Method and apparatus for improving refrigeration and air conditioning efficiency
09702599 ยท 2017-07-11
Inventors
Cpc classification
F25B1/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B41/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2400/16
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2400/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B40/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F25B41/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B40/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
A method and apparatus for improving refrigeration and air conditioning efficiency for use with a heat exchange system having a compressor, condenser, evaporator, expansion device, and circulating refrigerant. The apparatus includes is a liquid refrigerant containing vessel having a refrigerant entrance and a refrigerant exit with the vessel positioned in the heat exchange system between the condenser and the evaporator, and means for creating a turbulent flow of liquefied refrigerant. The apparatus further preferably includes a refrigerant bypass path to sub-cool a portion of the refrigerant within the vessel; a disk positioned at the liquid refrigerant entrance to develop a low pressure area on the back side and create a turbulent flow of refrigerant entering the vessel; and a refrigerant valve incorporated into the refrigerant path downstream of the expansion valve and before the coil which develops a vortex that continues through the refrigerant coil.
Claims
1. A method of enhancing the efficiency of a heat exchange system having a compressor, condenser, evaporator, a circulating refrigerant, and an expansion valve, said method comprising the steps of: providing a liquid refrigerant containing vessel between the condenser and the evaporator said vessel comprising: a refrigerant entrance in the top of the vessel and a refrigerant exit in the bottom of said vessel; a disc located proximate said refrigerant entrance, said disc comprising apertures for direct flow of refrigerant from the condenser into the vessel and a bypass tube passing through an opening in the centre of the disc and extending into the centre of the vessel, wherein said bypass tube permits a small amount of refrigerant to flow into the center of the vessel; and providing a means for generating a turbulent flow of said liquid refrigerant.
2. The method of claim 1 wherein said means for creating turbulence comprises a disk located proximate said refrigerant exit, said disk permitting the passage of exiting refrigerant; and at least one fixed angle blade formed in said disk, wherein said blade adds turbulence to said exiting refrigerant.
3. The method of claim 1 wherein said bypass tube terminates in at least one bypass exit port.
4. The method of claim 3 wherein said bypass tube includes a heat exchanger.
5. The method of claim 2 wherein said disk comprises three fixed angle blades.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) The invention will be better understood and objects other than those set forth above will become apparent when consideration is given to the following detailed description thereof Such description makes reference to the annexed drawings wherein:
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DETAILED DESCRIPTION OF THE INVENTION
(8) By way of introduction to the environment in which the inventive system operates, the following is a brief description of the functioning of a traditional refrigeration system.
(9) An expandable-compressible refrigerant is contained and cycled within an essentially enclosed system comprised of various refrigerant manipulating components. When a liquid refrigerant expands (within a heat exchanger or evaporator) to produce a gas it increases its heat content at the expense of a first surrounding environment which decreases in temperature. The heat rich refrigerant is transported to a second surrounding environment and the heat content of the expanded refrigerant released to the second surroundings via condensation (within a heat exchanger or condenser), thereby increasing the temperature of the second surrounding environment. As indicated, even though the subject invention is used preferably with a refrigeration system, adaptation to a generalized heat pump system is also contemplated. Therefore, for a heat pump, heating or cooling conditions are generated in the first and second environments by reversing the process within the enclosed system.
(10) The four basic components in all systems are: a compressor; a condenser (heat exchanger); an evaporator (heat exchanger); an expansion valve; and the necessary plumbing to connect the components. These components are the same regardless of the size of the system. Gaseous refrigerant is compressed by the compressor and transported to the condenser which causes the gaseous refrigerant to liquefy. The liquid refrigerant is transported to the expansion valve and permitted to expand gradually into the evaporator. After evaporating into its gaseous form, the gaseous refrigerant is moved to the compressor to repeat the cycle.
(11) A lower compression ratio reflects a higher system efficiency and consumes less energy during operation. During compression the refrigerant gas pressure increases and the refrigerant gas temperature increases. When the gas temperature/pressure of the compressor is greater than that of the condenser, gas will move from the compressor to the condenser. The amount of compression necessary to move the refrigerant gas through the compressor is called the compression ratio. The higher the gas temperature/pressure on the condenser side of the compressor, the greater the compression ratio. The greater the compression ratio the higher the energy consumption. Further, the energy (KW) necessary to operate a cooling or heat exchange system is primarily determined by three factors: the compressor's compression ratio; the refrigerant's condensing temperature; and the refrigerant's flow characteristics.
(12) The compression ratio is determined by dividing the discharge pressure (head) by the suction pressure. Any change in either suction r discharge pressure will change the compression ratio.
(13) It is noted that for refrigeration systems or any heat pump systems when pressure calculations are performed they are often made employing absolute pressure units (PSIA), however, since most individuals skilled in the art of heat pump technologies are more familiar with gauge pressure (PSIG), gauge pressures are used as the primary pressure units in the following exemplary calculations. in a traditional refrigeration system, a typical discharge pressure is 226 PSIG (241 PSIA) and a typical suction pressure is 68 PSIG (83 PSIA), Dividing 226 PSIG by 68 PSIG yields a compression ratio of about 2.9.
(14) The condensing temperature is the temperature at which the refrigerant gas will condense to a liquid, at a given pressure Well known standard tables relate this data. In a traditional example, using R22 refrigerant, that pressure is 226 PSIG. This produces a condensing temperature of 110 degrees F. At 110 degrees F., each pound of liquid freon that passes into the evaporator will absorb 70.052 Btu's. However, at 90 degrees F. each pound of freon will absorb 75.461 Btu's. Thus, the lower the temperature of the liquid refrigerant entering the evaporator the eater its ability to absorb heat. Each degree that the liquid refrigerant is lowered increases the capacity of the system by about one-half percent.
(15) Well known standard tables of data that relate the temperature of a liquid refrigerant to the power required to move Btu's per hour show that if the liquid refrigerant is at 120 degrees F., 0.98 hp will move 22873 Btu's per hour. If the liquid refrigerant is cooled to 60 degrees F., only 0.2 hp is required to move 29563 Btu's per hour.
(16) Additionally, refrigerant flow through the refrigerant system, in most heat pump systems, is laminar flow. Traditional systems are designed with this flow in mind. However, a turbulent flow is much more energy efficient as is known from well established data tables.
(17) Referring now to
(18) Concerning the condensing temperature for the adapted system, the liquid refrigerant temperature at T1 is about 90 degrees F. (lowered from the 110 degrees F. noted above for the traditional system). The 20 degrees F. drop in liquid refrigerant temperature yields a 10% increase in system capacity (20 degrees F. times one-half percent for each degree, as indicated above This was accomplished by the increased condensing volume provided by the subject device.
(19) The device influences the flow of the liquid refrigerant. Normally, when a vessel is introduced into a fixed pressure system (usually, for sub-cooling) a reduction in the system's capacity occurs because most fixed head pressure systems utilize a fixed orifice or capillary type expansion device. Such devices require pressure to force a proper volume of refrigerant through them in order to maintain capacity. The pressure is generated by the compressor. The greater the demand for pressure the greater the demand for energy (Kw).
(20) With the adaptation of a floating head pressure heat pump system by the subject device, the capacity is maintained. The capacity is maintained due to increased refrigerant velocity, volume, and refrigerant Btu capacity because of lower condensing temperature and an introduced spiral turbulent flow, rather than a straight laminar flow. As is well know in fluid dynamics, turbulent flow has an average velocity that is far more uniform than that for laminar flow. In fact, far from being a parabola, as in laminar flow, the distribution curve of the boundary region for a flowing liquid with turbulent flow is practically logarithmic in form. Thus, for turbulent motion, at the boundaries where the eddy motion must educe to a minimum, the velocity gradient is much higher than in laminar type flow. With the device and its influence on refrigerant flow, the hotter the condensing temperature and the higher the load, the better the adapted system functions.
(21) The vessel 1 has an internal volume 3 and is preferably fabricated from a cylinder 5 and top 10 and bottom 15 end caps of suitable material such a metal, metal alloy, or natural or synthetic polymers. Generally, the top 10 and bottom 15 end caps are secured to the cylinder 5 by appropriate means such as soldering, welding, brazing, gluing, threading and the like, however, the entire vessel 1 may be formed from a single unit with the cylinder 5 and top 10 and bottom 15 end caps as a unitized construction.
(22) A liquid refrigerant entrance 20 and a liquid refrigerant exit 25 penetrate the vessel 1. Preferably, the refrigerant entrance 20 is located in a top region of the vessel 1. The top region is defined as being approximately between a midline of the cylinder 5, bisecting the cylinder 5 into two smaller cylinders, and the top end cap 10. Although
(23) Usually, the bottom end cap 15 has an angled or sloping interior surface 30. However, the bottom end cap 15 may have an interior surface of other suitable configurations, including being flat.
(24) Liquid refrigerant liquefied by the condenser CX enters into the vessel 1 via the refrigerant entrance 20 and the associated components. The associated entrance components comprise a refrigerant delivery tube 35 and entrance fitting 40 that secures the vessel 1 into the exit portion of the plumbing coming from the condenser CX. The entrance fitting 40 is any suitable means that couples the subject device into the plumbing in the required position between the condenser CX and the evaporator EX.
(25) The refrigerant delivery tube 35 is configured to generate rotational motion in the entering refrigerant. The tube 35 penetrates into the top region and is formed into a curved configuration and generally angled down to deliver the entering refrigerant along a path suitable for generating a rotational motion of the refrigerant within the vessel 1. Other equivalent configurations of the tube 35 that generate such a rotational refrigerant motion are contemplated to be within the realm of the invention.
(26) To view the level of the liquid refrigerant within the vessel 1, a sight glass 45 is provided. The glass 45 is mounted in the cylinder 5 at a position to note the refrigerant level.
(27) The refrigerant exit 25 is comprised of an exit tube and fitting 50 that secures the subject device into the plumbing of the system. The exit fitting 50 is any suitable means that couples the subject device into the plumbing in the required position between the condenser CX and the evaporator EX.
(28) A second means for introducing a turbulent flow into the exiting liquefied refrigerant is mounted proximate the exit 25. A turbulator 60 is held in place by cooperation between the exit tube and fitting 50 or any other equivalent means. The turbulator is usually a separate component that is secured within the components of the exit from the vessel 1, however, the turbulator may be an integral part of the vessel 1 refrigerant exit. The turbulator comprises a disk with a central aperture and at least one fixed angle blade formed or cut into the disk. Preferably, a set of fixed angle blades are provided to add turbulence to the exiting refrigerant.
(29) The blades are angled to induce rotational, turbulent motion of the liquid refrigerant as the refrigerant exits the vessel 1. Various angles for the blades are suitable for generating the required turbulence.
(30) Preferably, the subject vessel 1 is placed in the adapted system so that the refrigerant exit 25 is no lower than the lowest portion of the condenser CX. Liquid refrigerant from the condenser CX enters the vessel 1 and is directed into a swirling motion about the interior volume 3 by the delivery tube 35. The swirling liquid refrigerant leaves the vessel 1 by means of the refrigerant exit 25 and then encounters the turbulator 60. The blades of the turbulator 60 add additional turbulence into the flow of the refrigerant.
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(32) After the refrigerant enters the vessel and starts to exit, it develops a shallow-well vortex at the bottom of the vessel 1. In the center of the shallow-well vortex, it develops a low-pressure area. The stronger the vortex, which increases as it becomes hotter, the greater the low-pressure area in the center of the vortex, thereby being able to sub-cool the refrigerant that passes over the heat exchanger 76 at the bottom of the bypass tube 72.
(33) With the development of the low-pressure area in the center of the vortex, the small amount of refrigerant entering the bypass path at the liquid refrigerant entrance 20 expands and comes out at the bypass path exit port 74 to sub-cool the refrigerant and allow the heat bubbles carried by the refrigerant to continue to condense so as to allow the refrigerant that is delivered downstream to the expansion valve to have less non-condensed refrigerant within it, thereby improving the operation of the system.
(34) In a preferred embodiment, the disk 70 positioned at the liquid refrigerant entrance 20 comprises an incremental expansion device disk. The disk develops a low pressure area on the back side and creates a turbulent flow of refrigerant entering the vessel, thereby improving refrigerant efficiency. The disk may be such as was disclosed above as turbulator 60 at the refrigerant exit; or disclosed in the heat pump efficiency enhancer of U.S. Pat. No. 5,259,213 (e.g.,
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(36) A 3-dimensional view of the inventive apparatus as seen in
(37) Referring now to
(38) With the addition of a condenser controller with adiabatic sub-cooling, it is possible to tune a refrigeration system using an adjustable thermostat expansion valve. Just as the thermostat expansion valve adjusts to varying conditions at the evaporator, this condenser control allows the condenser to be adjusted under varying conditions as well.
(39) For example, a first option allows a properly sized system to meet its set point sooner and turn off. Open up the thermostat expansion valve to the evaporator, being sure not to reduce below a 10 super heat at the compressor. This will load the compressor amps to rated load, but not over load. The condenser will load up and the condenser control will fill with cool liquid refrigerant from the sub-cooling section of the condenser, giving more room for good condensing in the condenser.
(40) A second option allows the system to run at a reduced amp load. Close up the thermostat expansion valve to reduce the load on the evaporator to the rated capacity, making sure not to exceed a 25 super heat at the compressor. This will unload the compressor to below rated amps. The condenser will have some sub-cooling and the condenser control will fluctuate the amount of refrigerant in or out of it, in order to balance pressure and temperature.
(41) A third option allows the system to run at reduced amps at the compressor and the evaporator will run slightly over rated capacity, so as to reduce run time and meet set point sooner, then turn off. Adjust the thermostat expansion valve until the super heat at the compressor is at 15 to 18 superheat, The compressor will be running at reduced amps, the condenser will be doing some sub-cooling, and the condenser control will be fluctuating in order to balance temperature and pressure within the system.
(42) The above disclosure is sufficient to enable one of ordinary skill in the art to practice the invention, and provides the best mode of practicing the invention presently contemplated by the inventor. While there is provided herein a full and complete disclosure of the preferred embodiments of this invention, it is not desired to limit the invention to the exact construction, dimensional relationships, and operation shown and described. Various modifications, alternative constructions, changes and equivalents will readily occur to those skilled in the art and may be employed, as suitable, without departing from the true spirit and scope of the invention. Such changes might involve alternative materials, components, structural arrangements, sizes, shapes, forms, functions, operational features or the like.
(43) Therefore, the above description and illustrations should not be construed as limiting the scope of the invention, which is defined by the appended claims.