Sensors, Update 13Henry Baltes, W. Göpel, Gary K. Fedder, J. Hesse, Jan G. Korvink Sensors Update includes information at the cutting edge of sensor research and related topics such as MEMS. An overview of highlights in this exciting area is presented that covers current developments in materials, design, production and application of sensors and other micro– and nanosystems. Volume 13 gives you an insight into the modelling and simulation of microdevice self–assembly, and the alternatives for smart sensor interfaces. Fluorescent microspheres for ion sensing are reviewed, and from the medical and biosciences sector, optical sensor applications, catheter sensors, microelectronic chips for molecular and cell biology as well as microvalves for bioassays, miniature GC systems and micro–fuel cells are presented. The unique approach makes Sensors Update a valuable reference work for scientists and engineers in industry and at universities, to sensors developers, distributors, and users. All volumes of Sensors Update are also available online at our Wiley InterScience® site: http://www3.interscience.wiley.com/cgi–bin/jhome/78505815 |
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Page 167
... functional integration is required in the view of the ' personal bioanalyzer ' , in which programmability needs to be increased with respect to the application - specific diagnostic systems . The integration of function into single ...
... functional integration is required in the view of the ' personal bioanalyzer ' , in which programmability needs to be increased with respect to the application - specific diagnostic systems . The integration of function into single ...
Page 206
... function is often described by the Henyey - Greenstein [ 6 ] phase function 1 1- g2 f ( 0 ) = 4ñ ( 1 + g2 − 2g cos 0 ) 3 / 2 ( 2 ) g is the anisotropy coefficient , which is equal to the average cosine of the scat- tering angle +1 g ...
... function is often described by the Henyey - Greenstein [ 6 ] phase function 1 1- g2 f ( 0 ) = 4ñ ( 1 + g2 − 2g cos 0 ) 3 / 2 ( 2 ) g is the anisotropy coefficient , which is equal to the average cosine of the scat- tering angle +1 g ...
Page 222
... function . The choice of autocorrelation function vs. power spectral density for presentation of the measurement depends on the application and the traditions within the different fields in which the LD method is applied . As a rule ...
... function . The choice of autocorrelation function vs. power spectral density for presentation of the measurement depends on the application and the traditions within the different fields in which the LD method is applied . As a rule ...
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accelerometer amplifier Anal analysis analytical applications array Beer-Lambert law biaxial binding blood flow blood vessels calibration capacitance catheter cell Chem chip circuit CMOS coil detection developed device dielectrophoresis displacement electrical electrode electromagnetic electroplating energy Equation fabrication filter flow cytometry flow rate fluid fluidic fluorescence fluoroscopy force frequency function guide wire HbO2 hemoglobin IEEE instrument integrated interface ionophore lab-on-a-chip laser Doppler layer lubricant magnetic field measurements membrane micro Microelectronic micromachined micropart microspheres microsystems microvalve miniaturization molecules monitor offset operating operational amplifier optical optodes orifice output oxygen oxygen saturation parameters particles Parylene phase photolithography photons piezoelectric polymerization position pressure Proc pulse pulse oximetry readout rotational sample scattering Schematic Sens sensor Sensors and Actuators shown in Figure signal silicon simulation Solid-State Sensors structure substrate surface techniques temperature tion tissue Transducers ultrasound valve voltage volume wafer