[0001] The present invention refers to a method for the safe application and transmission
of steady and monotonically or cyclically varying pressure. It is based, depending
on theconditions, on the use of a molten oxides mixture or an assembly of ceramic
microspheres coated by solid lubricant. The method is operative for a wide range of
temperatures, from very low (-50° C) to very high ones (up to 2700°C).
[0002] The major scientific and technical fields related directly with the invention include
Mechanics of Materials, Fluid Mechanics, Technology of Glasses and Ceramics and industrial
production processes where the simultaneous application of high pressure and temperature
is required.
[0003] The current state-of-the-art uses fluid media for pressure transmission (liquids
with low boiling point such as water, oils, etc. or gases for high temperature applications).
A series of drawbacks, especially when high temperature prevails, are generally reported
in these cases :
- Danger of explosive events due to rupture of specimen material with damaging and costly
consequences for the overall installation.
- High capital and operational costs due to the required safety design and measures
and the use of expensive and complicated facilities, particularly at high pressures.
- Limited available range of operating temperatures, especially when a usual liquid
medium is employed (upper limit set by its boiling point).
- Inability to observe closely or to execute measurements with optical and other costly
devices due to the potential danger for explosive events.
[0004] Recently, the use of a bed of mixed ceramic and graphite particles for shape casting
of metallic materials has been reported (US patent 4, 667, 497). Some of the above
drawbacks are then eliminated. On the other hand though, this method suffers from
difficulties in transmitting pressure uniformly, the need to impose high axial loads
in order to achieve adequate radial pressure values, and mainly, the inability to
apply time varying pressure (fatigue tests) due to the non-linear behaviour of the
bed during unloading (reduction of pressure). Evidently, any method that may substitute
(at least partially) the commonly employed one (use of a fluid medium) should be competitive
to the latter with reference to its basic advantages, namely the simplicity in geometric
design and the uniformity of the transmitted pressure in all directions.
[0005] The present invention deals with a method for safe pressure transmission based on
the use of different media depending on the prevailing temperature and the requirements
of the application for constant or time varying pressure (mechanical fatigue) under
constant or time varying temperature (thermal fatigue). More specifically :
- In the temperature range from -50°C to 1600°C, use is made of an assembly of ceramic
microspheres of sizes between 5 and 500 µm, covered by a solid lubricant. This allows
for the transmission of steady or monotonically increasing pressure under temperatures
that may vary with time.
- For temperatures between 300°C and 2700°C, a mixture of melted oxides with a specified
composition is employed, assuring suitable viscosities in the desired temperature
range and offering the capability for the transmission of steady or time varying pressure
under temperatures that may change with time in the above mentioned range.
[0006] For an efficient application of the method, the media used should satisfy the following
requirements :
- The material of the microspheres should withstand high temperatures and pressures
for long periods of time (hundreds of hours) and permit the production of uniformly
sized spherical particles with reasonable costs. A systematic search led to the selection
of the following ceramics : Al2O3 (alumina), SiO2 (silica), silicon carbide, silicon nitride, ZrO2 (partially or fully stabilised zirconia) and their mixtures. In addition, substantial
improvements in the efficiency of the method and the reduction of the required axial
load are realised by coating the microspheres with a high temperature resistant, solid
lubricant such as boron nitride or molybdenum bisulfide.
- The mixture of melted oxides should be characterised by suitable glass transition
temperature and low reactivity (basicity) when in contact with the pressurised metallic
materials for long time periods (hundreds of hours) under the high pressures and temperatures
of operation. Sufficient quantities of these oxides should be produced at an acceptable
cost. Experimental work and literature search led to the basic composition of the
oxides mixture shown below :
xB2O3 · (1-x) SiO2 (O ≦ x ≦ 1)
where x is the mole fraction of B
2O
3.
[0007] According to the specific needs, this basic composition can be modified by adding
appropriately small amounts of other oxides from the classes of glass formers, conditional
formers and modifiers (see Table bellow). Small amounts of alkali and alkaline earth
halide salts, sulfate or sulfide salts can be also added, depending on the desired
range of temperatures.
- i) Formers :
- GeO2, Al2O3, P2O5, V2O5 As2O5, Sb2O5, Sb2O3, Ca2O3, ZrO2, As2O3.
- ii) Conditional Formers :
- TiO2, MoO3, WO3, Cr2 O3, ZnO, PbO, FeO, Fe2O3, CdO, ThO2, In2O3, Bi2O3, PbO2, SnO2, HgO, MnO, CoO, NiO, BeO, SnO, TeO2, Nb2O5, Ta2O5, HfO2, ReO2, TeO2, RuO2, OsO2, Rh2O3, Ir2O3, IrO2, PdO, PtO2.
- iii) Modifiers :
- Li2O, Na2O, K2O, Rb2O, Cs2O, MgO, CaO, SrO, BaO, Y2O3, La2O3, Sc2O3, Tl2O, Tl2O3, CuO, Cu2O, Ag2O, Au2O3, R2O3 (R = Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dh, Ho, Er, Tm, Hb, Lu), SeO2, PaO2, UO3.
[0008] In relation to the aforementioned drawbacks of the techniques that use conventional
fluid media, the present method exhibits significant improvements concerning :
- The elimination of the danger for explosive events at high pressures and temperatures.
- The considerable reduction in the costs of equipment, installation, etc.
- The capability to perform measurements and close observations with important consequences
on the study of material behaviour.
- The extension of the available temperature range.
- The capability to perform safely fatigue tests (variable pressure and temperature)
based on the proper selection of the transmitting medium for each case.
[0009] With regard to the principal advantage of the conventional techniques (with fluid
media), i.e. the uniformity of the transmitted pressure in all directions, this is
assured in the present method by :
a) the selection of suitable ceramic particle size distribution such that the system
exhibits adequate "(pseudo) - fluidity". The latter is related to the ability of the
particles to roll and slide against each other changing continuously the microscopic
geometry of the pressure transmitting medium. The addition of high temperature resistant
lubricants contributes to the enhancement of this property (pseudo-fluidity). Tests
carried out with microspheres without lubricant coating do not result in satisfactory
performance of the method due to relatively large frictional effects. Moreover, the
use of the lubricating agent prevents atomic diffusion at the contact area between
particles thus avoiding sintering phenomena that might otherwise occur under the high
pressure and temperature conditions. It was found that boron nitride offers sufficient
lubrication as its structure permits intracrystalline sliding (fig. 1).
b) the selection of the viscosity of the melted oxides mixture at the temperature
range of interest, such that the minimum required fluidity of the medium is attained.
[0010] In the following paragraphs, a specific application of the invention is described
with reference to the attached figures exemplifying the realisation of the method
in the case of internal pressurization tests on a tubular specimen under elevated
temperature. Two distinct possibilities are examined :
(i) Thermal fatigue and steady or monotonically increasing pressure
[0011] If thermal fatigue (from e.g. room to high temperatures) is required with the application
of constant or monotonically increasing internal pressure, an assembly of spherical,
stabilised zirconia particles is employed for pressure transmission. This material
can sustain very high pressures before crushing and temperatures (up to 1800° C) without
melting or sintering problems. The particles are prepared by means of the electrofusion
process which permits the production of small (< 50 µm) spheres with the following
composition :
ZrO
2 67%
SiO
2 30%
Others 3% (mainly Al
2O
3)
[0012] The microstructure is based on monoclinic zirconia crystals (microhardness : 9 GPa)
uniformly embedded in silica glass (microhardness : 7 GPa). It is a result of the
manufacturing process and specifically of the cooling and crystallisation method following
the fusion of the mixture of oxides at high temperatures. The physical properties
thus obtained are :
| True relative density : |
3.85 |
| Bulk density : |
2.3 |
| Microhardness : |
7-9 GPa |
[0013] A testing programme has been undertaken to ensure the stable behaviour of the particles
at conditions reaching 400 bar and 750°C for several hours. No sintering was observed
macroscopically while the microscopic examination found no evidence of microcracking
or any surface damage that could alter the shape of the beads. The role of silica
glass in the required mechanical properties, the behaviour after thermal cycling,
and the performance in repeated cycles of loading / unloading, were also the subject
of intensive study using Scanning Electron Microscopy (SEM) with Energy Dispersed
X-Ray Analysis (EDXA) for Post-Experiment Examination of both the particles and the
metallic structure. The preservation of the spherical particle shape is an important
factor for the performance of the system as a pressure transmitting medium.
[0014] The procedure of covering uniformly the quite small and spherical zirconia particles
(average diameter of 40 microns) with the lubricant is similar to the preparation
of pharmaceutical tablets and involves ultrasonic cleaning of small batches of the
spheres, coating by boron nitride in a slowly rotating glass container that is externally
heated by air streams and internally periodically sprayed with water, and microwave
drying of the batch to avoid the formation of agglomerations. The thickness of the
lubricant layer on the individual particles is of the order of 1-10 µm, as shown by
microscopy measurements.
[0015] A system of two specially designed contoured cylinders placed inside the test specimen
cavity are called upon to compress the zirconia particles and introduce an internal
pressure which gives rise to transverse stresses on the thin walled test specimen
(Fig. 2).
[0016] The basic criteria for the efficiency of the method in comparison to the conventional
fluid media include the uniformity of the developing radial pressure along the specimen
gauge length and the ratio of radial to axial (vertical) pressure.
[0017] Detailed experimental data from the specimen with suitably configured compression
pistons (fig. 3) show that the present system offers adequate pressure transmission
efficiency (radial/axial pressure is equal to 0.51) and quite good uniformity along
the specimen (deviations of the strain gauges from the central reference one are less
than 0.13%, fig. 4). The relationship between the applied axial load and the obtained
radial pressure on the specimen is linear during the loading phase, shows satisfactory
repeatability during loading / unloading cycles (Fig. 5) and the unloading path is
easily mathematically modelled. It was also shown that large plastic deformations
of the specimen do not influence significantly the uniformity of the applied pressure
or the ratio of radial to axial load.
(ii) Mechanical fatigue and time varying temperature
[0018] In cases requiring mechanical fatigue (cyclic variation of load) under temperatures
higher than 500°C, the selected pressure trasmitting medium is a molten mixture of
SiO
2 and B
2O
3. The temperature of operation ranges between 500° and 900°C with a B
2O
3 mole fraction of x=77.65 mol%. The dependence of viscosity n on temperature is described
(for this specific composition) from the empirical relationship given below :

where T is the temperature in K and the above relation applies in the range 400-1100°C.
In fig. 6 the above equation is represented graphically (viscosity versus temperature).
Similar expressions hold for different mixture compositions. The main factor determining
the nature and the proportions of the oxides in the mixture is the attainment of viscosity
values (in melted state) of the order of 10
4-10
6 Poise in the desired temperature range (definitely above the glass transition temperature
of the mixture).
[0019] In the present application, this is accomplished in principle by varying the fraction
of B
2O
3 (fig. 7) up to its extremes (with x=0, i.e pure SiO
2, very high operation temperatures of the method can be achieved, as the viscosity
values of fig. 8 indicate). Furthermore, the addition of other oxides (as Li
2O in fig. 9, and GeO
2, Na
2O in fig. 10) contributes to the "adjustment" of viscosity in the temperature range
of interest.
[0020] Concerning the reactivity issue, a series of tests took place in which fused B
2O
3 (at temperature 950°C) was left in contact with Ni alloys for time periods ranging
from 4 to 40 hours. The Raman spectra of pure B
2O
3 and samples from the molten B
2O
3 after several hours of contact with Ni-alloy, have been compared showing that the
spectrum remains practically unchanged. This leads to the conclusion that no reaction
takes place between fused boron oxide, SiO
2 and Ni-alloy at least to a spectroscopically detectable scale. The tests were repeated
with several alloys with the same results. The experimental data from internal pressurization
of the tubular specimen with suitably configured compression pistons, indicate that
the present system exhibits a ratio of radial to axial pressure almost equal to unity
and excellent uniformity along the specimen gauge length. It is important to note
that the relationship between the applied axial (vertical) load and the attained radial
pressure remains linear during both the loading and unloading phases.
[0021] Finally, fluid mechanic calculations for the flow of a viscous liquid though slits
have been performed to assess the potential danger of molten glass being ejected under
high pressure from cracks during specimen rupture. For slits with dimensions 2000x10x2000
µm
3 and a prevailing internal pressure of 300 bar, low flowrates (of the order of 2 mm
3/min) are computed for liquids with viscosity 10
6 Poise. Such flowrates are low enough to exclude any damaging effects.
[0022] The calculation is conservative in the sense that the significant increase of viscosity
as the molten glass is cooled when exiting the specimen through the crack, has been
neglected.
FIGURE LEGENDS
Figure 1
[0023] Crystalline structure of boron nitride
◆ Boron o Nitrogen.
Figure 2
[0024] BIAXIAL CREEP MACHINE
T
axial = 100 KN, P
int = 40 MPa
temperature up to 700° C.
Table of Components.
[0025]
1. Specimen
2. Zirconia particles or molten oxides
3. Zirconia or molten oxides compression mechanism
4. Furnace
5. Loading plates (tension)
6. Compression bars
7. Equal displacement mechanism for plates (5).
8. Equal displacement mechanism for plates (6).
9. Fixed plate (tension)
10. Moving plate (compression).
11. Fixed basement plates
12. Fixed bars
13. Articulated bars with pulleys
14. Sliders
15. Fixed bars with pulleys
16. Tension transmitter
17. Pulleys
18. Dead-weight
19. Cylinder-Slider
20. Bearing Sliders
21. Bearing Sliders
22. Compression transmitting bars
23. Hydraulic actuator
24. Compression transmitting bars
25. Compression transmitting rods
26. Spacer
27. Machine basement
28. Vacuum chamber
29. Machine columns
Figure 3
[0026] Specimen/compression pistons configuration
1. Ceramic piston
2. Graphite sealing
3. Zirconia particles
4. Specimen
1. Method of transmitting time varying pressure, characterised by the use of zirconia
(ZrO2) microspheres with granulometry 5 - 500 µm in the temperature range from -50° to
1600°C, and by the use of a mixture of molten oxides in the temperature range from
300° to 1100°C.
2. The method of Claim 1, further comprising the step that the basic molar composition
of the mixture of molten oxides takes the form xB
2O
3 · (1-x)SiO
2, with 0.2 ≦x≦ 1. Depending on the desired viscosity, the operational temperature
and the reactivity of the mixture, its composition may be modified by adding suitable
quantities of other oxides that belong to the following categories :
i) Formers : GeO2, Al2O3, P2O5, V2O5, As2O5, Sb2O5, Sb2O3, Ga2O3, ZrO2, As2O3.
ii) Conditional Formers : TiO2, MoO3, WO3, Cr2 O3, ZnO, PbO, FeO, Fe2O3, CdO, ThO2, In2O3, Bi2O3, PbO2, SnO2, HgO, MnO, CoO, NiO, BeO, SnO, TeO2, Nb2O5, Ta2O5, HfO2, ReO2, TeO2, RuO2, OsO2, Rh2O3, Ir2O3, IrO2, PdO, PtO2.
iii) Modifiers : Li2O, Na2O, K2O, Rb2O, Cs2O, MgO, CaO, SrO, BaO, Y2O3, La2O3, Sc2O3, Tl2O, Tl2O3, CuO, Cu2O, Ag2O, Au2O3, R2O3 (R = Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dh, Ho, Er, Tm, Hb, Lu), SeO2, PaO2, UO3.
Small quantities of alkali or alkaline earth halide salts, and sulfide or sulfate
salts can also be added depending on the desired range of temperatures.
3. The method of Claims 1 & 2, further characterised by the fact that the transmitted
pressure and/or the operational temperature may remain constant with time.
4. The method of claim 1, further characterised by the use if zirconia microspheres as
pressure transmitting medium prefentially in the case of steady or monotonically increasing
pressure under steady or time dependent temperature.
5. The method of claim 1, further characterised by a preferential granulometry of 20-100
µm for the zirconia particles and further comprising the step of coating the particles
with a solid lubricant, preferentially boron nitride or molybdenum bisulfide.
6. The method of claim 1, further comprising the step that the microspheres may consist
of other ceramics exhibiting high mechanical strength and resistance to corrosive
oroxidising environments and high temperatures, such as silicon carbide (SiC or SiSiC),
silicon nitride (Si3N4) of different types, alumina (Al2O3), silica (SiO2) or mixtures of these ceramics.