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The present invention relates to an apparatus for pumping high-viscosity liquids, slurries and liquids with solids. More particularly, the present invention combines discoidal members of a centrifugal pump located in the pump housing so as to create a centrifugal pump that has better efficiency and lower maintenance cost than current pumps while pumping high-viscosity liquids, slurries and liquids with solids.
This invention relates generally to pumps for the handling of high viscosity liquids, slurries, and liquids with solids, collectively referred to as high-viscosity fluids (HVFs). Centrifugal pumps may be used for pumping HVFs; however, traditional centrifugal pumps have problems with cavitation, clogging, binding, and high wear when used with HVFs. This is due to the intrinsic nature of a typical centrifugal pump in which the impeller has vanes which are designed to shear and sling a liquid in order to impart a centrifugal force thereon.
To meet the shortcomings of traditional centrifugal pumps in pumping HVFs, those knowledgeable in the art have utilized various alternative types of pumps, including: progressive cavity pumps, screw pumps, gear pumps, lobe pumps, diaphragm pumps, and piston pumps. These pumps are used because they can have higher flow rates, outlet pressure, and efficiency than traditional centrifugal pumps; however, these alternative pumps are much more costly to maintain than centrifugal pumps. Further, these alternative pumps are more likely to degrade the quality of the fluid they pump because they are in direct contact with the HVFs and have tight tolerances.
Centrifugal pumps have been modified to meet the shortcomings of these alternative pumps in pumping HVFs. Such modifications include centrifugal pumps that use specially designed impellers. The more radical of these designs has completely done away with the vanes of a typical impeller. Some centrifugal pumps have been modified to create a vortex to help with pumping HVFs. These are known as recessed impeller pumps. Both of these designs are highly inefficient because they both have considerable slippage and dead zones.
Centrifugal pumps with disc impellers, despite being pumps that pump HVFs, are known to be highly inefficient because of dead zones. Disc impellers are impellers shaped like a disc that rotate in the fluid so as to impart motion on the fluid. Disc impeller can be provided with vanes or channels for imparting the necessary centrifugal force on HVFs. Alternatively, a disc impeller can be provided with no channels or vanes. Regardless of the existence of vanes on the disc impeller, dead zones are created at a certain distance away from the disc and slippage occurs at the surface of the disc. This is because disc pumps rely on boundary layer theory as the pumping mechanism, which means that HVFs are pumped by the movement created by friction between the surface of the disc and the HVFs. HVF speed is greatest next to the boundary where the surface of the disc meets the HVF. HVF speed decreases the further away it is from the disc surface until it reaches a distance where the HVF is stagnant. This is known as the dead zone, and dead zones create significant barriers to pumping efficiency in disc pumps.
Centrifugal pumps with disc impellers are also known to be highly inefficient because of slippage. The boundary layer theory explains why disc pumps are used with HVFs as opposed to low-viscosity fluids. The more viscous a HVF, the more likely it is to create friction with the surface of the disc. It is this friction that imparts motion on the fluid, so a fluid that is non-viscous would never pump because the friction at the disc boundary is too low to cause movement. Disc impellers do create enough friction to move HVFs, but nonetheless, slippage still exists for HVFs, and efficiency is sacrificed.
Vortex impellers, called “recessed impellers” because of their special design for pumping, also have slippage and dead zone problems. A recessed impeller's vanes are retracted compared to a typical impeller, with the front of the impeller being the small part of the cone and the back of the impeller being the larger part of the cone. This design creates a tornado effect through which torque is imparted unto the HVF by only contacting a portion of the HVF. As in disc pumps, dead zones exist at a distance away from the surface of the impeller (usually on the periphery of the housing near the inlet), but vortex pumps also have a dead zone at the tip of the recessed impeller. While the efficiency of vortex pumps is better than disc or dual disc pumps, it is still much lower than the alternative pump designs mentioned above.
U.S. Pat. No. 4,439,200, issued on Mar. 27, 1984 to Meyer et al., discloses a centrifugal pump utilizing a disc impeller with channels. This pump employs an impeller in the shape of a disc which acts directly upon the material to impart the necessary rotary motion. With this particular disc, centrifugal force is imparted on HVFs by radially extending channels on the surface of the disc. The HVFs flow through the channels to attain the desired rotary motion.
U.S. Pat. No. 6,315,532, issued on Nov. 13, 2001 to Appleby, discloses a centrifugal pump for pumping HVFs that has two disc impellers instead of just one. Both discs rotate so as to impart centrifugal force on HVFs. Efficiency of a dual disc design is improved over that of a single disc, but it is still relatively low because of the inherent nature of disc pumps. As discussed above, HVF speed in disc pumps is greatest at the boundary where the surface of the disc meets the HVF, and speed decreases as the HVF moves away from the surface, creating dead zones. Dual disc pumps reduce the size of the dead zone in disc pumps, but dead zones are not eradicated. Additionally, the dual disc design also has slippage just as the single disc design. Thus, efficiency is still a problem in dual disc pumps because of slippage and dead zones located between the disc impellers where there is no HVF movement.
U.S. Pat. No. 4,135,852, issued on Jan. 23, 1979 to W. Archibald, provides a centrifugal pump utilizing an impeller with vanes that creates a vortex to pump HVFs. In other words, the impeller only acts upon a small portion of the HVF passing through the pump vortex chamber and induces centrifugal forces within a vortex chamber so as to induce vortical movement of the HVFs.
Despite these modifications, these improved centrifugal pump designs are still highly inefficient because of considerable slippage and the existence of dead zones.
It is an object of this invention to provide a centrifugal pump for pumping HVFs.
It is a further object of this invention to provide a centrifugal pump that minimizes slippage and dead zones typically found in centrifugal pumps that pump HVFs.
It is still a further object of this invention to minimize the wear increase the efficiency of centrifugal pumps when pumping HVFs.
It is still a further object of this invention to couple a recessed impeller or half-regular closed impeller with another recessed impeller, half-regular closed impeller, or disc impeller so as to pump HVFs.
These and other objects and advantages of the present invention will become apparent from a reading of the attached specification and appended claims.
The present invention utilizes various pump configurations so as to minimize slippage and dead zones in a centrifugal pump when pumping high-viscosity liquids, slurries, and solids-containing liquids.
A first embodiment of the present invention has a recessed impeller design connected to a disc. The disc has a hole in the center allowing for the HVF to pass through and is connected to the recessed impeller via adjustable rods. The rods, for example, can have a thickness of three-eighths of an inch. In the preferred embodiment of the present invention, adjusting the rods can vary the distance between the recessed impeller and disc to suit the nature of the HVF.
A second embodiment of the present invention has two recessed impellers that face each other and are connected via adjustable rods. The front recessed impeller has a hole in the center allowing for HVF to pass through. The rods, for example, can be ⅜″ thick and allow for the space between the impellers to be adjusted to suit the nature of the HVF.
A third embodiment of the present invention has a regular closed impeller cut in half along the vanes between the front and rear shroud. The two halves are then connected via adjustable rods so that the gap between the halves can be varied to suit the nature of the HVF. The rods, for example, can be ⅜″ thick and allow for the space between the impellers to be adjusted to suit the nature of the HVF.
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The foregoing disclosure and description of the invention is illustrative and explanatory thereof. Various changes in the details of the illustrated construction may be made within the scope of the appended claims without departing from the true spirit of the invention. The present invention should only be limited by the following claims and their legal equivalents.
Number | Name | Date | Kind |
---|---|---|---|
1406297 | Stewart | Feb 1922 | A |
3901623 | Grennan | Aug 1975 | A |
4135852 | Archibald | Jan 1979 | A |
4439200 | Meyer et al. | Mar 1984 | A |
4662819 | Lakowske et al. | May 1987 | A |
5800058 | Cook | Sep 1998 | A |
6074167 | Olifirov et al. | Jun 2000 | A |
6315532 | Appleby | Nov 2001 | B1 |