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Instrumentation amplifiers for

Song, S., et al., 2013. A low-power noise scalable instrumentation amplifier for fetal monitoring applications. In 2013 IEEE International Symposium on Circuits and Systems (ISCAS2013), pp. 1926—1929. Available at http //ieeexplore.ieee.org/lpdocs/epic03/ wrapper.htm amumber=6572244. [Pg.268]

FIGURE 9.4 Circuit drawings for three different realizations of instrumentation amplifiers for biomedical applications. (a) Voltage follower input stage, (b) improved, amplifying input stage, and (c) 2-op-amp version. [Pg.140]

PalMs-Areny, R. and J.G. Webster. 1990. Composite instrumentation amplifier for biopotentials. Annals of Biomedical Engineering. 18, 251-262. [Pg.149]

FIGURE 5-4 An Instrumentation amplifier for reducing the effects of noise common to both inputs. The gain of the circuit is controlled by resistors RJa and Kfig. [Pg.66]

Denison T, Consoer K, Santa W, Avestruz AT, Cooley J, Kelly A (2007) A 2 p.W 100 nV/rtHz chopper-stabilized instrumentation amplifier for chronic measurement of neural field potentials. IEEE J Sohd-State Circ 42 2934-2945... [Pg.323]

The flow capacity of the transducer can be increased bv adding a booster relav like the one shown in Fig, 8-7.3/ , The flow capacity of the booster relav is nominally fiftv to one hundred times that of the nozzle amplifier shown in Fig, 8-7.3 3 and makes the combined trans-diicer/booster suitably responsive to operate pneumatic actuators. This type of transducer is stable into all sizes of load volumes and produces measured accuracy (see Instrument Society of America [ISA]-S5l, 1-1979, Process Instrumentation Terminology for the definition of measured accuracy) of 0,5 percent to 1,0 percent of span. [Pg.782]

The reference electrode (RE) is connected to the inverting input of an operational amplifier (for example Texas Instruments TL 074), and the setpoint is applied between ground and the noninverting input of the operational amplifier. For electronic reasons Equation 6.2-1 applies. [Pg.296]

Parsons was, first and foremost, a compulsive inventor. He spent his days inventing everything from children s toys to the Auxetophoiie, a mechanical amplifier for stringed musical instruments. His success as an inventor lies in his inquisitive nature and the fact that he was equally comfortable with the-oity and practice. [Pg.934]

Obtain the sensor amplifier module board from your instructor, and examine it closely as follows. Notice the outlined horizontal box in the top center of the board—it is labeled instrumentation amplifier. Notice the symbol of an amplifier in this box (refer to Figure 6.10). Also, notice the inputs to the amplifier (labeled P14 and P15). These are sockets for the wires that will bring the input signals to the amplifier. It is the difference between these two signals that is amplified. The output of the amplifier (the amplified signal) is connected to sockets P19 and P20. Wires inserted into these sockets allow us to observe the amplified signal with a voltmeter. [Pg.171]

Since the instrumentation amplifier is a difference amplifier, it amplifies the difference between the inputs at P14 and P15 by a factor set by the operator. This factor is set at the switch box labeled SW1. Notice that the amplification factor can be X5, XlO, X50, or X100. There are four switches, one for each of the factors. If all the switches are set to the left (off), then the amplification factor is Xl. When checking out each amplification factor, set all switches to off except for the factor being tested. [Pg.173]

Figure 2 shows a photoelectric cell suitable for the direct determination of the photoelectric work function of a metal under the conditions of chemisorption. The electrically conducting catalyst, used as a cathode, either is inserted as a metal foil B or is evaporated from E to B. A metal layer coating the inside of the photoelectric cell serves as the anode, with a lead wire C. B can be heated electrically the leads fc are sealed into quartz and connected to an instrument (electrometer or amplifier) for... [Pg.308]

Figure 6. Instrumental schematic for vacuum UV photofragmentation-laser induced fluorescence measurement of ammonia SHGC, second harmonic generation crystal SFMC, sum frequency mixing crystal BS, beam splitter BD, beam dump TP, turning prism CL, cylindrical lens R, reflector TD, trigger diode OSC, oscillator cell AMP, amplifier cell BE, beam expander G, grating OC, output coupler M, mirror BC, beam combiner L, lens A, aperture PD, photodiode SC, sample cell RC, reference cell FP, filter pack SAM.PMT, sample cell photomultiplier REF.PMT, reference cell photomultiplier PP, additional photomultiplier port EX, exhaust and CGI, calibration gas inlet to flow line. (Reproduced with permission from reference 15. Copyright 1990 Optical Society of America.)... Figure 6. Instrumental schematic for vacuum UV photofragmentation-laser induced fluorescence measurement of ammonia SHGC, second harmonic generation crystal SFMC, sum frequency mixing crystal BS, beam splitter BD, beam dump TP, turning prism CL, cylindrical lens R, reflector TD, trigger diode OSC, oscillator cell AMP, amplifier cell BE, beam expander G, grating OC, output coupler M, mirror BC, beam combiner L, lens A, aperture PD, photodiode SC, sample cell RC, reference cell FP, filter pack SAM.PMT, sample cell photomultiplier REF.PMT, reference cell photomultiplier PP, additional photomultiplier port EX, exhaust and CGI, calibration gas inlet to flow line. (Reproduced with permission from reference 15. Copyright 1990 Optical Society of America.)...
The electronic instrumentation necessary for the operation of the proportional counter is shown in Figure 18.6. Pulses from the detector pass through a preamplifier and amplifier, where they are shaped and amplified. Emerging from the amplifier, the pulses go to a discriminator. The discriminator is set so as not to trip on noise pulses but rather to trip on radiation pulses of any larger size. The number of discriminator pulses produced is recorded by the scaler. [Pg.546]

At the time US-A-3808435 (Texas Instruments Incorporated, USA, 30.04.74) was filed, a conventional infrared detector system had an array of infrared detectors and each detector had an amplifier for amplifying its output. The amplified output was connected to a multiplexer... [Pg.138]

Figure 8. Instrument schematic for a ratiometric modulation and the corresponding software to monitor oxygen using polymer immobilized [(dppe)Pt S2C2(CH2CH2-.lV-2-pyridinium) ] [BPh4]. [Adapted from (20).] LED-D, LED-frequency driver LED, 470 light emitting diode F(l), 470 40 nm bandpass filter SP, sensing patch F(2), 550 nm longpass PD photodiodes TIA transimpedance amplifiers. The frequencies used were co — 400 Hz and oy — 100 kHz. Figure 8. Instrument schematic for a ratiometric modulation and the corresponding software to monitor oxygen using polymer immobilized [(dppe)Pt S2C2(CH2CH2-.lV-2-pyridinium) ] [BPh4]. [Adapted from (20).] LED-D, LED-frequency driver LED, 470 light emitting diode F(l), 470 40 nm bandpass filter SP, sensing patch F(2), 550 nm longpass PD photodiodes TIA transimpedance amplifiers. The frequencies used were co — 400 Hz and oy — 100 kHz.
Fig. 2.17. Schematic layout of a microscope spectrophotometer system used to measure polarized absorption spectra of very small mineral crystals. The computer-operated, single-beam instrument shown here comprises a polarizing microscope equipped with a stabilized light source (xenon arc lamp or tungsten lamp cover the range 250-2000 nm), a modulator that chops the light beam with a frequency of 50 Hz (the amplifier for the photodetector signals is modulated with the same phase and frequency), and a Zeiss prism double monochromator. Single crystals as small as 10 ji.m diameter may be measured with this system. A diamond-windowed high-pressure cell can be readily mounted on the microscope scanning table for spectral measurements at very high pressures (after Burns, 1985, reproduced with the publisher s permission). Fig. 2.17. Schematic layout of a microscope spectrophotometer system used to measure polarized absorption spectra of very small mineral crystals. The computer-operated, single-beam instrument shown here comprises a polarizing microscope equipped with a stabilized light source (xenon arc lamp or tungsten lamp cover the range 250-2000 nm), a modulator that chops the light beam with a frequency of 50 Hz (the amplifier for the photodetector signals is modulated with the same phase and frequency), and a Zeiss prism double monochromator. Single crystals as small as 10 ji.m diameter may be measured with this system. A diamond-windowed high-pressure cell can be readily mounted on the microscope scanning table for spectral measurements at very high pressures (after Burns, 1985, reproduced with the publisher s permission).
Operational amplifier A versatile analog electronic amplifier for performing mathematical tasks and for conditioning output signals from instrument transducers. [Pg.1113]

FIGURE 4.16 Instrumentation scheme for impedance measurements 1 generator, 2, 4, and 6 amplifiers 3 attenuator 5 filter 7 zirconia oxygen sensor 8 osdlloscope C capacitance and Z electrochemical sensor impedance. (From Zhuiykov, S., In-situ diagnostics of solid electrolyte sensors measuring oxygen activity in melts by developed impedance method, Meas. Sci. Technol. 17 (2006) 1570-1578. With permission.)... [Pg.164]


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See also in sourсe #XX -- [ Pg.407 ]




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