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Temperature switches measurement

Additional information required to evaluate a sensor includes specifications on the bake-out temperature (during measurement or with the cathode or SEMP switched off), materials used and surface areas of the metal, glass and ceramic components and the material and dimensions for the cathode data is also needed on the electron impact energy at the ion source (and on whether it is adjustable). These values are critical to uninterrupted operation and to any influence on the gas composition by the sensor itself. [Pg.102]

Figure 9.57 shows the system for injecting an inhibitor into a reactor. The corresponding fault tree is presented in Fig. 9.58. The system mainly consists of the injector vessel containing the inhibitor, the corresponding measuring devices and valves, and a catch tank. In case the temperature is too high temperature switch TSH opens valve AV5 and the inhibitor is injected into the reactor by a pressure blanket inside the injector vessel. Redundantly, pressure switch PI opens valve... Figure 9.57 shows the system for injecting an inhibitor into a reactor. The corresponding fault tree is presented in Fig. 9.58. The system mainly consists of the injector vessel containing the inhibitor, the corresponding measuring devices and valves, and a catch tank. In case the temperature is too high temperature switch TSH opens valve AV5 and the inhibitor is injected into the reactor by a pressure blanket inside the injector vessel. Redundantly, pressure switch PI opens valve...
The proposed mechanism is outlined in Fig. 1.6 co-conformation [A ] corresponds to the switch open state and the metastable, co-conformation [B°] the switch closed state of the device. When the applied bias approaches +2 V, the [2]catenane 4" is oxidized to state [A ] wherein the TTF unit is positively charged and so experiences an electrostatic repulsion inside the tetracationic cyclophane, resulting in circumrotation of the macrocyclic polyether and formation of its co-conformational state [B ]. When the voltage is reduced to near-zero bias, the TTF cation radical is reduced, affording the metastable state [B°] which does not return spontaneously to its stable co-conformation [A ] by further circumrotation of the macrocyclic polyether via state [AB ] until the bipyridinium units in the tetracationic cyclophane are reduced. This electromechanical switching mechanism is consistent with temperature-dependent measurements, which indicate... [Pg.9]

Suitable solvent systems for MNA were identified for the solutiorvbased all-optical switching device. Dlmethylformamide (DMF), p-dioxane, propylene carbonate (PC) and tetrahydrofuran (THF) provided high solubility with a wide range of index choices. Solubility of MNA in each solvent (HPLC grade) at room temperature was measured for the determination of the range of refractive index available (Table 1). [Pg.583]

In the second method, the temperature of the calorimeter proper is measured with no power input. First, the calorimeter proper is heated at constant power for a known time interval to attain a certain temperature. After the power is turned off, the temperature is measured. Then, the current supply can again be switched in and next, after switching-off, the temperature will be measured. This cycle can be repeated several times. Such a procedure is called the intermittent-heating method. Both of the measurement procedures described above are used in practice. The first permits control of the temperature of the calorimetric shield in an easier way and it is certainly more convenient to obtain results in a full range of measurement. The second procedure permits study in a precise way of these temperature ranges where interesting phenomena (e.g. unknown phase transitions) are to be observed. [Pg.103]

Indirect point switches such as a pressure switch or temperature switch where the basic measurement is converted mechanically or electrically to a signal which has an adjustable limit value. [Pg.203]

In modem electrical engineering, measurement of temperature can performed by various different methods, starting from a most basic bimetal temperature switches up to laser pre-celebrated semiconductor sensors with high accuracy (Boyes, 2010). The most basic principle of measuring temperature in industrial plants is the use of thermocouple probes by exploiting the thermoelectric effect in metals (called the Seebeck effect) that... [Pg.102]

Another measure to improve the removal of ethanol is air injection into the mixer during the silanization step. Air can be injected from the bottom part of the mixer using existing valves without any special outlet for the injected air. In these experiments air injection is switched on once the compound reached the silanization temperature (145°C) and the rotor speed is adjusted in order to maintain the silanization temperature. Figure 29.13 shows the properties of this compound compared to a compound that was silanized under the same conditions except with air injection switched off. Air injection lowers the Payne effect, Mooney viscosity, and water content in the compound, and ethanol removal is more effective. All other properties are comparable to the properties of a standard silica compound. [Pg.812]

Fe(6-Mepy)2(py)tren] (004)2 Doped in PSS. Magnetic susceptibilities measured for a microcrystalline sample of the complex produce a magnetic moment value = 0.36 pg at 10 K and 0.61 pg at 150 K, followed by a gradual increase to Peff = 2.80 pe at 311 K [138]. Thus 26% of the complexes are in the HS state at 300 K if a magnetic moment of 5.1 Pe is assumed for the pure HS compound. On the other hand, the complex doped into a polystyrene sulfonate (PSS) film does not provide any evidence for a thermal population of the HS state up to 340 K as demonstrated by variable-temperature UV-VIS and Mossbauer spectra. In fact, all the complexes doped into the PSS film are in the LS state at temperatures below 340 K. However, if irradiated by a single pulse of a Q-switched Nd/YAG laser (532 mp), the complex is excited from the LS ground state to the HS J2 states via an intermediate MLCT state and the metal states. The subsequent back relaxation from the excited T2 state to the... [Pg.129]

Fig. 3.21 Example of temperature variation as measured by MIMOS II temperature sensors on MER (i) inside the rover body at MIMOS electronics board (black curve), (ii) outside the rover, at the MIMOS II SH (green and red curves), which is at ambient Martian temperature (a) inside the sensor-head, at the reference absorber position (green), (b) outside the SH at the sample s contact plate (red). Temperatures at the two SH positions are nearly identical (difference less than 2 K). During data transmission between the rover and the Earth (or the relay satellite in Mars orbit) the instrument is switched off resulting in immediate small but noticeable temperature changes (see figure above)... Fig. 3.21 Example of temperature variation as measured by MIMOS II temperature sensors on MER (i) inside the rover body at MIMOS electronics board (black curve), (ii) outside the rover, at the MIMOS II SH (green and red curves), which is at ambient Martian temperature (a) inside the sensor-head, at the reference absorber position (green), (b) outside the SH at the sample s contact plate (red). Temperatures at the two SH positions are nearly identical (difference less than 2 K). During data transmission between the rover and the Earth (or the relay satellite in Mars orbit) the instrument is switched off resulting in immediate small but noticeable temperature changes (see figure above)...
Before performing TPO, the wet catalyst was dried under N2 flowing 10 Fh at 120°C for a period of 17 h before being slowly cooled to 20°C. Once the catalyst was stabilized at 20°C the pure N2 was switched to a 4 vol.% O2 in N2 mixture flowing at 10 1/h while the catalyst s temperature was ramped to 800°C at the rate of 8°/min. The O2 content of the gas mixture leaving the catalyst bed was measured by an Oxynos 100 paramagnetic detector and plotted with respect to either time or temperature. The plot of the vol.% O2 with respect to time was used to determine the O2 consumption of the catalyst. [Pg.500]

Integration of Eq. (6) for S02 in Table V estimates the conversion achieved. Simulation of periodic symmetrical switching between a reactant mixture and air gave an estimate of 99.4% at 12 min after the switch to the S03/S02 reactant mixture in reasonable agreement with the overall conversion of 98.8% measured by Briggs et al. (1977). With respect to model sensitivity, it was found that bed midpoint temperature was sensitive to the wall and gas to particle heat transfer coefficients. An extensive study of sensitivity, however, was not undertaken. [Pg.217]


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See also in sourсe #XX -- [ Pg.377 , Pg.382 ]




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