Very small particles are used in a wide variety of manufactured products. In many of these products, the particles must be of extremely small size, but the small particles must be as uniform in size as possible. Examples of products containing extremely small particles of uniform size include pharmaceuticals, abrasives, inks, high-performance liquid chromatography columns, foodstuffs, and many others.
Separation of particles by size is a critical step in the production of such particles. Particles having an average size of about 40 microns or larger can be collected by using micromachined filters. To collect, or harvest, particles having an average size smaller than about 40 microns is often accomplished by air classification. Air classification uses Stokes drag to separate particles by size. A particle falling under the influence of gravity (either the earth's gravity or an artificially induced gravitational field such as that provided by a centrifuge) in a viscous fluid medium such as air will have a terminal velocity that is strongly dependent upon the diameter of the falling particle. Differently sized particles fall through air or other viscous fluid media at different rates, thus separating in space and enabling them to be easily harvested by size.
Air classification processes works tolerably well for the separation and harvesting of particle sizes down to about two microns. However, the efficiency of the classification process depends crucially on the properties of the viscous fluid medium through which the particles are sedimenting.
But when the particles to be separated, sized, and harvested have a geometric average diameter of less than about two microns, air classification and other systems are difficult to use. Reasons for this can be inferred from
It is accordingly the general object of this invention to provide a device for separating extremely small particles according to their average diameter or size. A related object is to provide such a device which will operate in a relatively rapid and reliable matter.
Another related object of the invention is to utilize a sedimentation medium which will encourage and permit particles of extremely small size to separate and sediment relatively rapidly and in a reliably predictable manner.
Yet another object of the invention is to provide a device for separating extremely small particles which can be operated relatively easily and at relatively small expense.
Although the preferred embodiment described below provides a device for separating particles by size, it is clear that in general the process could be extended to separate particles by shape, mass, density mechanical defect, or any other characteristic which causes some of the particles to fall through a medium faster than other particles.
Other objects and advantages of the invention will become apparent upon reading the following detailed description and upon reference to the drawings. Throughout the drawings, like reference numerals refer to like parts.
a is a sketch showing an extremely small particle and the wetting action imposed by a fluid surrounding the particle.
b is a sketch similar to
While the invention will be described in connection with certain preferred embodiments and procedures, it will be understood that it is not intended to limit the invention to these embodiments or procedures. On the contrary, it is intended to cover all alternatives, modifications and equivalents as may be included within the spirit and scope of the invention as defined by the appended claims.
To accomplish the above objects, the invention comprises a quantity of low viscosity high wetting parameter fluid; means for injecting the particles to be sorted, separated and sized into that fluid; and means for harvesting at least some of those separated particles from the fluid.
The properties of superfluid helium make it an excellent medium in which to separate small particles. Ordinary liquid helium at 4.2 degrees Kelvin has a viscosity 5.5 times less than that of air at 20 degrees centigrade. A low viscosity medium suggests a relatively high terminal velocity for particles passing through the medium. In addition, if a low temperature can be maintained in the medium, the effect of Brownian diffusion on particle dynamics will be minimized. Furthermore, liquid helium has a very high wetting parameter; that is, helium atoms have a greater affinity for foreign objects than they do for other helium atoms. As a result, and as suggested in
However, because liquid helium will boil under ordinary conditions, superfluid helium is an even better sedimentation medium. Superfluid helium can be produced relatively simply by lowering the pressure above a container filled with ordinary liquid helium. The physical properties of superfluid helium are so different from ordinary helium liquid helium, or Liquid Helium I, that superfluid helium is considered to be a unique state of matter; it is neither a solid nor liquid nor gas. Either 3He or 4He or a combination of 3He and 4He can be used.
The pressure and temperature constraints for superfluid helium or Liquid Helium II are shown in the phase diagram of
A device for sorting, separating and sizing extremely small particles is suggested schematically in
The closed, gas-tight loading chamber 20 includes a receiver 22 for receiving particles 10, 11 and 13 to be separated and for loading the particles 10, 11 and 13 into the cryogenic chamber 40. A gate valve 23 is interposed between the receiver 22 and the cryogenic chamber 40 for controlling the flow of particles from the loading chamber 20 to the cryogenic chamber 40.
Above or upstream of the receiver 22, a vacuum conduit 25 is connected via appropriate valving 27, 28 to a vacuum or exhaust pump (not shown) for drawing air from the receiver 22. A delivery conduit 29 delivers helium to the receiver 20 when appropriate valving 30, 27 is opened. The particles 10, 11, 14 to be classified, sorted and sized can be delivered from a remote source (not shown) through a conduit 32 and inlet valve 34 to the receiver 22. At appropriate time, the gate valve 23 is opened and the particles flow from the receiver 22 through a delivery conduit 36 extending into the interior of the cryogenic chamber 40 by a sufficient distance so that the particles are deposited within superfluid in the cryogenic chamber 40.
In accordance with one aspect of the invention, the cryogenic chamber is adapted to produce and maintain a column of very low viscosity, high wetting fluid such as superfluid helium 4He. An OptistatSXM Helium bath cryostat can be adapted and used for this purpose. This device is available from Oxford Instruments Superconductivity USA of 130A Baker Avenue Extension, Concord, Mass.
As indicated above, particles falling through the superfluid medium in the cryogenic chamber tend to separate according to their size; larger particles tend to fall faster and arrive at the bottom of the column before the slower-falling smaller particles. To distinguish between these differently sized particles in accordance with another aspect of the invention, differentiation or size recognition equipment 90 can be provided, as suggested in
This information about particles sizes can be used to harvest particles of a desired size or sizes and to discard particles which are excessively large or excessively small. This particle harvesting can be accomplished in any of a number of ways. For example, particles 11 which are too large will reach the bottom of the chamber apparatus first, before any particles of the desired size arrive. Under the circumstances, the superfluid helium in a discard conduit 42 can be pumped out, drawing off the oversized particles 11 with the fluid. Thereafter, when particles of the desired size begin to reach the bottom of the column, discard column pumping is halted and the superfluid helium and right-sized particles can be drawn-off from the column 40 by a harvest conduit 44 and pump (not shown). When particles 13 which are too small to meet requirements begin to arrive at the bottom of the column 40, pumping and particle draw off or removal through the harvest column 44 can be halted and particle withdrawal through the discard column 42 can be resumed.
Alternatively, a diverter baffle 47 can be located at the column bottom as illustrated in