This invention relates to a grinder for reducing material to small particles which can then be used, for example, as a fuel, fertiliser, or an additive to other constituents, broken down small size particles for convenient waste disposal, providing particles for use in industry, and also for separating material. In many cases, it is necessary for the small particles to be reduced down to small particles which have a size in the range of 5 to 50 microns and in some cases, less than 5 microns.
Many devices exist that can reduce material to small particle sizes, but most are large, slow, heavy, and consume large amounts of energy. However, very few machines exist which can economically reduce particles down to very small fine particle sizes.
Grinding of materials to very small particles is carried out by a variety of machines. These machines employ two main processes. The first and most common, is by crushing the material between hard moving elements made from such materials as steel or silicates until the particles are of the required size. Repeated recycling may be employed to aid the process. Such machines are rolling, ball or hammer mills.
The second method is by employing high-energy impact. Machines using this principle cause high speed, hard moving elements, to collide with the particles to be ground. The particles to be ground are usually transported into and out of the impact area by gravity and by a gas, usually air. In some cases, material to be ground is carried only by gravity into the impact zone in the same way. As well as collisions with the grinding element, there are particle to particle collisions. However, these impacts make only a very small contribution because the particles are of much the same kinetic level and are moving in much the same direction. To achieve significant particle size reduction, recycling of the process must also be employed. A beater hammer mill is typical of such machines.
The crushing process is slow and usually limited in the mining and primary metallurgy industry. Impact grinding has the potential for fast throughput and great size reduction for other industrial and commercial particle grinding. The problem with present impact machines is that particle to particle impacts make only a small contribution, and hence the necessary energy level from the momentum transfer from the impacting elements must be at the highest energy necessary to break up the particles, that is the energy levels of the particles remain only as high as the initial impact.
A need therefore exists for a small, even portable machine that can achieve these results fast and economically.
An object of a first invention is to provide an impact particle grinder which can reduce gross particles down to a much smaller particle size.
A first invention may be said to reside in an impact particle grinder, comprising;
Thus, the impact grinder works using two principles. The first is by repeatedly injecting energy at higher and higher levels into the particles as they are reduced in size. This is a continuous energy intensifying process.
The grinder therefore processes material step by step to higher energy levels as it impacts further out towards the periphery of the disc. This results in very great size reduction. Recycling therefore is only employed by the machine to act upon particles, which have not reached the requisite energy level by the time they impact with a radially most outward part of the disc.
Depending on the size of the particle required, the particles can simply be discharged from the machine. However, if very fine particles are required, the particles can undergo further processing to reduce the particles to fines.
In the preferred embodiment of the invention, the additional grinding to produce the small particles is performed in the grinder by establishing a further grinding zone between the periphery of the spinning disc and a stationary wall of the grinder. This embodiment requires the invention to operate in a gas rather than a vacuum, with the gas usually simply being air.
While operating in a transport medium such as air, each particle will, as it moves to the periphery and into the grinding zone. The grounding zone is formed by a sheer zone which causes comminution of the particles to form the small particles.
In the preferred embodiment of the invention, the inner wall of the housing is of inverted conical shape so that deflection of material from the inner wall tends to direct the material to the second location which is a small distance from the first location, thereby producing a significant number of impacts of the material with the disc as the material bounces between the disc and the inner wall. The result of this increased number of collisions produces a greater number of impacts which impart increased kinetic energy to the material, and therefore greater breakdown of the material due to those impacts and particle to particle collisions.
In one embodiment of the invention the grinder includes hot air inlet means for introducing hot air into the housing adjacent the disc for drying the material as the material is ground.
In one embodiment the grinder also includes inert gas introduction means for introducing inert gas to mix with the ground particles.
In one embodiment of the invention the outlet means is arranged above the disc.
In one embodiment, the outlet means comprises a plurality of outlets which are arranged at different heights above the disc so that particles of different sizes are collected in each of the outlets, the outlets being provided in a housing wall portion which is of conical shape.
The outlet means may include a recirculator for recirculating small particles from the outlet means back to the housing for reprocessing in the housing.
In one embodiment, the outlet means is connected to a cyclone particle collector.
Preferably the cyclone particle collector comprises means for creating a circular flow of air in the cyclone, inlet means connected to the outlet means for receiving particles from the housing and for conveying the particles into the cyclone for circulation in the circular air flow in the cyclone, an air outlet tube in the cyclone and a particle outlet in the cyclone, and wherein particles trapped in the circular flow of air are conveyed about the cyclone with the circular flow of air and separated from air flow so that the particles can be collected in the particle outlet and air exit the cyclone through the air outlet.
Preferably the air inlet means for creating the circular flow of air comprises a hot air inlet and a heater for heating air for supply to the hot air inlet.
In one embodiment of the invention, the disc has an outer periphery which is in close proximity to the inner wall of the housing so that when the disc is rotated by the rotating means, an annular rotating stream of air is formed between the periphery of the disc and the inner wall, so a sheer zone is created between the periphery of the disc and the inner wall so that when particles enter the space between the disc and the inner wall, they are subject to the shear zone to further reduce the particles to small particles.
An air inlet means is preferably provided below the disc in the housing for allowing air to enter the housing from below the disc to cause the air annulus to spill up the inner wall of the housing so that finely ground particles trapped in the rotating stream of air are carried by the spill of air to the outlet means.
In another embodiment of the invention, the outlet means is arranged below the disc. This embodiment would be used in environments in which the grinder is operating in a vacuum or extremely low air pressure environments, and in which the air stream at the periphery of the disc is therefore not created. Thus, in this embodiment, small particles have no option but to fall under the influence of gravity in the space between the periphery of the disc and the inner wall of the container to the outlet means below the disc.
In one embodiment the disc includes a plurality of vanes for imparting momentum to the air when the disc rotates to create the annular rotating stream of air between the periphery of the disc and the wall to create the sheer zone.
Preferably the vanes are angled upwardly relative to the horizontal so that the rotating stream of air is directed upwardly above the disc to facilitate the spill of air up the inner wall.
Preferably the inner wall of the housing includes a separate cylindrical wall which includes a contoured wall portion for trapping material so the material remains in the annular airflow for a long period to break down the material to small particles, before the small particles travel in the spill of air up the inner wall to the outlet.
This invention also provides a method of impact grinding a material, comprising;
A second invention is concerned with the breakdown of material into smaller particles.
This invention provides a grinder for producing small particles from material, comprising:
In this invention the particulate material may be delivered to the housing from an inlet direct to a location near the periphery of the disc for substantially direct feeding into the sheer zone.
Thus, in this embodiment the inlet may comprise an inlet tube extending within the housing from an upper portion of the housing to a position adjacent the periphery of the disc.
However, in another embodiment, the particulate material may be gross material which is first broken down by impact with the disc and the housing into small particle size which small particles then move to the sheer zone for further breakdown into small particles. In this latter embodiment the inlet generally comprises a tube which delivers the gross particulate material to a location inwardly of the periphery of the disc.
Preferably the housing has a gas inlet below the disc and the vanes are located on a lower surface of the disc for collecting the gas and directing the gas to the periphery of the disc to provide energy intensification to the gas so that the gas at the periphery of the disc moves with high speed, and the gas adjacent the stationary inner wall is at relatively low speed.
Preferably the grinding zone comprises a first region between the wall of the housing and an intermediate location between the wall and the periphery of the disc for establishing a heavy gas, and a second region between the periphery of the disc and the intermediate location for receiving particles from the disc so those particles can move into the heavy gas and be ground into small particles.
Preferably a sheer zone is created at the intermediate location between the first and second regions.
Preferably the vanes are located on the lower surface of the disc and are directed upwardly so that the vanes direct the gas to the periphery of the disc and upwardly relative to the disc so that the annular flow of gas created by each of the vanes between the disc and the inner wall, and within the confines of the disc for a short time period and then moves upwardly relative to the disc in annular fashion adjacent the inner wall of the housing.
Preferably the housing has an exhaust gas outlet arranged substantially centrally of the disc.
Preferably a standing wave is created between the exhaust gas outlet and the periphery of the disc so that particles which are broken down into small particles in the sheer zone are able to move upwardly with the airflow adjacent the inner wall of the housing to the outlet, or move inwardly of the disc where they meet the standing wave and are directed down back to the upper surface of the disc and move along the upper surface of the disc back to the sheer zone for further grinding, or travel with the exhaust gas to the exhaust outlet.
Preferably the outlet is connected to a first cyclone for separating gas from the small particles so the small particles can be collected at an outlet of the first cyclone.
Preferably the exhaust gas outlet is connected to a second cyclone so the gas and small particles can be separated in the second cyclone to enable the small particles to be collected at an outlet of the second cyclone.
Preferably the first cyclone has a gas exhaust outlet which is connected to the second cyclone so that any small particles which remain in the gas exhausted from the first cyclone are fed to the second cyclone for separation from the gas in the second cyclone.
Preferably the outlet from the first cyclone includes a gas lock for preventing high pressure gas from exiting the outlet and blowing small particles into the atmosphere.
Preferably the outlet from the second cyclone also includes a gas lock for preventing high pressure gas from exiting the second cyclone through the outlet.
This invention also provides a method of producing small particles from material, comprising:
Preferably the method includes allowing the gas to enter the housing from below the disc and providing vanes on a lower surface of the disc for collecting the gas and directing the gas to the periphery of the disc to provide energy intensification to the gas so that the gas at the periphery of the disc moves with high speed, and the gas adjacent the stationary inner wall is at relatively low speed, and wherein the grinding zone is created by the establishment of:
Preferably the annular flow of gas created by each of the vanes between the disc and the inner wall is maintained within the confines of the disc and at the sheer zone for a short time period and then moves upwardly relative to the disc in annular fashion adjacent the inner wall of the housing.
Preferably the method comprises extracting gas from an exhaust outlet arranged substantially centrally of the disc.
Preferably the method further comprises creating a standing wave between the exhaust outlet and the periphery of the disc so that particles which are broken down into small particles in the sheer zone move upwardly with the airflow adjacent the inner wall of the housing to the outlet, or move inwardly of the disc where they meet the standing wave and are directed down back to the upper surface of the disc, and move along the upper surface of the disc back to the sheer zone for further grinding, or travel with the exhaust gas to the exhaust outlet.
Preferably the method further comprises supplying the collected small particles to a first cyclone for separating gas from the small particles so the small particles can be collected at an outlet of the first cyclone.
Preferably small particles collected at the exhaust outlet are supplied to a second cyclone so the gas and small particles can be separated in the second cyclone to enable the small particles to be collected at an outlet of the second cyclone.
The invention also provides a grinder for producing small particles from material, comprising:
The invention still further provides a method of grinding material, comprising:
A third invention relates to a grinding installation for grinding material into small particles.
This invention provides a grinding installation for producing small particles from material, comprising a grinder having:
Preferably the first separator has a first exhaust air outlet and the first exhaust air outlet is connected to the second separator.
Preferably the first separator comprises a cyclone separator.
Preferably the second separator comprises a second cyclone separator.
A fourth invention provides a grinder for producing small particles comprising:
Preferred embodiments of the invention will be described, by way of example, with reference to the accompanying drawings in which:
With reference to
The cyclone 14 has a small particles outlet tube 22 and an air exhaust outlet tube 24. An air heater 26 is provided for heating air and for supplying hot air through delivery tube 28 to valve 30. A first inlet 32 is coupled between the valve 30 and the housing 12 for selectively supplying hot air to the housing 12, and a second inlet tube 34 extends between the valve 30 and the cyclone 14 for providing hot air into the cyclone 14 for creating a circular cyclonic flow of air within the cyclone 14.
The housing 12 is supported on a cylindrical casing 36 and flange 38 which connects to an electric motor 39.
As is best shown in
A disc 60 is mounted in the casing 46 and is supported on a shaft 62 which is arranged in bearings 66 and bushes 68 within the cylindrical casing 36. Thrust bearings 70 may also be provided if desired.
The cylindrical casing 36 is secured to the base 47 of the dish casing 46 by flange 68a on the cylindrical casing 38.
The flanges 44 and 52, the flanges 42 and 48 and the flange 70 and base 47 can be connected together by bolts 71, which are shown joining the flanges 44 and 52, as well as the flanges 42 and 48.
If the grinder is to be used for the breakdown of soft or very light material, such as feathers or the like, a separate removable cylinder 74 may be located in the housing 12 as shown in
The material inlet tube 20 is also used in situations where very soft or light material is to be ground. This tube 20 is also used if liquid or sludge type material is to be broken down by the grinder. In the case of light or soft material, the material can be directed through the tube 20 with an airflow injected into the tube 20 for carrying that material along the tube 20 to outlet end 80. As is shown in
As is best shown in
The inner wall 74 has a contoured wall portion 102 adjacent the periphery of the disc 60.
When the disc 60 is rotated, the disc 60 creates an annular or a circular air flow adjacent the periphery of the disc 60 between the disc 60 and the wall 74. By angling the vanes 100 upwardly, as is shown in
The base 47 of the casing part 46 has a plurality of air inlet openings 108 which also facilitate spillage of air up along the inner wall 40. Air can enter the inlets 108 and is drawn by the low pressure environment at the periphery of the disc (as will be described in more detail hereinafter) so as to tend to push the annular air stream at the periphery of the disc upwardly along the wall 40.
The casing 120 has a plurality of outlet openings 124 and 126 which are formed in the conical wall of the casing 120. The outlet openings provide for separation of particles of different sizes carried by the air flow which spills up the inner surface of the casing 40 and then up the inner surface of the casing 120. This separation process will be described in more detail hereinafter.
Also, in the embodiment of
It should also be noted in
It should of course be understood that the movement of the material between the disc 60 and the wall 40 is somewhat chaotic because of the breakdown of the material and therefore the change in size of the material, as well as the angle of collisions, which will deflect the material in various different directions. However, the general travel of material as the material breaks down will be in accordance with the arrows shown in
Whilst it is preferred that the wall 40 have an inverted conical shape, as is shown in
The breakdown mechanism described with reference to
When material is ground in the manner in which we described hereinafter, at least some of that ground material moves up the housing 12 to outlet tube 16. As previously explained, the outlet tube 16 supplies the ground particles to the cyclone 14. The cyclone 14 can be used to collect the fine ground particles and also to provide some separation of particle sizes.
As is shown by
The air and particulate material which exits the outlet 16 is supplied to the cyclone 14. The air supply through the outlet 16 to the cyclone 14 is directed tangentially into the cylindrical cyclone 14 as shown in
As is shown in
The cyclonic air flow within the housing 14 separates the particles from the air flow so that the particles are able to drop under the influence of gravity into particle outlet 22 whilst the air is able to exit the cyclone 40 through air outlet tube 24.
The outlet tube 24 will generally be at higher pressure than the reduced pressure region in the centre of the housing 12 and the air inlet 18 can therefore be connected to the outlet tube 24 for the supply of air back into the housing 12 through the inlet 18. Any very small particles which are still trapped in the air flow in the outlet 24 therefore have the opportunity to pass back into the housing 12 for reprocessing.
In other embodiments (not shown), as well as or instead of the cyclone 14, electrostatic or magnetic precipitators, or gas scrubbers, could also be used for removing fine particles. The electrostatic or magnetic precipitators or gas scrubbers could be used in the inlet 18 shown in
As previously mentioned, if desired, hot air can be supplied to the housing 12 through hot air inlet 32 (not shown in
In other applications where the supply of hot air is undesirable (such as the breakdown of coal or the like, which may ignite or explode during breakdown), the valve 30 can be shut off to ensure that no hot air is supplied to the housing 12. In other embodiments, the inlet 32 could be connected to an inert gas supply for supplying inert gas in the event of breakdown of volatile materials such as coal or the like, to eliminate the possibility of ignition or explosion of the material during breakdown in the grinder 12.
The grinder installation 11 is supported in a support frame 199 which could be mounted on wheels or casters 201 to enable the support frame and grinder to be moved from place to place. Alternatively, the support frame 199 may simply be fixed to the ground or floor. Support frame 199 merely supports all of the components of the grinder installation 11. In this embodiment, inlet tube 20 is vertical and is connected to a hopper 203. The hopper 203 may be connected to the inlet tube 20 by a feed regulating valve 205 so that, if desired, material in the hopper 203 can be feed in a controlled manner to the housing 12. The outlet tube 16 may also have a regulating valve 206 to control flow of ground small particles through the outlet 16 to the cyclone 14. A first blower 207 is provided for blowing air through air tube 208 to the housing 12. The air tube 208 may communicate with at least one of the holes 108 (see
Air exhaust 18 from the housing 12 connects to air exhaust outlet pipe 215 from the cyclone 14 and the outlet pipe 215 is connected to a second cyclone 216. The cyclone 14 has a small particle outlet 217 which is provided with a gas lock 218 (see
Thus, ground particle which exit the housing 12 through the outlet tube 16 are provided to the cyclone 14 where the particles are separated from the airflow and which can be collected in a container (not shown) arranged below the particles outlet 217. Air exits the cyclone 14 through outlet tube 215 and any very small particles which are still entrained in that airflow are supplied to the second cyclone 216. Those particles are separated in the cyclone 216 and are collected in a container (not shown) below the particles outlet 219. The air supplied to the cyclone 216 from the outlet tube 215 exhausts from the cyclone 216 through exhaust outlet tube 220. The outlet tube 220 may be connected to a final filter or scrubber for collecting the very fine particles which may remain entrained in the airflow exhausted from the second cyclone 216.
The gas locks 218 are shown in
Thus, small particle material which enters the inlet 221 collects in the space 227 between the vanes 224a and 224b. The particles which are collected in the space between the vanes 224b and 224c is allowed to drop through the outlet 223 and the space between the vanes 224a and 224c is empty. Thus, the outlet 223 is always sealed from the inlet 221 by the rotor 222 so that relatively high pressure air in the cyclone 216 (or 214 as the case may be) is not able to communicate with the outlet 223. This allows the fine ground material to simply drop under gravity out of the space between the adjacent pair of rotors as that space comes into communication with the outlet tube 223 and therefore will not be blown out in a cloud of fine dust, which may otherwise happen if the gas lock 218 was not provided. Thus, the spaces between adjacent vanes 224a, 224b or 224c are sequentially filled with fine ground material and are emptied as those spaces move into communication with the outlet tube 223 so that the small particles simply drop under the influence of gravity into the container (not shown) located below the outlet 223.
The periphery of the disc is spaced from the inner wall 102 by a distance of 10 to 30 mm. However, a larger space could be used depending on the nature of the material to be ground. The disc is about 400 mm in diameter and is rotated at a speed of about 4500 rpm. The disc has a weight of about 5 to 10 kg. However, obviously larger or smaller machines could be produced by scaling these dimensions.
When the disc 60 is rotated, the vanes 100 produce a flow of air from the air which enters the holes 108. The blower 207 may be used to provide an initial speed to the air as the air enters the housing 12 so that that air is collected by the vanes 100 as the disc 60 rotates to produce the high speed airflow at the periphery of the disc 60 generally in the vicinity of the contoured wall 102 which, together with the periphery of the disc 60, generally defines the main grinding zone Z. It should be understood that the blower 217 need not be used and air could simply enter the housing 12 through the openings 108 for collection by the vanes 100. Thus, the vanes 100 and the rotating disc 60 produce a generally lamina airflow at the periphery of the disc which is very fast immediately adjacent the periphery of the disc, and most preferably at least as fast as, if not faster that the speed of the periphery of the disc. The rotating disc, together with the vanes 100, therefore provides energy intensification of the air within the housing 12 at the periphery of the disc in the grinding zone Z. Thus, the stationary air below the disc 60 and within the housing 12 is therefore accelerated up to high speed at the periphery of the disc. If the air is introduced with some speed by the blower 207, then the speed of the air is further accelerated by the disc 60 and vanes 100.
As is shown in
If relatively large particulate material is deposited into the housing 12, such as broken glass which may have a size of about 10 mm or larger material, initial breakdown occurs due to impact with the disc 60 and the side wall of the housing 40 as previously described. Small particles will find their way into the grinding zone Z and further breakdown will occur due to particle to particle collisions in that zone and also possibly some collisions with the wall 102, although these latter collisions are likely to be much fewer than the particle to particle collisions. As the particles begin to break down into small particle sizes, the grinding zone Z starts to establish itself.
The manner in which the material is ground in the grinding zone Z will be described with reference to FIGS. 14 to 17. This form of grinding is applicable to both the embodiments of FIGS. 1 to 7 and 8 to 13. Small particles in the housing 12 will eventually find their way to the periphery of the disc 60. This can happen by breakdown of large gross material in the manner described with reference to
As the particles begin to break down into smaller particle sizes, a range of particle sizes will be created. Some of those particle sizes will be very small and probably in the order of about 200 to 800 nanometres. These particles are entrained in the annular gas flow created in the grinding zone Z between periphery 60a of the disc 60 and the wall 102. This air flow is made up of molecules of the gases making up the air and the small particles held in an aerosol suspension within the air. If the suspended particles are small enough, this air particle mixture will act generally as a gas within a certain range of temperatures and pressures, that is, it will obey gas laws relating to temperature and pressure and increase in kinetic energy of all of the particles when heated. This gas mixture is referred to herein as a heavy gas. This heavy gas generally forms in a region R1 which is radially outwardly of the periphery 60a of the disc 60. The reason for this is that the heavy gas is generally pushed out to this region by the gas flow created by the vanes 100. The very small particles which mix with the air molecules to form the heavy gas generally remain in the region R1 outwardly of the periphery of the disc 60 because they are adjacent to a stationary wall, and therefore move more slowly than the newly entering air from the vanes 100. The heavy gas region R1 is therefore moving at a slower speed than the gas in region R2 and which will form a boundary layer which will become the sheer zone S2 between the regions R1 and R2 when the larger particles migrated into the grinding zone Z from the disc 60. Thus, if heat is added to the heavy gas, kinetic energy is increased, thereby increasing the grinding effect with little, if any, added mechanical energy. The heavy gas therefore generally acts like a normal gas such as air, but is formed by molecular particles carrying a suspension of larger, but very small particles. The suspended particles usually cannot be filtered or settled in devices like cyclones, and are generally analogous to a liquid colloid suspension. As the heavy gas region R1 builds up, the sheer zone S2 is therefore created between the region R1 and the second region R2 between the sheer zone S2 and the periphery 60a of the disc 60. The region R1 of the heavy gas particles generally forms radially outwardly of the disc 60a because of the relatively small size of those particles. A low friction air cushion exists in a region R3 between the wall 102 and the region R1 which moves slower than the heavy gas flow in region R1 and a sheer zone S1 is created between the regions R3 and R1. In the region R3, the air is moving very slowly because of contact with the wall S1 and therefore the particles in the region R1 tend not to move into that region, but remain within the region R1 between the sheer zone S1 and the sheer zone S2. The larger particles which are initially provided in the region R2 will at random come into contact with the sheer zone S2 or pass through the sheer zone S2 into the region R1. At the sheer zone S2, or if they move into the region R1, they are bombarded by the heavy gas and, in particular, the small particles to cause breakdown of those larger particles into smaller particle sizes. This will in turn form particles of varying sizes and again, some of those particles will be of the very small size which simply add to the heavy gas in the region R1 and others will be slightly larger particles. The region R1 therefore fills with particles, both of a relatively small size to form the heavy gas, and also slightly larger sizes. Thus, some of the particles which pass through the sheer zone S2 or which simply arrive at the sheer zone S2 are comminuted into heavy gas particles by collision with existing heavy gas particles in the region R1 and at the sheer zone S2. Some of the particles which are communicated are not sufficiently small to behave as heavy gas particles, and some of those particles will be quickly ejected back to the region R2. This is because the differential air speeds of the heavy gas and the newly introduced gas from the vanes 100 will have a pressure difference. However, as the number of particles in the region R1 and R2 tends to build up, in the annular flow of air between the periphery of the disc 60a and the sheer zone S1, some of the particles will tend to spill upwardly out of the sheer zone Z along the wall 102. Movement of the particles in this direction is facilitated by the upwardly directed flow of air which is created by the vanes 100.
The particles which move out of the grinding zone Z will be largely particles which have entered the heavy gas region R1 and which are broken down into smaller particle sizes, but not sufficiently small to act as a heavy gas, together with some of the heavy gas particles, and also some of the particles from the region R2 which are still relatively large.
Of those particles which leave the region Z, most of the heavy particles will tend-to move into a complex field created above the disc 60, and which will be described in more detail hereinafter, and will be recirculated back down onto the disc 60 to migrate back to the grinding zone Z for further grinding. However, some of those larger particles, together with small particles, and also some heavy gas particles and small particles which are created in the grinding zone Z will either move with the upwardly moving air stream to the outlet 16, or be entrained in the exhaust gas exhausted from the housing 12 through the exhaust outlet 18.
Because the disc 60 has a plurality of vanes 100 and is rotating relatively fast, a very stable and coherent annular generally laminar flow of air is created at the grinding zone Z which is directed slightly upwardly relative to the disc 60 and therefore, a stable and coherent annular grinding zone Z is created in the annular region around the disc 60 between the periphery 60a and the wall 102, to therefore form a grinding zone Z which has a substantial size. The continued pumping of air into the grinding zone from the plurality of vanes 100 ensures that the airflow within the grinding zone Z is stable and coherent so that the heavy gas region R1 of heavy gas particles is established and maintained.
Thus, a stable and coherent grinding zone Z is built up and is maintained between the periphery of the disc 60a and the wall 102, which is comprised of the sheer zone S2 between the larger particles in region R2 and the heavy gas within the region R1. Because the disc 60 is spaced a relatively small distance from the wall 102 and effectively defines a uniform annular space between the periphery 60a and the wall 102, and air is continually fed into that space by the vanes 100 attached to the rotating disc 60 a uniform and coherent heavy gas annulus is maintained in the region R1.
Thus, as larger particles move into the region R2, those particles come into contact with the heavy gas in the region R1 at the sheer zone S2 and are further comminuted by particle to particle contact at the sheer zone S2 so that those larger particles in the region R2 contribute more fine particles to the heavy gas in the region R1. As the region R1 overfills with fine heavy gas particles and small particles which are larger than the heavy gas particles, those particles begin to spill upwardly along the wall 102.
The high energy environment of the heavy gas annulus in the region R1 will produce other changes in the particles within the region R1. Some of these changes will involve surface molecular dissociation and sublimation and will result in the production of continuously finer particles.
The particles remain in the region R1 for a relatively short time period, and probably significantly less than one revolution of the disc 60 (although very small particles may stay in the region R1for longer), as will be described in more detail with reference to
As can be seen from
As the number of heavy gas particles and small broken down particles build up in the region R1, the particles generally move upwardly with the airflow created by the vanes 100 which, as previously described, direct the airflow upwardly relative to the disc 60. The movement of the airflow may also entrain some of the particles from the region R2. The fine particles created in the region R1 with perhaps a few of the larger particles from the region R2 will move up the wall 103a and the wall 40 of the housing 12 in bands of rising air 260.
Those particles are entrained in a rotating, generally lamina flow of stream tubes 280 (which will be described in more detail with reference to
The particles which enter the complex vector field above the disc in the region 250 meet a generally standing wave 270 formed in the air above the disc 100. Large particles in those particles which meet the standing wave 270 tend to be moved back to the periphery of the disc 60 and back into the grinding zone Z for further grinding. The very light fines tend to do a loop as shown by arrow A in
The larger particle which meets the standing wave 270 and which are directed back down to the disc 60, moves back to the grinding zone Z as previously described, for more grinding until those particles are broken down into a particle size which will either travel up the wall 40 in the manner previously described, or which will be entrained in the airflow exiting the exhaust outlet 18.
In the preferred embodiments, the vanes 100 are directly upwardly as previously described. However, the vanes could be arranged substantially horizontally, and the angle of the wall 102 inclined more than that shown in the drawings so as to send the gas stream produced by the vanes 100 upwardly into the grinding zone Z.
If desired, pins or other like elements may extend upwardly from the base of the housing into the grinding zone Z at about the vicinity of the sheer zone S2 to create some turbulence at the sheer zone which tends to assist the mixing of particles from the region R1 at the sheer zone with the heavy gas in the region R2 to comminute the heavy particles into smaller particles at the sheer zone S2 in the region R1.
The preferred embodiment of the apparatus may also be used in a vacuum. If the apparatus is used in a vacuum, the initial grinding process described with reference to
If it is desired to grind very light particles such as feathers or wheat flour, and very fine particles required, it is necessary to establish the heavy gas other than from the material which is to be ground in the same manner as described above. In such embodiments, the heavy gas may be formed by adding water or some other particle such as the silicates or the like.
As is shown in
Since modifications within the spirit and scope of the invention may readily be effected by persons skilled within the art, it is to be understood that this invention is not limited to the particular embodiment described by way of example hereinabove.
Number | Date | Country | Kind |
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PS 2361 | May 2002 | AU | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/AU03/00588 | 5/16/2003 | WO | 11/16/2004 |