HEAT TRANSFER FROM A SOURCE TO A FLUID TO BE HEATED USING A HEAT DRIVEN LOOP
Oil in a storage tank is heated by providing one or more elongate conduits within the storage tank in the form of a loop extending from an inlet manifold across the tank and returning to an outlet manifold. The inlet manifold is connected to an evaporator section at a heat source and the outlet manifold acts as a return of the condensate. The conduit forms a loop and back flow in the loop is prevented by providing a head in the liquid in the conduit at a position adjacent to or at the evaporation section caused by a standing column of the liquid with optionally a pump. The flow around the loop at high speed sufficient to carry all condensate forwardly is caused solely by application of energy to the system by the heat source. Inert gases are collected immediately upstream of the trap and can be purged therefrom.
This application is a Continuation-in-Part application of application Ser. No. 10/474,774, filed Apr. 15, 2004 which is a National Phase Entry of PCT/CA02/00490, filed Apr. 11, 2002.
This application claims the benefit under 35 U.S.C.119 of the priority of Provisional Application Ser. No. 60/283,150, filed Apr. 12, 2001.
This invention relates to a heating system transferring heat from a heat source such as a combustion heating system to a fluid to be heated which is particularly but not exclusively designed for heating oil in storage tanks, oil emulsion treatment tanks and oil upgrading and refining process vessels.
BACKGROUND OF THE INVENTIONReference is made to U.S. Pat. No. 5,123,401 of the present inventor issued Jun. 23, 1992 which discloses a combustion heating device for use for example with oil processing equipment defines a combustion chamber within which combustion wholly takes place. The combustion chamber consists solely of a sleeve and end plate defining a vertical cylinder and a layer of ceramic fiber insulating material inside the sleeve defining the inner surface of the combustion chamber. A burner is mounted in a bottom plate of the device which can be pivoted to an open position exposing the burner for service. Air channels are defined on the outside of the sleeve so that incoming combustion air passes over the sleeve and acts as a heat recovery for any heat escaping from the insulating material. An outlet duct at an upper end of the combustion chamber at right angles to the combustion chamber extracts the combustion gases so that all heat exchange takes place outside of the combustion chamber. The device improves heating efficiency and reduces corrosion of heat transfer surfaces. In the arrangement shown, a similar combustion chamber vertical configuration and dimensioning with respect to the flame, together with the heat recovery method from the outside walls of the combustion chamber, which provided exceptionally high combustion efficiencies with a naturally aspirated burner in the order of 80%+ in that device, are employed.
Reference is made to US Published Application 200710000453 published Jan. 4, 2007 of King which discloses a heat exchange apparatus using a change of state of a liquid which is transported from an evaporator to a condenser so that the liquid form the condenser can return to be re-heated. In this application, the purported claim to function as a “heat driven loop” is not supported in that it is a “loop” only in the sense that the conduit containing vapor forms a loop, whereas the fluid flow does not. Both legs of the conduit exit the vaporization chamber above liquid level, which makes it incapable of bias of flow in one rotational direction. Neither is it “driven” because vapor simply travels up towards the top of the joined tubes and condensate runs down to the bottom of the joined tubes due to the effects of gravity only. It is, in effect, two parallel thermo-siphons joined together at the top and bottom ends and functions in accordance with the known principle of such devices.
Reference is made to Canadian Patent 1,264,443 (Spehar) issued Jan. 16, 1990 and U.S. Pat. No. 5,947,111 (Neulander et al) issued Sep. 7, 1999 to Hudson Products Corp (which corresponds to Canadian application 2,262,990) which describe prior art arrangements and the disclosure of these prior patents is hereby incorporated by reference to show the type of installation and use to which the present device can to be put.
Reference is also made to the prior U.S. Pat. No. 4,393,663 (Grunes) which shows a heat loop arrangement for heating various materials, primarily water, within a container. However this arrangement has not been proposed for and is not suitable for the heating of oil and particularly crude oil in a storage tank.
U.S. Pat. No. 4,216,903 Giuffre discloses a circuit using an evaporation section and a condensation section connected by a conduit with a trap located between the condensation section and the evaporation section for the returning liquid feeding to a receiver. The trap is discussed only in terms of blocking back flow and is never discussed as being an active element in providing drive for the fluid for useful purpose.
SUMMARY OF THE INVENTIONIt is one object of the present invention to provide an improved method of heat transfer from a heat source to a fluid to be heated.
According to the present invention there is provided method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section so that the thermal energy causes expansion of volume due to a change of state;
flow around the loop being biased in one direction by the creation of a head.
Thus the system provides in its broadest terms, a ‘heat driven’ loop; with as opposed to induced systems such as those gravity-drawn in both directions as in a thermo-siphon, or, capillary-drawn in one of the two directions as in a heat pipe, either in a looped tube configuration or in a single tube. Flow is biased in one rotational direction by restriction in the other rotational direction using a head but the specific means of providing this head is secondary to the concept.
The head provides a mechanism for prevention back flow which can be designed and arranged to not only prevent back flow, but also to utilize the adjustability of the head to provide sufficient back pressure and force of flow to maintain flow of vapor, carry-over liquid from the vaporizer and condensate, substantially in one direction, and drive this combination through resistance imposed by restrictions and deployments, above and below the level of the vaporizer, of the condenser.
The head also provides a block, for any residue of the inert gases that are used for initial purging plus any inert gases that are generated over a period of time by chemical interaction of the fluid[s] and the materials from which the device is constructed and the accumulation of which will progressively impair the effectiveness of the system, against which these gases will accumulate as swept along by the fluid flow while in operation and unable to pass through the head, in a location that is accessible from outside the vessel which enables these gases to be detected and purged from the system utilizing the pressure of the system while in operation. Thus the head is arranged so that it stops the forward flow of the inert gases at the head and there is provided an access opening which can be opened at the position immediately upstream of the head so that the gases can be purged, with the system under pressure so that the vapor drives out the inert gases until escape of vapor is detected.
According to a second aspect of the invention there is provided a method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
and causing boiling of the liquid in the evaporation section and flow of the vapor from the evaporation section to carry non-vapor additives in the liquid in the evaporation section into the conduit with the vapor.
According to a third aspect of the invention there is provided a method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
wherein the system is at least partly evacuated prior to start up such that during steady state operation the pressure in the system is less than 15 psi above atmospheric pressure.
According to a fourth aspect of the invention there is provided a method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
wherein the total volume of liquid in the system is less than 43.5 litres or 1.5 cu. ft.
According to a fifth aspect of the invention there is provided a method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
wherein flow around the loop is biased in one direction by a head created in part by a pump;
and wherein there is provided a viewing port for viewing passage of vapor from the evaporation section;
and wherein the operation of the process is controlled by varying the flow rate of the pump while viewing passage of vapor from the evaporation section so as to ensure passage substantially wholly of vapor with a minimal amount of liquid.
According to a sixth aspect of the invention there is provided a method for transferring heat from a combustion heat source to a fluid to be heated comprising:
providing a combustion heat source;
providing a fluid to be heated at a position spaced from the heat source;
providing a closed system including at least one conduit;
providing an evaporation section of the closed system at the heat source;
providing a condensation section of the closed system in the fluid to be heated;
providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
wherein flow around the loop is biased in one direction by a head created in part by a pump;
and wherein the pump is a positive displacement pump so that the rate of flow is directionally proportional to a rotation rate of the pump.
The system is primarily designed for use in heating crude oil in a tank but can also be used for other heating systems including heating air for forced air systems and space heating. The system can also be used for heating oil in a duct of pipe as it flows past the condensation section of the loop.
The system consists of a closed loop, sealed from atmosphere and containing a fluid. The fluid is vaporized in the energy absorbing section by the application of heat. The temperature and pressure of the system vary in a fixed relationship according to the vaporization characteristics of the fluid and the amount of heat applied. The vapor is conducted to the energy emitting section where it condenses giving off its latent heat. The condensate flows back through the head to the energy absorbing section. Vapor is driven in one rotational direction by the liquid differential pressure of the condensate gathering head which self-adjusts to overcome flow resistance through the energy emitting section of the loop.
The system consists of a single conduit or a multiplicity of such conduits connected by input and output manifolds to the evaporation section at the heat source outside the storage tank or fluid to be heated.
When the head is formed by a trap, the trap is not only self adjusting but its range of adjustability can be increased or decreased by increasing or decreasing the depth of the trap to permit greater liquid level differentials to offset greater energy emitting section resistance.
The configuration of the loop is such that the energy of the system is sufficient to both overcome the resistance of the energy emitting section but also to sustain a vapor flow velocity sufficient to carry along with it substantially all the condensate produced in the energy emitting section, plus a limited quantity of liquid physically carried out of the energy absorbing section due to boiling action. This is an important feature that should be designed into the configuration in order to assure the conveyance of additives, such as anti-corrosion agents and anti-freezing agents, throughout the loop rather than have them confined to the energy absorption section due to being precipitated due to vaporization or isolated due to selective vaporization. However, and this is important, the system should not carry over liquid from the vaporizer so as to substantially form a conventional bubble pump, such as in a percolator, so that the degree of bubble pump action must be controlled by the design such that it occurs only to the extent necessary to convey the additives and not to the extent that it contributes significantly in the conveyance of heat.
Conveyance of heat substantially totally occurs due to change of state at a fixed temperature rather then by loss of sensible heat from this liquid by a decreasing temperature of the liquid through the energy emitting section. In other words, the bubble pump action must not significantly interfere with the capability of the system to maintain a constant temperature across the heating element when utilized for heating purposes.
The only portions of the system where gravity is the principal force determining condensate flow, or liquid position, is the trap. Any transition from the energy emitting section to the energy absorbing section where condensate flow to the trap may be substantially directed by gravity, and, the portion of the energy absorbing section where liquid is held in direct proximity to the heat source by the configuration of that portion of the system.
Consequently, the heat energy emitting section of the loop can be of any lateral or vertical deployment in relation to the energy absorbing section, and can be of any sizing or other physically restricting configuration and can accommodate whatever other load demands requiring pressure differential that might be placed upon the system provided all of that is within the capability of the energy absorption section to absorb sufficient heat energy and, the capability of the head to withstand sufficient back pressure to overcome the resistance imposed by these.
A specific heat emission temperature can be selected by an appropriate choice of a fluid having the desired temperature/pressure relationship and a construction capable of withstanding the pressure associated with that temperature, and can be maintained while in operation by controlling the amount of heat that is absorbed, by controlling fuel flow to the burner. The controller can be actuated by sensing either temperature or pressure of the vapor issuing from the vaporizer, which have a fixed relationship.
In practice, the system is charged with water and additives, purged with an inert gas such as argon, the internal pressure reduced to close to a complete vacuum at normal ambient temperature, the system sealed, and then operated at below a maximum 15 psi. This pressure range is readily tolerated with conventional construction and is below the pressure that would warrant classification as a pressure vessel. In some applications, the system would then remain permanently sealed and initial setting of internal pressure in relation to temperature and the initial charge of fluid would remain for the service life of the device. In other applications, the system in its operational mode would be sealed but provision would be made for the periodic servicing such as; removal of buildup of inert gases due to chemical interactions between fluid[s] and conduit material, replacement of the fluid due to chemical degeneration, and re-establishment of vacuum at normal ambient due to leakage.
However the system can also be operated at higher temperatures and pressures and may use liquids different from water which may have a higher boiling point although water is well known to provide a very high latent heat of vaporization. The available selection of heat transfer fluids is limited only by practicality, and would include for example those shown in the attached Table, the principle considerations and limitations being the vaporization temperature/pressure relationship characteristics of the fluids and the chemical interactivity between the heat transfer fluid and the material utilized to construct the loop. A single or multiplicity of heat transfer liquids can be employed in a given system. In one arrangement, all of the transfer liquids may circulate throughout the system in admixture by vaporization and condensing. Alternatively, one or more of the liquids may act as a ‘boiling bed’ for others depending on the temperature and pressure range of the system from shutdown to full operation and the vaporization characteristics of the liquids. This is significant because additives may be required for such purposes as inhibiting chemical interaction and preventing freezing.
Because heat transfer is substantially wholly accomplished by change of state, the temperature of the energy emitting section is constant throughout its length and is selectable amongst fluids having appropriate temperature/pressure characteristics and chemical characteristics. Both of these characteristics are highly desirable for processes that are enhanced by selectability and controllability of temperature, such as the different processes involved in petroleum processing, which would include:
[a] Water and particulate matter separation from raw petroleum product which is facilitated by holding the raw product at as uniform and high a temperature as can be sustained below the boiling point of water in order to minimize viscosity which promotes separation and to avoid boiling creating foam which seriously disrupts the process due to interference with heat transfer and other effects. It is an important aspect of this system that not only does the uniform temperature of the heating elements contribute to maintaining a higher average temperature of the raw product just below the boiling point of water but, at no point on the element is the raw product exposed to localized temperatures above the boiling point of water causing localized vaporization of water and occasioning precipitation and accumulation of particulate matter on the surface of the heating elements which reduces their effectiveness for heat transfer and reduces their service life. This would be in contrast to direct fired immersion tube heaters which feature a large temperature differential over their length and
[b] Upgrading and refining of petroleum product, which are essentially a matter of exposure of crude product to a variety of temperatures which are selectable, controllable, and, as constant as can be achieved over the heat transfer surface for the purpose of producing by distillation various petroleum products which have characteristic vaporization temperatures. The effectiveness of the process, in terms of the purity of product, is enhanced by maintaining the crude product within as narrow a temperature band as possible.
Another important feature of this technology in that it is highly adaptable to optimizing, or maximizing, heat transfer capacity in relation to the internal volume of the system. This is of significance in relation to the regulatory requirements for pressure vessels. Pressure vessels are defined as containers in which pressure is generated as a consequence of applying heat a classic example being conventional steam boilers. There are two further stipulations to the definition; that the pressure generated be in excess of 15 psi, and that the volume of the vessel be in excess of 65 liters. Anything of less volume, regardless of pressure, is designated as a ‘fixture’ and is not subject to the requirements for operating a pressure vessel. These requirements are onerous in that they include constant attendance by a certified person and regular inspection. Such requirements may vary in specifics from jurisdiction to jurisdiction but will substantially involve maximum pressures and volumes.
Because the system described herein is capable of operating at a great variety of temperatures and pressures compared to conventional heat transfer systems involving steam or hot water due to the variety of fluids that can be employed having different temperature/pressure characteristics, much higher heating element temperatures can be generated than is common for steam or hot water systems and it is also possible to do so at lower pressures than would be produced with water.
For example, propylene glycol could be utilized which has a vaporization temperature of 605 Degrees F. at 16 psi gauge pressure compared to a vaporization temperature for water of 250 Degrees F. at 15 psi gauge pressure. Thus higher temperatures, and greater heat exchange, can be achieved with propylene glycol than with water at pressures below the limit specified for definition as pressure vessel. Alternatively, at 40 psi gauge pressure, water vaporization temperature increases to 287 Degrees F. while propylene glycol vaporization temperatures rise to 1048 Degrees F. Thus much higher temperatures and much greater heat exchange can be achieved with vessel volumes below the limit specified for classification as a pressure vessel and therefore classified as a fixture regardless of pressure.
Hence this system provides two means of enhancing capacity without encroaching upon the definition of a pressure vessel, by the utilization of the higher temperatures associated with higher pressures while maintaining volumes below the maximum for a fixture, and the utilization of fluids that have a temperature/pressure characteristic such that higher temperatures can be maintained at pressures below the maximum for pressures for pressure vessels and therefore unlimited in volume.
This aspect of this technology has particular significance with respect to space and air replacement heating applications. In such systems, self-contained, compact heater modules incorporating higher temperature heat exchangers are an alternate to systems consisting of conventional unit heaters, make-up air heaters, etc., incorporating larger, lower temperature heat exchangers, and connected to a steam boiler via a steam and condensate circulating system.
It is also significant in relation to the amount of material employed in relation to capacity which, in turn, relates to cost of manufacture.
The energy absorption section of the loop may be open to the combustion action or may be encapsulated within an enclosed housing which is filled with a liquid intermediate heating medium. The use of an encapsulation and heating medium allows the heating system to sustain an even, maximum tolerable temperature over the heat absorption surface thus minimizing the amount of surface required and contributing to the minimization of the volume of the system pursuant. In practice, the intermediate heating medium is preferably what is referred to as a thermal oil, capable of maintaining stability at temperatures close to the crystallization temperature of mild steel. The whole heat absorption surface is then covered with that temperature. To the contrary, when directly heated with combustion products, which normally would be of uneven temperature, only the peak temperature could be at that level otherwise the surface would be damaged and the average would be considerably less. Encapsulation also enables more than one heater module to be supplied with heat from one central fuel combustion device by transferring the intermediate heating medium from that device to any number of heater modules.
When used for heating a process liquid within a storage tank, the heating system preferably includes an arrangement in which one or more heating loops are heated externally of the tank and extend into the tank so that heat is transferred from the evaporation area at the heat source to the condensation area within the tank. The evaporation area is located within a vessel, which may contain high temperature heating oil in an encapsulating vessel where the vessel is heated by a burner so that the oil transfers heat to the condensation area of the single heat loop or of each loop if there is more than one.
Also, a multiplicity of condensing sections can be heated from one vaporizer such that more than one tank or more than one space or make-up air heater can be supplied with vapor from one vaporization source. The transition system from the vaporization section to the condensation section[s] may be with rigid or flexible conduit and may be such that the vaporizer can be located at ground or floor level with conduit conveying vapor to condenser[s] located at a higher level within the capability of the system to maintain fluid flow substantially in one direction.
The burner is controlled by thermostats which may be located within the tank so that the temperature of the oil within the tank is maintained within required limits. Alternatively, the temperature or pressure, as these are directly related, within the heat loop may be detected for maintaining the required amount of heat input to keep the temperature and pressure at the operating value.
An over temperature shut off is provided for safety. This may be provided within the loop itself preferably as a pressure sensor. Preferably the shut off is of the resetting type so that combustion is re-started after a predetermined cool down period since this overcomes problems should the over pressure situation causing the shut down to occur be temporary. This is particularly possible where very viscous materials around the heat emission part of the heat loop temporarily reduce or prevent convection currents in the process liquid in the tank causing the emission part to overheat since the viscous materials act as an insulator. Alternatively the over temperature shut off may be located within an encapsulating heating oil so that if the heating oil exceeds a predetermined temperature the burner is shut off. Thus there is no detection of temperature at the surface of the condensation area of the heat loop within the tank.
It is an important feature of this system that it is capable of cycling, fairly rapidly if need be, in response to an on/off condensation section temperature or pressure control, or, be capable of operating at reduced firing rates in response to a modulating condenser temperature or pressure control, during the start-up phase due to delays in establishing full heat exchange capacity from the condenser s at full firing capacity because of thermal and flow characteristics of the process fluid being heated. Establishing generalized convection circulation in vessels filled with raw petroleum products can be problematical during the heating startup phase due to high viscosities, the effect of low temperature exposure on viscosities variations in water content particularly as that is trapped next to heating elements, and, tendency of product to establish and accelerate flow along channels of least resistance rather than establish overall convection currents.
Reliable, stable operation during this initial startup period when demand for product temperature is at its maximum but tolerance of heat absorption is at its minimum is a major advantage of the arrangement described herein over the Grunes et al technology which requires stable operation above a minimum level of heat input over a minimum period of time to establish and maintain a liquid block at the ‘resistor’ in order to operate with the flow of vapor and liquid in one direction.
The heat loop is not a heat pipe of any form and does not use surface tension to pump the liquid back to the heated area. Instead the heat loop is a generally conduit with two generally upwardly extending legs and two generally transverse arms forming a loop. A trap is formed at the evaporation area at the bottom of one leg so that vapor is prevented from flowing up the leg at the evaporation area and thus the vapor is driven upwardly along the leg at the evaporation area and transversely along the top arm from the heat source outside the tank transversely into the body of the tank.
In one arrangement there is provided a coil to coil configuration because this is very cheap and effective. In this arrangement the head is developed solely by a height of liquid in the trap. In this arrangement the head in the trap is the height of the condensate in the conduit flowing downward and parallel to the vertical heat-in coil relative to the height of the vaporizing liquid in the heat-in coil, and this will drive the flow, including the condensate accumulation, through the horizontal heat-out coil. However the head developed by the leg of liquid can be supplemented by a pump. The condensate is thermally driven via expansion of the liquid into vapor, at a 1700 to 1 ratio of change of volume, so that condensate will always reservoir in the lowest part of the loop. Even suction pumps must have a steady supply of liquid to draw on to work in a recommended fashion. They will draw gases on start-up if need be, but thereafter are intended to run with a continuous supply of liquid. This reservoir, therefore, provides an element of standing head.
In the arrangement of the present invention, the drive to the material in the loop comes from the rapid expansion, due to the addition of heat, of liquid into a vapor by a volume expansion, with water, in the order of 1700 to 1. However, if totally unrestricted, that expansion will be in both rotational directions so that, by providing a restriction to flow in the undesired rotational direction by the head, flow is established in the desired rotational direction
Thus the system provides in its broadest terms, a ‘heat driven’ loop; with as opposed to induced systems such as those gravity-drawn in both directions as in a thermo-siphon, or, capillary-drawn in one of the two directions as in a heat pipe, either in a looped tube configuration or in a single tube. Flow is biased in one rotational direction by restriction in the other rotational direction but the specific means of providing this bias is secondary to the concept.
Thus the drive is created by the thrust of the 1700 to 1 expansion of the fluid, to the effect that this is the dominant feature. Loops as disclosed herein will incorporate at least some element of standing head, but such head could be quite minimal because of restriction of available height for a standing column such as where the condenser is deployed in a flat plain, such as in ground thawing applications where hoses are spread over ground surface. While the formation of a reservoir must occur because the condensate will pool in the lower part of the system, the nature of the configuration of that particular system does not provide much of what we would consider a reservoir or a standing column of water. Nonetheless, the liquid gets back to the inlet of the pump because it is driven by the 1700 to 1 expansion of fluid that is occurring behind it. in other words, while some element of standing head is always present, it may be dimensionally inhibited as above, in any event, thermal drive, not the specific nature of the configuration or the backstopping, is the dominant factor in keeping the loop going round, which, in the case of pumps, is by such force delivering the liquid back either to a trapping configuration which becomes a standing column at the inlet of the pump, or directly to the inlet of the pump with that force, in which manner such force of flow constitutes an ‘effective standing head’.
The arrangement described herein can be used in many possible areas of use two examples of which are portable and temporary heating applications including space heating and ground thawing and which is very compact, inexpensive and trouble-free for that purpose, and, petroleum industry applications particularly including both tank heating, the heating of liquids in a storage vessel, and line heating, the heating of gaseous and liquid fluids flowing through conduits. This particular configuration with or without pump is simply the most inexpensive and effective way to do these things.
Applications for this technology include, but are not limited to;
permanent installation for space and air replacement heating;
temporary and portable use for space heating, space heat treatment, and ground thawing;
vessel and pipeline heating;
can be employed with alternate heat sources, such as waste heat reclaim & recovery of geothermal heat;
The concept can be directed to any heating devices embodying;
the driving of a heat transferring fluid around a loop employing thermal energy;
via expansion of volume due to change of state
biased in one direction by the creation of a head with or without the assistance of a pump;
and which can be operated at all pressures from total vacuum through unlimited high pressure.
It is inherent to the principle, that practical designs based on the concepts described herein can either demand or permit:
minimal system volume in relation to capacity;
minimal material for heat exchange;
simplest of fabrication;
and the—simplest of componentry.
Therefore, units based on this principle:
achieve minimal unit cost in relation to capacity, compared to competitive principles;
are very compact, and;
are very dependable.
With regard to application regulation requirements and certifiable performance, the system:
can be operated at all capacities in the pressure range from total vacuum to zero gauge; therefore is self evidently completely benign with regard to pressure hazards;
the fluid employed can be water and food refrigerant so that it therefore is completely benign with regard to environmental concerns;
can also be operated at significant capacities in the higher positive pressures range with commensurately higher fluid temperatures and compactness, with a minimal volume containment such that, by regulation, the system is considered safe for unattended operation.
Also, the system:
readily achieves high efficiency [80%+] and very high efficiency [90%+] fuel combustion,
is not subject to off-cycle losses,
and separately vents combustion products to atmosphere and not into the space air;
it is flexible in application; vaporizer and heater sections can be in a single unit or widely separated as separate units horizontally and/or vertically;
can be operated indoors and in all outdoor ambient temperatures;
separately vents and does not place combustion products in the space air;
it is flexible in application; vaporizer and heater sections can be in a single unit or widely separated horizontally and/or vertically;
can be operated exposed to all ambient temperatures.
There is a great deal of consciousness, and sensitivity, regarding hazard in utilizing steam, both on the part of the general populace and regulatory authorities.
1. When operated as a “no-pressure” system, i.e., at neutral gauge pressure [0 psig] or less [in a vacuum], the system has no potentially explosive potential. On rupture, the fluid contained will simply go nowhere, or collapse in volume.
2. It is also a “no contaminant” system in that the fluid it contains is environmentally benign, a mixture of water, and propylene glycol which is commonly used as a coolant for exposed food products so that it is not considered to be a contaminant unless food is soaked such as to affect eating quality.
The system, described as operating under the above conditions, is not only safe, but is obviously safe.
Local regulations throughout North America having jurisdiction over pressure containing devices such as the HDL, are generally based on ASME codes but may contain some local variations. Therefore the following references to ASME based codes are to be considered as largely accurate generalizations. ASME codes have not anticipated a device such as the system described herein, and have envisioned ‘boilers’ in terms of relatively simple, voluminous vessels, always operated under positive pressure [0 psig and above].
Consequently, ASME based regulations do not specify 0 psig as a significant threshold which, when exceeded, would incur more stringent operational requirements.
In fact, the first significant threshold specified is 15 psig maximum, at and below which a boiler is designated a “low-pressure” system. At this level, the system is considered to have some explosive potential, but such that operational requirements imposed are only that the device must be inspected by regulatory authorities once per year, and there is no requirement that the boiler must have formally qualified persons [ticketed stationery engineers] in attendance while operating.
Since inspection-only does not impose significant economic hardship, the first significant pressure threshold officially encountered with the HDL is therefore actually at 15 psig. The advantage derived from this higher pressure, is that the boiling point of water at 5 psig is 100 deg C. or 212 deg F., while at 15 psig it is 121 deg C. or 250 deg F., making the system more effective at transferring heat in relation to the amount of material used in its fabrication.
Also from a regulation standpoint, the next and last significant threshold is over 15 psig, beyond which pressure a boiler is designated a “high-pressure” system, and also beyond which explosive potential is considered sufficiently greater that a requirement is imposed that, in addition to regular inspection, the boiler must have formally qualified persons [ticketed stationary engineers] in attendance while operating. That would constitute an economic hardship in a significant number of instances, and would, for example, preclude the utilization of the system in many potential applications envisioned, particularly; portable and temporary heating applications of all kinds where such qualified persons are not normally provided, and, smaller capacity permanently installed applications such as vessel and conduit heating where the additional cost of constant attendance would be quite onerous. Typically, high-pressure systems would operate at 250 psig with the boiling point of water at 232 deg C. or 450 deg F. Note the substantially higher operating temperature, again reflected in a lesser amount of material used in the systems fabrication. Such higher pressures and temperatures warrant greater consideration from a safety standpoint, however, the system qualifies for an exemption from all existing boiler regulations, regardless of its operating pressure and temperature, up a limited but comparatively quite large capacity compared to other systems.
In addition to the two operating conditions described above, there is a third operating condition that applies particularly significantly to the system, which becomes relevant with respect to regulatory jurisdiction. Explosive potential is a function, not just of pressure, but also of volume of fluid contained, particularly liquid that will flash into steam on pressure release. Therefore, ASME code based regulations, in order to exclude involvement what might be considered incidental usage of relatively small volumes of high pressure steam such as; steam clothes presses, coffee making machines, some steam washers, etc., exempt from jurisdiction applications wherein the wetted volume, when at rest, of the boiler is below a specified minimum at which the ASME codes, and the regulations on which they are based, are simply deemed not to have jurisdiction that is no inspection and no attendance requirements are imposed. Such exemption is quite common.
The significance of this with regard to the system herein, emanates from the fact that it is a minimal volume system throughout, including the vaporizer since small amounts of fluid can be driven through the system at very high velocities. These may theoretically reach velocities up to that of sound, at which point fluid compressibility related stall will occur. Consequently, heat-carrying capability tends to be quite large in relation to internal volume. So the third operating condition that applies to the present system that becomes pertinent in terms of practical ramifications is that of creating a construction where vaporizer wetted volumes are at or below the designated volume above which ASME based regulations are deemed to apply and below which they are not.
In practice the volume at which this regulation occurs is 43.5 litres or 1.5 cu. ft. The heating capacities which can be realized by the present system are many multiples higher than other devices qualifying for exemption under this regulatory provision related to volume. Furthermore, capacities realized up to 400,000 btuh and more are well within the range of practical usage in the applications envisioned. Hence a considerable further advantage can be realized by making avail of this particularly the exemption from qualified attendance that such exemption conveys.
ASME is a well informed and accepted authority with respect to the setting an exemption volume, and therefore the present system under this operating condition must be considered in fact reasonably safe.
Also, for most effective heat transfer, that the flow rate should be adjustable such that the flow as exiting from the vaporizer is predominantly vapor with a trace of liquid carry-over in order to assure that;
a) the fluid is substantially vapor and conveying latent heat, and does not include a proportion of superheated vapor conveying sensible heat, which is comparatively inefficient;
b) and that non-vaporizing liquid additives, such as anti-freeze to prevent freezing in the system during off cycles at low temperatures also passivating agents to inhibit corrosion, are conveyed throughout the loop.
In order to control the process, therefore there is provided a viewing port which allows the operator to view the vapor emerging from the evaporator so that the operator can control the flow rate by adjusting the head to achieve the above conditions.
Thus the system operates by providing a physical configuration such that the actionary force creating flow in the desired rotational direction, is offset by the reactionary force causing an accumulation of liquid in a vertical column such as to create by differential liquid levels, or head, a balance of forces and blockage of flow in the undesired rotational direction.
This can be achieved by means of the insertion of a pump into the loop at any point in the loop such as to create, substantially all or in part, an equivalent head. The inlet of the pump may be immersed in liquid from a column of the liquid or the pump, if not immersed in liquid, will impel vapor and draw liquid pocketed in the system to the inlet of the pump
The adjustment of the flow rate, for most effective heat transfer as set forth above, can be obtained by use of a pump, where the flow rate now also becomes adjustable by varying the rotational speed of the pump impeller or by adding a flow calibration valve or flow regulator to the system. With loops that are inherently tuned to optimum effectiveness by the specifics of their physical design and have a fixed overall configuration, and are not exposed to variable temperatures, a flow calibration valve or regulator may not be required to achieve optimum effectiveness.
It is to be noted that with all forms of pumps, flow rate is affected by standing columns of liquid in the system, and depending on their orientation with respect to flow direction, some will exert a positive effect on flow and some will exert a negative effect. Also, the extent of effect on flow rate of such standing columns will vary from one type of pump to another. For example, with centrifugal pumps, which do not in themselves constitute complete physical intervention with regard to flow in that there is continuous open passage through the rotor, the effects of standing columns tends to be most pronounced, while with positive displacement pumps which do provide physical intervention such effects are diminished. Hence, smaller variations tend to be handled satisfactorily, at least closely enough to permit fine-tuning, by the less expensive centrifugal pumps, while more extreme variations tend to require the more expensive positive displacement pumps which are commonly of the reciprocating type. Rotational pumps that exercise a substantial degree of positive displacement, such as gear and vane pumps, are intermediate both in producing satisfactory results and with respect to costs.
In some applications the relative locations of the vaporizer and condenser are not fixed. This may occur for example in applications where portable and temporary heat is required and the equipment is moved from site to site. Therefore the horizontal and vertical displacement of the vaporizer and condenser may vary as the equipment is moved on the site or from one site to another. This may occur particularly where the vertical displacement may be significant such as in instances where the vaporizer is at ground level and the condenser is placed at some level in a high rise building. In this case, the system is therefore capable of accumulating substantial liquid level differential heads. In this case it may be desirable to minimize the effects of such pressure exerted from the column through the pump by the utilization of a positive displacement pump. In such pumps, the adjustment of the flow rate to obtain most effective heat transfer can be achieved simply by varying the rotational speed of the pump. Alternatively a flow calibration valve or flow regulator can be added to the system to detect flow rate and to vary the pump to obtain a desired flow rate. In locating the pump, general good practice is to place the pump such that it constitutes the lowest point in the system, and that suction pumps, being more costly than lift pumps and prone to cavitation with the hot liquids employed, should not be utilized unless other factors proscribe the locating of the pump at the lowest point in the system. Where the vaporizer is at ground level and the condenser is located in the basement or a lower level, for example in a parkade, and, due to the extremity of the downward vertical displacement of the condenser from the vaporizer, and the system is therefore not capable of accumulating significant liquid level differential head, or delivering sufficient effective standing head, it may be necessary to maximize the effect of the pump by employing a pump of sufficient lift to raise the condensate from the condenser level and with proper adjustment deliver it with adequate head to achieve flow rate for most effective heat transfer. Most effective heat transfer is obtained where the heat transfer takes place as a result of change of state rather than by cooling, and this can be obtained by controlling the head generated by the standing column and where provided the pump so as to establish a mode where minimal liquid is transferred while providing the entrainment of a trace of liquids carrying over non-vaporizing additives such as anti-freeze and passivating agents into and throughout the system
Embodiments of the invention are described herein in conduction with the attached drawings as follows:
Table A attached hereto shows a list of possible fluids for use in the system as heat transfer medium.
DETAILED DESCRIPTIONIt will be appreciated that each of the different configurations shown and described herein can be used in different locations for heating different materials including water, oil or petroleum products and air. Thus in
The configuration shown in
However it will be appreciated that the configuration of the evaporation section as described hereinafter can vary and be selected from any one of the configurations shown herein for use with the different fluids to be heated. Yet further additional configurations can be provided for the evaporation section which are not shown herein.
Advantage can be obtained by encapsulation of the evaporation section within a heat communication medium such as a heating oil but this is not essential to any of the configurations shown.
Advantage can be obtained by providing a manifold which connects the evaporation section to the condensation section so that one or more conduit portions from the evaporation section can connect to a different number of conduit portions in the condensation section. However the use for the manifold is not essential and the system can comprise a single complete conduit which communicates with both the evaporation section and condensation section or can comprise a multiple number of separate conduits each independently connected to the evaporation section and to the condensation section.
Turning firstly to
The horizontal legs 13 and 14 are connected by vertical leg portions 17 and 18 which are short in comparison with the length of the legs 13 and 14.
The evaporation section 12 is located within an encapsulating container 19 which has a cylindrical peripheral wall as best shown in
The heat loop 10 contains a heat transfer medium 25 which is in liquid form at the bottom of the heat loop and in vapor form in the top of the heat loop. The amount of the heat transfer medium is arranged so that the surface 26 is within the leg 14 and is confined by a bulkhead trap member 27 at the junction between the leg 14 and the leg portion 18. Thus the bulkhead trap 27 extends downwardly at the leg portion 18 into the liquid below the surface 26 so as to provide a trap which prevents vapor from entering the leg portion 18 from below thus causing vapor to flow only in the clockwise direction and around the loop and preventing backflow of vapor.
In the evaporation section 12, the liquid is heated so as to generate a vigorous boiling action sufficient to generate vapor rapidly in the evaporation section. The vapor is prevented from running along the leg 14 by the trap 27 and thus must rise along the leg portion 17 and run along the leg 13 to generate a flow around the loop in the clockwise direction. The dimensions of the loop relative to the amount of heat applied through the intermediate heating oil 23 to the evaporation section is arranged so that the vapor moves at high velocity greater than 500 feet per minute and more preferably of the order of the speed of sound so as to generate rapid flow of significant volume of the vapor so as to transfer the latent heat of evaporation of all of that volume of vapor from the evaporation section to the condensation section where all that vapor condenses. The maximum efficiency can be obtained when all of the vapor is condensed and when little or no heat is transferred from the liquid to the fluid for A by cooling the liquid.
It will be noted that in the leg portion 18, there is a volume of liquid up to a surface 26A which generates a head of liquid at a height H which is responsive to a pressure differential across the trap 27. This pressure differential is equal to the drop in pressure caused by the resistance to flow of the vapor within the loop from the evaporation section to the condensation section.
In
Turning now to
The coil is spaced from the inner and outer walls of the cylindrical container leaving space for the oil to generate convection currents to transfer heat efficiently and constant temperature from the inside surface to the whole of the coil housed within the cylindrical container.
In this embodiment the trap within the bottom leg 14 is replaced by a U bend form of trap indicated at 27A. Thus there is formed two legs 27B and 27C of sufficient length to contain the head H of the liquid within the leg 27C to match the pressure drop through the loop caused by resistance to flow. It will be appreciated that the resistance to flow within the more complex loop shown in
In
In
In
In the embodiment of
In
Turning now to
In
The condenser heat exchanger which is a hollow section metal may have a single vaporizing section or may lead to one or a multiplicity of condensing sections.
The vaporizer water legs are fabricated metal containers forming manifolds for the condenser heat exchanger sections.
The vaporizer heat exchanger is a hollow section metal which may be finned and can be increased or decreased in number and length in order to increase or decrease efficiency of heat exchange from heating source.
The heating medium may be any liquid or liquid mix, typically water or water/glycol, generally including a metal passivating agent.
The heat source may be a direct flame from an introduced flame, or could also be heated via a secondary heating medium such as hot oil delivered to an encasement around the vaporizer heat exchanger tubes. A common source of hot oil can heat either a single or a multiplicity of Heat Driven Loops.
The pressure differential trap may be a condenser return leg extended down into the condensate tank.
The liquid level differential and pressure creates pressure that impels vapor into outlet leg of condenser and prevents back-flow of vapor into return leg.
Vapor flow, that is the velocity of vapor, as dictated by the cross sectional area of the outlet leg, the resistance to flow of the condenser, and the pressure differential across the outlet and return legs of the condenser created by the liquid level differential in the trap, carries all condensate in the direction of vapor flow.
Condensate flow, that is the condensate driven back to the vaporizer is effected by vapor flow but there may be some gravity assistance if condenser operating angle is above horizontal.
This allows a range of condenser operating angles from horizontal. The above principle is expected to be effective in moving the major flow of condensate in the same direction as the vapor at angles of at least 10 degrees from horizontal. ‘Effective’ can be defined as substantially achieving the enhancement of heat exchange associated with unidirectional flow of vapor and condensate as opposed to counter-directional flow. Theoretically, by increasing the trap differential pressure and regulating the size of the outlet leg of the condenser, the angle from horizontal could be extended to 90 deg.
There is a region of turbulent boiling in the sealed system and the starting pressure can be regulated to anything that can be achieved above a complete vacuum. Having established the starting pressure, the void space is generally purged with an inert gas, such as argon. Especially under vacuum conditions, boiling will be turbulent with large bubbles of steam carrying globs of liquid along with it, but without the liquid bridging the conduit to avoid the formation of a bubble pump. These globules of water will splash into the upper vaporizer heat exchanger tubes keeping them wet, and, to some extent, be carried into and possibly through the condenser.
It is the adjustability of the differential pressure between the supply and return legs of the condenser plus the ability to achieve higher pressures sufficient to overcome resistance imposed by more complex configurations, even involving the entraining and lifting of condensate, that distinguishes the arrangement of
Other load demands could consist of mechanical utilization of energy. This would include, for example, the driving of a turbine for any number of purposes including the generation of electricity, the direct driving of a pump, fan, etc.
It may be possible to utilize mechanical back-flow resisting devices such as ball-check, swing-check, or, spring-loaded valves such as to increase resistance to back pressure. However in practice, mechanical methods of blocking back pressure may be impractical in that they eventually will require maintenance. Conventional steam traps, for example, are susceptible to occasional problems. Compared to conventional steam systems the present invention may use different liquids, higher temperatures, higher vapor and condensate velocities etc, plus a need for rugged reliability. It is one of the distinguishing features of the present arrangement that it is entirely ‘thermodynamic’, i.e., heat driven, without any moving parts.
One problem which can arise is the accumulation of inert gases which is a commonly encountered phenomenon with this type of technology. A gradual build-up of inert gases occurs in these systems, depending on materials utilized and chemical action between them, which displaces vapor and decreases effectiveness, which, with single tube technology, sometimes determines service life because its effects are not readily monitored or remedied. It is inherent to the present principal of operation that this major concern becomes much more manageable and is therefore an important feature of the invention.
A loop with significant force of flow such as the present arrangement, has the advantage that any inert gases in the system will be driven into what is referred to as an accumulation sector, which is the sector of the loop just before the trap and will be confined there while the system is in operation due to the forward flow of the vapor and the locking or trap effect of the liquid in the trap. Thus an access opening 75 is located immediately in advance of the trap for sampling of the presence of inert gases and for purging of those gases. It will be appreciated that in the presence of such gases, the opening of the access opening by service personnel will cause the vapor pressure and flow to discharge the inert gases through the opening until the presence of vapor in the discharge indicates that all gases have been purged. Such inert gases may be introduced for purging and subsequently not fully evacuated, such as argon which is commonly used for this purpose, and/or produced as a result of chemical activity such as hydrogen as from reaction between water and iron, the predominant element in mild steels and present to some degree in stainless steels, and which occurs even in the absence of free oxygen, hence the need for passivating agents. With the arrangement as described herein, that sector would normally be out of or at least extending partly out of the immersed portion of the heating element, the significance being that it is accessible in that it will not be completely immersed. The build up of inert gases can be detected by a decrease in temperature in an area of the conduit immediately upstream of the trap which is caused by the inert gases preventing the vapor from condensing in that area and thus properly heating the conduit. Thus the temperature at this area can be monitored on an ongoing or periodic basis to detect an unacceptable build up of the inert gases. Alternatively, the inert gases when they build up will reduce the vacuum in the system when shut down and again their presence can be detected by service personnel carrying out a pressure test at shut down and detecting the presence or reduction of the initial preset vacuum level.
With single tube technologies whether tubes are employed singly or in a plurality, such as conventional heat pipes and thermo-siphons, as in the prior art of Spehar and Neulander mentioned above, and which are commonly employed sloped upwards into the vessel, the inert gases accumulate and remain, whether the system is in or out of operation, in what is referred to as a ‘block’ in the high end of the tube, which is the sector furthest immersed in the process fluid and most inaccessible.
In a sector where there is such accumulation of inert gases, heat exchange is significantly impaired because the inert gases block out vapor and preclude the change of state which is the substantial means of conveying heat. Only sensible heat from liquids that may flow through the sector would be transmitted from the accumulation sector.
With loops, the decline is such that effective heat exchange is significantly impaired but not altogether eliminated because there is at least some sensible heat available from condensate and throw-over liquid flowing through that sector. At the boundary between the sector of the heating element that is performing normally and maintaining a substantially constant temperature, and the sector where there is accumulation of inert gases, heating element temperatures start to decline in an observable, significant, and regular fashion.
However, with single tubes, there is no such flow of liquid and heating element temperatures will decline much more drastically and that sector is effectively ‘blocked’, or idled, for heat exchange purposes. Moreover, with loops, when in full operation and the system under positive pressure, the accumulation is moved to a sector that is normally accessible for measurement of temperature, the difference between the entry temperature of vapor to the heating element and the temperature in the accumulation sector being an indication of the degree of accumulation of inert gases, and purging of the inert gases, utilizing the operating pressure of the system itself, usually from the highest point in the system just prior to the trap.
There is no practically convenient means of either measuring, or even detecting, such accumulation with single tubes, which occurs at its greatest extension into the process fluid, and similarly, no practically convenient means of purging such accumulation if it could be detected. With single tubes, such measurement and purging devices would have to extend back through the tubes themselves or through the vessel. These are very difficult environments warranting correspondingly expensive solutions compared to the simple access provided by the present system.
This a significant improvement presented by the present system over all single tube technologies also over the prior art of the Grunes et al technology when operating below that critical level where it flips from unidirectional flow, which causes such accumulation to occur in a sector next to the trap as above, to counter-directional flow which, with its particular configuration, would likely cause dispersion of the inert gases throughout the system while in operation which would generally impair effectiveness, and, accumulation at a highest point when not in operation.
The heating of water and petroleum products, especially crude petroleum products that are towards the “heavy”, that is comparatively viscous end of the scale, present differing problems. Water is comparatively easy to heat. Resistance to heat transfer is at its minimum at commencement when temperature differential is at its greatest and increases as temperature rises. Convection currents are readily established and the whole process is quite dependable and predictable. For heating purposes, water properties are ‘constant’, on both a case to case basis, and with respect to any individual case. With petroleum, on the other hand, heating properties are much more variable and complex in that:
[a] Petroleum has ‘non-Newtonian’ flow characteristics. This has to do with viscosity varying not only with temperature but with also flow velocity and boundary effects between currents in different directions in the same vessel. In other words, flow, particularly convection flow, tends to be affected in rather unpredictable ways by specific configurations of vessels and heating elements. This effect tends to be more pronounced with heavier, more viscous, petroleum products.
[b] Crude petroleum product varies greatly in content and characteristics; viscosity of liquid petroleum product, proportion of liquid petroleum product, amount of entrained gaseous petroleum product, proportion of water, salinity of water, amount of entrained particulate matter, sand, usually and associated more with heavier product, these would be the main variables.
[c] Boundary effects between the heating elements and petroleum products are much more problematic, with crude petroleum especially, in that; resistance to heat transfer will always be higher than with water and will be variable depending on the effects of all of the forgoing, and, the flashing of petroleum products and/or entrained water into gases causes foam to collect in the immediate vicinity of heating elements which further resists heat transfer.
[d] Also, petroleum products, particular heavier crude products, have a tendency to ‘channel’, at least initially, when being heated, i.e., set up localized convection currents which get hotter, less viscous, and therefore more active, while bypassing volumes of un-circulating and unheated liquid. Eventually, enough heat is transmitted to these un-circulating volumes that they become entrained in an overall convection flow pattern.
[e] The foregoing are ‘non-constant’, as well as variable, in the sense that same configurations do not always set up same flow patterns and rates of heat transfer, as is the case with water, because the summation of the effects of the foregoing always produce some net differences with respect to flow and heat transfer characteristics and these differences are often not of an observable nature and scale.
With water, the heat loop system may have a heat transfer rate of 10,000 btuh/sq ft. of heat exchange surface at commencement of heating at somewhere just above freezing which will decrease in a regular fashion to perhaps 8,000 btuh/sq ft when the water reaches a control temperature of somewhere just below boiling. With a vessel of a given size and configuration, filled to a given level, and heated with a heater of a given size, configuration and capacity, this type of result will not vary from instance to instance.
With petroleum product, at commencement of heating with cold, stiff and highly adulterated product, the initial heat transfer might be very low, say in the order of 200 btuh/sq ft. of heat exchange surface. This may rise to 1000 btuh/sq ft as convection circulation is established and then decrease to 800 btuh/sq ft as control temperature is reached. As previously indicated, this may vary from instance to instance, even in a given application.
The differences between the heat transfer characteristics of wafer and petroleum products tends to be amplified with; cruder, as opposed to more refined, and, heavier, as opposed to lighter, petroleum products.
In other words, the technology must cope not only with great variation in demand, but great variation in heat transfer characteristics as load is imposed. It is inherent to the present design that it will self-adjust to all of his—there will be unidirectional flow from start up to shutdown, and at all levels, of operation.
That is not the case with the Grunes et al technology. Heating portable water is an application that lends itself readily to full on/full off operation. It is inherent to the Grunes et al technology that it will tend to flip back and forth between two modes of operation at intermediate levels of operation. It must get up to some minimum level of operation to either; flip over through boiling action, or create through condensation, enough liquid to maintain a level in the accumulator, which is critical to establishing and maintaining unidirectional flow. At below that level of operation, the restriction and the accumulator associated with it, which has a largely fixed, at least a minimum, draining rate, will remain clear of liquid. Vapor and condensate will flow in opposite directions in both legs of the device in the manner of a conventional, single tube thermo-siphon. It could actually be considered to be two single tube thermo-siphons abutting each other at both ends.
The arrangement of the present invention has an improved operation because:
[a] the amount of material employed in relation to the amount of heat transferred. Because transfer is being accomplished by change of state, the amount of energy that can be transferred by a given amount of fluid is proportionate to the rate at which the fluid is circulated each cycle representing the transfer of the total latent heat capacity of the amount of fluid in the system. By maximizing flow rate and therefore heat transfer rate both the amount of fluid required and the amount of material required to create the necessary volume to contain it will be minimized. That would be within the physical capability of the system to transfer heat in and out, of course, but that too can be enhanced in relation to volume enclosed by the addition of suitable fins to facilitate heat transfer, encapsulation to maximize average contact temperature, etc. Maintaining flow rate of vapor and condensate in one direction, as compared to vapor in one direction and condensate in the other and resisting each other, at all levels of operation, will maximize effectiveness. The capability of accomplishing and maintaining that at all levels of operation in this particular application represents a considerable improvement.
[b] the ability of the device to sustain a driving force through the system at all levels of operation. This extends beyond [a] above in that there are potential applications where the ability to create pressure differentials and overcome resistance is a critical to the devices operation. This would include any application where the system is utilized to perform a mechanical function. With the Grunes et al technology, at below some critical level of operation, such a device would cease to operate.
Points [a] and [b] in particular are general advantages that the present technology presents over the Grunes et al technology. The capability of maintaining stable operation under varying and unpredictable loading, a common condition in some aspects of petroleum processing, particularly with cruder and heavier products, is a specific advantage in that application but presents potential advantages in other applications as well. Point [b] above is not directly associated with the heating or processing of any particular substance it is simply an advantage to have a device that provides a force to operate something to be capable of doing so throughout a full range of operating levels as opposed to just an upper portion of that range.
There are a number of different types of traps which are possible for use with this construction;
1. A submerged bulkhead which is shown in
2. The “U” Trap shown in
3. The Down-leg Trap shown in
All these work according to the same principle—back pressure in the vaporization area opposed and balanced by liquid level differential pressure in the trap. The range of back pressure that can be tolerated can be adjusted in all three cases by increasing the depth of the trap.
The “U” Trap configuration presents the advantages;
It is a simple and straightforward matter involving minimal additional material to increase its pressure range by making the “U” deeper, whereas increasing the range of the other configurations would involve deepening the whole vaporization area, which would involve considerably more bulk, and, it is inherent to the “U” Tube approach that violent boiling action will not penetrate through to the up-leg because the up-leg will always be in its entirety below the boiling area, which is not necessarily the case with the other two configurations. It could be claimed that these configurations are more susceptible to violent boiling action reaching the up-leg of the trap which would then nullify or substantially impair the desired effect of driving flow in one direction.
However, having said all that, it is a simple matter to adjust the other configurations to these disadvantages simply by having the bulkhead and the open-ended conduit descend into a well provided for that purpose in the bottom of the vaporization area.
The submerged bulkhead and the Down-leg traps have an advantage over the “U” Trap in that extra material is not required for the up-leg.
The down leg trap shown in
Turning now to
The system further includes the heat transfer medium 101A as liquid; 50% water/50% propylene glycol, and 101B as vapor; liquid storage container[s] 102; solenoid valves 103 A and B; compressor with air cylinder and circuits 104 A and B; flow regulating pump 105; heat source 106; vaporizer 107; heat transfer pump 108; multiple port manifolds 111 A and return B; flow viewing ports supply 112 A and return 112 B; pressure control or relief 113 A and temperature control 113 B; sector where condensation is completed 114; flow calibration valve 115; loop vent valve 116 and generator 117.
At rest, after assembly on site all liquid heat transfer medium as liquid 101 is in the container 102, and the loop itself is void of liquid and at zero gauge pressure [0 psig]. The solenoid valves 103B are open and 103A are closed The liquid is in the liquid storage container 102 isolated from the Loop mode at initiation of the start-up procedure.
In preparation, the compressor 104 with circuits 104A open and 104B closed, is turned on, and air in the Loop pumped out to create a pre-selected partial vacuum, such as is attainable with equipment available for practical use in the field which may be in the order of 6 in Hg. Then the compressor 104 is automatically shut off in response to an internal control set at that proportion of vacuum.
In start-up, the solenoid valves are switched into the container 102 open to the Loop mode with the solenoids 103A and 103B open. Simultaneously, the flow regulating pump 105 and the heat source 106 are turned on. A charge of heat transfer medium as liquid 101 is drawn from the container 102 into the Loop, and thence through the pump 105 into the vaporizer 107. The transfer pump 108 may be utilized to assist in charging the Loop, depending on the vertical positioning of the container 102 relative to the Loop. The liquid 101 is heated in the vaporizer 107 by the heat source 106, and is increased in temperature until it changes state into a vapor, also occasioning an increase of pressure and a rapid and substantial increase in volume in the order of 1700 to 1 as that occurs. This rapid increase in volume tends to force the fluid in both directions, but flow is biased in one direction around the Loop by the reactive force of the head 109 at the pump inlet such as is trapped in the configuration of the Loop, which, with or without combination with a head created by a pump 105, depending on the adequacy of a reactive force created by the liquid column atone, to create such bias.
The Loop is maintained in the start-up mode until the fluid charge is sufficient in amount to complete a flow of liquid around the loop, as indicated by the fluid, subsequent to heat release and condensation in the ground thawing flexible hose 110, appearing predominantly or entirely as a liquid passing through the return viewing port 112B and thence providing an accumulation as the head at inlet of pump 109.
The pressure in the Loop will progressively rise during start-up in response to the continued operation of the heat source 106, until limited by a heat source pressure control 113A located at the outlet of the vaporizer 107 and set at 0 psig maximum, or alternatively, a temperature control 113B set at 212 degF., the temperature commensurate with vaporization at 0 psig. In practice, a combination of both a temperature control and pressure limiting control or relief device may be used to supervise temperature and limit pressure respectively, with the one acting in redundancy to the other.
During Continuous Operation; when operation shows stability as above, the solenoid valves are switched into the operating mode with 103B open and 103A closed, and the container 102 is isolated from the Loop.
At 0 psig, the vapor 101B has a temperature of 212 deg F. at the point of control where emitted from the vaporizer 107, which is the same as the boiling point of water when exposed to atmospheric pressure. However, downstream from that point in the Loop, and up to the pump 105, there will actually be a slight, progressive reduction of absolute pressure/increase of vacuum, and commensurate temperature, due to the draw of the pump 102. As well, in the section where heat loss and condensation are occurring, in the ground thawing flexible hosing 110, the initial temperature of the condensate will also be at 212 degF., and there will be a loss of sensible heat and temperature from the condensate as that progresses through the hosing 110, but this will be small in relation to the latent heat loss which is without decrease in temperature. Moreover, the collective temperature reductions of the two foregoing effects are minor such that for practical purposes and discussion, the temperature throughout the Loop whether it contains vapor or vapor/condensate mix, the temperature may be regarded as being at a constant 212 degF. and the pressure at a constant 0 psig. In any event, a hose 110 temperature which might stand at a full 212 degF. does not occasion any significant boiling of ground water from thaw because there would be instant surface cooling as cold ground water comes into contact with and absorbed heat from the hose.
It should be noted that, where it is practical and permissible, the system can be operated at higher and lower pressures than 0 psig, and at commensurately higher and lower temperatures that 212 degF., should that be desired. For example, operating at 15 psig might be considered in some instances because that has a commensurate temperature of 250 degF., and is officially considered “low pressure”, which is regarded as not presenting a particular hazard when operated without constant attendance.
Maintaining a head at pump inlet can be critical to continuous operation because the combination of a partial vacuum and elevated temperature may result in the pump being prone to internal cavitation, i.e., the liquid likely to flash into a vapor at the point where it enters the impellor where a further localized pressure drop occurs. Therefore, the amount of the fluid charge, and the configuration of the Loop, should be such that a liquid pressure will be continuously exerted on the inlet of the pump while in operation. Hence, the head at pump inlet, in combination with the thrust of the rapid expansion of fluid, serves three purposes; supplementing the impulsion of the pump in driving the fluid around the loop, contributing to prevention of pump cavitation, and, as an arrangement enabling accumulation of a protective surplus for the fluid charge required by the Loop for continuous operation.
With the system, a relatively steep downward temperature gradient in the Loop, typical of conventional hot-liquid systems, will commence only at the sector in the loop where condensation of fluid is completed 114. In an optimized system, as properly scaled and adjusted, that point is just before entry to the return manifold 111B.
The system is further optimized in terms of heat transfer capacity in relation to fluid mass flow and material employed, by; configuring the Loop, providing a fluid charge such that a small carryover of liquid from the vaporizer 107 can take place, and making the system adjustable, such that by viewing fluid flow through the supply viewing port 112A and adjusting the heat supply and the fluid flow rate, usually by setting the heat source 106 capacity to a maximum, and adjusting either the rotational speed of the flow regulating pump 105 or, with a fixed speed pump, adjusting the flow calibration valve 114, such that observation at the supply flow viewing port 112A indicates a trace of liquid passing through, otherwise entirely vapor. This assures that the fluid is virtually all being vaporized and is substantially conveying latent heat only, and is not being superheated and partly carrying sensible heat as well which by comparison with the former is inefficient. It is a function of the flow regulating pump to keep that mix of substantially vapor, minimally liquid at the point of entry into the condenser 110.
Also, that small amount of liquid carryover serves another useful purpose in that it assures that additives for other purposes such as the antifreeze to prevent freezing of the fluid in any part of the system, should there be shutdown in cold weather, and passivating agents to reduce corrosion, are conveyed throughout the Loop.
The use of a generator 117 to supply electrical power to the pumps and compressor in order to make the system entirely self sustaining and fully portables as opposed to connection to a fixed electrical outlet, is optional.
During shut-down, the heat source 106 and the pump 105 are shut off, and the Loop allowed to cool to facilitate handling. Liquid will remain in the pump 106, vaporizer 107 and head or liquid column portion of the Loop, and some condensate may remain in the flexible tubes 110 of the thawing section. The solenoid valves are switched into the liquid evacuation mode with 103A and 103B open. It is advisable at shutdown to then open the Loop vent 116 to atmosphere to neutralize the vacuum that will occur and increase as the Loop cools. The air compressor 104 is turned on and when the air storage cylinder is charged with pressurized air circuit 104B is opened. Compressed air is then released into the Loop, which drives the remaining liquid 101B out of the Loop and back into the storage container 102. Completion of this can be observed through the return viewing port 112B. Generally, the resistance of the pump 105 to reverse flow assures that this air pressure is exercised sufficiently in one direction to complete evacuation of liquid. To further assure this, a check valve 117 may be added to the Loop. Hence the fluid charge is evacuated from the Loop and returned to the storage container 102.
The system may now be unassembled and removed from the site.
Conventional hot-liquid-only ground thawing devices typically operate at a liquid charge temperature of 170 degF. at the supply manifold, which is reduced to 130 degF. at the return manifold, a reducing but average temperature of 150 degF., due to a sensible heat transfer to ground thawing of 40 btu for each lb of fluid circulated. Attempting to operate at higher temperatures is inhibited by localized flashing in the vaporizer of the water portion of the liquid charge in the system into steam, which creates appreciable loss of fluid through the venting to atmosphere.
By comparison, the present system holds a constant temperature of 212 degF. throughout, due to the fluid charge leaving the supply manifold as a vapor at 0 psig with a commensurate change of state temperature of 212 degF., and entering the return manifold as a liquid, with condensation completed in between at that change of state temperature, with a latent heat transfer to thawing ground of not less than 1000 btu for each lb of vapor/liquid circulated. Furthermore, the present system is sealed when operating, so there are neither boiling nor evaporative losses to atmosphere of the fluid charge.
Because thawing with the present system is at a significantly higher and constant temperature of 212 degF., as high as possible without causing ‘drying’, i.e., boiling away of ground water which can be detrimental to thawing, as compared to a declining but average temperature of 150 degF. with conventional thawing devices, the present system creates an appreciably faster rate of thaw.
Also, because with the present system mass flow circulation to carry a given capacity is significantly less, and, other than a small liquid feed pump to the vaporizer, the fluid is driven around the loop by thermal energy causing expansion, as compared to a much higher mass flow of liquid circulated wholly by an electrically driven pump, the electrical power requirement for the present system is comparatively quite small. This is readily supplied by a compact and relatively inexpensive portable generator making complete self containment and full portability more economical.
Also the system heat transfer medium, a mixture of propylene glycol which is a food refrigerant, and water, is officially rated as environmentally benign, and the fluid charge is retained in the system at a maximum pressure of 0 psig, which presents no pressure-related hazard. Furthermore, at significant capacities of 400,000 btuh and more, the volume of fluid contained is so small, that it is below the amount at which ASME based regulations apply. In other words, the present system is not only actually safe, but is readily appreciated by prospective users as self-evidentially safe, as well as being formally defined as safe under prevalent regulations.
Furthermore, the present system is compact and, in terms of; components, materials required, and manufacturing processes employed, is relatively simple and inexpensive to build.
It should also be noted that the particular system arrangement illustrated, enables charging the system with fluid from original containers—such as the barrels in which premixed liquids are received from liquid suppliers—and returning the charge to those same containers. This particular system arrangement produces considerable advantage in that liquid handling is minimized and storage simplified—as well as provides a simple means of measuring liquid loss by field users during as operating period simply by checking levels going out and back in.
Turning now to
As shown in
The evaporator section 201 is similarly mounted in a separate portable unit 207 and includes a combustion chamber 208 and a combustion burner 210 and an evaporation coil 211. The fluid is communicated between the evaporation coil 211 and the radiator 205 by tubing 209.
For permanent, and portable and temporary space heating, this arrangement has considerable flexibility in application. The vaporizer section and the condenser section, coupled together, may be deployed as a unit, located as desired and permitted in the space[s] to be heated. In such deployment, with some limitation at the lower end of capacities, the unit so formed, is competitive with, and superior in performance to, any other type of indirect fired heater.
However, the vaporizer and condenser sections may also be deployed as separate modules and be displaced from each other significant distances both horizontally and vertically.
This flexibility presents significant advantage in such applications as portable and temporary heating in urban high-rise buildings.
Currently, there are only two large scale distribution grid modes for the delivery of energy convertible to heat, the most familiar expressions of each being; the conduction of electricity though cables, and the conveyance of natural gas through pipelines; both modes being suitable for long range and localized distribution grids. The conversion to heat, for such requirement, at points of employment takes place through conductivity resistance in the one instance and combustion in the other. Practical characteristics of such grids are that they are flexible, relatively inexpensive, and that energy costs/losses in transmission are acceptably low in relation to energy delivered.
Other sources of heat energy would principally be liquid fuels delivered in bulk lots in containers—such as propane in which instance delivery is in pressurized containers and therefore storage is of particular concern and consequently heavily proscribed or even prohibited by regulation most notably in urban high-rise contexts.
However, this arrangement represents a third and new grid mode; it conveys energy from the heat source to the spot or points of heat application in the form of the latent heat constituent in vapor—and in a manner uniquely suited to smaller and portable grids.
What specifically is meant by in this instance by way of unique suitability and smaller scale grid distribution, are; a practical means of heat creating energy transmission, readily deployable and knocked down, of sufficient range such as to enable spot heating or multiple point space heating, throughout the interior of the type of high-rise buildings generally encountered in densely populated urban centers, both upwards into the commercial or living spaces and downwards into basement and parkade spaces—well beyond the practical range of electrical cabling from main panels—and inside and around which the storage of liquid fuel is heavily proscribed or prohibited.
In such applications, this arrangement presents options for the locating of the fuel consuming portion of the device, the vaporizer, and the space heat generating portion, the condenser or ‘heater’, not available with other types of systems, and that are economically acceptable.
With electricity, for example, the vaporizer, which is quite compact, can be located next to the electrical panel with energy for heat generation supplied with an acceptable size and length of cable from the panel. With propane, for example, the vaporizer can be located adjacent to its storage area if and as permitted, with fuel energy supplied in a standard manner with hose lengths that give proper clearances. The condenser[s], or heater[s], can be located as desired and are movable.
With this arrangement, the vapor can be driven at sufficiently high velocities through a grid of such type that energy cost/loss in relation to energy delivered, can be acceptably limited. Delivery of vapor and return of condensate are through acceptably small hoses that can be strung up and down through high-rises in numbers of ways; through openings generally available during construction, or stairwells and elevator shafts, or, on the exterior of buildings.
In applications where potential hazard from vapor and condensate hoses are a particular concern due to human habitation, it is proposed that this arrangement be operated at 0 gage pressure or less [no pressure] which presents no pressure-related hazard, also that fluid contained is a mixture of water and a commonly used food refrigerant, propylene glycol, which is rated benign with respect to human contact and environment.
It should also be noted with respect to such flexibility in application, particularly regarding vertical displacement of the vaporizer and condenser upwards and downwards, and with regard to the system being operated at optimum effectiveness, which may be defined as a combination of; [a] transmitting heat substantially as latent heat only, with the fluid exiting the vaporizer substantially as an unsuperheated vapor, and [b] while entraining a trace of liquid carryover including non-vaporizing liquid additives such as anti-freeze and passivating agents for corrosion prevention such that these will be carried throughout the system, with respect to which certain effects of variable vertical displacement must be considered.
In all applications for which this arrangement is proposed, there will be a combination of some standing head, water in a column, being exerted positively on flow, and some resistance to flow to be overcome, as well as in some instances standing heads being exerted negatively on flow that also have to be overcome. In applications where the condenser configuration is such that gravity would cause it to drain or stand in the lower portion of the condenser such as to create a standing head exerting positive effect on flow, there may be an absence of standing heads being exerted negatively on flow.
Additionally, in any configurations that tend to restrict the height of such standing columns, the thrust imparted to the flow of condensate by the 1700 to 1 expansion of fluid from a liquid to a vapor that is occurring behind the sector of the Loop where condensate is progressively accumulating will tend to drive the condensate into any available trapping configuration as well as into such trapping configuration as may be specifically provided at the inlet of the pump, and/or, directly into the inlet of a pump in which latter case, due to force of flow, it provides a head, which may be only a standing column of the liquid or it may be supplemented by the effects of a pump.
The foregoing will be the case both where flow is solely thermally driven, and where a pump or equivalent device supplements such flow. In other words there will always be some element of standing column and effective head in all forms of this arrangement.
It also follows that in applications where that standing column may be variable, such as in portable and temporary heating and ground thawing, where the vertical displacement of the vaporizer and condenser will vary from site to site and even on a given site, this will tend to cause flow rate to deviate from optimum effectiveness as that is described in the foregoing. Variable temperature exposure may also tend to cause flow to deviate from optimum effectiveness.
When the flow rate is too high in relation to heat absorption, the fluid will only partially vaporize and will alternate between surges of vapor and liquid, in the manner of a bubble pump, such that a significant portion of heat may be transmitted as sensible heat in the liquid which is less efficient in terms of material employed to achieve a given capacity. When the flow rate is too low in relation to heat absorption, the fluid will not only completely vaporize but will also superheat such that a significant portion of heat may be transmitted as sensible heat in the vapor which is also less efficient in terms of material employed to achieve a given capacity of heat transfer. In both these non-optimum instances, flow tends to be unstable in that in the first the heat exchanger material tends cool down and then regain temperature alternately, and in the second tends to overheat and then loose temperature alternately, with stability gained as optimum effectiveness is approached.
In such circumstances, the addition of a pump to the Loop will contribute to achieving optimum effectiveness in that a solely thermally driven Loop which depends only on a standing column to drive flow will be more profoundly affected by such variability and instability, than a Loop with a pump which tends to significantly dampen such effects. In fact, the addition of a pump plus a flow calibration valve or flow regulator to fine-tune flow rate, becomes a preferred means of assuring optimum effectiveness in all applications because of ease and the relative steadiness created in operation over a wide range of variable conditions. However, it should also be noted that in fixed configurations where relative locations of components do not vary and that are not exposed to variable temperatures, without or with a pump, it may be inherent to the physical nature of the design that flow is fixed at optimum effectiveness without the requirement of a calibration valve or flow regulator.
In variable configurations, as vertical displacement becomes more extreme, different types of pumps will be more effective than others in dampening variation of flow. Smaller variations tend to be handled to a satisfactory extent, in that fine-tuning can be provided by a flow calibration valve or flow regulator, by the less expensive centrifugal pumps, while more extreme variations tend to require the more expensive reciprocating positive displacement pumps. Rotational pumps that exercise a degree of positive displacement, such as gear and vane pumps, are intermediate in both producing satisfactory results and with respect to costs.
It should also be noted, that full utilization of the head created by the thermally created liquid level differential to the point of using it exclusively in applications where variability and instability are not a concern, will minimize or eliminate the electrical or other energy requirement to drive a pump, as well as the overall energy requirement of the loop when both a standing column and a pump are utilized, because thermal energy can be utilized directly from a fossil fuel source and at a very high efficiency level in this Heat Driven Loop.
In an arrangement where there is a considerable distance between the vaporizer and the condenser so that the hoses transporting the fluids therebetween are long, it may be desirable to apply electrical heat from a resistance heating wire in or on the hoses to compensate for excessive heat loss. In this way the vapor is maintained in the required vapor phase from the outlet of the vaporizer to the inlet to the condenser without the necessity to superheat the vapor. This technique will provide an improved efficiency of heat transfer which will overcome the extra heat energy required to heat the hoses electically.
Claims
1. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section so that the thermal energy causes expansion of volume due to a change of state;
- flow around the loop being biased in one direction by the creation of a head.
2. The method according to claim 1 wherein the conduit and condensation section have a resistance to flow of the vapor from the vaporizer section to and through the condensation section and wherein the head is arranged such that, subsequent to start-up and during steady state flow of the heat transfer fluid medium in the loop, the head defines a pressure in the liquid at least equal to a pressure drop in the vapor caused by the resistance to flow of the vapor in the conduit from the evaporation section to and through the condensation section.
3. The method according to claim 1 wherein the head is generated by a standing column of liquid without assistance from a pump.
4. The method according to claim 1 wherein the head is created by a combination of pressure developed by a pump and a standing column of the liquid.
5. The method according to claim 4 wherein the condenser is higher than the pump and there is arranged to be a column of liquid at the inlet to the pump.
6. The method according to claim 1 wherein there is provided a pump and the condenser is lower than the pump and the pump is arranged to generate a suction at the inlet acting to lift the liquid to the pump.
7. The method according to claim 1 wherein the head is partly generated by a pump and the operation of the process is controlled by varying the flow rate of pump.
8. The method according to claim 8 wherein there is provided a viewing port and the operation of the process is controlled by varying the pump while viewing passage of vapor from the evaporation section so as to ensure passage substantially wholly of vapor with a minimal amount of liquid.
9. The method according to claim 7 wherein the pump is a positive displacement pump so that the rate of flow is directly proportional to a rotation rate of the pump.
10. The method according to claim 9 wherein the condensation section is arranged at a height above the pump such that a column of liquid generated thereby generates a pressure greater than a required pressure for optimum operation and wherein the positive displacement pump generates an outlet pressure below that of the column.
11. The method according to claim 1 wherein the system contains a total volume of liquid less than 43.5 litres or 1.5 cu. ft.
12. The method according to claim 1 wherein the system is evacuated prior to start up.
13. The method according to claim 12 wherein the system is evacuated prior to start up so that the operating pressure in the vapor is less than 15 psi.
14. The method according to claim 12 wherein there is provided a compressor having a storage tank and the system is evacuated prior to start up by connecting the inlet of the compressor to the system and wherein the system is purged after shut down by compressed air from the storage tank.
15. The method according to claim 1 wherein the flow of vapor from the evaporation section to the condensation section is at sufficient velocity to carry all condensate forwardly to a position where it can flow around the loop under gravity back to the evaporation section.
16. The method according to claim 1 wherein substantially all the vapor generated in the evaporation section is caused to condense in the condensation section.
17. The method according to claim 1 wherein substantially no heat transferred is transferred to the fluid to be heated by cooling of the condensed liquid.
18. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
- and causing boiling of the liquid in the evaporation section and flow of the vapor from the evaporation section to carry non-vapor additives in the liquid in the evaporation section into the conduit with the vapor.
19. The method according to claim 18 wherein the conduit is arranged relative to the evaporation section such that boiling of the liquid in the evaporation section does not cause liquid to bridge the conduit so as to act as a bubble pump.
20. The method according to claim 18 wherein the conduit is arranged relative to the evaporation section such that the velocity of the vapor is greater than 500 ft/sec.
21. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
- wherein the system is at least partly evacuated prior to start up such that during steady state operation the pressure in the system is less than 15 psi above atmospheric pressure.
22. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
- wherein the total volume of liquid in the system is less than 43.5 litres or 1.5 cu ft.
23. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
- wherein flow around the loop is biased in one direction by a head created in part by a pump;
- and wherein there is provided a viewing port for viewing passage of vapor from the evaporation section;
- and wherein the operation of the process is controlled by varying the flow rate of the pump while viewing passage of vapor from the evaporation section so as to ensure passage substantially wholly of vapor with a minimal amount of liquid.
24. A method for transferring heat from a combustion heat source to a fluid to be heated comprising:
- providing a combustion heat source;
- providing a fluid to be heated at a position spaced from the heat source;
- providing a closed system including at least one conduit;
- providing an evaporation section of the closed system at the heat source;
- providing a condensation section of the closed system in the fluid to be heated;
- providing a heat transfer fluid medium within the closed system having a temperature of boiling from liquid to vapor such that heat from the heat source causes the liquid to boil to form a vapor in the evaporation section and such that release of heat from the condensation section to the fluid to be heated causes the vapor to condense to liquid in the condensation section;
- the at least one conduit forming a loop extending from the evaporation section through the condensation section and back to the evaporation section so as to conduct the heat transfer fluid medium from the evaporation section to the condensation section and back to the evaporation section;
- applying heat energy to the heat transfer medium by the heat source at the vaporizer section thermal energy causes expansion of volume due to a change of state;
- wherein flow around the loop is biased in one direction by a head created in part by a pump;
- and wherein the pump is a positive displacement pump so that the rate of flow is directionally proportional to a rotation rate of the pump.
25. The method according to claim 24 wherein the condensation section is arranged at a height above the pump such that a column of liquid generated thereby generates a pressure greater than a required pressure for optimum operation and wherein the positive displacement pump generates an outlet pressure below that of the column.
Type: Application
Filed: Sep 13, 2007
Publication Date: Jul 24, 2008
Inventor: Jack Lange (Winnipeg)
Application Number: 11/854,602
International Classification: F22B 1/02 (20060101);
