PROPULSION AND POWER FOR THE TWENTY-FIRST CENTURY


Thermoacoustic engines - Thermopneumatic engines - What are they?   

Thermoacoustics is the term for soundwaves generated by heat. Thermopneumatics is control of thermally-generated pressure in gases.  The latter term is typically used in describing MEMS devices.  FRG has developed a hybrid engine, using both, that develops high energy conversion efficiency.

One might accurately say that all heat engines, like those in automobiles and jet planes, generate sound and pressure from heat. Internal combustion (IC) engines burn fuel and generate combustion noises that rumble or roar, depending on the type of engine.  Noise and pressure are by-products of the engines' energy conversion process.  The pressure component usually performs the work in the system, while the acoustic signature is an indicator of system resonance, which  is related to efficiency. 

Typical internal-combustion (IC) engines burn fuel mixed with air to produce hot, expanding gases that drive pistons and turbines directly. A Thermoacoustic Cycle (TAC) engine, however, is a different animal altogether. The usual arrangement consists of a closed, resonant chamber containing two or more heat exchangers and a working medium--generally a dry gas under pressure. Heat from outside the resonator is injected into the internal working fluid via the hot-side heat exchanger (HXh), causing localized pockets of increased pressure. At the other end the resonator, a coolant circulating through the cold-side heat exchanger (HXc) removes the heat energy from the working fluid, causing a reduction in pressure.

Thermopneumatic Cycle (TPC) engines use an external heat source to expand an internal dry gas (working fluid)  to drive a piston or diaphragm.  Stirling Cycle engines use a similar process, but in the Stirling Cycle engine the working fluid is scavenged by mechanical pistons and physically moved between heat exchangers in order to effect thermal expansion and contraction.  Our thermopneumatic engine uses traveling pressure waves, moving through a static gas, to transfer energy from point-to-point.  The result is an engine capable of three orders of magnitude greater power density than a typical thermoacoustic engine, and almost double that of a Stirling engine, without the mechanical complexity.  The FRG engine is lightweight, powerful, economical to make.

In accordance with Boyle's and Charles' Laws, a confined gas will increase in pressure by 1/273rd for each degree of increase in Celsius temperature. If the resonator cavity is pressurized to twenty atmospheres static pressure to begin with (Ps), and the temperature of the gas is increased by 600 Co, the peak dynamic pressure (Pd) will be:

Pd = Ps / 273 * T + Ps
Pd = 20 atm / 273 * 600 + 20 atm
Pd = 64 atm

Neglecting gas losses and thermal reactance in the materials of the resonator, the dynamic (fluctuating) pressure will be:

64 atm - 20 atm = 44 atm

The hot and cold heat exchangers respectively are HXh and HXc.  HXh is swept periodically by a traveling wave that brings a cooler parcel of gas into contact with the hot internal surface of the heat exchanger (HXh) and expands it explosively to produce an expanding pressure wave.  This periodic "cooling" of the HXh surface
causes HXh to act as a "thermal capacitor" (Ct).  HXh is Ct. The properties of Ct is the heart of the FRG engine. 

Ct acts something like a transistor oscillator, in that it teeters back and forth thermally, taking up energy from the external heat source, then giving it up to the internal working fluid.  The effect is that of an acoust pump that periodically pushes in a cool parcel of gas, expands it explosively, and exhausts it into the cold-side heat exchanger (HXc).  The timing of this periodic "push" is accomplished by tailoring the thermal mass and conductivity of Ct to conduct thermal energy into the working fluid at a specific rate. This permits resonator design variations not restricted by geometry. Energy acquisition and decay in Ct is illustrated below:

The result is a resonator, or engine, with a rapidly fluctuating pressure gradient and no moving parts. This oscillating pressure gradient can tapped off to drive a piston, and a linear alternator that produces electricity.

For example, a pressure swing of 44 atm (45 kg/cm2) is a significant force, and when it occurs five hundred times per second, the potential power output is quite high. For example, at this dynamic pressure, a diaphragm 10 centimeters in diameter has a surface area of 78 sq.cm.  This tympanic diaphragm, with a travel of only one millimeter (0.001 meter), operating at a frequency of five hundred Hz, will produce:

45 kg/cm2 * 78 cm2 *.001 m * 500 = 1,766 kg-m/sec =  (1,766 * 9.8/1000) = 17.3 kilowatts = 23 horsepower

Extraordinary performance, from an engine the size of a hockey puck.

The FRG engine is attractive for several reasons. It has only one moving part, and the overall part count is low.  That means low manufacturing costs. The engine can be adapted to operate over a wide temperature range, so energy recover from waste heat in industrial processes and cogeneration power plants, and even power generation from resources such as solar energy and moderate thermoclines in lakes and brine ponds, becomes economically viable.

The FRG engine is a Carnot engine, in that overall efficiency is governed primarily by the temperature delta across its isothermal heat exchangers, HXh and HXc, i.e.:

n = (T1 - T2) / T1

Low production costs mean that lower operating efficiencies can be tolerated, and the installed cost per Watt of generating capacity remains low.   Because efficiency is not necessarily a cost barrier, FRG engines may permit economical harvesting of low temperature heat sources that are not economically viable using other technologies. For instance, we intend to develop low temperature biomedical applications in which miniaturized engines will generate power for medical prostheses from body heat, at single-digit efficiencies. These microminiature (MEMS) devices are called MEMS-TARs (Micro-miniature Electro-mechanical Systems-Thermoacoustic Resonator). Hearing aids, pacemakers, baby crib monitors, personal security alarms for women and children, physiological monitors for policemen, firemen, soldiers and hospital outpatients, in the form of a ring or wristwatch, will all operate indefinitely, and without batteries, acquiring energy through contact with the body. Since they will never require maintenance, they may even be implanted permanently inside the body.  One design conception illustrating the nominal size of these microchip scale devices is illustrated below:


Applications are almost limitless. The heat generated by the CPU in a laptop computer can be used by the MEMS-TAR to recharge the battery, extending operating time between charges. Automobile exhaust heat can be used to charge the vehicle battery, doing away with the alternator and reducing fuel consumption and air pollution. Passenger planes can generate power for aircraft systems from waste engine heat, saving fuel. Pets and wildlife can be monitored via implanted MEMS-TAR powered locator beacons.

Copyright 2009 by Oscar L. Fellows
Fellows Research Group, Inc.

More information on TARs and TAC engines can be found on FRG's website at:

http://www.io.com/~frg

e-mail FRG at: frg@io.com