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Effects of the ratio of attached mass to the beam mass, rotation speed, hub ratio, orthotropy ratio, position of attached mass, beam theory and length to thickness ratio are analyzed in detail.
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The results show that the C F boundary condition of BNNRs are more sensitive to attached mass than the C C boundary condition and also the sensitivity range for BNNRs.
The value of frequency shift was larger when the location of the attached mass was closer to the free end.
However, the sensitivity quickly dropped as the location of the attached mass was closed to the fixed end.
In addition, when the location of the attached mass is closer to the free end, the frequency shift is more significant and that makes the sensor reveal more sensitive.
Changes in the resonance frequency, f, related to attached mass (including coupled water), and in the dissipation (D), related to frictional (viscous) losses in the adlayer, were recorded using QSoftTM control software (supplied by the QCM-D instrument).
The attached mass causes a shift to the resonant frequency of resonator.
The changes in the frequency (f), related to the attached mass (including coupled water), and the changes in dissipation (D), related to the frictional (viscous) properties of the adsorbed laccase layer, were recorded using QSoft™ control software (Q-Sense, Sweden).
The atomic-scale mass sensing with a resonator is based on the fact that the resonant frequency is sensitive to the attached mass.
The principle of mass detection using carbon nanotube (CNT) resonators is based on the detection of the resonant frequency shift due to an attached mass.
In addition, most of the finite element method (FEM) analysis models that are used to predict the resonant frequency shift due to attached masses have been implemented in the linear oscillation regime.
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