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Thermal Matching of a Thermoelectric Energy Scavenger with the ...

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<strong>the</strong> wrist, has usually similar or less thickness, <strong>the</strong>refore, <strong>the</strong>radiator can be moved out <strong>of</strong> <strong>the</strong> convection layer and <strong>the</strong>heat transfer into <strong>the</strong> air improves.Second, if using small-size <strong>the</strong>rmopiles, like, e.g.,MEMS <strong>the</strong>rmopiles, <strong>the</strong> TEG becomes almost empty [3], sothat <strong>the</strong> plate-to-plate radiation heat exchange can beeffectively suppressed using <strong>the</strong> plates <strong>with</strong> low emissioncoefficient.Third, proper positioning <strong>of</strong> <strong>the</strong> TEG on human being<strong>of</strong>fers much lower <strong>the</strong>rmal resistance <strong>of</strong> <strong>the</strong> body than itsaverage value [2, 3].Forth, a small radiator instead <strong>of</strong> a cold plate effectivelyreduces <strong>the</strong> <strong>the</strong>rmal resistance <strong>of</strong> ambient air [2].Finally, <strong>the</strong> <strong>the</strong>rmal resistance <strong>of</strong> <strong>the</strong> body itself can bedecreased using a radiator as shown in [3] through changing<strong>the</strong> local heat flow in humans under <strong>the</strong> device.<strong>Thermal</strong> matching <strong>of</strong> MEMS <strong>the</strong>rmopilesThanks to <strong>the</strong> laws <strong>of</strong> scaling, small MEMS <strong>the</strong>rmopilesFigure 4. <strong>Matching</strong> <strong>of</strong> <strong>the</strong> MEMS TEG <strong>with</strong> <strong>the</strong> ambience(squares) and parallel matching <strong>of</strong> <strong>the</strong>rmopiles (circles) to<strong>the</strong> air in a TEG (similar to points 2-3 in Fig. 2).can be as effective as commercial <strong>the</strong>rmopiles. The rules <strong>of</strong>designing <strong>the</strong> TEG remain <strong>the</strong> same as discussed above. Atall <strong>the</strong>rmally conducting pillar, however, has to be added to<strong>the</strong> TEG for <strong>the</strong>rmal interconnection <strong>of</strong> <strong>the</strong> <strong>the</strong>rmopile chip<strong>with</strong> <strong>the</strong> well-separated plates [3]. Fig. 4 illustrates <strong>the</strong>rmalmatching <strong>of</strong> 3 µm-tall BiTe micromachined <strong>the</strong>rmopile <strong>with</strong>1 µm 2 leg cross section <strong>of</strong> <strong>the</strong> design reported in [4] in a3 cm × 3 cm TEG at a temperature <strong>of</strong> 22 °C. Taking intoaccount <strong>the</strong> helpful hints <strong>of</strong> <strong>the</strong> previous section, a pinfeaturedradiator [2] replaces <strong>the</strong> cold plate and provides a<strong>the</strong>rmal resistance in <strong>the</strong> human body <strong>of</strong> 200 cm 2 K/W.Numerical calculations show that even <strong>the</strong> TEG <strong>with</strong>one-stage 3 µm-tall <strong>the</strong>rmopile on humans, can beeffectively <strong>the</strong>rmally matched <strong>with</strong> <strong>the</strong> ambience, providingR TEG,0 = 1.4R amb,opt , which shows potential advantage <strong>of</strong> <strong>the</strong>MEMS <strong>the</strong>rmopiles for wearable devices as compared <strong>with</strong><strong>the</strong> existing industrial technology. Comparing <strong>the</strong> parallelmatching <strong>of</strong> two resistors composing <strong>the</strong> TEG, Fig. 1, onecan notice that <strong>the</strong> <strong>the</strong>rmal matching required (squares inFigs. 2, 4) calls for smaller <strong>the</strong>rmal resistance <strong>of</strong> <strong>the</strong> TEG incase <strong>of</strong> commercial <strong>the</strong>rmopiles, Fig. 2, and for <strong>the</strong> largerone in case <strong>of</strong> MEMS <strong>the</strong>rmopiles, Fig. 4. One can mentionthat despite very small height <strong>of</strong> <strong>the</strong> micromachined<strong>the</strong>rmopile, a power exceeding 16 µW/cm 2 can be obtained.<strong>Thermal</strong> matching in wearable devices <strong>of</strong> tomorrowApplication <strong>of</strong> <strong>the</strong> <strong>the</strong>rmal matching for designing <strong>the</strong>TEGs <strong>with</strong> different types <strong>of</strong> <strong>the</strong>rmopiles gives <strong>the</strong> limit forpower generation on human beings equal to 30 µW/cm 2 (on24-hour average) at an ambient temperature <strong>of</strong> 22 °C and aZT <strong>of</strong> 1. The TEGs fabricated in 2005-2006, have alreadyclosely approached this limit producing 20 µW/cm 2 at a ZT<strong>of</strong> about 0.8 – 0.85.The modeling <strong>of</strong> advanced MEMS <strong>the</strong>rmopiles <strong>with</strong>large aspect ratio [5] shows that in order to make universalwearable <strong>the</strong>rmoelectric energy scavenger for all seasons,<strong>the</strong> <strong>the</strong>rmal matching must be performed for <strong>the</strong> airtemperatures very close to skin temperature, e.g., for 35 °C.The smaller lateral size <strong>of</strong> <strong>the</strong> <strong>the</strong>rmocouple legs is neededas compared <strong>with</strong> <strong>the</strong> TEG optimized to 22 °C, in addition,<strong>the</strong> number <strong>of</strong> <strong>the</strong>rmocouples must be more than double. TheTEG <strong>the</strong>n will produce over 2 V at an air temperature <strong>of</strong> 35°C which is more than enough to power advanced electroniccircuits. Therefore, wearable devices <strong>with</strong> such <strong>the</strong>rmopileswill be powered all year round. The o<strong>the</strong>r approach is to uselarge rechargeable Li cell to keep self-powered devicesworking when <strong>the</strong> temperature difference minimizes insummer time. Then, <strong>the</strong> matching is to be performed for atypical ambient temperature, e.g., to 22 °C. The <strong>the</strong>rmalmismatching in summer does not exceed about 10% because<strong>the</strong> <strong>the</strong>rmal resistance <strong>of</strong> <strong>the</strong> body decreases whileapproaching 36 °C air temperature. According to <strong>the</strong>modeling, this device still produces a power <strong>of</strong> 0.5 µW/cm 2at a voltage <strong>of</strong> 1.1 V at 35 °C, however, <strong>the</strong> powerproduction becomes only periodical <strong>with</strong>in <strong>the</strong> 35–37 °C; itstill occurs due to natural fluctuation <strong>of</strong> <strong>the</strong> air and skintemperatures in a real life.Conclusions<strong>Thermal</strong> matching <strong>of</strong> energy scavengers to <strong>the</strong> ambienceis required to maximize <strong>the</strong> generated power. It serves as a<strong>the</strong>rmal equivalent <strong>of</strong> electrical matching <strong>of</strong> a generator to itsload. The derived <strong>the</strong>rmal matching equations result in aspecific design <strong>of</strong> TEGs for autonomous devices, whichinclude radiator, multi-stage commercial <strong>the</strong>rmopiles or amicromachined <strong>the</strong>rmopile on a tall pillar, and at leastseveral millimeters separation in between <strong>the</strong> plates <strong>of</strong> <strong>the</strong>TEG. It is shown that <strong>the</strong> <strong>the</strong>rmal optimization is valid forany <strong>the</strong>rmopile irrespective <strong>of</strong> its particular design. Thedesign method is extensively tested in applications on man.In a moderate climate, a power <strong>of</strong> about ZT/30 mW/cm 2 onaverage can be reached. This value is a limit imposed by<strong>the</strong>rmal matching conditions and by personal acceptance <strong>of</strong><strong>the</strong> device on a body. The energy scavengers fabricated in2005-2006, which are <strong>the</strong>rmally matched to <strong>the</strong>environment, show power generation near <strong>the</strong> <strong>the</strong>oreticallimit.References1. Kishi, M., Nemoto, H., Hamao, T. et al, “Micro-<strong>Thermoelectric</strong>Modules and Their Application to Wristwatchesas an <strong>Energy</strong> Source”, Proc 18 th Int Conf on <strong>Thermoelectric</strong>s(ICT), Aug. 29-Sept. 2, 1999, pp. 301-307.2. Leonov, V., Torfs, T., Fiorini, P., Van Ho<strong>of</strong>, C,“<strong>Thermoelectric</strong> Converters <strong>of</strong> Human Warmth for

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