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Amplifier circuit

Some proportional detectors are combined in the same instrument with a suitable transducer which can perform some of the functions of a controller. For example, for pneumatic systems the primary sensing element actuates a variable air jet, thus modulating an air pressure which is transmitted to a further controller or direct to the controlled device. Electric and electronic detectors such as the infrared detector include the sensing and amplifying circuits of the instrument. [Pg.327]

R., Gelperin, A., Katz, H. E. and Bao, Z. (2001) Organic oscillator and adaptive amplifier circuits for chemical vapor sensing./. Appl. Phys., 91, 10140. [Pg.201]

The preamplifier amplifies the voltage pulse. Further amplification is obtained by sending the signal through an amplifier circuit (typically about 10 volts maximum). The pulse size is then determined by a single channel analyzer. Figure 10 shows the operation of a single channel analyzer. [Pg.48]

In this experiment, you will become familiar with an instrumentation amplifier circuit that is used to amplify weak sensor output signals. [Pg.171]

Figure 7.7. Detector amplifier circuit used in our studies. HSH = signal high HOUT = signal out HSL = signal low PF = picofarad. Figure 7.7. Detector amplifier circuit used in our studies. HSH = signal high HOUT = signal out HSL = signal low PF = picofarad.
The tunneling current occurring in STM is very small, typically from 0.01 to 50 nA. The current amplifier is thus an essential element of an STM, which amplifies the tiny tunneling current and converts it into a voltage." The performance of the current amplifier, to a great extent, influences the performance of the STM. There are natural limits for the overall performance of current amplifiers, as determined by the thermal noise, stray capacitance, and the characteristics of the electronic components. In this section, we will present these issues by analyzing several typical current amplifier circuits, which can be easily made and used in actual STMs. [Pg.251]

One of the first things you should do when you are simulating an amplifier circuit is to check the transistor operating point. If the transistor bias is incorrect, none of the other analyses will be valid. If another analysis does not make sense, check the operating point. When PSpice finds the bias point, it assumes that all capacitors are open circuits and that all inductors are short circuits. [Pg.187]

The frequency components of a signal can be obtained directly from PSpice by enabling the Fourier option in the Time Domain (Transient) setup. We will use the common-emitter amplifier circuit shown on page 361. To modify the Time Domain (Transient) setup select PSpice and then Edit Simulation Profile. [Pg.371]

We will now find the minimum and maximum gain of the amplifier shown on page 298. The amplifier circuit is repeated below ... [Pg.526]

Three different measurements were made in order to characterize the performance of this amplifier circuit and show the correlation of the breadboard results to the SPICE models. The three inputs and their resulting measurements are described in detail in Table 6.1. [Pg.160]

TABLE 6.1 Characteristic Measurements Made on Class AB Amplifier Circuit... [Pg.161]

Figure 4.1 Basic principles of a Faraday cup and amplifier circuit a) incoming charge of ions is converted into a voltage by an operational amplifier with a high ohmic feedback resistor (R) and b) dual ion detector for direct measurements of two ion currents ( and l2 using two amplifiers with resistors R, and R2. Figure 4.1 Basic principles of a Faraday cup and amplifier circuit a) incoming charge of ions is converted into a voltage by an operational amplifier with a high ohmic feedback resistor (R) and b) dual ion detector for direct measurements of two ion currents ( and l2 using two amplifiers with resistors R, and R2.
In order to appreciate the principles of analog semi-integration, let us first review the classical operational amplifier circuits shown in Fig. 30. The output of circuit (a) is a voltage proportional to the instantaneous value of the current input... [Pg.134]

Fig. 30. Classical operational amplifier circuits, (a) A current follower (b) a current integrator. Fig. 30. Classical operational amplifier circuits, (a) A current follower (b) a current integrator.
D. Stout and M. Kaufman, Handbook of Operational Amplifier Circuit Design, McGraw-Hill, New York, 1976. [Pg.236]

Rotating platinum screens have been used for electrogravimetric analyses. Commercial instruments employ two concentric cylindrical platinum screen electrodes with one or both electrodes rotating to increase convection. The cell itself is usually a beaker with a sample volume of about 150 mL. Typically, no cell top is used, and when running multiple analyses, there should be adequate ventilation to prevent accumulation of hydrogen. A simple operational amplifier circuit can be constructed for the instrument. The commercial instruments available are expensive given the simplicity of this type of experiment. [Pg.278]

This expression is the basic description for the use of the pyroelectric effect in a host of sensor applications including the well known optical detection devices (82,83). A particularly useful way of describing this type of system is with an equivalent circuit where the pyroelectric current generator drives the pyroelectric impedance and the measuring amplifier circuit as shown in Figure 11. [Pg.22]

Electrical measurements with both types of cells were made by using two devices as the gain-controlling elements of an inverting operational amplifier circuit which was driven with a constant input voltage (E. ). The ratio of the resistance of the reference device,... [Pg.157]

Katz, and Z. Bao, Organic oscillator and adaptive amplifier circuits for chemical vapor sensing , Journal... [Pg.421]

Detection of the particles is accomplished by means of their attenuation of a light beam provided by a halogen lamp and collimated by two slit assemblies. A silicon photodiode and an operational amplifier circuit are used to monitor the light intensity. Adjustable gain and offset potentiometers are located on the control module. The signal can be displayed on a stripchart recorder and is monitored by means of a digital panel meter. [Pg.181]

The home-made heat-flow calorimeter used consisted of a high vacuum line for adsorption measurements applying the volumetric method. This equipment comprised of a Pyrex glass, vacuum system including a sample holder, a dead volume, a dose volume, a U-tube manometer, and a thermostat (Figure 6.3). In the sample holder, the adsorbent (thermostated with 0.1% of temperature fluctuation) is in contact with a chromel-alumel thermocouple included in an amplifier circuit (amplification factor 10), and connected with an x-y plotter [3,31,34,49], The calibration of the calorimeter, that is, the determination of the constant, k, was performed using the data reported in the literature for the adsorption of NH3 at 300 K in a Na-X zeolite [51]. [Pg.286]

The rapid development of solid-state electronic devices in the last two decades has had a profound effect on measurement capabilities in chemistry and other scientific fields. In this chapter we consider some of the physical aspects of the construction and function of electronic components such as resistors, capacitors, inductors, diodes, and transistors. The integration of these into small operational amplifier circuits is discussed, and various measurement applications are described. The use of these circuit elements in analog-to-digital converters and digital multimeters is emphasized in this chapter, but modern integrated circuits (ICs) have also greatly improved the capabilities of oscilloscopes, frequency counters, and other electronic instruments discussed in Chapter XIX. Finally, the use of potentiometers and bridge circuits, employed in a number of experiments in this text, is covered in the present chapter. [Pg.538]

Operational amplifier circuit to deliver current at a standard Weston cell voltage. [Pg.554]

Another commonly used detector is the scintillation detector. This makes use of a crystal that produces a scintillation (pulse of visible light) upon absorption of an x-ray photon. The visible light is detected by a photomultiplier tube and associated amplifier circuit, which is sensitive enough to detect nearly every scintillation. The scintillating crystal is usually sodium iodide doped with an activator such as thallous iodide. [Pg.613]

The metastability phenomena influence the performance of the active matrix arrays. Defect creation in the channel causes a threshold voltage shift when a TFT is held on for an extended time and results in a slow drift of the on-current. Fortunately the rate of defect creation is low at room temperature and represents a minor problem. There is a larger effect on the characteristics of the high voltage TFTs. Resistors fabricated from n a-Si H change their resistance slowly because of defect equilibration and can affect the gain of amplifier circuits. [Pg.395]


See other pages where Amplifier circuit is mentioned: [Pg.420]    [Pg.341]    [Pg.22]    [Pg.266]    [Pg.154]    [Pg.298]    [Pg.379]    [Pg.160]    [Pg.158]    [Pg.924]    [Pg.536]    [Pg.88]    [Pg.428]    [Pg.72]    [Pg.24]    [Pg.101]    [Pg.35]    [Pg.226]    [Pg.185]    [Pg.126]    [Pg.546]    [Pg.547]   
See also in sourсe #XX -- [ Pg.185 ]




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