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Theoretical analysis of laterally vibrating microcantilever sensors in a viscous liquid medium

Russell Cox
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TLDR
In this article, the hydrodynamic forces on the microcantilever as a function of both Reynolds number and aspect ratio (thickness over width) were first calculated using a combination of numerical methods and Stokes' solution.
Abstract
THEORETICAL ANALYSIS OF LATERALLY VIBRATING MICROCANTILEVER SENSORS IN A VISCOUS LIQUID MEDIUM Russell Cox, B.S., M.S. Marquette University, 2011 Dynamically driven microcantilevers are normally excited into resonance in the out-of-plane flexural mode. The beam’s resonant frequency and quality factor are used to characterize the devices. The devices are well suited for operation in air, but are limited in viscous liquid media due to the increased viscous damping. In order to improve these characteristics, other vibration modes such as the in-plane (or lateral) flexural mode are investigated. In this work, microcantilevers vibrating in the in-plane flexural mode (or lateral direction) in a viscous liquid medium are investigated. The hydrodynamic forces on the microcantilever as a function of both Reynolds number and aspect ratio (thickness over width) are first calculated using a combination of numerical methods and Stokes’ solution. The results allowed for the resonant frequency, quality factor, and mass sensitivity to be investigated as a function of both beam geometry and medium properties. The predicted resonant frequency and quality factor for several different laterally vibrating beams in water are also found to match the trends given by experimentally determined values found in the literature. The results show a significant improvement over those of similar devices vibrating in the out-of-plane flexural mode. The resonant frequency increases by a factor proportional to the inverse of the beam’s aspect ratio. Moreover, the resonant frequency of a laterally vibrating beam shows a smaller decrease when immersed in water (5-10% compared to ~50% for transversely vibrating beams) and, as the viscosity increases, the resonant frequency decreases slower compared to beams excited transversely. The quality factor is found to increase by a factor of 2-4 or higher depending on the medium of operation and the beam geometry. Due to the increased resonant frequency and the decreased effective mass of the beam (compared to beams excited transversely), the estimated mass sensitivity of a laterally excited microcantilever is found to be much larger (up to two orders of magnitude). The improvement in these characteristics is expected to yield much lower limits of detection in liquid-phase bio-chemical sensing applications.

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Effect of hydrodynamic force on microcantilever vibrations: applications to liquid-phase chemical sensing

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Oscillation of cylinders of rectangular cross section immersed in fluid (vol 22, 052001, 2010)

TL;DR: In this article, the hydrodynamic load experienced by an oscillating rigid cylinder, of arbitrary rectangular cross section, that is immersed in an unbounded viscous fluid was analyzed. And the validity and accuracy of the widely used infinitely-thin blade approximation for out-of-plane motion was evaluated.
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Lateral-Mode Vibration of Microcantilever-Based Sensors in Viscous Fluids Using Timoshenko Beam Theory

TL;DR: In this article, a new model was developed to incorporate viscous fluid effects and Timoshenko beam effects (shear deformation, rotatory inertia) to more accurately model microcantilever resonant behavior in liquids.

Effect of Support Compliance on the Resonant Behavior of Microcantilever-Based Sensors in Viscous Fluids

TL;DR: In this paper, the authors derived an analytical model for the lateral-mode dynamic response of a microcantilever in a viscous fluid, including the effects of support compliance, by employing dimensional analysis and 3-D FEA.
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Higher-Order Models for Resonant Viscosity and Mass-Density Sensors.

TL;DR: Advanced fluid models relating viscosity and density to resonance frequency and quality factor of vibrating structures immersed in fluids are presented, and methods for model parameter calibration and the inversion of the models to determine viscosities and/or density from measured resonance parameters are shown.
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