Abstract
In this work, we employ a kinetic-theory-based approach to predict the hydrodynamic forces on electromechanical resonators operating in gaseous media. Using the Boltzmann-BGK equation, we investigate the influence of the resonator geometry on the fluid resistance in the entire range of non-dimensional frequency variation 0≤τω≤∞ here the fluid relaxation time τ=μ/p is determined by the gas viscosity μ and pressure p at thermodynamic equilibrium, and ω is the (angular) oscillation frequency. Our results here capture two important aspects of recent experimental measurements that covered a broad range of experimental parameters. First, the experimentally observed transition from viscous to viscoelastic flow in simple gases at τω≈ 1 emerges naturally in the numerical data. Second, the calculated effects of resonator geometry are in agreement with experimental observations.
| Original language | English |
|---|---|
| Pages (from-to) | 241-257 |
| Number of pages | 17 |
| Journal | Journal of Fluid Mechanics |
| Volume | 652 |
| DOIs | |
| State | Published - Jun 2010 |
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