Frequency response of microcantilevers immersed in gaseous, liquid, and supercritical carbon dioxide

a b s t r a c t The frequency response of ferromagnetic nickel microcantilevers with lengths ranging between 200 m and 400 m immersed in gaseous, liquid and supercritical carbon dioxide (CO2) was investigated. The resonant frequency and the quality factor of the cantilever oscillations in CO2 were measured for each cantilever length in the temperature range between 298 K and 323 K and the pressure range between 0.1 MPa and 20.7 MPa. At a constant temperature, both the resonant frequency and the quality factor were found to decrease with increasing pressure as a result of the increasing CO2 density and viscosity. Very good agreement was found between the measured cantilever resonant frequencies and predictions of a model based on simplified hydrodynamic function of a cantilever oscillating harmonically in a viscous fluid valid for Reynolds numbers in the range of (1;1000) (average deviation of 2.40%). At high pressures of CO2, the experimental Q-factors agreed well with the predicted ones. At low CO2 pressures, additional internal mechanisms of the cantilever oscillation damping caused lowering of the measured Q-factor with respect to the hydrodynamic model predictions.

[1]  H. Craighead,et al.  Mechanical resonant immunospecific biological detector , 2000 .

[2]  F Meriaudeau,et al.  Observation of Knudsen effect with microcantilevers. , 2003, Ultramicroscopy.

[3]  H. Hosaka,et al.  DAMPING CHARACTERISTICS OF BEAM-SHAPED MICRO-OSCILLATORS , 1995 .

[4]  J. Colton,et al.  Microcantilevers: sensing chemical interactions via mechanical motion. , 2008, Chemical reviews.

[5]  Tianjun Li,et al.  Dissipation of micro-cantilevers as a function of air pressure and metallic coating , 2011, 1110.6629.

[6]  Sergei G. Kazarian,et al.  Polymer Processing with Supercritical Fluids , 2006 .

[7]  John E. Sader,et al.  Experimental validation of theoretical models for the frequency response of atomic force microscope cantilever beams immersed in fluids , 2000 .

[8]  J. Sader Frequency response of cantilever beams immersed in viscous fluids with applications to the atomic force microscope , 1998 .

[9]  B. E. Alaca,et al.  A Magnetically Actuated Resonant Mass Sensor With Integrated Optical Readout , 2008, IEEE Photonics Technology Letters.

[10]  Eric Bourillot,et al.  Effects of temperature and pressure on microcantilever resonance response. , 2003, Ultramicroscopy.

[11]  T. Thundat,et al.  Adsorption-desorption characteristics of explosive vapors investigated with microcantilevers. , 2003, Ultramicroscopy.

[12]  G. Hähner,et al.  Simultaneous determination of density and viscosity of liquids based on resonance curves of uncalibrated microcantilevers , 2006 .

[13]  M. Esashi,et al.  Energy dissipation in submicrometer thick single-crystal silicon cantilevers , 2002 .

[14]  Alain Blouin,et al.  All-optical measurement of in-plane and out-of-plane Young's modulus and Poisson's ratio in silicon wafers by means of vibration modes , 2004 .

[15]  Liviu Nicu,et al.  Rheological behavior probed by vibrating microcantilevers , 2008 .

[16]  Todd Sulchek,et al.  Mercury vapor detection with a self-sensing, resonating piezoelectric cantilever , 2003 .

[17]  Eric J. Beckman,et al.  Supercritical and near-critical CO2 in green chemical synthesis and processing , 2004 .

[18]  M. Moldover,et al.  Ab Initio Values of the Thermophysical Properties of Helium as Standards , 2000, Journal of research of the National Institute of Standards and Technology.

[19]  P. Hefti,et al.  Experimental Determination of the Q‐factors of Microcantilevers Coated With Thin Metal Films , 2009 .

[20]  Measurements of the phase transition and the average length of the density fluctuation under supercritical fluid using micromechanical resonators , 2011 .

[21]  J. Sader,et al.  Rheological measurements using microcantilevers , 2002 .

[22]  D. N. Buckley,et al.  Complete synthesis of germanium nanocrystal encrusted carbon colloids in supercritical CO2 and their superhydrophobic properties. , 2011, Langmuir : the ACS journal of surfaces and colloids.

[23]  N. Fleck,et al.  Young's modulus of electroplated Ni thin film for MEMS applications , 2004 .

[24]  A. Maali,et al.  Hydrodynamics of oscillating atomic force microscopy cantilevers in viscous fluids , 2005 .

[25]  Oliver Brand,et al.  Geometrical optimization of resonant cantilevers vibrating in in-plane flexural modes , 2010, 2010 IEEE Sensors.

[26]  J. Zacharias,et al.  The Temperature Dependence of Young's Modulus for Nickel , 1933 .

[27]  Detection of microviscosity by using uncalibrated atomic force microscopy cantilevers , 2008 .

[28]  R. Rajagopalan,et al.  Brownian Fluctuation Spectroscopy Using Atomic Force Microscopes , 2000 .

[29]  Thomas Thundat,et al.  Viscous drag measurements utilizing microfabricated cantilevers , 1996 .

[30]  I. Dufour,et al.  A straightforward determination of fluid viscosity and density using microcantilevers: From experimental data to analytical expressions , 2011 .

[31]  Minhang Bao,et al.  Squeeze film air damping in MEMS , 2007 .

[32]  F. Omnès,et al.  High sensitivity of diamond resonant microcantilevers for direct detection in liquids as probed by molecular electrostatic surface interactions. , 2011, Langmuir : the ACS journal of surfaces and colloids.

[33]  Robert W. Stark,et al.  Cantilever Micro-rheometer for the Characterization of Sugar Solutions , 2008, Sensors.