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Tip vibrating amplitude

To compare this expression with our experimental results (which are the oscillation amplitudes A(t)), one assumes that the tip vibrating amplitude A(t) is ... [Pg.146]

Fig. 10.1. A vibrating system vvith one degree of freedom and its transfer fnnction. (a) The vibrating system. A mass M is connected to the frame through a spring and a viscous damper. Regarding STM, there are two realizations of this model. First, the frame represents the floor, and the mass represents the STM. Second, the frame represents the base plate (with the sample) in STM, and the mass represents the tip assembly, (b) The transfer function, which is the ratio of the vibration amplitude of the mass to that of the frame at different frequencies. (After Park and Quate, 1987.)... Fig. 10.1. A vibrating system vvith one degree of freedom and its transfer fnnction. (a) The vibrating system. A mass M is connected to the frame through a spring and a viscous damper. Regarding STM, there are two realizations of this model. First, the frame represents the floor, and the mass represents the STM. Second, the frame represents the base plate (with the sample) in STM, and the mass represents the tip assembly, (b) The transfer function, which is the ratio of the vibration amplitude of the mass to that of the frame at different frequencies. (After Park and Quate, 1987.)...
Fig. 13.3. Forces and signals in UFM (a) tip-surface interaction force versus indentation for approach and retraction (solid and dashed respectively) approach (solid) and retraction (dashed) differ at the verge of the tip-surface contact (b) non-linear detection of ultrasound at increasing ultrasonic vibration amplitude (c) oscilloscope traces of ultrasound detection in a UFM (Kolosov and Yamanaka 1993 Dinelli et al. Fig. 13.3. Forces and signals in UFM (a) tip-surface interaction force versus indentation for approach and retraction (solid and dashed respectively) approach (solid) and retraction (dashed) differ at the verge of the tip-surface contact (b) non-linear detection of ultrasound at increasing ultrasonic vibration amplitude (c) oscilloscope traces of ultrasound detection in a UFM (Kolosov and Yamanaka 1993 Dinelli et al.
The oscillation amplitude A is the primary variable in AM-AFM. Its representation as a function of the average tip-surface separation d is called amplitude curve. The numerical solution of the weakly perturbed oscillator shows in some situations two different solutions for the vibration amplitude, a low (L) and high amplitude (H) solution. If the tip-surface separation and the external parameters are unchanged, the initial conditions will determine which solution is realized. [Pg.19]

Fig. 1.12 Tip-sample distance d and free vibration amplitude A0. When the tip approaches the surface, the value of A0 will decrease. In tapping, the tip touches the surface at each cycle, which changes the oscillation amplitude to A. The setpoint at which images is done is defined as A/A0... Fig. 1.12 Tip-sample distance d and free vibration amplitude A0. When the tip approaches the surface, the value of A0 will decrease. In tapping, the tip touches the surface at each cycle, which changes the oscillation amplitude to A. The setpoint at which images is done is defined as A/A0...
For imaging experiments, the tip can be employed in either contact, intermittent, or noncontact mode with the surface. This is often in conjunction with a feedback loop that operates to maintain a constant cantilever deflection (or vibration amplitude), by adjusting the tip-sample separation. [Pg.416]

In noncontact mode, the system vibrates a stiff cantilever near its resonant frequency (typically 100-400 kHz) with an amplitude in the range of ten to several hundred angstroms. Any change in resonant frequency or vibration amplitude as the tip nears the surface can be detected. The sensitivity of this technique allows sub-angstrom vertical resolution to be achieved. [Pg.2957]

The work functions of ITO, PEDT, and PAni layers were determined using a scanning Kelvin probe (SKP, UBM Messtechnik GmbH) in a chamber equipped with silica gel giving a relative humidity of 0%. A Cr or Ni wire with a tip diameter of 80 p,m was used as a vibrating reference electrode. The tip was positioned about 20 p,m above the specimen, the vibration amplitude was +10 p,m, and the vibration frequency of the needle was 1.75 kHz. As measurements could not be performed in ultrahigh vacuum, gold was used as reliable reference material. [Pg.1102]

Integration of SM A wires into the composite skin of a fin of 0.5 m in height has been realised within the EU-funded project ADAPT [70]. SMA wires of 150 pm thickness were integrated into the glass fibre reinforced composite skin which could then be actuated. An initial simple test showed that tip deflection amplitudes could be reduced by around a half in a vibration test once the SMA wires had been heated up to an austenitic condition (Fig. 8.18). [Pg.386]

Figure 9.5 Quartz tuning fork with a goid-tip glued at one of the prongs used shear-force for tip-sampie distance control. Typical vibration amplitudes are on the order of 0.1 nm. Adapted from PhD-Thesis of Marcus Sackrow, University of Tubingen. Figure 9.5 Quartz tuning fork with a goid-tip glued at one of the prongs used shear-force for tip-sampie distance control. Typical vibration amplitudes are on the order of 0.1 nm. Adapted from PhD-Thesis of Marcus Sackrow, University of Tubingen.
The apparatus, being able implementing shear force distance control must be set with an actuator for providing the tip vibration and an amplitude detecting unit. Usually piezoelectric actuator is connected to the stem of the tip. It keeps it oscillating at resonance frequency. For detecting the amplitude different techniques are used. From the optical methods laser spot diffraction from the vibrating probe [54], or interferometric technique [68], has been successfully used for distance detection. [Pg.296]


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