rods 50 are imbedded or
encapsulated in a plastic tape 52. These rods 50 are disposed in
two rows with the rods in one row staggered in relation to the rods
of the other row. The rods preferably extend in the direction of
the length of the tape 52 and in the construction shown, the rods
50 are of the same diameter.
The rods 50 are parallel to one another and are spaced from one
another. It is desirable to have the diameters of the rods at least
one row greater than the spacing of the rods of the other row so
that the projections of the rods on the top and bottom surfaces of
the tape cover the entire area of these surfaces.
FIGS. 8 and 9 show a modified construction in which plates 56 are
substituted for the rods 50. These plates have widths greater than
the spacing between them and they are staggered so that the
projections of the plates cover the entire areas of the top and
bottom surfaces of the tape 58. As shown, the plates 56 provide
substantially a double layer of metal in the tape 58.
FIGS. 10 and 11 show another construction in which a sheet or tape
of metal 60 is of continuous extent throughout the length and
breadth of a tape 62. This metal 60 is a low-loss magnetic metal,
as in the case of the rods and plates of FIGS. 6--9, and its
flexibility is increased by having it corrugated with the
corrugations extending transversely of the length of the tape, and
preferably at right angles to the length of the tape. The metal 60
is coated on both sides with plastic 64.
The magnetic low-loss metal alloys and the flexible combination or
composite magnetic materials previously described, can be used in
the form of pipes, sheets, tapes, strips or any other form suitable
for the proposed application. The materials can be used in single
or multiple layers, they can be plain or embossed, they can be
coated or not coated. In the case where they are used in the form
of tapes, they may be applied butt and if the thickness allows,
overlapped. The magnetic shield materials to be used in the
described systems have to be able to: withstand the mechanical
stresses, which may be developed during installation or service
life of the cables without breaks or tears; they have to be
compatible with the oils (natural or synthetic) used in cable
installations; and they have to be able to withstand the cable
service temperatures. Some high polymer materials, such as
polytetrafluorotheylene, hexafluropropylene, polyethylene
terephtalate, polypropylene, polycarbonate and others are
appropriate for use as encapsulating materials; however, any other
materials providing the above characteristics could be used for
this application. The combination or composite material can be
irradiated to improve the memory and thermal characteristics of the
plastic.
In cases where the tape used for the special magnetic shield has
electrical resistance which is otherwise too high, the insulation
shield can be connected to the metallic pipe by a continuous strip
of highly conductive material applied intercalated with the
magnetic shield material. It should be understood that the low-loss
magnetic materials used for the special magnetic shield of this
invention can be applied in either single or multiple layers; and
that the material can be plain or embossed and coated or not
coated, as conditions warrant.
FIG. 12 is a graph showing new results obtained with this
invention, as compared with the results obtained by the prior
art.
FIG. 12 allows the comparison of two sets of AC/DC resistance
ratios measured at various currents on an assembly of three cables
in a triangular configuration. In both cases, the same 10 inches ID
steel pipe was used. The upper curve indicates AC/DC resistance
ratios for the cables installed in the pipe without a magnetic
shield (present practice). The lower curve indicates AC/DC
resistance ratios for the same cables installed using the
high-permeability, relatively high-resistivity screen in accordance
with one of the variations of the disclosure (wrapped as
illustrated in FIG. 2). The pipe used for these tests is similar to
that used by an electric utility for the installation of 345 kV,
HPOF cables. The high-permeability material used in this particular
case consisted of a grain-oriented silicon steel tape, 2 inches
wide, 14 mil thick, insulated with an inorganic coating. This
material had a relative magnetic permeability (.mu.) of about 6000
at a flux density of 50 gausses and a resistivity of 50
microhm-centimeter.
FIG. 12 gives the AC/DC resistance ratios; which are practically
independent of the current. For any given current the AC/DC ratio
is equal to the ratio of watts loss when carrying
alternating-current to the watts loss when carrying
direct-current.
Further tests indicate that by using other variations of these
methods, considerable savings in electric power or increase in
current-carrying capacities can be obtained. As an example,
following are a few of the results of measurements made at 800
amps. with the cables in a triangular configuration in the
previously described steel pipe:
Cable Assembly: AC/DC Resistance Ratios
__________________________________________________________________________
1. In a steel pipe as presently used 1.66 2. In a steel pipe lined
with a high permeability silicon steel, except for a longitudinal
strip 1 inch wide 1.45 3. In a steel pipe lined with a high
permeability silicon steel (100 percent coverage) 1.42 4. In a
steel pipe with the three cables wrapped in a sheet of high
permeability silicon steel 1.42
__________________________________________________________________________
It was found that with the cables and conditions used during these
tests, an increase in the thickness of the silicon steel above the
14 mils used would not produce any further significant decrease in
the AC/DC resistance ratios of this cable system.
The preferred embodiments of the invention have been illustrated
and described and they are defined in the appended claims.
* * * * *