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Photonic crystals in biology - NanoTR-VI

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PPPP Hans-EliasP andPoster Session, Thursday, June 17Theme F686 - N1123Hydroflown: A MEMS Based Underwater Acoustic Particle Velocity Sensor123M. Berke Gür,Pde BreePUTuncay AkalUP P*PDepartment of Mechatronics Eng<strong>in</strong>eer<strong>in</strong>g, Bahçeehir University, stanbul 34353, TurkeyPMicroflown Technologies, Han University of Applied Sciences, Arhhem 6826, The Netherlands3PSUASIS Ltd., TUBITAK MRC Campus, Gebze-Kocaeli 41470, Turkey21Abstract-An acoustic field is fully described by two different but related variables: the scalar acoustic pressure and the vector valued acousticparticle velocity. Conventional hydrophones measure the acoustic pressure variable only. However, it is the particle velocity that carriesdirectional <strong>in</strong>formation and provides a more complete description of the acoustic field. Hydroflown is a novel MEMS based underwater acousticparticle velocity sensor under development, when comb<strong>in</strong>ed with a MEMS hydrophone is capable of completely measur<strong>in</strong>g the underwateracoustic field. Unlike conventional accelerometer based underwater acoustic particle velocity sensors, the sensor will not exhibit resonance andis expected to have a flat frequncy response from dc to 20 kHz.An underwater acoustic wave is a propagat<strong>in</strong>g energypacket which causes a disturbance <strong>in</strong> the ambient pressure and<strong>in</strong>duces a small volumetric motion (whose rate is termed theparticle velocity). Although the amplitudes of the acousticpressure and particle velocity are related, the latter is a vectorvalued and hence, carries directional <strong>in</strong>formation regard<strong>in</strong>gacoustic energy propagation. While the scalar valued acousticpressure is easily measured us<strong>in</strong>g a hydrophone, low costsensors capable of accurately measur<strong>in</strong>g the particle velocityhas rema<strong>in</strong>ed a major challenge. Several underwater sensorsdesigned for this purpose (all which are not commerciallyavailable) rely on accelerometers that are packaged such thatthe sensor is naturally buoyant <strong>in</strong> water [1,2,3].Recently, a novel MEMS based acoustic particle velocitysensor, called the Microflown, capable of measur<strong>in</strong>g theparticle velocity <strong>in</strong> air was developed [4]. This paper outl<strong>in</strong>esthe prelim<strong>in</strong>ary concepts and work done for extend<strong>in</strong>g theMicroflown sensor to underwater applications. The newsensor is termed appropriately the Hydroflown. TheMicroflown measures the particle velocity us<strong>in</strong>g two paralleloriented plat<strong>in</strong>um wire resistances. The wires are 200 nm th<strong>in</strong>and 5m wide (see Figure 1). When voltage is applied acrossthe wire term<strong>in</strong>als the wires heat up to 300°C. An acousticwave propagat<strong>in</strong>g perpendicular to the wires results <strong>in</strong> atemperature difference between the wires. The upstream wirewill cool down more compared to the downstream wire due toconvective heat transfer, which will result <strong>in</strong> a change <strong>in</strong> theresistance of the wires. The particle velocity is proportional tothe voltage change <strong>in</strong>duced by the change <strong>in</strong> the resistance.The sensor has a flat frequency response from dc up to 20kHz.The Hydroflown sensor is to be manufactured by firstdeposit<strong>in</strong>g a 300nm layer of Silicon Nitride (SiR3RNR4R) on aSilicon wafer followed by the deposition of a photoresist. ThisSilicon Nitride layer is used as a mask for the wet chemicaletch<strong>in</strong>g process <strong>in</strong> the follow<strong>in</strong>g steps. Next, a 200nmPlat<strong>in</strong>um layer is added us<strong>in</strong>g the sputter technique. Theresistive wires and the term<strong>in</strong>als are patterned from thisPlat<strong>in</strong>um layer us<strong>in</strong>g the lift-off technique. Afterphotolithography, the Silicon Nitride layer is removed us<strong>in</strong>greactive ion etch<strong>in</strong>g. F<strong>in</strong>ally, the Silicon wafer is etched withanisotropic wet chemical etch<strong>in</strong>g us<strong>in</strong>g Potassium Hydroxide(KOH) to create the channel and the bridge.Although the work<strong>in</strong>g pr<strong>in</strong>ciple of the Hydroflown sensor isTable 1. A comparison of the acoustic properties of air andseawater.Property Air SeawaterSpeed of Sound (m/s) 340 1500Density (kg/m 3 ) 1,2 1025Acoustic Impedence (Pa s/m) 415 1,54×10 6Specific Heat (kJ/kg/K) 1,0 4,0Thermal Conductivity (W/m/K) 0,025 0,596similar to the Microflown sensor, the former is designed towork underwater. S<strong>in</strong>ce water will start to boil above 100°C,the sensor is required to be encapsulated <strong>in</strong> an acousticallytransparent package filled with another fluid with a higherboil<strong>in</strong>g temperature. A comparison of the acoustic propertiesof air and seawater are presented <strong>in</strong> Table 1.In summary, Hydroflown, a novel underwater sensor formeasur<strong>in</strong>g the acoustic particle velocity is <strong>in</strong>troduced. Thework<strong>in</strong>g pr<strong>in</strong>ciples of the sensor are def<strong>in</strong>ed. The lab tests ofthe sensor are currently <strong>in</strong> progress and the first sea trials arescheduled for the summer of 2010. The Hydroflown sensor isexpected to provide higher quality measurements with fewersensors compared to conventional pressure measur<strong>in</strong>ghydrophone based systems. Initial applications of the sensorare planned for uniform l<strong>in</strong>e arrays. This work is supported bythe EUROSTARS Programme grant E!-4224 Hydroflown.*Correspond<strong>in</strong>g author: tuakal@suasis.comFigure 1. A scann<strong>in</strong>g electron microscope image of a bridgetype Microflown MEMS acoustic particle velocity sensor clearlyshow<strong>in</strong>g the Plat<strong>in</strong>um resistive wires and the term<strong>in</strong>als.[1] K. J. Bastyr et al., J. Acoust. Soc. Am. 106, 6 (1999).[2] W. D. Zhang et al., Sensors 9 (2009).[3] V. Shchurov, Vector Acoustics of the Ocean, engl. transl. (2006).[4] H.-E. de Bree, Acoust. Aust. 31 (2003).6th Nanoscience and Nanotechnology Conference, zmir, 2010 687

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