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Charge amplifiers

A crystal material is excited by the force imposed on it by an internal I v mounted mass. A voltage is produced by the crystal proportional to accel eration. This voltage is then amplified by a charge amplifier type signal conditioner from whence the signal can be transmitted long distance. (1.000 feet is not uncommon) to the monitor/readout unit. It is calibrated in terms of gravitational units (g), which are proportional to force. Force is ttnc of the most reliable indicators of equipment distress. [Pg.352]

Synthesis of single crystals of TBPDA (Cgo)2 was described elsewhere [4], Photoconductivity was excited by white light of a 150 W halogen tube. Photoconductivity was characterized by current T running through indium contacts attached to one of the faces of the samples with silver paste. The contacts were under direct voltage of 10-50 V. Current values were measured with a charge amplifier connected with PC. The cell filled with the sample was put in a resonator of a standard Radiopan SE/X 2547 spectrometer. [Pg.168]

Signals from both transducers are fed through charge amplifiers. The acceleration signals x. (t) and x o(t) are then fed into a differential amplifier to obtain x.(t)-XQ(t). The force and acceleration signals fj(t) and x (t are fed into a mass cancellation circuit which produces f(t) as an output (see Equation 13). The force and acceleration difference signals f(t) and x (t)-Xo(t) are then fed into a spectrum analyzer where they are Fourier transformed, and multiplied by the appropriate constants according to Equations 12 and 15. G (jw) is then computed internally. [Pg.101]

At low light levels the major source of noise in the CID system is a combination of Johnson noise and shot noise from the first stage of the charge amplifier. The system noise and gain of our CID camera were evaluated using the mean-variance method (10). The system noise for a single readout is 800 electrons (rms) and the gain is set for 1350 electrons per A/D count. [Pg.121]

Signals from the transducers and microphones are amplified, filtered, and analyzed. Typically, charge amplifiers are used for the microphones, and voltage amplifiers, for the transducers. High-pass filters are applied to the signals to eliminate low-frequency mechanical noise, such as pipe vibration. The signals are analyzed by either a true RMS voltmeter or a wide-band spectrum analyzer. [Pg.196]

In principle a biosensor could be fabricated from the material by immobilizing an enzyme on one surface and flowing a substrate solution past the film sensor. A simple charge amplifier might be used to measure the difference between the two surfaces of the sensor. This in turn could be related to concentration. In practice a somewhat different approach needs to be taken. [Pg.150]

The piezoelectric sensor is then connected to a charge amplifier designed to assure an appropriate low-fiequency response to accurately di lay the relatively slow breathii movement A simple Labview program was developed to display the signal in a PC equipped with a data acquisition board. [Pg.383]

Elastic Epoxy (Polysciences Inc., Warrington, PA). When the IPMC-PVDF structure is bent due to the actuation of I PMC or some external force, charges are generated on the PVDF film, which are then measured with a differential charge amplifier as shown in Fig. 8.2. [Pg.203]

Fig. 8.2 Schematic of the differential charge amplifier. Reprinted from [Chen et al. (2007a)j. Fig. 8.2 Schematic of the differential charge amplifier. Reprinted from [Chen et al. (2007a)j.
Experiments were conducted to calibrate the PVDF sensor. To avoid the influence from the actuation voltage, we simply tapped the composite beam tip and measured simultaneously the charge amplifier output and the tip displacement. The displacement was measured with a laser distance sensor (OADM 20I6441/S14F, Baumer Electric, Southington, CT). Fig. 8.3(a) shows the measured charge response under the damped beam oscillation at 42 Hz, while Fig. 8.3(b) depicts the measured charge vs. the actual displacement, from which we can conclude that the beam tip displacement can be well captured by the PVDF sensor. [Pg.204]

Fig. 8.3 Experimental validation of the PVDF sensor and the charge amplifier circuit ... Fig. 8.3 Experimental validation of the PVDF sensor and the charge amplifier circuit ...
The micro-force sensor, attached at the end of the IPMC-PVDF beam, has a similar structure as the IPMC-PVDF composite beam shown in Fig. 8.16, except that the IPMC layer is replaced by a (relatively) rigid passive film. In the prototype, we used 200 pm thick polyester film as the middle layer. The same charge amplifier circuit as in Fig. 8.17, with possibly different gains, is used for the force sensor. Analogous to the case of measuring the bending displacement, one can derive the sensitivity of the force sensor in terms of the electromechanical properties and dimensions of the layers [Chen et al. (2008)]. [Pg.217]

The oscilloscope used for these experiments is of the two-beam type. The horizontal beam is used for time recording, and the vertical one for voltage recording. The oscilloscope is combined with a charge amplifier for the vertical deflection of the beam. [Pg.108]

The principle of the dynamic pressure determination piezoelectric pressure transducer is described in Section 3.1. In its simplest version, the measuring equipment includes a charge amplifier and a storage oscilloscope. From the voltage signal recorded on the oscilloscope, the shock wave pressure as a function of time is obtained and the shock wave impulse as well. [Pg.209]

Instrumentation for the generation of dynamic forces and the monitoring of responses is shown in Fig. 2. Forces applied to the damper-ring are measured by quartz load cells connected to suitable charge amplifiers. The displacement responses of the damper ring are measured by two sets of non-contacting capacitance probes, two in the vertical plane and two in the horizontal plane. [Pg.341]

Thermal offset voltage Thermal offset current Low-level amplifier High-impedance amplifier Charge amplifier Integrating amplifier Wideband amplifier Video amplifier Precision amplifier... [Pg.318]

Preferably, the charges are amplified by a charge amplifier according to Fig. 7.7 and converted into a voltage. The advantage over a simple voltage amplifier is the largely linear frequency response and the associated lower noise, which shows at least... [Pg.162]


See other pages where Charge amplifiers is mentioned: [Pg.45]    [Pg.135]    [Pg.226]    [Pg.16]    [Pg.19]    [Pg.50]    [Pg.229]    [Pg.229]    [Pg.254]    [Pg.635]    [Pg.172]    [Pg.327]    [Pg.226]    [Pg.51]    [Pg.226]    [Pg.118]    [Pg.120]    [Pg.402]    [Pg.65]    [Pg.1885]    [Pg.312]    [Pg.75]    [Pg.76]    [Pg.77]    [Pg.182]    [Pg.261]    [Pg.304]    [Pg.358]    [Pg.17]    [Pg.361]    [Pg.361]    [Pg.365]   
See also in sourсe #XX -- [ Pg.254 ]




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