Online proceedings - EDA Publishing Association
Online proceedings - EDA Publishing Association
Online proceedings - EDA Publishing Association
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
7-9 October 2009, Leuven, Belgium<br />
Thermal matching of a thermoelectric energy<br />
harvester with the environment and its application in<br />
wearable self-powered wireless medical sensors<br />
V. Leonov 1 , P. Fiorini 1 , T. Torfs 1 , R. J. M. Vullers 2 , C. Van Hoof 1<br />
1<br />
IMEC<br />
Kapeldreef 75<br />
3010 Leuven, Belgium<br />
2<br />
Holst Centre / IMEC<br />
High Tech Campus 31<br />
Eindhoven 5656 AE, The Netherlands<br />
Abstract-In this work, we discuss why classical thermoelectric<br />
theory is not enough to design an optimized energy harvester.<br />
Then, the general conditions are defined, which are required to<br />
make a thermoelectric converter effective in such application.<br />
The necessity of the work has been prompted by the fact that<br />
while modeling the harvesters neither the constant temperature<br />
difference, nor the heat flow cannot be assumed. We show that<br />
simple equations obtained using electro-thermal analogy allow<br />
optimization of energy harvesters to reach their top<br />
performance characteristics. Thermal matching in MEMS<br />
thermopiles is discussed then. The examples of application<br />
thermally matched thermopiles for powering state-of-the-art<br />
wearable wireless sensors are discussed in the end.<br />
I. INTRODUCTION<br />
Powering wireless autonomous sensors by using energy<br />
harvesters could move such devices into mass production.<br />
Batteries and wiring are excluded as unrealistic ways. One<br />
thousand wireless sensors per each person is a current vision<br />
of the future wireless sensor network called “ambient<br />
intelligence”. These should be self-powered, preferably<br />
using photovoltaic cells. The thermoelectric conversion of<br />
wasted heat from low temperature sources however is the<br />
best way to provide power autonomy to the devices in<br />
locations, where no daylight and indoor illumination take<br />
place. However, because of energy saving reasons, wasted<br />
heat flows are usually minimized with the use of thermally<br />
isolating materials. Thermoelectric conversion of waste heat<br />
is complicated by the high thermal resistance of the heat sink<br />
(air) and, frequently, of the heat source (e.g., walls of<br />
buildings, plastic pipes, or living beings). The remaining<br />
heat flows and temperature differences available for energy<br />
harvesting are therefore relatively small. However, these<br />
wasted heat flows can be used for eliminating the need of<br />
primary batteries in most of autonomous devices placed<br />
inside buildings, machinery, or in closed compartments, and<br />
forming smart self-organizing autonomous networks. This<br />
paper discusses the principles of designing thermoelectric<br />
generators optimized for energy harvesting on lowtemperature<br />
sources of waste heat. As a proof of concept,<br />
the examples of fully self-powered wearable medical devices<br />
are designed, fabricated and briefly described.<br />
II. THERMOELECTRIC THEORY AND OPTIMIZED<br />
THERMOPILE<br />
In the thermoelectric theory, the optimization of a<br />
thermopile in power generation mode is discussed for two<br />
basic regimes of operation: (i) the heat flow through the<br />
thermopile, W, is constant, i.e., independent of its thermal<br />
resistance R tp<br />
and (ii) the temperature drop on the thermopile,<br />
ΔT, is constant, solid lines in Figs. 1a and 1b, respectively.<br />
There are also the second-order effects that discussed in the<br />
theory. These are Joule heating of thermopiles due to<br />
generated current and Peltier effect. However, these effects<br />
are minor and become important only in case of hightemperature<br />
operation (more than 100°C) and low serial<br />
thermal resistance of the environment, R env , therefore in the<br />
following discussion of energy harvesters we omit these<br />
effects for the sake of simplicity. The power generated by a<br />
thermopile on the matched load in this case is<br />
P = V 2 /4r el = α 2 ΔT 2 /4r el , (1)<br />
Fig. 1. Two regimes of a thermopile operation in power generation mode:<br />
(a) constant heat flow; R tp > R env .<br />
©<strong>EDA</strong> <strong>Publishing</strong>/THERMINIC 2009 95<br />
ISBN: 978-2-35500-010-2