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Heat loss conductive

In order to account for the heat loss through the metallic body of the cone, a heat conduction equation, obtained by the elimination of the convection and source terms in Equation (5.25), should also be incorporated in the governing equations. [Pg.163]

The kieveisible phenomena represent entropy gain through irrecoverable heat losses as follows, where X is the thermal conductivity and /is the length ... [Pg.506]

Actual temperatures in practical flames are lower than calculated values as a result of the heat losses by radiation, thermal conduction, and diffusion. At high temperatures, dissociation of products of combustion into species such as OH, O, and H reduces the theoretical flame temperature (7). Increasing the pressure tends to suppress dissociation of the products and thus generally raises the adiabatic flame temperature (4). [Pg.517]

The maximum velocity at the axis is twice the average, whereas the velocity at the wall is zero. The effect of the burner wall is to cool the flame locally and decrease the burning velocity of the mixture. This results in flame stabilization. However, if the heat-transfer processes (conduction, convection, and radiation) involved in cooling the flame are somehow impeded, the rate of heat loss is decreased and the local reduction in burning velocity may no longer take place. This could result in upstream propagation of the flame. [Pg.523]

Radiation differs from conduction and convection not only in mathematical structure but in its much higher sensitivity to temperature. It is of dominating importance in furnaces because of their temperature, and in ciyogenic insulation because of the vacuum existing between particles. The temperature at which it accounts for roughly half of the total heat loss from a surface in air depends on such factors as surface emissivity and the convection coefficient. For pipes in free convection, this is room temperature for fine wires of low emissivity it is above red heat. Gases at combustion-chamber temperatures lose more than 90 percent of their energy by radiation from the carbon dioxide, water vapor, and particulate matter. [Pg.569]

An upper limit of die heat losses tluough the reaction container wall, usually in the form of a cylindrical ciiicible with an increasing diameter from bottom to top, by assuming that die whole reaction mixture achieves the hnal reaction teiiiperamre immediately, and heat losses occur dirough the ciiicible refractory walls by conduction. The solution of Fourier s equation... [Pg.344]

The total heat loss over 30 minutes, tf, per unit area where k is the drermal conductivity of the container, is given by... [Pg.345]

Now, the heat conducted from the cell will be considered to be controlled by the radial conductivity of the total cell contents and not by the cell walls alone. Furthermore, the axial conductivity of the cell will be ignored as its contribution to heat loss will be several orders of magnitude less than that lost by radial convection. [Pg.223]

Liquified gases are sometimes stored in well-insulated spherical containers that are vented to the atmosphere. Examples in the industry are the storage of liquid oxygen and liquid ammonia in spheres. If the radii of the inner and outer walls are r, and r, and the temperatures at these sections are T, and T, an expression for the steady-state heat loss from the walls of the container may be obtained. A key assumption is that the thermal conductivity of the insulation varies linearly with the temperature according to the relation ... [Pg.518]

Airway surfaces, like skin, are continually exposed to the ambient environment. In contrast to skin submucosal vessels, however, w hich shed excess heat by vasodilating when heated and conserve heat by vasoconstricting when chilled, it is unclear how the airway vasculature responds to temperature extremes. Inspiring cold air poses two challenges to conducting airway tissues the risk of tissue injury should inadequate heat reach the airway surface and excessive body heat loss due to increasing the radial temperature gradient. Vasodilation would protect airway tissue but increase heat loss, while vasoconstriction would produce the opposite effect. [Pg.206]

Heat losses and gains by heat conduction through the building envelope... [Pg.423]

In many industrial halls, conduction inro the ground is a major factor for heat loss. Therefore, an adequate modeling of the floor slab and the underlying, thermally active, soil is very crucial for reliable simulation resuirs. In this case, the soil model in the TRNSYS model was established using results from an additionally performed finite-element program analysis. [Pg.1078]

Heat loss, dry The heat exchange that fakes place from the human body to the surroundings by convection, radiation, and conduction but not by evaporation. [Pg.1447]

Thermal discomfort Discomfort experienced due to excessive heat loss or gain from or to the human body due to radiation, convection, conduction, evaporation, or air movement. [Pg.1482]

Transparent polyethylene can be also applied to the protection of window glass against aggressive media, e.g., the effect of hydrogen fluoride on the plants producing superphosphate fertilizers. The use of transparent polyethylene film for window glass makes it possible to cut down on the heat losses due to the lower thermal conductance of polyethylene as compared to glass. [Pg.76]

To measure the efficiency of a whole window, special testing takes into account all heat transfer from conduction, convection, and radiation. Certain values are used to represent the thermal and solar efficiency of high-performance windows by measuring reduced thermal heat loss (measured by the U-... [Pg.1227]

Heat loss through insulation can be calculated from knowledge of the thickness and thermal conductivity of the insulation and the emissivity of the outer surface of the insulation/cladding system. [Pg.112]

Insulation of hot water storage vessels The requirements for these tanks and cylinders will be met if the heat loss is not greater than 90W/m. The thickness of insulation needed will therefore vary not only according to its thermal conductivity but also to the temperature of the water being stored. In practice, as long as the water is not hotter than 100°C the insulation thickness needed is likely to be of the order of 20-35 mm. [Pg.116]

Estimate the heat loss per square metre of surface through a brick wall 0.5 m thick when the inner surface is at 400 K and the outside surface is at 300 K. The thermal conductivity of the brick may be taken as 0.7 W/mK. [Pg.390]

A furnace is constructed with 0.20 m of firebrick, 0.10 m of insulating brick, and 0.20 m of building brick. The inside temperature is 1200 K and the outside temperature is 330 K. If the thermal conductivities are as shown in Figure 9.7. estimate the heat loss per unit area and the temperature at the junction of the firebrick... [Pg.391]


See other pages where Heat loss conductive is mentioned: [Pg.640]    [Pg.640]    [Pg.1098]    [Pg.17]    [Pg.427]    [Pg.154]    [Pg.97]    [Pg.63]    [Pg.528]    [Pg.460]    [Pg.451]    [Pg.334]    [Pg.292]    [Pg.459]    [Pg.764]    [Pg.217]    [Pg.218]    [Pg.347]    [Pg.41]    [Pg.374]    [Pg.112]    [Pg.58]    [Pg.602]    [Pg.602]    [Pg.603]    [Pg.603]    [Pg.1232]    [Pg.241]    [Pg.245]    [Pg.248]    [Pg.116]    [Pg.587]   
See also in sourсe #XX -- [ Pg.281 , Pg.282 , Pg.283 ]

See also in sourсe #XX -- [ Pg.281 , Pg.282 , Pg.283 ]




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Heat conductance

Heat conduction

Heat conductive

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