1. Field of the Invention
The present invention relates to apparatus and methods for converting heat energy into mechanical energy.
2. Description of the Prior Art
The law of conservation of energy states that energy may be transformed from one kind to another, but it cannot be created or destroyed. Further, energy is defined as the ability to do work. Mechanical energy is more convenient for doing work of most kinds, various apparatus for converting heat energy into mechanical energy have been developed. These are generally called “heat engines.”
The steam engine is an engine in which water is superheated to create high pressure steam, that in turn pressurizes a cylinder containing a piston. The pressure causes the displacement of the piston. The axial motion of the piston translates its energy to a crankshaft that rotates as a result of the piston motion. This results in mechanical work.
The steam turbine also utilizes super heated water vapor to generate mechanical work. The high pressure steam in this system applies a force normal to the turbine fins attached to a rotating armature. Hence the applied force results in the armature rotating.
The Stirling engine is a well known heat engine operating in two general modes during a cycle. In the first mode, the expansion cycle heats the internal gas via an external heat source. The gas expands and moves a first piston. In the second mode, the gas is cooled, retracting a second piston.
According to the ideal gas law, PV=nRT, where P is pressure, V is volume, n is the number of moles of gas, R is a gas constant and T is temperature. So temperature is proportional to pressure time volumes. Hence, when a gas is heated it expands if possible, and otherwise the pressure increases.
The Stirling cycle has four phases, Isothermal Compression, Constant Volume Heating, Isothermal Expansion, and Constant Volume Cooling (these phases are somewhat simplified for this explanation). Isothermal Compression occurs as heat is transferred from the hot gas 116 to a cold sink, and the gas compresses, drawing piston 108 up from its full capacity. In the present case, the heat is removed by cooler 104, perhaps by simply conducting the heat away from the engine. Some heat is also stored in the regenerator 114 (which might be a network of wires or the like).
Once cold piston 108 is in its intermediate position, the Constant Volume Heating phase begins. Cold piston 108 moves up to its minimum capacity position and then hot piston 106 moves down to an intermediate position. Gas 116 hence passes through regenerator 114 and is heated. Since volume remains the same and the temperature of the gas increases, pressure goes up.
In the third phase, Isothermal Expansion, heater 102 heats the gas. It expands and moves hot piston 106 down to its full capacity position. In the Constant Volume Heating phase, hot piston 106 moves up to its minimum capacity position and then cold piston 108 moves down to its minimum capacity position, again passing gas 116 through regenerator 114. Heat is passed from the gas to the regenerator, so its pressure and volume both remain constant.
Practical Stirling engines have been built. For example, some submarines use Stirling engines. A recent example of a Stirling engine is described in U.S. patent application Ser. No. 6,062,023 to Kerwin et al. Known Stirling engines generally require an extremely hot heat source (600 to 800 degrees Celsius) and a temperature gradient of at least 400° C. The gases used in these engines, for example Nitrogen and Carbon Dioxide are in the gas phase at all times. Thus, current Stirling engines operate at impractically high temperatures and do not take advantage of the liquid phase of the working gas.
A need remains in the art for improved heat engines that operate at more practical temperatures, do not require extreme heat gradients, and utilize the liquid phase of the refrigerant.
It is an object of the present invention to provide an improved heat engine.
The heat engine of the present invention operates at practical temperatures and utilizes the liquid phase of the refrigerant. It does not require extreme heat gradients. In addition, the structure of the present heat engine is an improvement.
A heat engine according to the present invention utilizes a liquid refrigerant and a hot thermal fluid to convert heat into mechanical work. The heat engine comprises (1) an expansion chamber having a piston disposed to execute strokes within a cylinder and a thermal fluid jacket containing the hot thermal fluid and disposed around the cylinder, wherein the expansion chamber heats the liquid refrigerant via heat transfer from the hot thermal fluid in the thermal fluid jacket and allows the refrigerant to expand, the expansion causing the piston to execute strokes and thereby generate work, (2) a dynamic throttling valve for injecting liquid refrigerant into the cylinder adjacent to the piston, wherein the valve injects a minimal flow of liquid refrigerant at the beginning of the piston stroke and a maximal flow as the piston stroke continues, (3) a pressure injector for injecting the liquid refrigerant into dynamic throttling valve under pressure, (4) a compressor for compressing the expanded gas refrigerant from the expansion chamber, and (5) a condenser for returning the compressed gas refrigerant from the compressor to a liquid state for use by the pressure injector.
The thermal fluid might be hot water.
In one preferred embodiment, two expansion chambers are used, and the piston in the second expansion chamber reciprocates with respect to the first. As a feature, the pressure injector includes a magnetically assisted hydraulic element having two paths for the refrigerant with an input three way switch and an output three way switch to channel the refrigerant through paths and increase pressure.
The dynamic throttling valve may comprise a tapered pin at the end of the piston fitting into a tapered opening in the injector and a concave area on the piston surrounding the pin for allowing the minimal flow of refrigerant at the beginning of the stroke.
The fluid jacket preferably includes heat transfer bars and heat transfer rings to increase turbulent flow and maximize heat transfer. The heat transfer bars also extend into the cylinder to transfer heat to the refrigerant. Heat transfer fins extend from the fluid jacket into the cylinder to transfer heat to the refrigerant.
Input hot fluid inlet tubes inject the hot fluid into the fluid jacket and cold fluid outlet tubes remove the cold fluid from the jacket after it has warmed the refrigerant.
Preferably the heat transfer rings are toothed and the fluid passes through the teeth in a turbulent manner. The teeth on a ring are offset from teeth on an adjacent ring. Heat transfer bars pass through teeth on one or more rings. Also, heat transfer bars pass between the heat transfer fins.
A listing of parts and reference numbers is helpful in understanding the present invention.
Note that the term “refrigerant” is used herein to designate not only traditional refrigerants such as R410-A, freon and the like, but also any suitable substance that has a cooling effect when converted from a liquid state to a gas state.
The heart of heat engine 200 is reciprocating expansion chamber 202, which converts heat from hot fluid 212 into mechanical work 214. Reciprocating expansion chamber 202 is shown in more detail in
One very beneficial use of heat engine 200 is in the internal combustion engine of a car (not shown). Hot fluid (for example hot water) 212 can be generated by the car engine, and cold fluid 216 may in turn be used to cool the engine. Hence, the only extra element the engine needs to provide is the work to compress and condense refrigerant 210. As refrigerant 210 is preferably R410-A or the like, this is easily achieved.
The purpose of the magnetic assist on the high pressure injector is to increase the fluid injection pressure and rate of injection of the fluid into the cylinder. Increasing the fluid pressure helps to ensure that the refrigerant remains a liquid as it is injected, and increasing the rate of injection increases the work done by the engine. Increasing or decreasing the power to the magnetic assist also provides a throttling function.
In use, core 310 is alternatively pulled toward coil 306 and coil 308. When core 310 moves towards coil 306, it increases the pressure in branch A of the injector. When core 310 moves towards coil 308, it increases the pressure in branch B of the injector. Control block 312 energizes coil 306 to attract core 310 when switch a and b are open. Hence, control block 312 energizes coil 308 to attract core 310 when switch 302a and switch 304b are open. Control block 312 energizes coil 306 to attract core 310 when switch 302b and switch 304a are open.
In the heat engine of the present invention, heat is transferred to a working gas, or refrigerant, via conduction through the cylinder head and walls. The present invention is structured to maximize the heat transfer. The preferred embodiment of
Equation for heat transfer due to conduction:
Q/t−kA(Thot−Tcold
Where:
Q=heat transferred in time=t
k=thermal conductivity of the conductor
A=area
T=temperature
d=thickness of conductor
Thot=temperature of the outer surface of tabbed heat ring internal to fluid transport jacket
Tcold
Equations for heat transfer due to forced convection:
Q=hA(TS−T∞)
Where:
Q=Loss of Thermal energy
h=Heat transfer coefficient
TS=Surface temperature
T∞=Fluid ambient temperature
A=Area of heat element
The relationship for the forced convection heat transfer coefficient (h) for a cylinder in cross-flow follows a non-dimensional correlation.
NNU=C*(Re)m*(Pr)n
Where:
NNU=Nusselt number=(hd)/κ
C=Constant
Pr=Prandtl number=(ρVd)/μ
m=Coefficient
n=Coefficient
h=Heat transfer coefficient
d=Sensor diameter
κ=Thermal conductivity of fluid
μ=Fluid viscosity
Cp=Specific heat of the fluid
ρ=Fluid density
V=Fluid velocity
ρV=Mass velocity
The Prandtl number for gases is approximately 0.7 and does not vary much with temperature so it is generally dropped from the equations. The heat transfer coefficient (h) is:
h=(Cκ/d)*(ρVd/μ)m
In order to initially keep the refrigerant in a liquid state as it is being injected, the refrigerant is injected into a high pressure and thermally isolated chamber 2. Refer to the left hand cylinder diagram in
As the refrigerant continues to be heated, the pressure reaches its maximum, and then decreases in proportion to the increasing volume caused by the piston extending. Thus, the pressure is reduced by the time the piston is fully extended. See the right hand cylinder diagram in
In operation, refrigerant 210 enters injector 3 from high pressure injector 208 (see
As piston 31 moves back upward, the vaporized compound gas refrigerant 210, now in its low pressure, hot gas phase 218, exits gas exhaust ports 20.
Returning to
This figure also shows the locations and spacing of gas exhaust ports 20, hot fluid inlet tubes 25, and cold fluid outlet tubes 26. Cylinder lower ring 29 and cylinder lower ring seal 28 are positions at the bottom of water jacket 27. Piston 31 comprises piston pin 33, piston seal 30, piston lower seal capture ring 32, and piston connecting rod 34. When the cylinder assembly is put together, jet 16 is inside of cylinder 24, which is inside the top portion of cylinder body 19. Water jacket 27 is outside of cylinder body 19. Piston 31 is inside cylinder body 19, with pin 33 fitted to the inside of jet 16 when the piston is in the uppermost position.
Those skilled in the art will appreciate that various modifications to the exemplary embodiments are within the scope of the patent.
Number | Name | Date | Kind |
---|---|---|---|
4230024 | Becker | Oct 1980 | A |
4918937 | Fineblum | Apr 1990 | A |
5061391 | Scaringe et al. | Oct 1991 | A |
6062023 | Kerwin et al. | May 2000 | A |
6694731 | Kamen et al. | Feb 2004 | B2 |
Number | Date | Country | |
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20060059906 A1 | Mar 2006 | US |