U.S. patent number 3,730,966 [Application Number 05/219,398] was granted by the patent office on 1973-05-01 for cryogenic cable.
This patent grant is currently assigned to Compagnie Generale D'Electricite. Invention is credited to Marcel Aupoix, Francois Moisson-Franckhauser.
United States Patent |
3,730,966 |
Aupoix , et al. |
May 1, 1973 |
CRYOGENIC CABLE
Abstract
Cryogenic cable of great length consisting of two co-axial
structures, each comprising, a cryogenic fluid transport tubing, a
first layer of conductive material surrounding the tubing, a second
layer of superconductive material surrounding the first layer and
separated from it by a ring having high resistivity, this ring
enabling the flow of the cryogenic liquid between the layers and
preventing any thermal disturbances by magnetic interaction between
layers. The layers of conductors or superconductors and the ring
are wound helically.
Inventors: |
Aupoix; Marcel (Paris 15e,
FR), Moisson-Franckhauser; Francois (91
Bretiany-sur-Orge, FR) |
Assignee: |
Compagnie Generale
D'Electricite (Paris, FR)
|
Family
ID: |
9070663 |
Appl.
No.: |
05/219,398 |
Filed: |
January 20, 1972 |
Foreign Application Priority Data
|
|
|
|
|
Jan 21, 1971 [FR] |
|
|
7102012 |
|
Current U.S.
Class: |
174/15.5;
174/113R; 174/115; 335/216; 174/29; 174/125.1 |
Current CPC
Class: |
H02H
7/001 (20130101); H01B 12/02 (20130101); Y02E
40/641 (20130101); Y02E 40/68 (20130101); Y02E
40/60 (20130101) |
Current International
Class: |
H01B
12/02 (20060101); H02H 7/00 (20060101); H01v
011/00 () |
Field of
Search: |
;174/15R,15C,DIG.6,28,29,113,126CP,126R,128,130,131A,115
;335/216 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Broome; Harold
Assistant Examiner: Grimley; A. T.
Claims
We claim:
1. Cryocable constituted by a structure comprising a first layer of
conductive material, means for cooling said first layer, a second
layer of superconductive material, means for affording electrical
contact between said first and second layers and a material of high
electrical resistivity interposed between said first and second
layers in the form of a keeper ring helically wound on said first
layer, said means for affording electrical contact being
incorporated in said material of high electrical resistivity, in
contact with both said first and second layers.
2. Cryocable according to claim 1, characterized in that the said
material of high resistivity is an electrical insulator, the said
means for affording electrical contact being connections provided
only at points between the said first and second layers.
3. Cryocable according to claim 1, characterized in that it
comprises:
an inner structure and an outer structure, the said inner and outer
structures being coaxial with each other, and the said inner
structure being separated from the said outer structure by an
electrical insulator;
two conduits to convey a cryogenic fluid, one about the said
external structure and the other in the axis of the said internal
structure, the said layers of superconductive material being
situated between the said layers of conductive material.
4. Cryocable according to claim 3, characterized in that the said
second layers of the said inner and outer structures are helically
arranged, with the same pitch and in the same direction.
5. Cryocable according to claim 4, characterized in that the said
helically wound keeper ring has a thickness at least equal to that
of the said second layer of superconductive material.
6. Cryocable according to claim 5, characterized in that the said
insulating element separating the said inner and outer structures
is of polyethylene.
Description
BACKGROUND OF THE INVENTION
The present invention relates to cryogenic cables.
It is known to manufacture cryocables which are capable of carrying
d.c. or a.c. (monophase or polyphase) currents. One such cryocable
comprises a central conduit, generally prepared from an insulating
material, permitting the circulation of a cryogenic fluid. A first
sheet of a conductive metal surrounds the said central conduit, the
said sheet being itself surrounded by a second sheet of a super
conductive material. An insulating sheet surrounds the two
above-mentioned sheets, and the same layered structure is repeated
coaxially. A further conduit providing for the circulation of a
cryogenic fluid surrounds these coaxial layered structures.
In known cryocables, it has been particularly attempted to
eliminate mechanical stresses which might be set up at the level of
the various sheets on the latter being subjected to cooling in a
cryogenic fluid. Such mechanical stresses are radial and
longitudinal stresses.
It is a particularly important condition with respect to such
cryocables to prevent the magnetic field produced by the passage of
current in the superconductive sheet (or layer) of a structure as
described hereinabove from disturbing the adjacent conductive
layer, there by setting up induced magnetic fields therein. Such
induced fields produce an increase in the temperature of the
cryocable, the consumption of cryogenic fluid is increased and
there is thereupon a risk of blocking of the superconductive layer.
This is one of the disadvantages of known cryocables.
In such cryocables, the "sheet" or layer of superconductive
material is constituted by juxtaposed tapes which are helically
wound. Generally, for two successive layered structures, the
superconductive layers have flowing through them equal currents of
opposite direction. Penetration of the magnetic field into the
adjacent conductive layer takes place if the helices of the
superconductive layers are of different pitch or if the said layers
are irregular or comprise, for example, windings in which the turns
are not contiguous.
Another cryocable structure comprises a superconductive layer
deposited on a cryoresistive material. The electrical and thermal
resistance of this structure must be as low as possible, so as to
permit the stabilization of the composite conductor as formed. On
transition of the superconductive layer towards the normal or
blocked state, the current passes into the cryoresistive layer. The
manufacture of such a structure is a delicate matter and a
structure of this kind has the disadvantage that it limits the
blocking of the superconductive layer only to a zone of small
extent, which may result in deterioration due to thermal effect
and, furthermore, locally oppose the return of the superconductive
layer towards it initial superconductive state.
SUMMARY OF THE INVENTION
It is the object of the present invention to remedy the above
described disadvantages experienced in cryocables, and it relates
to a cryocable constituted by a structure comprising means for
cooling a first layer of a conductive material, and a second layer
of superconductive material, characterized in that it comprises
means for providing electrical contact between the first and second
layers, and a material of high electrical resistivity interposed
between the said first and second layers.
BRIEF DESCRIPTION OF THE DRAWINGS
Purely by way of entirely non-limitative illustration, an example
of the carrying into effect of a cryocable according to the
invention will be described hereinbelow with reference to
diagrammatic figures.
FIG. 1 shows, in perspective and in "tiered" section, a
diagrammatic view of a cryocable according to the invention.
FIG. 2 shows a diagrammatic view, in longitudinal section, of the
said cryocable.
Like elements in the two figures have been given the same reference
numerals.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
FIG. 1 shows, in perspective and in "tiered" section, a cryocable
constituted by an inner, coaxial structure 1, comprising:
a central conduit 2 in the axis of the inner structure, providing
for the circulation of a cryogenic fluid. The said conduit may, for
example, be manufactured from a perforated, insulating synthetic
material;
a first "sheet" or layer 3 of a conductive material constituted by
thick strips of aluminum or cryoresistive copper helically wound
about the central conduit 2;
a second layer of a superconductive material 4 comprised of niobium
strips or tapes helically wound about the first layer, the winding
direction of the helices thereof being opposite to the winding
direction of the helices of the first layer;
a material 5 of high electrical resistivity, notably at low
temperature (also called cryoresistive) interposed between the
first and second layers. The said material is interposed between
the two layers in the form of a filament or keeper ring of large
cross-section, helically wound with non-contiguous turns on to the
first layer 3 of conductive material.
The thickness of the said keeper ring is at least equal to that of
the layer of superconductive material.
The cryocable is constituted, furthermore, by an external, coaxial
structure 7 separated from the inner structure, for example, by
thick polyethylene taping 8 electrically insulating the inner and
outer structures.
The said outer structure comprises:
a first layer of a superconductive material 9 comprising for
example niobium tapes or strips helically wound about the thick
insulating taping 8;
a keeper ring 10 of high electrical resistivity, as in the case of
the first structure, being a filament of large cross-section
helically wound with non-contiguous turns about the first
layer;
a second layer 11 of a conductive material comprised of a thick
aluminum tape helically wound about the keeper ring 10;
a further conduit 12 providing for the circulation of a cryogenic
fluid about the two coaxial structures.
Also shown in the said figure is a wide tape 14 helically wound on
the central conduit 2. The said tape may be of copper and its
purpose is to promote thermal exchange between the cryogenic fluid
circulating in the central conduit and the first aluminum layer.
The said central conduit is formed with grooves 16 and perforations
17, the purpose of which it is to permit the propagation of the
cryogenic fluid as far as the second layer of superconductive
material. The cryogenic fluid reaches the said second layer through
the perforations 17 and through the spaces between the helices of
the first layer of conductive material 3.
The insulating keeper ring 5 is wound in helices having widely
spaced turns, thus permitting the cryogenic fluid to circulate
readily between the first layer 3 and the second layer 4, so that
it directly contacts the said second layer of superconductive
material. The insulating element 8 electrically insulates the first
and second structures and is wound in superposed layers.
The external structure is provided with a wide copper strip 15
contacting the second layer of conductive material 11; this
helically wound strip promotes thermal exchange between the
cryogenic fluid circulating at 18 in the conduit 12 and the
conductive layer 11. As in the case of the first structure, the
cryogenic fluid readily reaches the first superconductive layer 9
and readily circulates between the first and second layers 9 and 11
respectively, due to the provision of the keeper ring 10 helically
wound with widely spaced turns.
It is clear that the tapings 14 and 15, the purpose of which it is
to promote thermal exchange may be dispensed with.
The keeper ring 10 plays an extremely important role in each of the
structures. It permits the presence of the cryogenic fluid between
the cryoresistive and superconductive layers. It spaces these two
layers apart so as to prevent the leakage field due to the small
spaces between the strips of superconductive material from reaching
the layer of conductive material which would result in excessive
heating of the said layer. Its main task is to condition the
distribution of the current between layers in the event of loss of
the superconductive stage and to afford a detection process
permitting effective protection of the cryocable.
The layers of conductive material 3 and 11 of the inner and outer
structures are helically wound in different directions and with
different pitches, but substantially at the same angle relatively
to the axis of the cryocable. The purpose of this is to prevent
axial and radial mechanical stressing from being exerted between
the structures when the cryocable is cooled. Furthermore, this
arrangement prevents any considerable torsion couple from damaging
the cryocable when the latter is wound on a reel for transport
purposes and for laying on the terrain. The aluminum strip of the
first layer and the superconductive strip of the second layer have,
for the same purpose, been given a relatively considerable
thickness.
The superconductive strips are helically wound with the same pitch
and in the same direction in both structures, so as not to set up a
magnetic field at the level of the inner layer of conductive
material 3.
This particularly advantageous arrangement makes it possible to
provide a cryocable of great length (400 meters, for example), and
the length of which does not vary when it is cooled, and the
structure of which is not damaged by mechanical stressing due to a
high degree of thermal variation or deformation of the cryocable
when it is wound on a reel.
The advantages of the cryocable according to the invention will
become clear with reference to the description of FIG. 2 which
shows the cryocable in longitudinal diagrammatic section.
In that figure, there are also shown electrical connecting wires
19,20,21,22.
According to a first variant of the invention, the connecting wires
19 and 20 are connected at certain points on the keeper ring 5 made
from a material of high electrical resistivity on the first
structure, the wires 21 and 22 being connected to the keeper ring
10 of the second structure.
Each cryocable section has a length of 400 meters for example and a
connecting wire is disposed at each end of the section. According
to the said first variant of the invention, the keeper ring is a
high-resistivity wire (approximately 100 ohm-centimeters, for
example, made from charged polyethylene). If the superconductive
layer blocks, the current will flow in the conductive layer through
intermediary of the high-resistivity keeper the turns of which
contact each of the two conductor and superconductor layers. The
connecting wires thus described permit, furthermore, the protection
of that section of the cryocable which has passed from the
superconductive state to the blocked state. The current in each
layer depends on the abscissa of the blocked zone along the
section.
According to a second variant, the high-resistivity material
constituting the keeper ring is an electrical insulator. The
electrical contact is established only at predetermined points
along the cryocable section concerned. For example, at points 23
and 24 for the inner structure and at points 25 and 26 for the
outer structure.
Detecting wires 19,20,21,22 are disposed as hereinabove for
detecting the blocking of the superconductive layers. On the
superconductor layer blocking, the current passes into the
superconductive layer through intermediary of contacts such as
23,24,25,26. The said detecting wires are surrounded by a lead
sheath and debouch for example into the central conduit 2 for the
inner structure and into the conduit 12 for the outer
structure.
The connecting wires permit permanent monitoring of the
satisfactory functioning of the cryocable. Any incident resulting
in a local loss of superconductive state in the superconductive
layer is indicated by slow heating of this layer. The connecting
wires permitting the detection of this incident furthermore permit
protection of the cryocable by means of circuit breakers the
operating velocity of which is relatively low. On blocking,
according to the first variant of the invention, the current flows
through the conductive layer over a length of 200 meters, on either
side of the blocked zone, with reference to sections 400 meters
long. This particularly advantageous arrangement permits rapid
reduction of the current strength in the superconductive layer at
the level of the blocked zone of the superconductive layer, thereby
preventing damage to that zone. It should be noted that, on
blocking taking place, the impedance of the superconductive layer
is higher than that of the conductive or cryoresistive layer.
The voltage drop brought about by the passage of current in the
conductive layer over some hundreds of meters enables the blocking
to be detected.
Thus, the connecting wires permit detection of the presence of a
magnetic field in the space between the conductive layer and the
superconductive layer. The said magnetic field appears in
consequence of the blocking of the superconductive layer. An
induced voltage appears between the points 23 and 24 or between the
points 25 and 26. Localization of the blocked zones is effected by
comparing the voltages at the ends of the connecting wires of
different adjacent sections.
According to the second variant of the invention, the
high-resistivity keeper ring is an electrical insulator. Electrical
contact is established at regular intervals between conductive and
superconductive layers, for example, at the end of each section,
every 400 meters. Blocking detection is effected in the same manner
as in the first variant, but the current in each layer does not
depend on the abscissa of the blocked zone along the section.
It is clear that the number of points of connection, which has been
selected equal to two for each structure of a 400 meter section,
may be higher.
It is also clear that the diagrammatic figures just described are
merely an example of the carrying into effect of a cryocable
according to the invention. One material could be replaced by
another material without thereby exceeding the scope of the
invention. The said cryocable and the associated detection system
described with reference to a.c. current could be employed with
d.c. current.
* * * * *