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Current time-temperature integrators

The complete analytical system is under the control of a Motorola 6802 microprocessor. All switching of gas flows, timing, temperature control, error detection, analog to digital conversion, FID current measurement, signal Integration and manipulation, and data storage and transfer are controlled by this system. [Pg.226]

Because dark current limits the integration times obtainable at room temperature, Peltier cooling (to -150C) is used to reduce thermal population of the conduction band. In contrast to the silicon vidicon and the SIT [vide infra], where the presence of intense radiation may bloom out the entire sensor, blooming is greatly reduced with photodiode arrays even when intense lines saturate individual diodes. [Pg.42]

A comparison of the results of the predictions of Table 5-5 with values obtained via the integration of the spectral results calculated from the narrowband model in RADCAL is provided in Fig. 5-22. Here calculations are shown for pcL =pwL = 0.12 atm m and a gas temperature of 1500 K. The RADCAL pr ictions are 20 percent higher than the measurements at low values of pL and are 5 percent higher at the lai e values of pL. An extensive comparison of different sources of emissivity data shows that disparities up to 20 percent are to be expected at the current time [Lallemant, N., Sayre, A., and Weber, R., Prog. Energy Combust. Sci., 22, 543-574, (19 )]. However, smaller errors result for the range of the total emissivity measurements presented in the Hottel emissivity tables. This is demonstrated in Example 11. [Pg.718]

The maximum integration time AT is limited by the dark current /d, which therefore also limits the attainable signal-to-noise ratio. At room temperature typical integration times are in the millisecond range. Cooling of the diode array by Peltier cooling down to -40 C drastically reduces the dark current and allows integration times of 1 —100 s. The minimum detectable... [Pg.197]

The power consumption of the barrel and die heaters can be determined by measuring voltage and current to the heater. This works well in current proportioned temperature control. It does not work well with on-off control or time-proportioning temperature control. In the latter case, a wattmeter should be used with a power integrating function. In this case, the integrated power over a certain time period can be measured so that the average power consumption of the barrel heater can be established. Commercial extruders generally do not have sufficient instrumentation... [Pg.108]

Measured perform lnce and figures of merit are summarized in Table 1. Dark currents as low as 18e /s were measured, with a strong onset of ther-maRy activated current at temperatures above 8K. This dark current would aRow integration times on the order of lO s in ultra-low badcground condi-... [Pg.327]

By the integrating the current over the time for each peak we determine the number of charge carriers which equals the number of traps N, (under the condition that all traps were occupied at the starting temperature) ... [Pg.152]

The considerations so far rely on constant heating power, and the way how this power is applied to the microhotplate does not play a role. In fact, a monolithically integrated control circuitry does not apply constant power but acts as an adjustable current source. Moreover, for measuring the thermal time constant experimentally, either a rectangular voltage or rectangular current pulse is applied. Analyzing the dynamic temperature response of the system leads to a measured time constant, which... [Pg.26]


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See also in sourсe #XX -- [ Pg.44 , Pg.176 , Pg.177 , Pg.178 , Pg.179 , Pg.180 , Pg.181 , Pg.182 , Pg.183 , Pg.184 ]




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