This invention pertains to the use of thermoelectric devices in combination with hot fluid streams produced by an operating internal combustion engine. The high temperature sides of the devices are in heat transfer contact with, for example, the hot engine exhaust stream and the low temperature sides are in heat transfer contact with ambient air so as to produce electrical power. More specifically this invention pertains to the use of light weight, high thermal conductivity foam materials in contact with the high temperature sides and/or low temperature sides of the devices to increase their output of electrical power.
Improved thermal management is a leading research objective in many fields. For example, approximately 30% of the energy contained in automotive fuel may be lost to the environment as thermal energy in the exhaust gas of an internal combustion engine. It is desirable to recover a portion of this waste heat in the form of electrical power to be used in the automobile. The recovery of waste heat could reduce the power demand on the alternator of an automobile and result in improved fuel efficiency. Many aerospace and electronic applications are also seeking to improve thermal management.
Thermoelectric devices convert thermal energy into electrical energy by means of a temperature gradient. These devices have no moving parts. Therefore, thermoelectric devices are amenable to relatively low production costs in high volume and have a potential for high reliability. Thermoelectric devices may be used in recovering waste thermal energy of internal combustion engine based vehicles, for example to generate electrical power using the hot exhaust gas stream. In order to maximize the temperature gradient across the thermoelectric materials to maximize the electrical power output, it is important to have efficient heat exchangers at the hot and the cold sides of the thermoelectric devices. Therefore, there is a need for improved heat exchanger materials and design.
A thermoelectric module may comprise two or more elements of n-type and p-type doped semiconductor material(s) that are connected electrically in series and thermally in parallel. These thermoelectric elements and their electrical interconnects often are mounted between two ceramic substrates. The thermoelectric elements are mounted with one or more junctions at a high temperature side of the module and with one or more junctions at a lower temperature side of the module. The substrates hold the overall structure together and electrically insulate individual elements from each other and from external mounting surfaces. By way of example, many thermoelectric modules range in size from approximately 2.5 to 50 mm2 in area and 2.5 to 5 mm in height. In general, when the module experiences a larger temperature difference between its hot and cold junctions it produces a larger electrical output.
In many automotive vehicles a hydrocarbon fueled internal combustion engine produces a hot exhaust gas that is released through an exhaust pipe to the atmosphere. The hot exhaust gas provides a relatively high temperature source that might be exploited at the high temperature junctions of one or more thermoelectric devices. A grouping of such thermoelectric devices may, for example, be located along an exhaust gas conduit with the high temperature sides of the devices in heat exchange contact with the hot flowing gas stream. Similarly, the engine is typically cooled using a coolant liquid that is circulated within the engine and heated by it. The coolant is then circulated through a heat exchanger to release its heat to ambient air. Although a liquid coolant is at a lower temperature than combustion exhaust gas, the coolant also offers a relatively high temperature source for operation of a grouping of thermoelectric devices. In both situations, ambient air may provide the low temperature side of an interposed thermoelectric device. In order to improve the operating efficiency of a thermoelectric system that uses such a high temperature source, it is necessary to improve heat transfer at hot and cold junctions of the thermoelectric device. Such groupings or combinations of thermoelectric power generating devices may be connected for electrical current series flow and/or electrical current parallel flow to conduct generated electrical power to a battery for storage or to an electrical power consuming device on the vehicle or near a stationary engine.
This invention provides a combination of (i) a light weight, open pore, foam material with very high thermal conductivity and (ii) a thermoelectric device for improved utilization of a hot fluid stream associated with a vehicle engine (and/or a relatively cool stream of ambient air). This combination is devised to produce a high electrical output for powering an electrical device on a vehicle.
In one embodiment the high thermal conductivity foam may be carbon foam, a material formed from graphite fibers. Such a carbon material may be produced from pitch. The graphitic foam body or layer is used to increase heat transfer from a hot engine exhaust stream or a hot engine coolant stream to the high temperature side of a thermoelectric device. The foam body is designed and used to increase the temperature of the high temperature side. In another embodiment, a graphitic foam body may be used to improve heat transfer between ambient air and the low temperature side of a thermoelectric device. Again, the foam body is designed and used to decrease the temperature of the low temperature side of the thermoelectric.
Thus, the foam is used to increase the temperature difference between the hot and cold sides of the thermoelectric device so as to increase the effectiveness of the device. The high open pores of the foam permit, for example, at least some exhaust gas flow through it for improved heat transfer to the hot side of the thermoelectric device. And, likewise, the foam may permit internal ambient air flow for improved heat transfer from the thermoelectric and a lower temperature at its cold side.
The low density of the foam allows the design of effective heat transfer paths to and from the thermoelectric device(s) without adding significant weight to a vehicle.
Other objects and advantages of the invention will be more apparent from a description of illustrative embodiments of the invention which follows in this specification.
One embodiment includes a thermoelectric system including high conductivity foam to convert waste thermal energy captured from a combustion engine into electrical power. The waste thermal energy may be captured from exhaust gases or coolant from the internal combustion engine. The waste thermal energy may include any thermal energy which is available after the internal combustion engine of a vehicle has performed its normal functions, such as, for example, heat remaining in the exhaust gases or heat transferred to a liquid coolant.
In this embodiment thermoelectric device or module 10 comprises a plurality of elements of complementary thermoelectric materials indicated generally as 22 in
In the embodiment of
The complementary pairs of thermoelectric elements are in heat transfer relationship with their respective high temperature sides 12 and the low temperature sides 14. The temperature gradient between the hot side 12 and the cold side 14 causes the electrons in the thermoelectric element pairs to move away from the hot side 12 and toward the cold side 14. The electrons jump to a higher energy state by absorbing thermal energy at the high temperature side 12. The electrons flow from each pairing of n-type semiconductor N to an adjacent p-type semiconductor P through the electrical connector 30, dropping to a lower energy state and releasing energy through the low temperature side 14. An electric current is thus generated in each thermoelectric module in a direction from the n-type N to the p-type semiconductor P. As shown in
The electrical power generation is increased by increasing the temperature difference between the hot side 12 and the cold side 14, and by using thermoelectric materials 22 with larger ZT values, where ZT is the thermoelectric figure of merit. ZT is a dimensionless parameter and embodies the relationship of conversion efficiency (i.e., thermal energy to electrical energy) to material properties. ZT is conventionally defined as: ZT=S2σT/κ, where S, σ, κ, T are the Seebeck coefficient, electrical conductivity, thermal conductivity, and absolute temperature, respectively. The larger the ZT, the higher the conversion efficiency of the thermoelectric material. An efficient thermoelectric material should have a large Seebeck coefficient, high electrical conductivity, and low thermal conductivity. The thermoelectric material 22 may be, for example but not limited to, a skutterudite, Bi2Te3-based alloy, Zn4Sb3, PbSeTe/PbTe quantum dot superlattice, Bi2Te3/Sb2Te3 superlattice, AgPb18SbTe20, PbTe-based alloy, SiGe-based alloy, or other high efficiency thermoelectric material. The thermoelectric material 22 may be doped with impurities to form the n-type material and may be doped with impurities to form the p-type material.
In one embodiment, the source of heat that is transferred to the thermoelectric material to generate electricity is a hydrocarbon internal combustion engine (such as diesel, gasoline, and the like) that generates heated effluent. One example of heated effluent is heated exhaust gas. Another example of heated effluent is liquid coolant in a radiator. Thus, the thermoelectric device 10 may function to cool the exhaust stream or liquid coolant and convert thermal energy into electrical energy.
According to one embodiment, the temperature gradient between the hot side 12 and the cold side 14 may be increased by using a high conductivity foam material (shown in
Such carbon foam has extremely high thermal diffusivity and conductivity. For example, the room temperature bulk thermal conductivity of the carbon foam may range from 50 W/m·K to over 100 W/m·K. The maximum bulk thermal conductivity reported is 175 W/m·K. When weight is considered, the specific thermal conductivity of the carbon foam may be more than four times greater than the specific thermal conductivity of copper. The carbon foam also has thermal conductivity equivalent to aluminum alloys at the same volume and ⅕ of the weight of the carbon foam. The cell walls of the carbon foam are made of highly oriented graphite planes, or ligaments, similar to high performance carbon fibers. The room temperature thermal conductivity of the ligaments within the carbon foam's cell walls may be greater than 1700 W/m·K.
The porous structure and light weight nature of the carbon foam make it possible to form a direct heat exchanger. The open porous structure of the carbon foam results in a specific surface area of greater than 4 m2/g, which is more than 100 times greater than that of typical heat exchangers. The size of the pores in the carbon foam may be about 50 to 300 microns. The carbon foam also has a low density of 0.2 to 0.7 g/cm3. The unique combination of material properties also result in excellent acoustic absorption and sound damping performance (low noise). In fact, a finned heat sink made from carbon foam can be up to 3 times more efficient than an aluminum heat sink of the same volume, yet at ⅕ the weight (effectively 5 times more efficient per gram of heat sink). The maximum operating temperature of the carbon foam is 500° C. in air.
Typically, the exhaust gas from an internal combustion engine exits the engine exhaust manifold and enters an exhaust pipe 34. The exhaust gas stream exiting the engine may have an average temperature of 500-650 degrees Celsius. The exhaust pipe 34 may include a catalytic converter, at least one silencer, and a tailpipe where the gas exits into the ambient air. The thermoelectric heat recovery system may be positioned along the exhaust pipe between the catalytic converter and the tailpipe. The thermoelectric heat recovery system 32 converts heat from the exhaust gas stream into electrical power. In one embodiment, the thermoelectric heat recovery system may extend for one to two feet along the exhaust pipe 34.
The thermoelectric heat recovery system 32 includes the thermoelectric device 110 positioned and secured between the exhaust pipe 34 and a casing or enclosure pipe 36. In one embodiment, the enclosure pipe 36 may be stainless steel. In this embodiment, the exhaust pipe 34 and the enclosure pipe 36 are round in cross-section. The exhaust pipe may be filled with porous graphite foam 38. The size of the pipe and the length of the foam 38 in the pipe 34 are devised to permit suitable exhaust gas flow without excessive back pressure. The carbon foam 38 may include passages 41 extending the length of the carbon foam 38 in the pipe 34. The exhaust gas flows through the highly thermally conductive foam and/or passages 41 in the foam to increase the temperature at the inside surface of exhaust pipe 34. The passages 41 may contribute to the maintenance of desired back pressure and better heat exchange efficiency. In various embodiments, the passages 41 may include through-thickness patterns that can be machined, carved, or cut on the carbon foam block. The passages 41 may be of any suitable shape and dimension. The passages 41 may be, for example, circular in cross-section with varying diameters. Or the passages 41 may be, for example, slits or lines that are parallel or crossing.
Any suitable number of semiconductor pairs 124 (four shown in
The high conductivity foam material may be in the form of a body or layer, and may be used as a heat exchanger on the hot side and/or the cold side of the thermoelectric system 32. The foam material 38 in exhaust pipe 34 is used to increase heat transfer from a hot stream to the high temperature side 12 of the thermoelectric device 10. The foam material 38 increases the temperature of the high temperature side 12. In another embodiment, like foam material 39 may be used to improve thermal conductivity between a cold fluid, for example ambient air, and the low temperature side 14 of the thermoelectric device 10. In
Referring to
The electrical power generated by the thermoelectric heat recovery systems 32, 232, or 332 may be stored in an energy storage device. In one embodiment, the thermoelectric heat recovery system 32, 232, or 332 may be electrically connected to a thermoelectric power control system which controls the flow of electrical power from the system 32, 232, or 332 to electric power controls. An energy storage device, such as a battery or capacitors, for example, may be electrically connected to the electric power controls for the storage of electrical power generated by the thermoelectric heat recovery system 32, 232, or 332. The electrical power may then be used in the vehicle.
It is further understood that the invention encompasses thermoelectric heat recovery systems 32, 232, and 332 that recover heat released from any vehicle application. The term “vehicle” encompasses all devices and structures for transporting persons or things, including automobiles, cars, trucks, buses, motorcycles, locomotives, ships, airplanes, aerospace equipment, and the like.
The practice of the invention has been illustrated with certain embodiments but the scope of the invention is not limited to such examples.
The United States Government has rights in this invention pursuant to Cooperative Agreement No. DE-FC26-04NT42278 awarded by the United States Department of Energy. The United States Government has rights in this invention pursuant to contract no. DE-AC05-00OR22725 between the United States Department of Energy and UT-Battelle, LLC.