Field of the Invention
[0001] This invention relates to the field of isostatic molding and more particularly to
an improved process for isostatic molding of powdered metal, carbon or ceramic particles
into densified compact articles of uniform preselected density.
Background of the Invention
[0002] Isostatic molding is a pressing process for densifying a powdered composition into
a compact shape at pressures sufficient to obtain near theoretical density. Powder
and particulate matter is densified under pressure acting through a suitable fluid
medium preferably a liquid to achieve an omnidirectional high green density.
[0003] Current state of the art isostatic molding recognizes that density more than any
other property influences the final mechanical and physical properties of the pressed
material. Density determines the strength and physical properties of the compact billet
both in the green and final sintered state. In current practice the green density
level of the compressed product is indirectly controlled during the molding operation
by setting a target pressure and controlling the rate of pressurization of the press
until the target pressure is realized. Secondary process variables also include: temperature,
hold time under compression mold filling techniques, and depressurization controls.
Unfortunately, experience has shown that product uniformity, particularly for a carbon
or ceramic composite cannot be achieved with a high degree of accuracy by control
of pressure with or without adjustment of the other indicated process variables. Instead,
a wide range of variability in the characteristics of the product is found to exist
due to non-uniformity in product density. To guarantee product repeatability particularly
for graphite and ceramic products, the product density must be held to within a limited
narrow range of density.
Summary of the Invention
[0004] The isostatic molding process of the present invention comprises the steps of:
loading a powder charge of metal, carbon or ceramic into a mold assembly of known
weight and volume;
weighing the mold assembly with the powder charge;
calculating the weight of the powder charge inside the mold assembly;
loading the mold assembly and powder charge into an isostatic pressure vessel;
filling the pressure vessel with a fluid medium;
pressurizing the pressure vessel;
weighing the combined mold assembly and powder charge inside the pressure vessel
during pressurization;
calculating the weight of the powder charge inside the pressure vessel by computing
the difference in weight between the mold assembly in the fluid medium inclusive and
exclusive of the powder charge with the latter weight determined by the difference
between the weight of the mold assembly outside of the pressure vessel and a product
represented by its known volume multiplied by the density of the fluid; and
computing the density of the compressed powder charge in accordance with the following
algorithm:

where
W
m = weight of powder charge in mold assembly outside of pressure vessel;
W
mf - weight of powder charge in fluid medium within the pressure vessel;
ρ
f - density of fluid medium;
ρ
p - density of power charge in vessel; and
depressurizing the pressure vessel when the computed density for the compressed
article equals a preselected product density.
Brief Description of the Drawings
[0005]
Figure 1 is a typical density versus pressure relationship for cold isostatic pressing
"CIP".
Figure 2 is a block diagram of the isostatic molding system of the present invention;
and
Figure 3 is a time-density characteristic curve for a production run of a graphite
billet in accordance with the Example described in the present invention.
Figure 4a shows a typical density versus time relationship for isostatic molding under
conventional practice where pressure is varied linearly to control green density;
Figure 4b shows a pressure versus time relationship corresponding to Figure 4a;
Figure 5a shows a density versus time relationship for isostatic molding following
the practice of the present invention; and
Figure 5b shows the pressure versus time relationship corresponding to Figure 5a.
Detailed Description of the Invention
[0006] A typical density versus pressure relationship for a isostatically pressure molded
product is illustrated in Figure 1. In the conventional process of isostatic molding
the relative green density of the product is established indirectly through its known
correspondence with press pressure. The pressure in the pressure vessel is monitored
and varied until a target pressure is achieved. Regulation of the actual pressure
in the pressure vessel is accomplished by adjusting the rate of pressurization of
the pressure vessel, the hold time at a given pressure level, temperature and the
rate of depressurization. However, even under highly controlled pressure cycle conditions,
variations in mold filling, molding powder preparation and temperature cause variations
in the molded product density. It is the molded product density which governs product
uniformity.
[0007] The system 10 of the present invention as illustrated in Figure 2 is designed to
directly monitor the density of the powder charge in-situ during compaction. The system
equipment, of itself, is conventional and includes a pressure vessel 11, a pump 12
and a liquid tank 14 containing an isostatic fluid 15 such as water. A mass flow meter
16 for measuring the quantity of fluid pumped into the pressure vessel is also desirable
particularly for practicing the alternate embodiment of the invention which will be
explained in greater detail later in the specification. The pump 12 is arranged in
a control loop 17 containing a control valve 18 to permit the pump 12 to be operated
throughout the operating cycle. The pressure vessel 11 is fitted with a weighing system
20 which allows a removable mold assembly 22 to be weighed during pressing in accordance
with the process of the present invention. The system 10 is integrated to operate
automatically in conjunction with a computer controller 24 although it may be operated
manually.
[0008] To press a powdered composition into a densified compact shape, a conventional elastomeric
mold or "bag" (not shown) of known weight is charged with the desired powder composition.
The mold is then sealed to prevent ingress of isostatic fluid and loaded into a supporting
structure (not shown) of conventional construction to form the mold assembly 22. The
weight of the powder charge in the mold assembly is computed by simple subtraction
of the weight of the mold with and without the powder charge. The mold assembly 22
is then placed in the pressure vessel 11. Prior to introduction into the pressure
vessel 11 the weight and volume of all of the component parts of the mold assembly
22 are recorded. The weight and volume data are loaded into the computer controller
24 by an operator through a modem 26 or by hand.
[0009] The weighing system 20, as outfitted in the pressure vessel 11, consists of a conventional
weighing platform (not shown) built into the bottom of the press with conventional
load cells (not shown). The load cells must be capable of accurately measuring the
underwater weight of the mold assembly 22. In the preferred embodiment the mold assembly
22 is weighed throughout the pressurization cycle. Accordingly, to accurately weigh
the mold assembly under pressure the load cells should be hydrostatically compensated.
Hydrostatically compensated load cells are presently commercially available.
[0010] The sequence of events that take place during a density controlled pressing cycle
are as follows:
1. The mold assembly 22 is placed in the pressure vessel 11 on the weighing platform
of the weighing system 20. The mold assembly 22 may optionally be warmed prior to
and/or during introduction into the pressure vessel.
2. The pressure vessel 11 is filled with water and sealed.
3. The pressurization pump 12 is turned on and the controller 24 activated.
4. The controller 24 continuously calculates the in-situ density of the product during
the press cycle as follows:

where:

. This is determined outside the press.



The calculation of target density for the compressed powder charge may also be expressed
in accordance with the following algorithm, which was derived from the above relationships:

where
Wm = weight of powder charge in mold assembly outside of pressure vessel;
Wmf = weight of powder charge in fluid medium within the pressure vessel;
ρf = density of fluid medium;
ρp = density of compacted power charge in vessel; and
where
Wmf is computed from the difference in weight between the mold assembly in the fluid
medium inclusive and exclusive of the powder charge with the latter weight determined
by the difference between the weight of the mold assembly outside of the pressure
vessel and a product represented by its known volume multiplied by the density of
the fluid.
5. The pressure in the pressure vessel 10 is raised at a controlled rate while monitoring
the product density. The pressure may be raised by a manual operation or continuously
under automatic instruction from the controller 24.
6. When the computed product density reaches a preselected target density the pressure
vessel 10 is depressurized. This preselected target density may be chosen to allow
for springback of the billet during depressurization.
7. The system is depressurized at a controlled rate once the preselected density is
achieved. The pump 12 is sized so that the bulk of the pump output flow always goes
back through the control valve 18 to its suction side. In this way, the control loop
can be more easily tuned for both pressurization and depressurization.
8. The product is removed from the press and unloaded from the mold assembly.
[0011] The real time computation of product density in-situ is based upon the use of Archimedes'
principle of buoyancy which equates buoyant force in a fluid medium to the weight
of the body of fluid which a submerged body displaces. The product density is equal
to the powder charge weight divided by the powder charge volume. The weight of the
powder charge outside the mold assembly is readily calculated. Since the density of
the isostatic fluid is known based upon the fluid composition, temperature and pressure
the powder volume in-situ becomes simply a weight relationship permitting in-situ
density to be calculated directly from weight and volume data. The algorithm for product
density as expressed heretofore was computed from the above analytical relationships
and may be expressed in many different ways.
[0012] The real time computation of product density in-situ may also be computed by an alternative
procedure involving an initial computation of powder density at an initial preselected
press pressure or before pressure is applied. Once this initial powder density is
computed every pound of incompressible fluid pumped into the press results in a weight
gain of one pound as the powder densifies. The controller can therefore use the initial
density computation and calculate the amount of fluid added into the pressure vessel
in pounds during the press cycle. The added fluid can be measured by the mass flow
meter 16 or alternatively by a level drop in a feed reservoir. The controller 24 then
calculates product density by a recomputation of "Wmf" by means of simple addition
of the weight of the powder charge at the initial condition, i.e., at the preselected
press pressure or before pressure is applied and the weight of fluid added into the
pressure vessel. Once "Wmf" is recomputed the final density is computed in accordance
with the algorithm of page 7 as hereafter restated:

Where W
mf is computed, at the initial condition with pressure either at ambient or a preselected
value above ambient, as heretofore described by computing the difference in weight
between the mold assembly in the fluid medium inclusive and exclusive of the powder
charge with the latter weight determined by the difference between the weight of the
mold assembly outside of the pressure vessel and a product represented by its known
volume multiplied by the density of the fluid. W
mf at the final condition equals the weight of fluid added into the pressure vessel.
[0013] Figure 4a and 4b illustrate the conventional density and pressure relationship with
respect to time respectively. The non linear density versus time curve results from
the indirect control of density using pressure as the control variable. In the present
invention density, itself, is the control variable and may be linearly varied with
time resulting in a nonlinear pressure versus time relationship as exemplified in
Figures 5a and 5b. In the alternative embodiment of the invention density is measured
and controlled in-situ by regulating the fluid added to the pressure vessel. This
may be done in combination with the principal embodiment or used solely to check the
results obtained following the practice of the principal embodiment. It should also
be understood that direct control of density permits the relationship of density with
time to follow any desired pattern including a curve where density is held relatively
constant over a fixed time until, for example, the final density is approached and/or
during the period of depressurization.
Example of InSitu-Density Control
[0014] In this example, a molding powder was prepared from a fine grain carbonaceous filler
material mixed with a coal tar pitch binder.
[0015] A cylindrical rubber molding bag and top closure weighing 7.392 pounds and having
a density of 57.81 lbs/ft³ was used as a mold. The bag was placed in a stainless steel
cylindrical holder weighting 20.40 pounds and having a volume of 0.1176 ft³. A vacuum
applied to the outside of the holder pulled the bag tight against the holder as powder
was loaded into the bag. The powder was deairated during bag filling by vertically
jolting the assembly 71 times. A rubber top closure containing a flanged stainless
steel valve was then sealed to the bag with hose clamps. The valve weight was 0.9546
lb; its volume of 0.00225 ft³.
[0016] Air was removed from the loaded and sealed mold assembly with a vacuum pump. The
mold assembly was then warmed to a desired molding temperature before placement in
the press.
[0017] The press computer control system prompts the operator for the weight of the molding
bag, a stainless steel holder identification letter, in this case "E", and the final
weight of the loaded mold assembly. The computer then calculates three numerical constants
that it will use to control the pressing cycle.

. This is equal to the weight of molding powder in lbs ÷ 62.428; in this example
= 1.724.

. This is equal to the negative of the volume in cubic feet of all but the molding
powder; in this example = -0.23117.

; in this example = 135.4.
During the press cycle, the computer calculates the density of the molding powder
billet in grams/cc as follows.

The computer measures the total immersed weight with an underwater load cell. It
calculates the density of the press water in lbs/ft³ by measuring the press temperature
and pressure using the following known relationship:
The computer control program is divided into seven segments. After the assembly
is loaded into the press and the air is bled from the system, the computer program
is started.
Segment #1
[0018] During the first 90 seconds of the program, the assembly is supported by a hydraulic
cylinder rather than the load cells. At this time, the computer stores the load cell
reading with no load as the "tare" weight. The weight is then lowered until it is
supported by the load cell.
[0019] When the pump is turned on, the computer controls the press pressure at 25 psig for
five minutes. At the end of this five minute period, the computer checks to see if
stable control of ± 2 psi from the setpoint has been achieved. If it has, the computer
stores the current density reading as the initial billet density and advances the
program to segment #2.
[0020] During segment #2, the billet density is calculated by three different methods. This
is a feature of the Pilot Plant system aimed at comparing the accuracy of each method.
Only one of the methods is necessary in order to obtain accurate control of density.
[0021] Since the load cell zero shift is usually linear and reproducible, method #1 uses
a stored factor based on a calibration of zero shift in order to correct load cell
readings. In this method, for this example, the corrected load cell reading equals
the Raw Load Cell Reading - Tare weight Stored in Segment #1 - (.001 x System Pressure
in psig).
[0022] In method #2, no calibration is stored in the computer. Instead, the zero shift is
determined directly during segment #3 by taking the weight off of the load cell while
the system is under pressure. This is accomplished with an underwater hydraulic linkage
that the computer activates during segment #3. Segment #3 is triggered when the billet
density is close to its target value. The corrected load cell readings by this method
are obtained as follows:
· Segment #1 to Segment #3

· Segment #4 to Segment #7

In method #3, the load cell readings are only used to obtain an initial density
during segment #1. After that, billet density is calculated by measuring the amount
of water pumped into the press. This compares with load cell readings since (barring
water leaks) every pound of water pumped in should increase the immersed weight of
the billet by one pound.
[0023] Segment #3 is triggered when the billet density calculated by method #1 reaches a
first target density level selected to be approximate (just below) the desired final
target density.
Segment #3
[0024] This program segment lasts two minutes. While the program is in segment #3, it locks
in the density values calculated at the end of segment #2. The pressure setpoint is
also held constant. The computer activates a hydraulic linkage which removes the weight
from the load cell. It holds the weight off for 90 seconds while the tare weight for
the density calculation by method #2 is updated. The tare weight for method #1 is
left unchanged. After the new tare weight is locked in, the weight is returned to
its position on the load cell.
[0025] At the end of segment #3, segment #4 begins and density by all three methods resumes
being calculated.
Segment #4
[0026] During this segment, the pressure is ramped up at a rate of 10 psi/min. The billet
density is calculated continuously and when it reaches the final target valve, the
computer advances to segment #5. The final target density is selected in order to
obtain the desired value after "spring back". "Spring back" is a small density drop
that occurs as the pressure is released.
Segment #5
[0027] The pressure is ramped down at a rate of 100 psi per minute to 35 psi.
Segment #6
[0028] The pressure is held at 35 psi for three minutes. This allows stable low pressure
readings to be taken of final billet density with sufficient pressure to keep the
rubber molding bag tight on the billet.
Segment #7
[0029] During this segment, all of the pressure is released and the computer prints the
results of the pressing cycle.
Billet Inspection
[0030] The billet was removed from the press and taken out of its frame and inspected. The
billet was then weighed in and out of water to check its density.
1. An isostatic process for molding metal, carbon or ceramic particles into a densified
compact having a preselected density comprising the steps of:
(a) loading a powder charge of metal, carbon or ceramic into a mold assembly (22)
of known weight and volume:
(b) weighing the mold assembly (22) with the powder charge;
(c) calculating the weight of the powder charge inside the mold assembly (22);
(d) loading the mold assembly (22) and powder charge into an isostatic pressure vessel
(11);
(e) filling the pressure vessel (11) with a fluid medium (15);
(f) pressurizing the pressure vessel (11);
(g) weighing the combined mold assembly (22) and powder charge inside the pressure
vessel (11) during pressurization;
(h) calculating the weight of the powder charge inside the pressure vessel (11) by
computing the difference in weight between the mold assembly (22) in the fluid medium
(15) inclusive and exclusive of the powder charge with the latter weight determined
by the difference between the weight of the mold assembly (22) outside of the pressure
vessel (11) and a product represented by its known volume multiplied by the density
of the fluid (15); and
(i) computing the density of the compressed powder charge in accordance with the following
algorithm:

where
Wm = weight of powder charge in mold assembly outside of pressure vessel;
Wmf - weight of powder charge in fluid medium within the pressure vessel;
ρf - density of fluid medium;
ρp - density of powder charge in vessel; and
depressurizing the pressure vessel (11) when the computed density for the compressed
article equals a preselected product density.
2. An isostatic process as defined in claim 1 wherein said mold assembly (22) comprises
an elastomeric mold for the powder charge and support means.
3. An isostatic process as defined in claim 2 wherein the pressure vessel (11) is pressurized
at a controlled rate.
4. An isostatic process as defined in claim 2 wherein the pressure vessel (11) is pressurized,
so as to produce a controlled product density versus time relationship.
5. An isostatic process as defined in claim 3 wherein the mold assembly (22) inside the
pressure vessel is weighed intermittently during pressurization.
6. An isostatic process as defined in claim 5 wherein the pressure vessel (11) is depressurized
at a controlled rate.
7. An isostatic process as defined in claim 1 wherein the loaded mold assembly (22) is
warmed to a predetermined temperature before it is placed in the pressure vessel.
8. An isostatic process as defined in claim 1 wherein the pressure vessel (11) is pressurized
to a first predetermined pressure and further comprising the steps of:
computing the density of the powder charge in the pressure vessel (11) at said
first predetermined pressure using step (i):
measuring the amount of fluid pumped into said pressure vessel: and
computing the final density of the compact charge based upon the increase in the
amount of fluid (15) pumped into the pressure vessel (11) after reaching said first
predetermined pressure.
9. An isostatic process as defined in claim 8 wherein said first predetermined pressure
is ambient pressure.
10. An isostatic process as defined in claim 8 wherein said first predetermined level
above ambient preselected pressure.
11. An isostatic process as defined in claim 10 wherein said final density is computed
in accordance with step (i) with Wmf computed first at an initial condition corresponding to said first predetermined
pressure and then at a final condition based upon the weight of fluid (15) added to
the pressure vessel (11) and added together to compute final density.
1. Isostatisches Verfahren, um Metall-, Kohlenstoff- oder Keramikteilchen zu einem verdichteten
Preßling mit vorgewählter Dichte zu formen, wobei das Verfahren folgende Schritte
umfaßt:
(a) Einbringen einer Pulverfüllung aus Metall, Kohlenstoff oder Keramik, in eine Formvorrichtung
(22) mit bekanntem Gewicht und Volumen;
(b) Wiegen der Formvorrichtung (22) zusammen mit der Pulverfüllung;
(c) Berechnen des Gewichtes der Pulverfüllung in der Formvorrichtung (22);
(d) Einbringen der Formvorrichtung (22) mit der Pulverfüllung in einen isostatischen
Druckbehälter (11);
(e) Füllen des Druckbehälters (11) mit einem flüssigen Medium (15);
(f) Ausüben eines Drucks auf den Druckbehälter (11);
(g) Wiegen der Formvorrichtung (22) mit der Pulverfüllung in dem Druckbehälter (11)
während der Druckausübung;
(h) Berechnen des Gewichtes der Pulverfüllung in dem Druckbehälter (11), indem der
Gewichtsunterschied zwischen der Formvorrichtung (22) in dem flüssigen Medium (15)
mit und ohne die Pulverfüllung berechnet wird, wobei letzteres Gewicht durch den Unterschied
zwischen dem Gewicht der Formvorrichtung (22) außerhalb des Druckbehälters (11) und
einem Produkt aus dem bekannten Volumen der Formvorrichtung multipliziert mit der
Dichte der Flüssigkeit (15) bestimmt wird; und
(i) Berechnen der Dichte des Pulverpreßlings in Übereinstimmung mit dem folgenden
Algorithmus:

mit
Wm= Gewicht der Pulverfüllung in der Formvorrichtung außerhalb des Druckbehälters;
Wmf= Gewicht der Pulverfüllung im flüssigen Medium innerhalb des Druckbehälters;
ρf= Dichte des flüssigen Mediums;
ρp= Dichte der Pulverfüllung in dem Behälter; und
Abbau des Druckes in dem Druckbehälter (11), wenn die berechnete Dichte des Preßlings
einer vorgewählten Produktdichte entspricht.
2. Isostatisches Verfahren nach Anspruch 1, wobei die Formvorrichtung (22) eine elastomere
Form für die Pulverfüllung und eine Halterung umfaßt.
3. Isostatisches Verfahren nach Anspruch 2, wobei der Druckbehälter (11) mit einer kontrollierten
Geschwindigkeit unter Druck gesetzt wird.
4. Isostatisches Verfahren nach Anspruch 2, wobei der Druckbehälter (11) so unter Druck
gesetzt wird, daß eine kontrollierte Beziehung zwischen Produktdichte und Zeit erzeugt
wird.
5. Isostatisches Verfahren nach Anspruch 3, wobei die Formvorrichtung (22) innerhalb
des Druckbehälters während der Druckausübung diskontinuierlich gewogen wird.
6. Isostatisches Verfahren nach Anspruch 5, wobei der Druck in dem Druckbehälter (11)
mit einer kontrollierten Geschwindigkeit abgebaut wird.
7. Isostatisches Verfahren nach Anspruch 1, wobei die gefüllte Formvorrichtung (22) vor
Einbringen in den Druckbehälter auf eine vorbestimmte Temperatur erwärmt wird.
8. Isostatisches Verfahren nach Anspruch 1, wobei der Druckbehälter (11) auf einen ersten,
vorbestimmten Druck gebracht wird und das ferner folgende Schritte umfaßt:
Berechnen der Dichte der Pulverfüllung in dem Druckbehälter (11) bei diesem ersten,
vorbestimmten Druck entsprechend Schritt (i);
Messen der in den Druckbehälter gepumpten Menge an Flüssigkeit; und
Berechnen der endgültigen Dichte der Preßkörper-Füllung auf Grundlage des Anstiegs
der Menge der in den Druckbehälter (11) gepumpten Flüssigkeit (15) nach Erreichen
des ersten, vorbestimmten Druckes.
9. Isostatisches Verfahren nach Anspruch 8, wobei der erste, vorbestimmte Druck Umgebungsdruck
ist.
10. Isostatisches Verfahren nach Anspruch 8, wobei der erste vorbestimmte Druck oberhalb
Umgebungsdruck liegt.
11. Isostatisches Verfahren nach Anspruch 10, wobei die endgültige Dichte entsprechend
Schritt (i) berechnet wird, wobei Wmf zuerst bei einem dem ersten, vorbestimmten Druck entsprechenden Anfangszustand und
dann bei einem Endzustand, der auf dem Gewicht der dem Druckbehälter (11) zugegebenen
Flüssigkeit (15) beruht, berechnet wird und diese Werte dann zur Berechnung der endgültigen
Dichte addiert werden.
1. Procédé isostatique pour le moulage de particules de métal, de carbone ou de céramique
en un comprimé densifié ayant une masse volumique préalablement choisie, comprenant
les étapes qui consistent :
(a) à introduire une charge de poudre de métal, de carbone ou de céramique dans un
ensemble à moule (22) de poids et de volume connus ;
(b) à peser l'ensemble à moule (22) avec la charge de poudre ;
(c) à calculer le poids de la charge de poudre à l'intérieur de l'ensemble à moule
(22) ;
(d) à introduire l'ensemble à moule (22) et la charge de poudre dans une enceinte
(11) à pression isostatique ;
(e) à remplir l'enceinte (11) de pression avec un milieu fluide (15) ;
(f) à mettre sous pression l'enceinte (11) de pression ;
(g) à peser la combinaison formée par l'ensemble à moule (22) et la charge de poudre
à l'intérieur de l'enceinte (11) de pression pendant l'application de la pression
;
(h) à calculer le poids de la charge de poudre à l'intérieur de l'enceinte (11) de
pression en calculant la différence de poids entre l'ensemble à moule (22) dans le
milieu fluide (15) en incluant et en excluant la charge de poudre, le dernier poids
étant déterminé par la différence entre le poids de l'ensemble à moule (22) à l'extérieur
de l'enceinte (11) de pression et un produit représenté par son volume connu multiplié
par la masse volumique du fluide (15) ; et
(i) à calculer la masse volumique de la charge de poudre comprimée conformément à
l'algorithme suivant :

où
Wm = poids de la charge de poudre dans l'ensemble à moule à l'extérieur de l'enceinte
de pression ;
Wmf - poids de la charge de poudre dans le milieu fluide à l'intérieur de l'enceinte
de pression ;
ρf - masse volumique du milieu fluide ;
ρp - masse volumique de la charge de poudre dans l'enceinte ; et
à éliminer la pression de l'enceinte (11) de pression lorsque la masse volumique
calculée de l'article comprimé est égale à une masse volumique préalablement choisie
pour le produit.
2. Procédé isostatique selon la revendication 1, dans lequel ledit ensemble à moule (22)
comporte un moule élastomérique pour la charge de poudre et des moyens de support.
3. Procédé isostatique selon la revendication 2, dans lequel l'enceinte (11) de pression
est mise sous pression à une vitesse réglée.
4. Procédé isostatique selon la revendication 2, dans lequel l'enceinte (11) de pression
est mise sous pression afin d'établir une relation maîtrisée de la masse volumique
en fonction du temps.
5. Procédé isostatique selon la revendication 3, dans lequel l'ensemble à moule (22)
à l'intérieur de l'enceinte de pression est pesé par intermittence pendant l'application
de la pression.
6. Procédé isostatique selon la revendication 5, dans lequel la pression de l'enceinte
(11) de pression est supprimée à une vitesse réglée.
7. Procédé isostatique selon la revendication 1, dans lequel l'ensemble à moule chargé
(22) est réchauffé jusqu'à une température prédéterminée avant d'être placé dans l'enceinte
de pression.
8. Procédé isostatique selon la revendication 1, dans lequel l'enceinte (11) de pression
est amenée à une première pression prédéterminée, et comprenant en outre les étapes
qui consistent :
à calculer la masse volumique de la charge de poudre dans l'enceinte (11) de pression
à ladite première pression prédéterminée en utilisant l'étape (i) ;
à mesurer la quantité de fluide introduite par pompage dans ladite enceinte de
pression ; et
à calculer la masse volumique finale de la charge comprimée sur la base de l'accroissement
de la quantité de fluide (15) introduite par pompage dans l'enceinte (11) de pression
après que ladite première pression prédéterminée a été atteinte.
9. Procédé isostatique selon la revendication 8, dans lequel ladite première pression
prédéterminée est la pression ambiante.
10. Procédé isostatique selon la revendication 8, dans lequel ledit premier niveau prédéterminé
est supérieur à la pression ambiante préalablement choisie.
11. Procédé isostatique selon la revendication 10, dans lequel ladite masse volumique
finale est calculée conformément à l'étape (i), Wmf étant calculé en premier dans un état initial correspondant à ladite première pression
prédéterminée, puis dans un état final basé sur le poids de fluide (15) ajouté à l'enceinte
(11) de pression, les deux valeurs étant additionnées pour calculer la masse volumique
finale.