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Force oscillation signalling

Typical examples of load-time traces of pre-cracked Charpy specimens at impact rates from 0.1 up to 3.3 m/s are shown in Fig. 4a for PVC. While the recorded non-damped signal up to about 0.5 m/s is of sufficient quality to directly determine the fracture force, Fp, significant force oscillations are visible on the signals for higher loading rates. [Pg.191]

Vanishing contrast may be caused by selecting a setpoint that is almost equal to the differential signal for the undeflected cantilever and equal to the rms amplitude of the freely oscillating forced oscillator for CM and TM, respectively. [Pg.72]

Clearly these oscillations are undesirable as they may obscure nearby weaker peaks. Assuming that it is not an option to increase the acquisition time, the way forward is to apply a decaying weighting function to the FID so as to force the signal to go to zero at the end. Unfortunately, this will have the side effects of broadening the lines and reducing the SNR. [Pg.63]

For brevity, this naming scheme follows the usual distinction between the emitter of a wave, the oscillator, and what is emitted, the wave. The system natural pulsation features the oscillator, whereas the wave pulsation is one of the variables of a wave. Without entering in too many details, it will be just said that the latter is a state variable, more precisely an effort of an energy variety present in waves called phase or wave energy. It becomes equal to the system natural pulsation (Oq only in peculiar cases of matching between emitter and emitted signal, as in the conservative harmonic oscillator treated here, but in a damped oscillator (see case study H7 in Chapter 11) or in case of forced oscillations for instance, the two variables will not coincide. [Pg.361]

Ashkin and Dziedzic (1977) used the radiation pressure force of a laser beam to levitate microdroplets with the apparatus presented in Fig. 15. A polarized and electro-optically modulated laser beam illuminated the particle from below. The vertical position of the particle was detected using the lens and split photodiode system shown. When the particle moved up or down a difference signal was generated then a voltage proportional to the difference and its derivative were added, and the summed signal used to control an electro-optic modulator to alter the laser beam intensity. Derivative control serves to damp particle oscillations, while the proportional control maintains the particle at the null point. [Pg.29]

Fig, 19, Differences between noncontact and tapping mode AFM, The signal for the former is dependent on the change in oscillation due to the force gradient, while the latter is dependent on the oscillation change due to the contact, (Courtesy of Digital Instruments, Veeco... [Pg.238]

Better control of the cantilever oscillation in liquid environment can be achieved when the cantilever is oscillated directly by an external force. This idea was implemented by the so-called Magnetic-Alternative-Current Mode (MAC Mode) [194]. A magnetic cantilever is driven by an external magnetic field which is generated by a solenoid placed beneath the sample. The direct excitation of the cantilever avoids unwanted resonance s from the cantilever holder, the fluid body, and the sample itself. Furthermore, the improved signal-to-noise ratio allows smaller oscillation amplitudes and set point ratios Asp/Af closer to 1. Both factors result in a significant reduction in the energy deposited into the sample,... [Pg.93]

As discussed in Sect. 2.2.2, FMM images can lose the material contrast when the sample stiffness exceeds the stiffness of the cantilever. In addition, the net signal contains friction effects because of the cantilever bending and the sample indentation. Furthermore, in liquid samples, capillary forces dominate the response at low frequencies [ 127]. These drawbacks can be overcome by operating the microscope above the contact resonance frequencies. In the so-called con-tact-mode scanning local-acceleration microscope the cantilever oscillates at very low amplitudes of ca. 0.1 nm which still provides strong enough contrast with respect to the mechanical properties [122]. Since the response of the canti-... [Pg.130]


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