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Wake-up signals with the RF power supply provided by the external readout unit. 

Wake-up signals with the RF power supply provided by the external readout unit. 

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In this paper, an autonomous sensor system, with low-power electronics for radio-frequency (RF) communication, incorporating a thermoelectric energy-harvesting module for unattended operation is presented. A target application is proposed for temperature measurement of walled-in pipes. When the autonomous sensor is placed on the heat source, a ther...

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... R in is the internal electrical resistance of the TEG. The power density of the adopted TEG module is 4 μ W/mm 2 for a temperature difference Δ T of 5 ◦ C in matched-load conditions. The dc–dc converter TPS61200 is the used voltage boost (step-up) converter that switches on when the input voltage goes beyond 0.5 V, providing a regulated output voltage that is set to 2.1 V. The external readout unit consists of a read/write base station U2270B, which is able to supply power to the transponder driving the coil antenna and to demodulate the digital signal. The readout unit is supplied by a 5 V voltage supply. The operating voltage of the microcontroller is 5 V, and the bus frequency is 7.38 MHz. A timer unit is used to decode the demodulated signal, and the data collected are transferred to a personal computer using a serial communication interface. III. C HARACTERIZATION OF A UTONOMOUS S ENSOR S YSTEM The output voltage generated by the TEG as a function of the temperature difference applied was measured. The TEG characterization was performed by heating one side of the module by means of a heater, which was externally powered, while a heat sink was applied on the other side to maintain it at a lower temperature by using the setup described in [14]. The temperature difference Δ T between the two faces of the TEG was measured using two NTC thermistors, which were attached with thermoconductive grease. The output power generated by the TEG, which was measured under different load conditions and various applied temperature gradients, is shown in Fig. 2. As expected from (2), the output power has a maximum when R L matches R in , which, in our case, is about 8 Ω . The output voltage of the TEG was then measured versus the applied temperature difference Δ T in the range from 0 ◦ C to 13 ◦ C in both open-circuit and loaded conditions, which was reported as V G and V L , respectively. In the loaded condition, the dc–dc converter, temperature sensor, and microcontroller are powered by the TEG. The obtained experimental results are shown in Fig. 3, which reports both V G and V L as a function of the temperature difference Δ T . As expected from (1), the open-circuit output voltage V G and the temperature difference Δ T are directly proportional. When the temperature difference is lower than about 3 ◦ C, the TEG voltage is less than 0.3 V, and the dc–dc converter is off. In this case, there is no loading effect on the TEG, and the curves of V G and V L overlap. When Δ T goes beyond 4 ◦ C (“Intermediate phase”), the dc–dc converter attempts to switch on, sinking a comparatively high current that decreases the voltage V L . In this condition, the output voltage V CC of the dc–dc converter is lower than the set value of 2.1 V. When Δ T reaches a value of about 8.5 ◦ C and above, the dc–dc converter switches on completely, and its output voltage steadily goes to 2.1 V. The autonomous sensor has two different operational modes: measurement and data-saving mode, which is powered by the TEG module, and RF communication mode, which is powered by the magnetic field generated by the external readout unit. In Fig. 4, the main signals, which are the output voltage of the TEG module ( V L ) , the output voltage of the dc–dc converter ( V CC ) , and the microcontroller clock, are shown during the system wake-up due to the increase of the power-harvesting supply. In the initial time interval (“Start-up boost converter”), when V L exceeds 300 mV, the dc–dc converter begins to start up, and when V L exceeds 0.5 V, the dc–dc converter is completely on, generating a stable output voltage of 2.1 V. From this moment, the sensor and the microcontroller are powered, and the system works continuously as long as the temperature gradient is maintained. During the “Start-up μ C” time interval, when the dc–dc converter output voltage V CC reaches 1.8 V, the microcontroller begins to switch on. In the performed tests, the autonomous sensor system, when powered by the TEG, can save the measurement data into a nonvolatile memory every 2 s. In this situation, the microcontroller and the temperature sensor require a power supply of about 0.9 mW, with a current consumption of about 0.4 mA and a voltage level of about 2.1 V. The measured data can then be collected at subsequent times using the external readout unit by RF communication. In the reading operation, the presence of a heat source is not strictly necessary, since the power supply is provided via electromagnetic field through the coil antenna of the transponder interface. The wake-up signals when the RF field supplies the sensor are shown in Fig. 5. The signals are the differential voltage of the reader antenna, the voltage of the transponder antenna, the supply voltage of the microcontroller, and the microcontroller clock. In the time interval labeled as “Start-up transponder,” the reader is turned on, and the electromagnetic field begins to power the transponder. In the second time interval labeled as “Start-up μ C,” the transponder is turned on, while the microcontroller begins to be powered. The total wake-up time is about 100 ms. The data communication starts after 20 ms from microcontroller clock wake-up, as shown from the transponder antenna signal. A transmission of the measured temperature data that were previously stored in the flash memory between the autonomous sensor and the readout unit is shown in Fig. 6. The low- power microcontroller sends the digital signal to the transponder (“Digital signal transponder”) for the transmission. In the lower graph of the figure, the sensor antenna signal is reported, and the OOK modulation of the digital signal is visible. The base station receives the back-reflected signal (“Output Signal Base Station”) and extracts the Manchester- encoded information (“Digital Signal Base Station”). In this experimental configuration, by turning off the unnecessary modules of the microcontroller and keeping a distance between the autonomous sensor and the readout unit of about 15 mm, the current consumption during RF communication is about 190 μ A at 2.58 V, corresponding to a power level of 0.5 mW. The power required by the autonomous system in the two operational states are reported in Table I, while Table II shows the values of the current for each device of the autonomous sensor in the two operational states. The measurements are obtained using two multimeters (Fluke 8840A). Different tests to evaluate the maximum operating distance between the autonomous sensor and the readout unit were performed, also varying the dimensions of the sensor antenna. Three antennas, whose characteristics are reported in Table III, have been tested. The inductances have been measured with an impedance analyzer (HP4194A). The transponder voltage supply has been measured with a multimeter (Fluke 8840A) when the autonomous sensor system is transferring data, and the results are shown in Fig. 7. The distance z between the antenna of the readout unit and the autonomous sensor is changed from 50 to 100 mm using a micrometer screw. The correct working operation is achieved for a supply voltage that is higher than 1.8 V. The antenna A1 presents the best readout distance, and it has the largest diameter. IV. E XPERIMENTAL S YSTEM An experimental setup has been arranged to evaluate the capability of the autonomous sensor system to measure the temperature along a walled-in pipe of a heating plant. The experimental system is shown in Fig. 8. It consists of a pipe, throughout which hot air is fluxed, two autonomous sensors, and an external readout unit separated by a dummy wall. The heater system represents a simplified model of a generic building heating plant. A round burner with a diameter of 65 mm has been used as heater, which, when supplied with GPL gas, is able to produce a heating power of about 1 kW. When the gas burner is turned on, it heats the air above it, which generates a hot air flux along the pipe from bottom to top. The hot air is conveyed into a metallic pipe, heating its surfaces. The pipe is made of enameled iron and has a thickness of 1 mm, a square cross section with sides of 100 mm, and a length of 1 m. The external temperature distribution along the pipe was measured using five NTC thermistors placed every 20 cm from the lower end of the pipe, while for the internal hot air temperature, a thermocouple was positioned inside at the center of the pipe, as shown in Fig. 9. The NTC sensors were fixed with thermoconductive grease and sealed with silicon glue. The burner gas flame was set at three different intensity levels. Typical steady-state values of temperatures are shown in Fig. 10, which were measured about 500 s after burner ignition. Two autonomous sensors were placed on the external side of the pipe at 20 and 60 cm from the lower end of the pipe, near NTC 2 and NTC 4, respectively. One side (“hot side”) of the TEG of the autonomous sensor was placed on the external side of the pipe, while on the other (“cold side”), a heat sink was mounted to permit heat exchange with the environment. This allows us to maintain the cold side temperature as low as possible and, as a consequence, a temperature gradient across the TEGs as high as possible. The temperature sensor LM94022 was placed near the reference NTC thermistor. Thermoconduc- tive grease was used to improve thermal contact between the pipe wall, TEG, heat sink, and sensor. The output voltages of the dc–dc converters placed near NTC2 and NTC4, which are labeled Vcc1 and Vcc2, respectively, and the time trend of temperatures were measured with the burner ...

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Thesis
The advent of the Internet of Things has enabled the roll-out of a multitude of Wireless Sensor Networks. These networks can be used in various fields, such as agriculture, industry or the smart city, where they facilitate fine optimization of processes. These devices are often powered by primary or rechargeable batteries, which limits their battery life. Moreover, it is sometimes not possible or financially viable to change and/or recharge these batteries.A possible solution is to harvest energy from the environment to power these sensors. But these energy sources are unreliable, and the sensor must be able to prevent the complete depletion of its energy storage. In order to adapt its energy consumption, the node can match its quality of service to its energetical capabilities. Thus, the device can continuously operate without any service interruption.This thesis presents the methods used for the conception of a completely autonomous sensor, powered by energy harvesting and communicating through a long range LoRa network. In order to ensure its power supply, a board has been designed to harvest energy from multiple energy sources simultaneously. A power management software module has then been developed to calculate an energy budget the sensor can use, and to choose the best way to spend this budget over one or multiple tasks. This work has enabled the development of an energy autonomous industrial sensorprototype.