As the need for smaller and smaller coated particles increases, the principle barrier to achieving uniform, contiguous coating has been the tendency for particles below 10 to 15 microns to severely agglomerate and clump.
Ordinary horizontal fluidized beds and barrel coaters are simply unable to overcome the strong interparticulate attractors, such as van der Waals forces, that increase with decreasing particle diameters.
Few of the prior art methods and apparatus are capable of effectively coating contiguous and homogeneous coatings on Geldart Class C powders.
This benefit, however, is considerably offset by the principal limitations of fluidized beds: agglomeration and bonding of the powders.
As is well-known, for example, when fluidized beds are used for the production or coating of very fine powders, particles in the bed are susceptible to (a) agglomeration by van der Waals and other interparticulate attractor forces and/or (b) sintering or cementing together of particles by the coating being deposited on their surfaces at high temperature.
If these agglomerated or sintered particles are not continuously broken apart, their points of contact prevent complete coating and the lumps may tend to grow and settle to the bottom of the fluidizing bed, greatly reducing effective surface areas.
Because most coated powder applications require complete and homogeneous coating layers, the foregoing factors prevent the use of all but a small number of the methods and apparatus taught in the prior art.
Even such reactors, capable of fluidizing, deagglomerating, and coating uniform Geldart Group C particles, are challenged beyond their capabilities of coating contiguous and homogeneous coatings in many practical industrial situations.
For example, an important limitation of the RFFB-CVDR and other high gas-shear reactors is that the gas-stream deagglomeration principle fundamentally requires high gas stream velocities.
Temperature or diffusion stress cracking and size reduction due to chemical reactions and shrinkage can also result in fine particles.
This occurs because small particles that are expelled from the top of the bed have high velocities that require greater distance to slow down and turn around to return to the bed.
The elutriation phenomenon leads to a major limitation of the RFFBCVDR.
Thus, heavy powder particles averaging below about 0.5 microns and light density particles averaging below about 5 to 10 microns contain major percentages of particles that are extremely difficult to separate from gas streams which overload the particulate collection systems and rapidly clog them.
When it is a primary objective to coat smaller Geldart Class C powders, as in the case of Tough-Coated Hard Powders (TCHP), operating this equipment was traditionally difficult to impossible.
It has been demonstrated using the RFFB-CVDR equipment on commercially-available 2-micron titanium nitride core powders, that nanofines quickly overload and clog the dust collection and filtration system.
Avoiding this condition requires an expensive and quality-degrading (oxygen-inducing) Stokes Law sedimentation classification process to separate the fines and substantially reducing the yield of the incoming core powders.
Another major disadvantage is that the RFFB-CVDR, which operates in turbulent gas flow fluidization conditions, cannot be scaled down to smaller-diameter, smaller-capacity fluidized beds for research and development and for high-value products.
Test increments of different coating weight percentages of the intermediate and binder coatings, plus test increments of extremely expensive core powder such as cubic boron nitride or diamond, or test increments involving different carbon percentages all become practically and economically out of reach because milling in test increments breaks off the coatings and blending has been found to be highly ineffective at these grain sizes.
Yet another major disadvantage of the RFFB-CVDR