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Positive Frequency Shifts Observed Upon Adsorbing Micron-Sized Solid Objects to a Quartz Crystal Microbalance from the Liquid Phase

机译:从液相吸附微米级固体物体到石英晶体微天平上观察到的正频移

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By specifically binding derivatized colloidal particles and physisorbing nonderivatized particles to the surface of a quartz crystal microbalance (QCM), we have observed positive shifts of frequency, (DELTA)f, in contrast to the negative frequency shifts typically found in adsorption experiments. Evidently, the Sauerbrey relation does not apply to this situation. A comparison of frequencies shifts and bandwidths on different overtones reveals a coupled resonance: at low overtones, (DELTA)f is negative, whereas it is positive at high overtones, with maximal resonance bandwidth observed at the crossover point. As predicted by the Dybwad model, the spheres bound to the surface form resonating systems on their own. A composite resonator is formed, consisting of a large crystal with resonance frequency omega and the adsorbed spheres with resonance frequency (omega)_(S). In the case in which the resonance frequency of the small spheres (firmly attached to crystal), (omega)_(S), is higher than the resonance frequency of the crystal, omega, (DELTA)f of the composite system is negative (leading to the Sauerbrey limit). In the opposite limit (that is, in the case of large adsorbed particles bound to the sensor surface via a sufficiently weak bridge) (DELTA)f is positive. Such a behavior is known from sphere-plate contacts in the dry state. Finite element calculation demonstrates that this phenomena is also plausible in liquid phase media, with (DELTA)fcritically dependent on the strength of the sphere-plate contact. Operated in this mode, the QCM most likely probes the contact strength, rather than the mass of the particle.
机译:通过将衍生的胶体颗粒特异性结合并物理吸附非衍生化的颗粒到石英晶体微天平(QCM)的表面,我们观察到了频率Δf的正向偏移,这与吸附实验中通常发现的负向频率偏移相反。显然,索伯里关系不适用于这种情况。比较不同泛音上的频移和带宽可发现耦合共振:在低泛音下,Δf为负,而在高泛音下为正,在分频点观察到最大共振带宽。正如Dybwad模型所预测的,与表面结合的球体自身形成了共振系统。形成一个复合谐振器,该谐振器由谐振频率为ω的大晶体和谐振频率为ω_(S)的吸附球组成。在小球(牢固地附着在晶体上)的共振频率ω_(S)高于晶体的共振频率的情况下,复合系统的ωf为负(导致Sauerbrey极限)。在相反的极限中(即,在大吸附颗粒通过足够弱的电桥结合到传感器表面的情况下),Δf为正。从干燥状态下的球板接触知道这种行为。有限元计算表明,这种现象在液相介质中也是合理的,其中Δ严重依赖于球-板接触的强度。在这种模式下运行,QCM最有可能探测接触强度,而不是颗粒的质量。

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