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Water temperature, constant

Schulenberg and Starflinger (2012) reported about a constant pressure start-up and shut-down system for the three-pass core design of the HPLWR, trying to keep the feed-water temperature constant to minimize thermal stresses of the reactor pressure vessel. This concept also includes a warm-up procedure for the deaerator during startup from cold conditions. A battery of cyclone separators is foreseen outside of the containment to produce some steam from depressurized hot coolant of the reactor. [Pg.213]

In a 250 ml. flask place 75 ml, of water, 24 g. (20 ml.) of concentrated hydrochloric acid and 14g. (13-7 ml.) of aniline. Shake vigorously (1) and then add 50 g. of crushed ice. Rim in a solution of 5-2 g. of so um nitrite in 12 ml. of water, with constant shaking, during a period of 5-10 minutes. Allow to stand with frequent shaking (1) for 15 minutes, and add a solution of 21 0 g. of crystallised sodium acetate in 40 ml. of water during 5 minutes. A yellow precipitate of diazoaminobenzene begins to form immediately allow to stand with frequent shaking for 45 minutes and do not allow the temperature to rise above 20° (add ice. [Pg.626]

For most cooling towers in the United Kingdom, the exit air is saturated at a temperature close to the mean water temperature in the tower. Hence, if the water temperatures and the air inlet conditions are known, AH, AT, and AT can all be calculated, and Tcan be deterrnined. It was found that the quantity C was approximately constant for these towers, ca 0.4—0.5 (34). If the value of C is known for a given tower, then the left side of equation 49 can be computed and, setting this equal to Z9, the allowable Hquid flow rate can be found. Alternatively, when and air-inlet conditions are given, the... [Pg.105]

Figure 12-16 illustrates the type of performance curve furnished by the cooling-tower manufacturer. This shows the variation in performance with changes in wet-bulb and hot-water temperatures while the water quantity is maintained constant. [Pg.1165]

Recent developments in cooling-tower fan energy management also include automatic variable-pitch propeller-type fans and inverter-type devices to permit variable fan speeds. These schemes involve tracking the loaa at a constant leaving-water temperature. [Pg.1166]

The variable-pitch arrangement at constant motor speed changes the pitch of the olades through a pneumatic signal from the leaving-water temperature. As the thermal load and/or the ambient wet-bulb temperature decreases, the blade pitch reduces air flow and less fan energy is required. [Pg.1166]

If the water temperature is held constant and the water is still, Table 7.7 can be used to evaluate the temperature of the water surface (at room air temperature 20 °C and RH = 70%). When the water is stirred, the surface temperature can be assumed to be equal to the mean water temperature. [Pg.429]

The metabolic rate can be measured in several ways. When no external work is being performed, the metabolic rate equals the heat output of the body. This heat output can be measured by a process called direct calorimetry. In this process, the subject IS placed m an insulated chamber that is surrounded by a water jacket. Water flows through the jacket at constant input temperature. The heat from the subject s body warms the air of the chamber and is then removed by the water flowing through the jacketing. By measuring the difference between the inflow and outflow water temperatures and the volume of the water heated, it is possible to calculate the subject s heat output, and thus the metabolic rate, in calories. [Pg.176]

Figure 6-32 illustrates ejector systems with large condensable loads which can be at least partially handled in the precondenser. Controls are used to maintain constant suction pressure at varying loads (air bleed), or to reduce the required cooling water at low process loads or low water temperatures [2]. The cooler W ater must not be throttled below the minimum (usually 30%-50% of maximum) for proper contact in the condenser. It may be controlled by tailwater temperature, or by the absolute pressure. [Pg.379]

Figure 9-111. Typiccil effect of hot water temperature on tower characteristic, KaV/L at constant L, Ga wet buib temperature and packed height. Note L and G shown in chart are hourly rates. Reproduced by permission of the American Institute of Chemical Engineers, Kelly, N. W., and Swenson, L. K., Chemical Engineering Progress, V. 52, No. 7 (1956) p. 263 all rights reserved. Figure 9-111. Typiccil effect of hot water temperature on tower characteristic, KaV/L at constant L, Ga wet buib temperature and packed height. Note L and G shown in chart are hourly rates. Reproduced by permission of the American Institute of Chemical Engineers, Kelly, N. W., and Swenson, L. K., Chemical Engineering Progress, V. 52, No. 7 (1956) p. 263 all rights reserved.
In other words, at its boiling point water requires the further addition of 970 Btu of energy to convert one pound of water to steam, which is 5.39 times as much energy as required to raise the water temperature from 0 °C (32 °F) to 100 °C. The temperature of the hot water remains constant until it has been entirely vaporized, at which point the steam is fully saturated with heat and the enthalpy of the steam (heat content as calculated from a starting point ofO °C) is 1,150 Btu/lb. [Pg.4]

Two methods of changing the humidity and temperature of a gas from Aidj. JP x i to B(()2. J 2) may be traced on the humidity chart as shown in Figure 13.11. The first method consists of saturating the air by water artificially maintained at the dew point of air of humidity (line AC) and then heating at constant humidity to 82 (line CB). In the second method, the air is heated (line AD) so that its adiabatic saturation temperature corresponds with the dew point of air of humidity JP2- It is then saturated by water at the adiabatic saturation temperature (line DC) and heated at constant humidity to 82 (line CB). In this second method, an additional operation — the preliminary heating—is carried out on the air, hut the water temperature automatically adjusts itself to the required value. [Pg.760]

C06-0018. Adding 1.530X 10 Jof electrical energy to a constant-pressure calorimeter changes the water temperature from 20.50 °C to 21.85 °C. When 1.75 g of a solid salt is dissolved in the water, the temperature falls from 21.85 °C to 21.44 °C. Find the value of gp for the solution process. [Pg.399]

The cold-water supply for the tempered water system will be ordinary cooling water. No attempt will be made to keep its temperature constant. The hot-water temperature will be maintained constant by opening and closing the steam input to the hot-water storage tank. Close control is not necessary. [Pg.175]

Samples were analyzed by gas chromatography (GC). Water solubility was determined by equilibration of analytical grade material with water at constant temperature. Equilibrium was approached from both under and super saturation conditions and samples were analyzed by GC. Vapor pressures were determined by the Knudsen effusion method. [Pg.232]

Alaee, M., Whittal, R.M., Strachan, W.M., J. (1996) The effect of water temperature and composition on Henry s law constant for various PAHs. Chemosphere 32, 1153-1164. [Pg.900]

The calculation of the concentrations of dissolved carbon species from total dissolved carbon and alkalinity is carried out in subroutine CARBONATE, presented in program DGC09. I have specified the equilibrium constants as functions of water temperature by fitting straight lines to the values tabulated by Broecker and Peng (1982, p. 151). [Pg.49]

The ability to smell a solute relies on it having a vapour pressure above the solution. Analysing the vapour above a gravy dish shows that it contains molecules of both solvent (water) and solute (gravy), hence its damp aroma. The vapour pressures above the gravy dish do not alter, provided that we keep the temperature constant and maintain the equilibrium between solution and vapour. [Pg.309]

One of the major differences among the phases of water at the molecular level is the motions of the water molecules. Using the phase diagram (Figure 7), we can follow the effects of temperature and pressure on the molecular mobility of water. For example, if we hold pressure constant (say at 1 atm) and increase temperature, molecular mobility increases as we move from the solid to the liquid to the gas phase regions. Conversely, if we hold temperature constant (say at 100°Q and increase pressure, molecular mobility decreases as we move from the gas to the liquid phase region. [Pg.13]


See other pages where Water temperature, constant is mentioned: [Pg.497]    [Pg.497]    [Pg.505]    [Pg.353]    [Pg.474]    [Pg.250]    [Pg.1123]    [Pg.1163]    [Pg.1166]    [Pg.1146]    [Pg.66]    [Pg.70]    [Pg.144]    [Pg.771]    [Pg.841]    [Pg.167]    [Pg.592]    [Pg.505]    [Pg.108]    [Pg.630]    [Pg.84]    [Pg.46]    [Pg.49]    [Pg.605]    [Pg.85]    [Pg.930]    [Pg.307]    [Pg.79]    [Pg.403]    [Pg.801]   
See also in sourсe #XX -- [ Pg.24 , Pg.27 ]




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