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Learn about the concept of energy harvesting for pervasive sensing, which utilizes power sources in the local environment to power devices and systems. Discover various power sources and their applications in wireless sensor networks.
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Energy Harvestingfor Pervasive Sensing Paul D. Mitcheson, Eric M. Yeatman Department of Electronic & Electrical Engineering Imperial College London
Energy Harvesting: what is it? • Taking useful advantage of power sources already present in the local environment • This energy would otherwise be unused or wasted as e.g. heat • “local” being local to the powered device or system • Extracted power levels generally not limited by source, but by size and effectiveness of generator (“harvester”)
Energy Harvesting: what is it for? • Normally not as a primary source of power, but for applications where mains power is not suitable, because of: • Installation cost • Mobility • Remote/inaccessible/hostile location • Usual alternative is batteries: • Avoid replacement/recharging • Avoid waste from used batteries
How Much Power? World electrical generation capacity 4 terawatts Power station 1 gigawatt House 10 kilowatts Person, lightbulb 100 watts Laptop, heart 10 watts Cellphone power usage 1 watt Wristwatch, sensor node 1 microwatt Transmitted Cellphone signal 1 nanowatt
Cost example: • Mains electricity: consumer price 15¢ / kWhr • Alkaline AA battery: 1 € / 3 Whr • Factor of 2,000
Energy Harvesting Applications • Key application is wireless sensor networks • Sensors can be very low power • Small size often important • Minimal maintenance crucial if many nodes • Implementation of WSNs could lead to higher energy efficiency of buildings etc
Sensor Node Power Requirements – How much power does our harvester need to supply? • Sensing Element • Signal Conditioning Electronics • Data Transmission
Sensing Element Simple signals - temperature, pressure, motion – require electrical power above thermal noise limit. NT 10-20 W/Hz For most applications, this is negligible
Signal Conditioning Likely principal function: A/D Converter Recent results: Sauerbrey et al., Infineon (’03) Power < 1 mW possible for low sample rates!
5 0 4 0 Typical indoor Loss exponent (3.5) 3 0 2 0 1 0 Transmit Power (dBm) 0 - 1 0 - 2 0 - 3 0 Ideal free-space propagation - 4 0 - 5 0 1 1 0 1 0 0 1 0 0 0 Range (m) Data Transmission: Required Power Conclusions: Power independent of bit-rate for low bit-rate -30 dBm (1 mW) feasible for room-scale transmission range Figure: F. Martin, Motorola
Estimated Total Power Needs • Peak power 1 – 100 uW • Average power can be below 1 uW • Batteries: Present Capability • 10 mWyr for 1 cm3 battery feasible • Not easy to beat! • Useful energy reservoir for energy harvesting
Fuel-Based Power Sources • Energy density much higher than for batteries, 10 kJ/ cm3 • Technology immature, fuel cells most promising Fraunhofer Inst. Micro fuel cell, Yen et al.
Solar Cells • highly developed • suited to integration • high power density possible: • 100 mW/cm2 (strong sunlight) • but not common: • 100 mW/cm2 (office) • Need to be exposed, and oriented correctly Solar cell for Berkeley Pico-Radio
Solar Cells in Energy Harvesting Applications: • Cost not the main issue • Availability of light is key
Thermal • need reasonable temperature difference (5 – 10C) in short distance • ADS device 10 mW for 5C • even small DT hard to achieve Heat engine, Whalen et al, Applied Digital Solutions
Ambient Electromagnetic Radiation Graph: Mantiply et al. 10 V/m needed for reasonable power: not generally available
Motion Energy Scavenging • Direct force devices • Inertial devices
Direct Force: Heel Strike Heel strike generator: Paradiso et al, MIT
Direct Force: larger scale • East Japan Railway Co. • Energy harvesting ticket gates
Inertial Harvesters • Mass mounted on a spring within a frame • Frame attached to moving “host” (person, machine…) • Host motion vibrates internal mass • Internal transducer extracts power
Available Power from Inertial Harvesters • Peak force on proof mass F = ma = mw2Yo • Damper force < F or no movement • Maximum work per transit W = Fzo = mw2Yozo • Maximum power P = 2W/T = mw3Yozo/p
How much power is this? 10 x 10 x 2 mm 3 x 3 x 0.6 mm • Plot assumes: • Si proof mass (higher densities possible) • max source acceleration 1g (determines Yo for any f)
Sensor node watch cellphone laptop Achievable Power Relative to Applications • Plot assumes: • proof mass 10 g/cc • source acceleration 1g
Implementation Issues: Transduction Mechanism • Piezoelectric? • Difficult integration of piezo material • Reasonable voltage levels easy to achieve • Suitable for miniaturisation
Typical Inertial Generators Piezoelectric Wright et al, Berkeley Ferro solutions
Implementation Issues: Transduction Mechanism • Electromagnetic? • Dominant method for large scale conversion • Needs high df/dt to get damper force (f = flux) • df/dt = (df/dz )(dz/dt ) • Low frequency (low dz/dt) needs very high flux gradient • Hard to get enough voltage in small device (coil turns) • Efficiency issues (coil current) • Variant: magnetostrictive
Typical Inertial Generators Magnetic Southampton U. CUHK
Implementation Issues: Mechanism • Electrostatic? • Simple implementation, no field gradient problem • Suitable for small size scale • Damping force can be varied via applied voltage • But needs priming voltage (or electret)
Typical Approach: Constant Charge Input phase Output phase
Prototype MEMS Device Assembled generator Detail of deep-etched moving plate
Device Operation Output > 2 mW
Other Options: Rotating Mass Example : Seiko Kinetic
Large Inertial Generators • Backpack: U Penn • 7 watts!
Conclusions • Power levels in the microwatt range are enough for many wireless sensor nodes • Small energy harvesters can achieve these levels • Help enable pervasive sensing by eliminating maintenance burden • Contact: paul.mitcheson@imperial.ac.uk • Review Paper: Mitcheson, Yeatman et al., “Energy Harvesting From Human and Machine Motion for Wireless Electronic Devices”, Proceedings of the IEEE 96(9), 1457-1486 (1998).