 |
Description  |
|
|
BACKGROUND OF THE INVENTION
The invention relates to equalizing arrangements for low temperature lines
in general and more particualrly to such an arrangement which prevents
undesired forces.
Low temperature lines having at least one rigid inner tube which contains
at least one tubular compensating element for the equalization of length
changes and is enclosed by an outer tube, the lines being used for the
conduction of a cryogenic medium, are known. These and other low
temperature lines are provided for the transport of gaseous or liquefied
cryogenic media whose temperatures are considerably below the ambient
temperature of these lines. In general, they contain at least one inner
tube through which the cryogenic medium flows and which, therefore, has a
temperature level in its operating state which at least approximates that
of the cryogenic medium.
Low temperature cables having at least one dc or ac conductor cooled to low
temperature and kept at low temperature by a cryogenic medium disposed in
an inner tube are special types of low temperature lines. Where
superconductive material is provided as the conductor material, the
cryogenic medium is perferably helium. It is for this reason that the
inner tube of such a cable is also called helium tube.
Such low temperature lines operate with relatively good thermal efficiency
if additional measures are taken to limit heat exchange between the
cryogenic medium in the inner tube and the outside temperature. In a
special embodiment of such a low temperature line, therefore, the inner
tube is concentrically enclosed by another tube. This other tube serves as
a thermal shield and is also called a radiation shield. The radiation
shield may expediently be kept, by another medium such as liquid nitrogen,
at a temperature level higher than that of the inner tube. The radiation
shield in turn is surrounded by an outer tube insuring the vacuum
tightness of the entire low temperature line, this outer tube also acting
as protection against mechanical damage to the inner tube and the
radiation shield. Between the inner tube, in which are disposed, for
example, electric conductors, and the outer tube there may, moreover, be
disposed a large number of insulating foil layers to prevent heat transfer
between the outer and inner tube. These insulating foil layers are also
known as superinsulation. A stable positioning of the tubes enclosing each
other is obtained by appropriate mechanical structures which allow simple
assembly of these tubes and which keep the heat transfer between the tubes
to a minimum.
One difficulty with such lines is that a rigid inner tube opposite a rigid
outer tube changes its length when cooled to the operating temperature
from the ambient temperature, or when it must be reheated from the
operating temperature to the ambient temperature, such as in the case of a
malfunction. For, all materials which can be used for the inner tubes to
carry cryogenic media such as liquefied or gaseous nitrogen, hydrogen or
helium, will shrink considerably when cooled from room temperature to the
operating temperature. For example, at a temperature drop from 300 K to 4
K, this shrinkage amounts to 4.2.permill. for aluminum, 2.8.permill. for
chrome-nickel steel and 3.2.permill. for copper. Even the shrinkage of
special steel alloys, known by the name Invar, which shrink by only about
0.3.permill. for the temperature drop mentioned, cannot be neglected when
long tubular lines are involved. In order to equalize length reductions of
these lines it is generally necessary, therefore, to insert appropriate
compensation elements such as sections of corrugated tubing in the inner
tubes.
An appropriate embodiment of a low temperature line in which both the outer
tube and the inner tube, in which conductor wires cooled to low
temperature may be disposed, for example, are or rigid design, is
described in the journal "Naturwissenschaften" 57 (1970), pages 414 to 422
in particular page 420, FIG. 7b.
The inner tube contains a compensating element in the form of a corrugated
tube, by means of which shrinkage differences between the inner and outer
tube, occurring when the inner tube is cooled to the operating temperature
of the cryogenic medium flowing in it, can be equalized. Moreover, a
radiation shield is disposed between the inner and the outer tube. This
radiation shield is provided with cooling tubes in which another coolant
may flow and which contain corresponding compensation elements for the
equalization of shrinkage differences.
In order to keep the heat input into the cryogenic media carried by such
low temperature lines as small as possible, a high vacuum is provided
between the outer and the inner tube, and superinsulation and radiation
shields are generally disposed between these tubes. In addition, it is
necessary to fix the inner tube inside the outer tube so as to be as free
of forces as possible in order to be able to design support or suspension
devices of small cross-sectional area for the inner tube. It is then
possible to keep the introduction of heat through these devices
correspondingly low.
However, a study of the function of the cooling circuits for such low
temperature lines during a cooling process, during operation or while
their inner tubes are warming up will reveal that the known corrugated
tube compensating elements only imperfectly meet the requirement that the
inner tubes be held inside the outer tubes without stress. For example, in
order to cool an inner tube continuously from room temperature to the
intended operating temperature by means of a cooling gas such as helium, a
considerable pressure such as of 10 to 15 bar is required because of the
relatively low heat capacity of the gas. The tube diameter of inner tubes
which may be intended to accommodate superconducting phase conductors of a
superconducting cable are as large as 120 mm or even larger, for example.
If a corrugated tube is now inserted in such an inner tube, it will be
pushed apart with a corresponding, considerable force which may be as
great as 1.1 to 1.7 tons. But the elastic force of a corrugated tube
beyond its unstressed position is generally only 100 to 120 kg. Therefore,
it is well below that sufficient to counteract the force acting on the
corrugated tube. In order to not overstress the corrugated tube, it must,
therefore generally be provided with a travel limiting device.
At the start of a cooling process of such a low temperature line whose
inner tube is still warm, a corrugated tube inserted into the inner tube
will therefore be expanded, due to the internal pressure, to its maximum
length predetermined by the travel limiting device. The stretched inner
tube is then too long by an amount equal to the travel of the corrugated
tube. If, for example, the terminations of such a low temperature line are
disposed perpendicular to the longitudinal direction of the line, the
flanges at the terminations and at the required elbows are stressed in
shear. If, on the other hand, the terminations are in the continuation of
the straight inner tube, the corrugated tube will be compressed, but the
terminations will be acted upon by the force mentioned.
Similar conditions prevail if a boiling cryogenic medium is immediately
admitted to an inner tube of the low temperature line. The cryogenic
medium then enters the inner tube, which is still at room temperature, at
one end of the low temperature line. It is evaporated immediately and
heated to room temperature after a short transition zone. In this process,
a pressure of several bar is generated which exerts a force on the
corrugated tube in the manner already described. Therefore, the corrugated
tube is pushed apart while almost the entire length of the inner tube is
still at room temperature. The same stresses will then occur at the
terminations.
The forces occurring during the cooling processes described above dissipate
only gradually with dropping inner tube temperature and disappear only
when the operating temperature has been attained over the entire length of
the inner tube. This means that the corrugated tube inserted in the inner
tube is actually ineffective because it is constantly in its limit
position determined by the travel limiting device. It behavior during a
cooling process is approximately that of a smooth, rigid piece of tubing.
SUMMARY OF THE INVENTION
Accordingly, it is an object of the present invention to create, for the
above described low temperature line containing a length compensating
element, an equalizing arrangement in which the difficulties described
above are either completely avoided or at least greatly minimized.
According to the present invention, this problem is solved, for an
equalizing arrangement of the type mentioned above, by associating an
expansion device, which permits the length of the compensating element to
be preset as a function of the inner tube temperature, with the
compensating element.
The compensating element such as a piece of corrugated tubing, inserted
into the inner tube of a low temperature line, is compressed by a
predeterminable amount at room temperature, i.e., when the inner tube is
still warm, and its expansion is released only to the extent that the
inner tube is shortened due to shrinkage during a cooling process. Loads
on supports and suspensions between the inner and outer tube and on
terminations associated with the line are advantageously avoided by these
measures. Thus, an unstressed connection of the inner tubes to
terminations is obtainable because the length of the inner tube including
the compensating element can be kept constant over the entire temperature
range of the low temperature line.
To vary the length of the compensating element, the expansion device is
provided in one embodiment with spindles, operable mechanically by hand or
by means of a motor, as a function of the instanteous temperature of the
inner tube or of a force acting upon the inner tube in lengthwise
direction of the line due to temperature changes.
According to another particularly advantageous embodiment of the equalizing
arrangement according to the invention, the expansion device contains at
least one first, rigid component of an axial length predetermined at room
temperature and of predetermined coefficient of expansion, and parallel
thereto, at least one other component whose axial length at room
temperature is shorter by the amount of the length of the compensating
element and whose coefficient of expansion is greater than that of the
first component. The components may, in particular, be concentric pieces
of tubing rigidly joined to each other at one end while their other ends
are each rigidly connected to a section of inner tubing which is attached
to the compensating element. The lengths and coefficients of expansion of
the components are advantageously selected so that the length of the
compensating element is increased by the amount by which the inner tube
shrinks in the cooling process as a function of temperature. This system
is practically an automatic control and requires no separate mechanical
actuating devices.
Moreover, the expansion device used as a compensating element, may
advantageously be used at the same time for carrying the cryogenic medium
between the individual sections of the inner tube. This embodiment of an
equalizing arrangement is characterized by a particularly simple design
because it makes it possible to obviate expandable parts such as sections
of corrugated tubing.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a longitudinal cross sectional view of a first embodiment of an
equalizing arrangement according to the present invention.
FIGS. 2 to 4 are similar views of additional embodiments of the equalizing
arrangement of the present invention.
DETAILED DESCRIPTION OF THE INVENTION
In FIG. 1 a partial longitudinal section of a low temperature line with an
equalizing arrangement according to the present invention is shown. The
low temperature line contains a rigid inner tube 2 which is divided into
at least two individual sections 3 and 4, and is concentrically enclosed
by a rigid outer tube 6. The inner tube 2 carries a cryogenic medium such
as liquid helium or liquid hydrogen which may be provided to cool
conductors such as superconductors, not shown in the figure. Therefore,
the inner tube 2 has at least approximately the temperature level of the
cryogenic medium. This medium and, if applicable, the electric current for
the conductors are fed into the line at one end by means of a termination
8, not detailed in the figure, and discharged at the other end of the line
through a corresponding termination 9. A high vacuum may expediently be
provided between the inner tube 2 and the outer tube 6, as may if
applicable, at least one radiation shield and superinsulation, in order to
limit the heat transfer losses from the outer tube to the inner tube. Also
required within the outer tube are support or suspension devices, not
shown in the figure, in order to fix the inner tube and, if applicable, a
radiation shield.
For the equalization of length variations a compensating element expandable
in the lengthwise direction of the line, such as a section of corrugated
tubing 11 is inserted between the two individual sections 3 and 4 of the
inner tube 2. This section of corrugated tubing may be joined to the
individual sections 3 and 4 by means of flanges, for example, or it may be
welded to them. A fastening element such as rings 13 and 14 extending
radially outward relative to the axis of the line, is rigidly attached to
the outsides of the ends of the individual sections 3 and 4 which are
joined to the piece of corrugated tubing 11. These rings may, for example,
also act as connecting flanges between the section of corrugated tubing 11
and the individual sections 3 and 4 of the inner tube 2. Between the rings
an expansion device 15, is provided by means of which the length L of the
piece of corrugated tubing 11 can be preset. In essence, this expansion
device consists of threaded spindles 16 passing through the rings 13 and
14. The spindles may be movable, for instance, manually from the outside
or by a servo motor 18.
On the inner tube 2, for instance on a flange 20 or 21, where two sections
of the inner tube are joined together, there is disposed at least one
sensor 22, by means of which the contraction and expansion forces
occurring between the tube sections in the lengthwise direction of the
line during temperature variations can be measured. Strain gage foils or
load cells, for instance may be used as sensors 22. Depending on the
forces occurring, the sensors 22 transmits a signal to a control amplifier
23 which provides an output to drive the servo motor 18 until the length L
of the piece of corrugated tubing 11 is changed by the associated spindles
16 so that an unstressed connection of the inner tube sections is obtained
at the flanges. It is thus possible to keep the entire length of the inner
tube 2 and of the section of corrugated tubing 11 constant over the full
temperature range and therefore even during during a cooling process, so
that virtually no forces are exerted on the terminations 8 and 9 by the
inner tube 2.
In FIG. 2, another embodiment of an equalizing arrangement for a rigid
inner tube 2 of a low temperature line is shown schematically in a
longitudinal section. The other details not shown in FIG. 2 may, for
example, correspond to those of the low temperature line of FIG. 1. The
equalizing arrangement is disposed between two individual sections 35 and
26 of the inner tube 2 and contains sections of corrugated tubing 28 as
the length compensating element. At the ends 29 and 30 of the sections 25
and 26 of the inner tube 2, which ends face the section of corrugated
tubing 28, rings 32 and 33 are rigidly joined to their outsides such as by
welding. These rings are disposed in radial planes relative to the axis of
the line, and they are of different outside diameter. Disposed between the
rings is an expansion device 34 containing two tubular components 35 and
36. The face of the one section of tubing 35 of the expansion device is
joined to the larger ring 32 fastened to the end 29 of the inner tube
section 25. It encloses concentrically the piece of corrugated tubing 28
and a part of the inner tube section 26. Its axial length at room
temperature is designated L.sub.1. Fastened to the ring 33 of small
outside diameter is, correspondingly, the second section of tubing 36 of
the expansion device 34, which is disposed concentrically between the
inner tube section 26 and the first section of tubing 35 and which is
enclosing said inner tube section 26 for a length L.sub.2 at room
temperature. The length L.sub.2 of the section of tubing 36 attached to
the ring 33 is chosen so that its lateral face, facing away from the ring
33, lies in a common radial plane with the corresponding face of the
section of tubing 35. Both faces are connected to each other via a ring 38
such as by being welded to this ring. Thus, the length difference L.sub.1
- L.sub.2 of the two sections of tubing 35 and 36 of the expansion device
34 determines the length L of the section of corrugated tubing 28.
The section of tubing 35 having the length L.sub.1, of the expansion device
34 is made of a material which shrinks only relatively little when cooled
from room temperature to a low operating temperature. For example, a
special ceramic may be used as the material for this component. On the
other hand, the shorter section of tubing 36 of the length L.sub.2 is made
of a material which shrinks as much as possible in the desired temperature
range. This section of tubing may consist, for example, of high density
polyethylene which shrinks about 2.9% for a temperature drop from 300 K to
4 K. If aluminum is provided for this section of tubing 36, the resultant
shrinkage for the same temperature drop is approximately 4.2.permill..
At room temperature, the lengths L.sub.1 and L.sub.2 of the sections of
tubing 35 and 36, respectively, are chosen so that the section of
corrugated tubing 28 is compressed to a predetermined length L. If the
inner tube 2 is now cooled, the sections of tubing 35 and 36 will also
assume the inner tube temperature due to heat conduction. Therefore, the
ring shaped fastening means 32 and 33 are expediently made of a highly
heat conducting material. Whereas the length L.sub.1 of the section of
tubing 35 remains almost unchanged during a cooling process the section of
tubing 36 shrinks as a function of the temperature decrease and thus
allows the section of corrugated tubing 28 to expand. The length
dimensions L.sub.1 and L.sub.2 of the sections of tubing 35 and 36 are
chosen so that their shrinkage corresponds at least approximately to the
amount of shrinkage of the inner tube sections 25 and 26 connected to the
piece of corrugated tubing 28. Where the section of tubing 36 has a
relatively small coefficient of expansion, the lengths L.sub.1 and L.sub.2
of the two sections of tubing 35 and 36 should be increased accordingly.
For example, assume a total length of 35 m for the inner tube sections 25
and 26. If these inner tube sections consist of a special nickel-iron
alloy known by the name Invar, and if they are cooled from 300 to 4K, they
will shrink 0.035.permill., i.e., by approximately 12.25 mm. Now, if the
longer section of tubing 35 of the expansion device is likewise made of
this special alloy while high density polyethylene having a shrinkage of
approximately 2.9% for the given temperature range is selected as the
material for the shorter piece of tubing 36, then at room temperature, the
length L.sub.1 of the section of tubing 35 must be 48 cm and the length
L.sub.2 of the section of tubing 36 must be 42.8 cm.
If the aluminum is used for the section of tubing 36, the resulting
corresponding tube lengths are considerably greater. At an original length
L of the piece of corrugated tubing 28 of 6 cm, the section of tubing 35
must then be 3.18 m long, assuming that the shrinkage of this material is
4.2.permill. for the given temperature drop.
If, for design reasons, such a great length of the two sections of tubing
of the expansion device according to FIG. 2 cannot be provided, these
sections of tubing may be divided into at least two concentric tube
lengths as illustrated by FIG. 3. In the embodiment of an equalizing
arrangement according to the present invention as shown on FIG. 3, two
tubular components 40 and 41 of the expansion device 42 are attached to
annular plates 44 and 45 in the same manner as in the embodiment per FIG.
2.
However, the faces of these tubular components 40 and 41 opposite the
annular plates are not connected to each other directly by means of
another annular plate, but rather via two other tubular components 47 and
48. These tubular components, which are of the same axial length but of
different diameter, are disposed concentrically to the axis of the line
between the tubular components 40 and 41. At one end they are rigidly
joined to each other by means of an annular plate 49. The other lateral
end of the tubular component 47, having the larger diameter, is fastened,
together with the corresponding end of the tubular component 40, to an
annular plate 50, whereas the tubular component 48 of the smaller diameter
is connected to the tubular component 41 in corresponding manner via an
annular plate 51. In the longitudinal cross section of the expansion
device 42, a meander arrangement of the tubular sections 40, 47, 48 and 41
is thus obtained.
It is advantageous to provide the material of the innermost tubular
component 41 as the material for the component 47 which encloses the
component 48, whereas the component 48 consists of the material of the
outermost tubular component 40. Thus, the four tubular components 40, 47,
48 and 41, when viewed from the outside towards the inside, alternate in
the magnitude of their coefficient of expansion.
If the individual components of the expansion device 34 of FIG. 2, or 42 of
FIG. 3, are connected to each other and to the inner tube sections
associated with them in such a manner that they define a chamber which is
tight for the cryogenic material, the section of corrugated tubing between
the two inner tube sections having the reference symbols 53 and 54 can be
eliminated as illustrated by the equalizing arrangement of FIG. 4. The
length compensating element of this equalizing arrangement whose length L
at room temperature can thus be predetermined as desired and can be very
short for example, is practically formed only by its expansion device 55.
This device, conforming to the embodiment of FIG. 2, contains two tubular
components 57 and 58, one enclosing the other concentrically. These
components may rest directly on each other or be radially spaced from each
other slightly, as shown in the figure.
Since the temperature dependent shape of the curves of the coefficients of
expansion of the materials provided for the tubular components of the
expansion devices of FIGS. 2 to 4 are approximately the same in first
approximation, the slight differences in the shrinkage of these materials
need not be taken into consideration.
For the actual design of the expandable parts between the individual inner
tube sections, simple sections of corrugated tubing may be used because
their axial guidance and limitation is assumed in the above described
manner by the expansion device according to the invention.
It is also possible to use several rod-shaped elements having appropriate
coefficients of expansion in place of the tubular components provided in
FIGS. 2 and 3.
The premise in the embodiments illustrated is that only one equalizing
arrangement is provided between two individual sections of an inner tube.
But such equalizing arrangements may also be disposed at the beginning or
end of a low temperature line. In addition, for reasons of guiding and
limiting the compensating elements, it is generally expedient to insert a
greater number of appropriate elements of shorter length in an inner tube
instead of only one element of long length. This applies particularly to
the cooling of lines with boiling media, in order to achieve good
temperature equalization at the respectively associated inner tube
section.
In an application where rigid tubes are also used for a radiation shield in
a low temperature line, appropriate equalization arrangements according to
the present invention can be provided for the equalization of shrinkage
differences.
* * * * *
|
|
 |
|
 |
Description |
|
