Dry powder pressing techniques are the most
cost-effective, flexible choice for the manufacture of a wide range of ceramic
components. Identifying powder blends and granulates that are best suited to
such applications is an essential element of process development, but it brings
its own challenges. One critical factor is to select an appropriate method for
characterizing ceramic powders, the importance of which is illustrated here
using experimental data from a study of die filling.
A first step toward the successful manufacture of a ceramic component using a
powder pressing technique is to develop an appropriate feed material. As
ceramic powders are often supplied as submicron or nano-sized particles, it is
usual practice to include an initial granulation step. The ideal outcome from
granulating a well-specified mix of ceramic powder, binders, lubricants and
dispersants to a suitable endpoint will be a feed of consistent composition that
delivers high levels of productivity and meets product quality targets.
Material must flow easily from a hopper, fill a die adequately, and compress to
form a stable green body that can be successfully ejected from the mold before
sintering and final machining. A good match between the feed and the rest of
the plant will result in a robust and stable process that maximizes throughput
and quality.
Developing granulates with properties that are suitable for a defined
application requires careful manipulation of a variety of parameters, including
particle size and distribution, degree of agglomeration, composition (e.g.,
binder content), and particle shape and texture. It is common, for example, to
select relatively fine granules for the production of ceramics that have very
demanding specifications, such as those used for medical applications. Finer
particles tend to form more homogeneous green bodies and ultimately deliver a final
product with few defects.
One of the major challenges implicit in this development process is how
to characterize granulates in ways that relate to in-
process performance and finished product quality. Without appropriate
measurement tools, the performance of a potential feed material can be assessed
only through plant trials on either a lab- or pilot-scale-a costly and
time-consuming option. Characterizing powder properties effectively can both
accelerate and optimize the development cycle.
Characterizing Powders for Ceramic Processing
Although ceramic processors have a wide
selection of powder characterization techniques from which to choose, the
applications within the industry exert some quite specific (though not unique)
demands. Quantifying flowability is essential because the material needs to
flow freely, in a controlled way, out of a hopper into the feed shoe and from
there to the die. Understanding the response of the powder to air is also
critical.
Air exerts a major influence on powder flow properties and is especially
important in die filling via gravity.
1,2,3 Here, the air
content of the powder in the feed shoe, while often uncontrolled, affects
flowability during discharge. Powder entrains air as it leaves the shoe, which
lubricates the filling process and simultaneously reduces bulk density. If this
air is not easily released as the powder settles in the die, then bulk density
remains low, compromising fill weight. De-aeration behavior is therefore also
highly pertinent. Sensitive differentiation in all of these areas is a vital attribute
of a truly useful characterization tool.
Many conventional powder measurement methods are limited by their lack
of reproducibility and questionable relevance to the manufacturing process. For
example, zirconia has excellent flow characteristics when tested using the Hall
flowmeter, but can flow poorly during die-filling
operations.
1 Furthermore, many techniques record just a
single parameter for a given powder, failing to capture the behavioral
complexity that ceramic processors need to assess. Powder characterization
technology has, however, developed significantly over the past decade. The
maturation of dynamic measurement techniques and the emergence of universal
powder testers that offer multi-faceted characterization are both worthy of
note.
A universal powder tester* combines conventional shear and bulk testing
with more modern dynamic methodologies. Dynamic measurements of the powder in
motion not only quantify flowability in an intuitively relevant
way, but also permit investigation of the impact of air. Samples can be
measured in a compacted, conditioned, aerated or even fluidized state. Closely
defined test protocols and sample conditioning give such instruments the
excellent reproducibility that makes them highly differentiating. They are
therefore valuable to those charged with developing ceramic granulates that
process well.
One example of a universal powder tester is
the FT4 from Freeman Technology.
The Importance of Conditioning
Powder samples arrive in a laboratory with a
processing history. They may have caked or compacted in storage, for example,
or become aerated during pneumatic conveying. Conditioning a sample prior to
measurement largely eliminates this history, setting a baseline state for analysis.
Gentle agitation of the powder bed, using a closely defined procedure, breaks
up weak agglomerates, releases air from an overly aerated sample, or introduces
it into a compacted one, leaving a homogeneous, loosely packed bed.
Pre-measurement conditioning greatly improves analytical reproducibility.

Figure 1. Schematic drawing for the die-filling process.
Investigating Die-Filling Performance
To compare and contrast the in-process
behavior of various materials, conditioned samples of tungsten, aluminum and
glass beads of two sizes were processed in a lab-scale die-filling rig. The rig
mimics a commercial operation and consists of a stationary die and a motor unit
that drives a powder-filled shoe across the die surface at a controlled
velocity of between 50 and 300 mm/s (see Figure 1). The cylindrical die has a
volume of 10 ml and diameter of 25 mm.
The mass transferred into the die during a single pass of the shoe was
measured for each powder to determine filling ratio (the ratio of actual mass
of powder in the die to a mass calculated from die volume and conditioned bulk
density). The experiment was repeated three times for each material, using a
newly conditioned sample of powder.

Figure 2. Die-filling ratio as a function of shoe speed for four different materials.
Filling ratios for all four materials are
shown in Figure 2. The larger glass bead sample, GL, clearly processes most
successfully in this unit, while tungsten gives the worst performance. High
filling ratios are achievable with tungsten when shoe speed is low, but this
would translate to a productivity restriction in an industrial setting.

Figures 3 and 4. The die-filling properties under different powder packing conditions of aluminum (top) and tungsten powder (bottom).
To broaden the study, the impact of the
packing state of the material in the shoe was assessed for two materials:
tungsten and aluminum (see Figures 3 and 4). This was achieved by switching
from a conditioned feed to an aerated one, and, in a separate experiment, to
one that was slightly compacted. The compacted feed was produced by tapping the
sample 20 times, while a lightly aerated state was reached by passing air
through the material at a velocity of 20 mm/s (aluminum) and 10 mm/s (tungsten)
immediately before loading the shoe.
Compacted powders are less likely than conditioned or aerated materials to flow
freely under gravity because of their closer particle packing and the loss of
entrained air. However, powders vary in this respect: cohesive powders can be greatly
affected, while coarse-grained materials often are not. Here, the aluminum
flows more freely into the die when aerated, improving the filling ratio. In
contrast, when the feed is slightly compacted, filling ratio falls. With
tungsten, a more dramatic reduction in filling performance is observed with the
compacted material, but results for the aerated and conditioned feed were
similar. In some cases with the tapped material, the powder bed formed a stable
bridge that prevented flow from the shoe, prohibiting any further filling.

Figure 5. The size and
morphology of tested powders by SEM: (a) GL glass beads, (b) GS glass beads,
(c) granular aluminum powder, and
(d) tungsten powder.
Rationalizing Process Performance
The particle size and shape of the four
materials were characterized by laser diffraction and scanning electron
microscopy, respectively, to provide some general information about the powders
(see Table 1 and Figure 5). Measuring an array of bulk, shear and dynamic
properties for all four materials produces a database of values that permits
rationalization of the observed processing performance (see Table 2†).
†All results in Table 2 were
generated using the FT4 from Freeman Technology; see References 4 and 5 for
additional details.

Table 1. General powder properties for four different materials.
The flow energy parameters of specific energy
and basic flow energy, which reflect flow behavior under unconfined and forced
conditions, respectively, indicate that tungsten is considerably less
free-flowing than the GS glass beads. Other indicators of flowability include
consolidation index, shear stress, cohesion, unconfined yield strength and
compressibility. Generally speaking, lower values of all of these parameters
are associated with powders that flow more readily.

Figure
6. Plot showing the relationship between filling ratio (at shoe speed of 230
mm/s) and specific energy.
The “flow” variables suggest that the
flowability ranking of the four materials is (from the most free-flowing to the
least): GS glass, GL glass, aluminum, tungsten. While this ordering broadly
correlates with die-filling performance, there is an obvious anomaly in that
the small glass beads exhibit lower die-filling ratios than the larger ones
(see Figure 6). In this case, analyzing flowability only partly rationalizes
process behavior, failing to accurately predict the relative behavior of the
two different samples of glass beads. The response of the powders to air is the
missing link.

Figure 7. Graph showing flow energy as a function of aeration velocity.
With a powder rheometer, aeration behavior is
studied directly by measuring flow energy as a function of air velocity through
the sample. Figure 7 shows how flow energy varies with air velocity (the raw
data from aeration testing), while Figure 8 is a normalized, derivative plot
illustrating the rate of change of flow energy as a function of air velocity.
The latter is an especially effective method of presenting the data in order to
clarify differences between the samples.

Figure 8. Normalized graph showing the rate of change of flow energy as a function of air velocity.
The results show that the GS glass beads
aerate to the point of fluidization extremely quickly (total energy of ~ 0 mJ).
Even at relatively low flows, air permeates evenly through the entire powder
bulk, separating virtually all of the particles and causing the bed to
fluidize. The flow energy of the tungsten also reduces rapidly with air flow,
but, importantly, it never becomes fluidized. Instead, it
stabilizes at a total energy of around 300 mJ. The strong inter-particulate
bonding of the fine tungsten particles gives the bed a cohesiveness that
prevents fluidization; the air channels through the sample rather than
lubricating each particle. Aluminum and the GL glass beads both fluidize, but
at significantly higher air velocities than the GS glass beads. The GL beads,
in particular, require a significantly larger air flow to reach the fluidized
state.
Permeability data suggest why this might be. Permeability, which is a
measure of how easily a material can transmit a fluid (in this case, air)
through its bulk, is influenced by many physical properties such as particle
size and distribution, cohesiveness, particle stiffness, shape, surface texture
and bulk density. It is important in many process environments and matters for
this study because it determines the discharge rate of entrained air during die
filling.
6 
Table 2. Dynamic, shear and bulk properties of four different samples.
The large spherical GL beads give rise to a
bed with significant voidage and relatively high permeability (low pressure
drop, see Table 2), from which air is easily released. The relatively large,
irregularly shaped aluminum granules produce a similar effect. In contrast, the
GS beads are around six times less permeable than the larger bead and are
therefore much more likely to retain air.
According to these data, the GL beads are more difficult to fluidize than the
GS beads for two reasons. First, they have a higher mass-to-surface area ratio,
which means that the upward force needed to support them, a pre-requisite of
fluidization, is greater. Second, the fact that the GL bed is highly permeable
means that it provides little resistance to air flow and easily releases any
entrained air, so fluidization is more difficult.
In combination with specific energy measurements, aeration and
permeability results rationalize the superior die filling ratios achieved with
the GL bead sample. Good flowability is confirmed by a low value of specific
energy, describing its excellent filling potential, and a high aeration ratio,
quantifying low cohesive strength. Once in the die, it rapidly releases air as
quantified by its high permeability.
In contrast, although it is more free-flowing (lower SE, higher AR), the
GS sample holds on to air in the die, reducing bulk density and consequently
the mass fill. This behavior was confirmed visually, though not quantified, by
observing bed collapse rates for all materials.
With its high aeration ratio, the aluminum sample shows it has minimal
cohesive strength, and, with its relatively high permeability, it is clear it
would de-aerate efficiently in the die. However, due in part to its irregular
particle morphology and lower bulk density, its filling performance is not as
good as either of the glass beads, as shown by a higher specific energy. It is
likely that a modification of the particle shape to a more spherical morphology
would transform this material into one that has the highest filling ratio.
These
findings suggest that optimal die filling performance requires a powder that is
free-flowing with relatively high permeability. An ideal powder aerates enough
to flow easily yet de-aerates sufficiently quickly to ensure complete die
filling. Quantifying these characteristics provides a specification for feed
materials that will perform well in this piece of equipment.
In Conclusion
Powder characterization that is both reliable
and relevant to the process makes it easier to develop a blend or granulate
suitable for ceramic powder processing applications. The study described here
highlights correlations between dynamic, bulk and shear properties, and performance
in die-filling operations.
Experimental data demonstrate that if powder flowability, aeration/de-aeration
characteristics and permeability are quantified reliably, it is possible to
predict die-filling performance. Modern universal powder testers sensitively
and precisely determine these essential characteristics of powder behavior,
supporting and accelerating development of the best possible feed materials.
For
more information regarding powder characterization, contact Freeman Technology
Ltd., Boulters Farm Centre, Castlemorton Common, Welland, Worcestershire, England,
WR13 6LE; call (44) 01684-310860; fax (44) 01684-310236; e-mail
tim.freeman@freemantech.co.uk; or visit www.freemantech.co.uk.Links