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HARNESSING NO-COST ENERGY FROM RADIO TRANSMISSIONS Saptarshi Bandyopadhyay Indian Institute of Technology Bombay Powai, Mumbai (Stream EB, Application No. 516435) The idea that forms the basis of this project is to trap the energy carried by radio wave broadcasts that is unused by the receiver and store this energy for later use. This results in a no-cost source of energy transmitted via radio waves. Origin of Idea: The idea originated in the summer of 2006 when I was working on a research project at the Giant Meterwave Radio Telescope (GMRT) facility near Pune. In the course of my work I encountered the massive amount of radio noise termed Radio Frequency Interference (RFI) which frequently plays havoc with data collected by the radio telescopes. This has a detrimental effect on observations but reduction of such noise is not undertaken. Hence I attempted to utilize this radio noise productively. Motivation: In the present urban scenario, extensive radio signals are broadcast by major radio stations operating in metropolitan cities. Back of the envelope calculations yield the following results: Each radio station transmits 10 to 30 Kilowatts of power. An ordinary handheld radio receiver requires about 1 microwatt of power for normal performance. Given the above facts, even if the entire population of a city of 10 million had their radios playing, the amount of power used would still fail to exceed 50100 watts. The remainder of the energy goes unutilized. The aim of this project is to tap into this energy and make it a viable zero-cost power source. Yet another significant source of radio noise is telecommunication. Today when mobile communication holds sway over the populace, mobile antennae are erected almost every kilometer apart. These antennae transmit about 1 kilowatt of power. Modus operandi: The following is a brief outline of my attempt to harness the unutilized energy transmitted via radio waves I constructed several antennae to measure the amount of power received. Results show that this value is low. However since this energy is available free of cost I judged the effort to tap it as being worthwhile. I have to make either passive or semi-active circuits (output greater than input from battery) to rectify the alternating signals received from the radio waves. The energy output by the circuit in the form of a rectified DC signals needs to be stored for future use. On successful completion of the above, other ideas like addition of power from different antennae could be implemented. Saptarshi Bandyopadhyay Page 1 9/12/2006 Progress to date: Monopole antenna for 93.5FM (λ = 3.20m) The theory of monopole antennas states that the length of the monopole antenna must be λ/4 (about 80cm in this case) for the antenna to get impedance matched with the surroundings at that wavelength. However this applies only to the ideal situation where the ground plane extends infinitely. The aluminum plate used as the ground plane in my experiments in the laboratory measured 70.3 ( ± 0.1 )cm × 70.5 ( ± 0.1) cm. Hence the length of the monopole used was 93.7( ± 1 )cm. The reason for such a large relative error in the measurement of the length of the monopole, which is an aluminum rod of diameter 6mm, is because the shape is rather crooked; hence precision in length measurement reduces. Image of monopole antenna in laboratory Saptarshi Bandyopadhyay Page 2 9/12/2006 Network analyzer showing impedance matching of antenna The impedance matching of the monopole is seen through the network analyzer. It is seen that the standing wave ratio is good in the range of measurements. Hence there are fewer reflections in the circuit and most of the power is transferred. Measurements were then carried out using the spectrum analyzer. As the results show, many peaks are obtained in the 90 MHz to 95 MHz band. Each of these peaks gives above 100 nanowatts (at 300 micro volts) of power. When integrated over the entire spectrum, power received is approximately 2 to 3 microwatts at voltages of about 10 to 12 millivolts. All these are received purely in the form of alternating signals, which are actually the carrier waves for the actual data transmitted. I got access to these instruments in Prof. Girish Kumar’s lab in Electrical Department, IITB. Saptarshi Bandyopadhyay Page 3 9/12/2006 Table of signal strengths at different wavelengths FREQUENCY STRENGTH 90.96MHz -59.3dBm 92.4MHz -52.1dBm 93.48MHz -53.4dBm 96.0MHz -71.0dBm 98.28MHz -66.8dBm 100.4MHz -74.0dBm Decibels milli (dBm) is the unit used to measure the power carried by radio signals. Its relationship with the Watt is: 1 dBm = 10 X log10 [1 Watt/ 10-3 Watt] Spectrum analyzer showing frequency distribution of radio signals received Saptarshi Bandyopadhyay Page 4 9/12/2006 Monopole antenna for mobile frequencies (800 to 900MHz) An antenna was then built for wavelengths in the mobile range from 800MHz to 1GHz, in the form of a 10.1 ( ±0.1 )cm copper wire and the same ground plane previously used. Initially the same ratio as previously was used for computing the length of the monopole (9cm) for the wavelength of 33cm (900MHz). However there was some impedance mismatch seen in the network analyzer, which I conclude was due to the change in ratio of the ground plane size to the monopole length. The new length was a little larger than the one previously calculated. The impedance matching of the monopole antenna is as shown in the network analyzer. Mobile monopole antenna Saptarshi Bandyopadhyay Page 5 9/12/2006 Network analyzer showing impedance matching of antenna Then some measurements were carried out with the spectrum analyzer. As seen in the image below, the mobile antenna appears to give certain ranges in which strong signals are received. Hence I attempted to find the average strength of these signals. Spectrum analyzer showing frequency distribution of radio signals received Saptarshi Bandyopadhyay Page 6 9/12/2006 Table of strengths of the signals FREQUENCY RANGE STRENGTH 870-920MHz -63 to -55 dBm 943-975MHz -62 to -52 dBm 992-1017MHz -63 to -60 dBm Active rectifier circuit for AC signals in millivolts (mV) Half wave rectifier circuit by a single diode The simplest half wave rectifier circuit is shown above. But for this rectifier to function, the diode needs a threshold voltage of 0.7V. Since my signals will be having very low wattage and voltage, I cannot use this rectifier directly. Preliminary active circuit for rectification of signals Saptarshi Bandyopadhyay Page 7 9/12/2006 The preliminary circuit made for the rectifier is as shown in the diagram. It is active and rectifies the signal at much lower than its threshold voltage of the diode. The high pass filter at the input allows only the signals of very high frequency (above 1MHz) to pass through the circuit. But since the normal diodes frequency response is not good at such high frequencies, I have to use the schottky diode in its place. Another circuit that can be used is the precision full wave rectifier circuit. Although the operational amplifiers need a ±5V supply, the current drained can be reduced by high resistances. Precision Full wave rectifier circuit The rectified output signal compared to the input signal as seen in the CRO Saptarshi Bandyopadhyay Page 8 9/12/2006 Results obtained from experiments: The first conclusion from the 93.5FM antenna is that it is receiving power in microwatts inside IITB. This is a good value since normal handheld quartz watches work with micro watt of power. Also on approaching the transmission station at Tardeo, about 30km from IITB, the power received should increase by the inverse square relationship and taking into consideration factors like attenuation due to structures. There I expect the antenna to sense power in watts, which means even conventional rectifier circuits will work there. Almost similar inference is derived from the mobile antenna. To increase responsiveness and coverage of the mobiles, mobile companies have set up low power transmitting towers after every few kilometers. In IITB, there is a set of antennae outside the main gate and another set of antennae on the main building, barely 800m apart. This shows there is significant attenuation of the signals in the city, largely because of concrete structures. The rectifiers are able to convert the low wattage, low voltage AC signals to DC. But they are all active circuits. I think passive circuits are possible as they won’t be disobeying the law of conservation of energy, when they will be storing the energy from the antenna. Future plans: I plan to evaluate the increase in the power absorbed by the antennae as I approach the radio transmission station. The radio station transmits about 10 kilowatt of power. I expect to tap approximately 1 Watt with the antenna within 100m of the transmission tower. I also plan to find whether metallic objects like pillars, metal cupboards, metal window frames etc can be easily impedance matched so that they too behave as antennae and capture power. This is because any metallic object can behave as an antenna in theory; hence availability of metal antennae is not subject to scarcity any longer. The crucial point of my future work will be making the circuit to be connected to the antenna. It should preferably be passive or at least semi-active. The circuit will be in two parts 1. To convert the AC signal at such high frequencies to a DC signal. 2. Storing of power received from the DC signal for later use. Innovative component in the design: The main advantage of this method of trapping energy is that it is completely free of cost. This is basically a recycling of energy which would have otherwise gone unused. The method is highly cost effective since it is not required to put up any antennae. Any object that conducts can act as an antenna and can be used to harness the energy. The only external input will be a small circuit, which is a small initial investment, not more than Rs50. Once connected, it is a continuous source of energy, with almost no maintenance costs. This source of energy is completely environment-friendly and does not cause pollution in any form, thermal, atmospheric or noise. Saptarshi Bandyopadhyay Page 9 9/12/2006 The sole disadvantage is that there needs to be a continuous and strong source of radio energy received by the antenna. There are AM radio stations which transmit all over the country and hence no part of the country will be completely in a radio free zone. However this concept will work best near the transmitters, in urban areas where there are many radio stations broadcasting. Also a lot of communication is by means of radio; hence the circuit can harness large amounts of energy within metropolitan cities or in areas where there is a large concentration of radio waves. A frequently asked question is if my harnessing the energy will decrease the range of the transmission as there is a removal of some energy from it. The answer is NO for the following reason: As aforementioned, assume the transmitter transmits 10 kilowatts of power but only about 100 watts of it is used by all the radios tuned in to it. A major part of the remaining energy is sent into outer space, and another significant proportion is earthed by all the metallic conducting pillars in buildings, bridges, light posts etc. My circuit will be attached to such elements and will be trapping the energy which they are earthing and thereby wasting. There is no necessity to erect any new antenna for this purpose; hence I will not be in any way reducing the range or the strength of the radio signals when I use my circuit, but turn it to advantageous use. Future scope for implementation: Anyone receiving a lot of radio energy can use this method to trap some energy, especially people living close to radio transmitting towers. It can also be used for a large number of practical purposes, like running watches, streetlights, signals, etc. This method can be used for powering in areas where wiring is too expensive or not possible at all. Future age satellites and space vehicles could use it as a primary source of energy or at least as a reserve source if their solar cells malfunction. As humanity explores reaches further from the sun, if we embark on long intergalactic space missions, radio energy in the form of synchrotron radiation will become an important source of energy, quite comparable to solar energy. Conclusion: Tapping of power from radio waves can provide a viable alternative to other energy conversions. With this technology hopefully implemented someday in the future, it provides a platform for man to tap energy out of the air, figuratively, which to date has been done only in science fiction. This project is the beginning of another journey whereby fantasies in the realm of science are transformed into fact for the good of our world. # ~~~~ # ~~~~ # ~~~~ # ~~~~ # Saptarshi Bandyopadhyay Page 10 9/12/2006