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Heat transfer tubes

Effect of Uncertainties in Thermal Design Parameters. The parameters that are used ia the basic siting calculations of a heat exchanger iaclude heat-transfer coefficients tube dimensions, eg, tube diameter and wall thickness and physical properties, eg, thermal conductivity, density, viscosity, and specific heat. Nominal or mean values of these parameters are used ia the basic siting calculations. In reaUty, there are uncertainties ia these nominal values. For example, heat-transfer correlations from which one computes convective heat-transfer coefficients have data spreads around the mean values. Because heat-transfer tubes caimot be produced ia precise dimensions, tube wall thickness varies over a range of the mean value. In addition, the thermal conductivity of tube wall material cannot be measured exactiy, a dding to the uncertainty ia the design and performance calculations. [Pg.489]

This implies that the LMTD or M I D as computed in equations 20 through 26 may not be a representative temperature difference between the two heat-transferring fluids for aU tubes. The effective LMTD or M ID would be smaller than the value calculated, and consequentiy would require additional heat-transfer area. The tme value of the effective M I D may be determined by two- or three-dimensional thermal—hydrauUc analysis of the tube bundle. Baffle—Tube Support PlateXirea. The portion of a heat-transfer tube that passes through the flow baffle—tube support plates is usuaUy considered inactive from a heat-transfer standpoint. However, this inactive area must be included in the determination of the total length of the heat-transfer tube. [Pg.489]

A vertical cylindrical, and mechanical agitated pressure vessel, equipped with baffles to prevent vortex formation is the most widely used fermenter configuration. The baffles are typically one-tenth of the fermenter diameter in widtli, and are welded to supports tliat extend from the sidewall. A small space between the sidewall and the baffle enables cleaning. Internal heat transfer tube bundles can also be used as baffles. The vessels must withstand a 45 psig internal pressure and full vacuum of -14.7 psig, and comply with the ASME code. [Pg.857]

X, y, z are empirical exponents k = thermal conductivity d = heat transfer tube diameter p = density of fluid or specific gravity p = viscosity of fluid... [Pg.319]

A low-pressure process has been developed by ICl operating at about 50 atm (700 psi) using a new active copper-based catalyst at 240°C. The synthesis reaction occurs over a bed of heterogeneous catalyst arranged in either sequential adiabatic beds or placed within heat transfer tubes. The reaction is limited by equilibrium, and methanol concentration at the converter s exit rarely exceeds 7%. The converter effluent is cooled to 40°C to condense product methanol, and the unreacted gases are recycled. Crude methanol from the separator contains water and low levels of by-products, which are removed using a two-column distillation system. Figure 5-5 shows the ICl methanol synthesis process. [Pg.151]

The size of the tube will be such that the velocity of the boiling fluid within it will cause turbulence to promote heat transfer. Tube diameters will vary from 9 mm to 32 mm, according to the size of coil. [Pg.84]

Unless adequate BD is provided, these boilers may very rapidly develop severe scale buildup on the external side of the heat-transfer tubes, originating from the total evaporation of the ebullient cooling water. [Pg.53]

Economizers are heat transfer tube bundles that preheat MU water or FW flowing within the tubes by extracting waste heat from the flue gas during its exit path to the stack. They typically account for approximately 10% of the total boiler heat transfer surfaces, while absorbing only 7% of the total heat generated in the boiler system. [Pg.86]

Fired heaters are extensively used in the oil and gas industry to process the raw materials into usable products in a variety of processes. Fuel gas is normally used to fire the units which heat process fluids. Control of the burner system is critical in order to avoid firebox explosions and uncontrolled heater fires due to malfunctions and deterioration of the heat transfer tubes. Microprocessor computers are used to manage and control the burner system. [Pg.114]

Fig. 11.5. Diagram illustrating the components of an ESI source. A solution from a pump or the eluent from an HPLC is introduced through a narrow gage needle (approximately 150 pm i.d.). The voltage differential (4-5 kV) between the needle and the counter electrode causes the solution to form a fine spray of small charged droplets. At elevated flow rates (greater than a few pl/min up to 1 ml/min), the formation of droplets is assisted by a high velocity flow of N2 (pneumatically assisted ESI). Once formed, the droplets diminish in size due to evaporative processes and droplet fission resulting from coulombic repulsion (the so-called coulombic explosions ). The preformed ions in the droplets remain after complete evaporation of the solvent or are ejected from the droplet surface (ion evaporation) by the same forces of coulombic repulsion that cause droplet fission. The ions are transformed into the vacuum envelope of the instrument and to the mass analyzer(s) through the heated transfer tube, one or more skimmers and a series of lenses. Fig. 11.5. Diagram illustrating the components of an ESI source. A solution from a pump or the eluent from an HPLC is introduced through a narrow gage needle (approximately 150 pm i.d.). The voltage differential (4-5 kV) between the needle and the counter electrode causes the solution to form a fine spray of small charged droplets. At elevated flow rates (greater than a few pl/min up to 1 ml/min), the formation of droplets is assisted by a high velocity flow of N2 (pneumatically assisted ESI). Once formed, the droplets diminish in size due to evaporative processes and droplet fission resulting from coulombic repulsion (the so-called coulombic explosions ). The preformed ions in the droplets remain after complete evaporation of the solvent or are ejected from the droplet surface (ion evaporation) by the same forces of coulombic repulsion that cause droplet fission. The ions are transformed into the vacuum envelope of the instrument and to the mass analyzer(s) through the heated transfer tube, one or more skimmers and a series of lenses.
Heat Transfer Heat-exchange surfaces have been used to provide the means of removing or adding heat to fluidized beds. Usually, these surfaces are provided in the form of vertical or horizontal tubes manifolded at the tops and bottom or in a trombone shape manifolded exterior to the vessel. Horizontal tubes are extremely common as heat-transfer tubes. In any such installation, adequate provision must be made for abrasion of the exchanger surface by the bed. The prediction of the heat-transfer coefficient for fluidized beds is covered in Secs. 5 and 11. [Pg.11]

Circulating Beds These fluidized beds operate at higher velocities, and virtually all the solids are elutriated from the furnace. The majority of the elutriated sohds, still at combustion temperature, are captured by reverse-flow cyclone(s) and recirculated to the foot of the combustor. The foot of the combustor is a potentially very erosive region, as it contains large particles not elutriated from the bed, and they are being fluidized at high velocity. Consequently the lower reaches of the combustor do not contain heat-transfer tubes and the water walls are protected with refractory. Some combustors have... [Pg.29]

Example 16.5. Teflon heat transfer tubes that are thin enough to flex under the influence of circulating liquid cause a continual descaling that maintains good heat transfer consistently, 20-65 Btu/(hr)(sqft)(°F). Circulating types such as Figures (d) and (e) of ten are operated in batch mode, the former under vacuum if needed. High labor costs keep application of batch crystallizers to small or specialty production. [Pg.539]

T is the Kelvin temperature and "a" is the area in cm2. At 20°C the vapor pressure is 1.75 x 10-l torr and the evaporation rate is 2.9 x 10 7g/sec from a sample whose area is 5mm2. At this rate the glycerol would last 14 minutes and at 40°C only 5 minutes. At 100°C it would disappear in about 2 seconds. This illustrates the importance of maintaining a cooled target and source below 30°C. Heating transfer tubes and analyzers should be avoided. Data can be taken at higher temperatures, but the short lifetimes require excellent preparation and impose insufficient time for optimization. [Pg.136]

Locational inaccuracy means that it is not possible to determine with certainty whether the tracer makes contact with the tube surface. Therefore, the method shown schematically in Figure 5 was adopted a notional cylindrical surface is drawn around the heat transfer tube at a certain distance from it, and the time for which the tracer remains within this outer surface is determined. This is termed the residence time. [Pg.158]

The analysis system consisted of a Shimsdzu QC-6A gas chromatograph, a chemically deactivated four-way valve for solvent ventilation, a heated transfer tube interface, a Beenakker-type TM0i0 microwave resonance cavity, and an Ebert-type monochromator (0.5m focal length). [Pg.354]

Conceptual design of the HTTR-IS nuclear hydrogen production system Detection of the heat transfer tube rupture in intermediate heat exchanger... [Pg.387]

This paper summarises the FITTR-IS nuclear hydrogen production system and discusses detection method of heat transfer tube rupture of IHX and system analysis results during IHXTR. [Pg.388]

In order to reduce radionuclide transportation from the primary to the secondary cooling system, containment isolation valves should be installed. These valves will be automatically closed by the signal detecting the heat transfer tube rupture of IHX. Meanwhile, the current engineered safety features actuating system is not designed to detect the rupture since the scenario did not impact on the reactor safety of the original HTTR. Therefore, a detection method of heat transfer tube rupture of IHX should be established. [Pg.390]


See other pages where Heat transfer tubes is mentioned: [Pg.79]    [Pg.489]    [Pg.490]    [Pg.5]    [Pg.6]    [Pg.528]    [Pg.472]    [Pg.2387]    [Pg.51]    [Pg.1]    [Pg.319]    [Pg.35]    [Pg.148]    [Pg.32]    [Pg.156]    [Pg.155]    [Pg.257]    [Pg.373]    [Pg.234]    [Pg.489]    [Pg.490]    [Pg.406]    [Pg.543]    [Pg.600]    [Pg.178]    [Pg.472]    [Pg.26]    [Pg.387]   
See also in sourсe #XX -- [ Pg.11 , Pg.13 ]




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Concentric tubes, heat transfer

Conventional Heat Transfer Correlations for Macroscale Tubes and Channels

Fire tubes heat transfer

Forced convection heat transfer inside tubes

Forced convection heat transfer outside tubes

Forced convection heat transfer tube bundles

Heat Transfer for Flow Inside Tubes

Heat Transfer for Flow Outside Tubes

Heat Transfer in Channels and Tubes. Account of Dissipation

Heat Transfer in Circular Tubes

Heat Transfer in Laminar Tube Flow

Heat transfer coefficient tube diameter effect

Heat transfer coefficient tubes

Heat transfer coefficient, for tubing

Heat transfer coefficients tube-side

Heat transfer coefficients water in tubes

Heat transfer in tubes

Heat transfer in vertical tubes

Heat transfer outside tubes

Heat transfer, annular tubes

Heat transfer, fluidized beds horizontal tubes

Heat transfer, fluidized beds vertical tubes

Ideal tube bank heat transfer coefficients

Packed reactor tubes, heat transfer

Sensible heat transfer Inside tubes

Submerged heat-transfer tubes

Tube banks pressure drop heat transfer

Tube bundles heat transfer coefficient

Tube flow turbulent heat transfer

Tube-side heat-transfer coefficient and pressure drop (single phase)

Turbulent Heat Transfer in Circular Tube and Plane Channel

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