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Heat total rate

Given the mechanisms and temperatures, waste combustion systems typically employ higher percentages of excess air, and typically also have lower cross-sectional and volumetric heat release rates than those associated with fossil fuels. Representative combustion conditions are shown in Table 11 for wet wood waste with 50—60% moisture total basis, municipal soHd waste, and RDF. [Pg.58]

If the substitute fuel is of the same general type, eg, propane for methane, the problem reduces to control of the primary equivalence ratio. For nonaspiring burners, ie, those in which the air and fuel suppHes are essentially independent, it is further reduced to control of the fuel dow, since the air dow usually constitutes most of the mass dow and this is fixed. For a given fuel supply pressure and fixed dow resistance of the feed system, the volume dow rate of the fuel is inversely proportional to. ypJ. The same total heat input rate or enthalpy dow to the dame simply requires satisfactory reproduction of the product of the lower heating value of the fuel and its dow rate, so that WI = l- / remains the same. WI is the Wobbe Index of the fuel gas, and... [Pg.524]

An equation representing an energy balance on a combustion chamber of two surface zones, a heat sink Ai at temperature T, and a refractory surface A assumed radiatively adiabatic at Tr, inmost simply solved if the total enthalpy input H is expressed as rhCJYTv rh is the mass rate of fuel plus air and Tp is a pseudoadiabatic flame temperature based on a mean specific heat from base temperature up to the gas exit temperature Te rather than up to Tp/The heat transfer rate out of the gas is then H— — T ) or rhCp(T f — Te). The... [Pg.586]

Rotary kilns operate at various temperatures throughout their length. A graph of approximate gas and charge temperatures for wet-process cement is shown in Fig. 12-67. The maximum charge temperature is 1700 to 1800 K for the gases, 1800 to 1925 K. Overall heat-transfer rates have been estimated to be in the range of 25 to 60 KJ/(s-m ) on the basis of total kiln volume. [Pg.1206]

The overall heat-transfer rate is almost entirely dependent upon the film coefficient between the inner jacket wall and the solids, which depends to a large extent on the solids characteristics. Overall coefficients may range from 30 to 200 J/(m s K), based upon total area if the diyer walls are kept reasonably clean. Coefficients as low as 5 or 10 may be encountered if caking on the walls occurs. [Pg.1214]

As shown in Fig. 13-92, methods of providing column reflux include (a) conventional top-tray reflux, (b) pump-back reflux from side-cut strippers, and (c) pump-around reflux. The latter two methods essentially function as intercondenser schemes that reduce the top-tray-refliix requirement. As shown in Fig. 13-93 for the example being considered, the internal-reflux flow rate decreases rapidly from the top tray to the feed-flash zone for case a. The other two cases, particularly case c, result in better balancing of the column-refliix traffic. Because of this and the opportunity provided to recover energy at a moderate- to high-temperature level, pump-around reflirx is the most commonly used technique. However, not indicated in Fig. 13-93 is the fact that in cases h and c the smaller quantity of reflux present in the upper portion of the column increases the tray requirements. Furthermore, the pump-around circuits, which extend over three trays each, are believed to be equivalent for mass-transfer purposes to only one tray each. Bepresentative tray requirements for the three cases are included in Fig. 13-92. In case c heat-transfer rates associated with the two pump-around circuits account for approximately 40 percent of the total heat removed in the overhead condenser and from the two pump-around circuits combined. [Pg.1330]

The heat evolution rate per unit mass, the vent capacity per unit area, physical properties (e.g.. latent heat of liquid, specific heat, and vapor/liqnid specific volumes) are constant. It allows for total vapor-liqnid disengagement of fluids that are not natural" surface active foamers. ... [Pg.974]

H = total heat transfer rate, BTU/hr. For heat exchangers. Ref [33a] recommends that this value be taken as the maximum exchanger duty during operation. [Pg.446]

The total furnace heat absorption may be estimated by using the calculated furnace exit gas temperature and analysis to determine the enthalpy (excluding the latent heat of water vapor) and thus deducting the heat rejection rate from the net heat input rate. [Pg.347]

Mullis (M10), Bastress (B4), and Carlson and Seader (Cl) have conducted experimental studies to determine the heat-transfer characteristics of typical rocket-exhaust igniters. In these studies, the total rate of heat transfer to the propellant or simulated propellant surface was measured as a function of mass flow rate, geometry, and impingement angle between the igniter exhaust... [Pg.21]

It has been shown that for heat flux rates up to 3.2 kW/m2 the product fdb is constant and that the total heat flow per unit area q is proportional to n. From equation 9.191 it is seen that qb is proportional to n at a given pressure, so that q oc qb. [Pg.491]

Transient computations of methane, ethane, and propane gas-jet diffusion flames in Ig and Oy have been performed using the numerical code developed by Katta [30,46], with a detailed reaction mechanism [47,48] (33 species and 112 elementary steps) for these fuels and a simple radiation heat-loss model [49], for the high fuel-flow condition. The results for methane and ethane can be obtained from earlier studies [44,45]. For propane. Figure 8.1.5 shows the calculated flame structure in Ig and Og. The variables on the right half include, velocity vectors (v), isotherms (T), total heat-release rate ( j), and the local equivalence ratio (( locai) while on the left half the total molar flux vectors of atomic hydrogen (M ), oxygen mole fraction oxygen consumption rate... [Pg.174]

Desorption Rates. Using the above model for the temperature jump associated with pulsed laser heating, the rate of desorption versus time and the total number of molecules desorbed from a finite surface area heated by the laser can be calculated. For the particular case of first-order desorption kinetics, the desorption rate is ... [Pg.240]

This result for the most likely change in moment is equivalent to Fourier s law of heat conduction. To see this take note of the fact that in the steady state the total rate of change of moment is zero, E = 0, so that the internal change is... [Pg.63]

Physically the variational procedure based on the second entropy may be interpreted like this. If the flux E were increased beyond its optimum value, then the rate of entropy consumption by the subsystem would be increased due to its increased dynamic order by a greater amount than the entropy production of the reservoirs would be increased due to the faster transfer of heat. The converse holds for a less than optimum flux. In both cases the total rate of second entropy production would fall from its maximum value. [Pg.65]

Calculate the rate of vaporisation from the total heat-transfer rate, and compare with the value assumed in step 1. If the values are sufficiently close, proceed. If not, return to step 2 and repeat the calculations for a new design. [Pg.742]

Q, Total heat-transfer rate from gas phase ml2t... [Pg.788]

The latent heat transport accounts for only 2% of the total heat flux in this case. However, it was observed by several investigators that the total heat transfer rate is proportional to this value, <7, lenl, because it is proportional to the bubble volume and the number of bubbles that cause intense agitation of the liquid layer close to the surface. This agitation, termed microconvection, together with the liquid-vapor exchange, were considered to be the key to excellent characteristics of boiling heat transfer (Forster and Greif, 1959). [Pg.75]

Since the total heat input represents the time integral of the heat transfer rate, it is evident from equations 10.1.9, 10.2.7, and 10.2.8 that... [Pg.353]

Total Heat Release From Wall Assemblies. We examined the total heat release from the wall assemblies as total heat contribution. The total heat release is obtained by integrating the area under the heat release rate curve with time and it is expressed in megajoules (MJ). The total heat release data from ignition to different times are shown in Table III for the wall assemblies. [Pg.421]

In general, walls A-l, B-l, and C-l had the highest heat release. Walls A-2, B-2, and C-2 had consistently less heat contribution because of the insulation. Walls A-3, B-3, and 03 and A-4, B-4, and C-4 had no significant heat contribution. The values in these tests vary because of initial errors associated with the perturbations at the beginning of the tests. However, total heat release did not grow, indicating zero heat release rate when gypsum was present. [Pg.425]

The total rate of heat release in the room is assumed to come from five sources the gas burner, the vertical wall area behind the burner, a horizontal strip of material corresponding to the vertical height og the ceiling jet at the ceiling-wall intersection, the wall... [Pg.575]

The amount of heat actually taken up by the particles was an important quantity, as tubes operate under heat transfer limited conditions near the tube inlet. Fig. 30 shows a plot of Q against r, where Q was the total energy flow into the solid particles, for the entire segment. For inlet conditions, Q varied strongly at lower r, but was almost constant at higher values. As rcut/rp decreased from 0.95 to 0.0 and the effectiveness factor increased from nearly zero to one, the active solid volume increased by a factor of 7. If the solid temperature had remained the same, the heat sink would also have had to increase sevenfold. This could not be sustained by the heat transfer rate to the particles, so the particle temperature had to decrease. This reduced the heat sink and increased the driving force for heat transfer until a balance was found, which is represented by the curve for the inlet in Fig. 30. [Pg.376]

From the circuit in Figure 11.7, the equivalent conductance, h, allows the total heat flow rate to be represented as... [Pg.351]


See other pages where Heat total rate is mentioned: [Pg.466]    [Pg.309]    [Pg.316]    [Pg.926]    [Pg.934]    [Pg.367]    [Pg.537]    [Pg.276]    [Pg.537]    [Pg.534]    [Pg.686]    [Pg.137]    [Pg.77]    [Pg.175]    [Pg.175]    [Pg.40]    [Pg.108]    [Pg.430]    [Pg.543]    [Pg.254]    [Pg.461]    [Pg.421]    [Pg.545]    [Pg.547]    [Pg.398]    [Pg.374]   
See also in sourсe #XX -- [ Pg.63 ]




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