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Heats of transfer

The final restriction of simple columns stated earlier was that they should have a reboiler and a total condenser. It is possible to use materials fiow to provide some of the necessary heat transfer by direct contact. This transfer of heat via direct contact is known as thermal coupling. [Pg.151]

Consider now the possibility of transferring heat between these two systems (see Fig. 6.76). Figure 6.76 shows that it is possible to transfer heat from hot streams above the pinch to cold streams below. The pinch temperature for hot streams for the problem is 150°C, and that for cold streams is 140°C. Transfer of heat from above the pinch to below as shown in Fig. 6.76 transfers heat from hot streams with a temperature of 150°C or greater into cold streams with a temperature of 140°C or less. This is clearly possible. By contrast. Fig. 6.7c shows that transfer from hot streams below the pinch to cold streams above is not possible. Such transfer requires heat being transferred from hot streams with a temperature of 150°C or less into cold streams with a temperature of 140°C or greater. This is clearly not possible (without violating the ATmin constraint). [Pg.167]

Details of how this design was developed in Fig. 6.9 are included in Chap. 16. For now, simply take note that the targets set by the composite curves are achievable in design, providing that the pinch is recognized, there is no transfer of heat ac ss it, and no inappropriate use of utilities occurs. However, insight into the pinch is needed to analyze some of the important decisions still to be made before network design is addressed. [Pg.169]

As shown in preceding sections, one can have equilibrium of some kinds while inhibiting others. Thus, it is possible to have thennal equilibrium (7 = T ) tln-ough a fixed impemieable diathemiic wall in such a case /i need not equal p, nor need /t equal It is possible to achieve mechanical equilibrium (p =p ) through a movable impemieable adiabatic wall in such a case the transfer of heat or matter is prevented, so T and p. [Pg.352]

Solidification. The heat of the electric arc melts a portion of the base metal and any added filler metal. The force of the arc produces localized flows within the weld pools, thus providing a stirring effect, which mixes the filler metal and that portion of the melted base metal into a fairly homogeneous weld metal. There is a very rapid transfer of heat away from the weld to the adjacent, low temperature base metal, and solidification begins nearly instantaneously as the welding heat source moves past a given location. [Pg.345]

The rapid transfer of heat and the mechanics of blowiag the bottie creates both thermal and mechanically iaduced stresses ia the newly formed bottie. To reheve the stresses, the newly formed botties ate put through an annealing process. [Pg.451]

Conduction furnaces utilize a Hquid at the operating temperature to transfer the heat from the heating elements to the work being processed. Some furnaces have a pot filled with a low melting metal, eg, lead, or a salt mixture, eg, sodium chloride and potassium chloride, with a radiation-type furnace surrounding the pot. Although final heat transfer to the work is by conduction from the hot lead or salt to the work, the initial transfer of heat from the resistors to the pot is by radiation. [Pg.137]

The color development of photochromic compounds can also be utili2ed as a diagnostic tool. The temperature dependence of the fa ding of 6-nitroindolinospiropyran served as the basis for a nondestmctive inspection technique for honeycomb aerospace stmctures (43). One surface of the stmcture to be exarnined was covered with a paint containing the photochromic compound and activated to a violet color with ultraviolet light. The other side of the stmcture was then heated. The transfer of heat through the honeycomb stmcture caused bleaching of the temperature-dependent photochromic compound. Defects in the honeycomb where heat transfer was inhibited could be detected as darker areas. [Pg.165]

Tc- This may require Carnot engines or heat pumps internal to the system that provide for the reversible transfer of heat from the temperature of the flowing fluid to that of the surroundings. Since Carnot engines and heat pumps are cychc, they undergo uo net change of state. [Pg.544]

Conduction is the transfer of heat from one part of a body to another part of the same body, or from one body to another in physical contact with it, without appreciable displacement of the particles of the body. [Pg.554]

Convection is the transfer of heat from one point to another within a fluid, gas, or liquid by the mixing of one portion of the fluid with another. In natural convection, the motion of the flmd is entirely the result of differences in density resiilting from temperature differences in forced convection, the motion is produced by mechanical means. When the forced velocity is relatively low, it should be reahzed that Tree-convection factors, such as density and temperature difference, may have an important influence. [Pg.554]

Materials or combinations of materials which have air- or gas-fiUed pockets or void spaces that retard the transfer of heat with reasonable effectiveness are thermal insulators. Such materials may be particulate and/or fibrous, with or without binders, or may be assembled, such as multiple heat-reflecting surfaces that incorporate air- or gas-filled void spaces. [Pg.1098]

Introduction Insoluble hquids may be brought into direct contact to cause transfer of dissolved substances, to allow transfer of heat, and to promote chemical reaction. This subsection concerns the design and selection of equipment used for conduc ting this type of liquid-hquid contact operation. [Pg.1636]

The pipe has also been used for the transfer of heat between two immiscible liquids in cocurrent flow. For hydrocarbon oil-water, the heat-transfer coefficient is given by... [Pg.1639]

Direct-contac t condensers involve the simultaneous transfer of heat and mass. Design procedures available for absorption, humidification, cooling towers, and the like may be apphed with some modifications. [Pg.2191]

The flashed steam method is less efficient and its requirements for steam properties—cleanliness, high temperature, and high pressure— are usually unavailable in most geothermal fields. The situation is different with the binary cycle system, which is quite efficient and widely used. This wet system involves the transfer of heat from the hot well stream into a more manageable boiling fluid to generate power through a turboexpander. [Pg.136]

To understand the flow in turbomachines, an understanding of the basic relationships of pressure, temperature, and type of flow must be acquired. Ideal flow in turbomachines exists when there is no transfer of heat between the gas and its surroundings, and the entropy of the gas remains unchanged. This type of flow is characterized as a rever.sible adiabatic flow. To describe this flow, the total and static conditions of pressure, temperature, and the concept of an ideal gas must be understood. [Pg.113]

Since temperatures farther down the tower are higher than at the top, heat is available at a higher level. This permits transfer of heat to the incoming feed, thus reducing fuel requirements and furnace investment. [Pg.216]

Technology Description Fluidized bed incinerators utilize a very turbulent bed of inert granular material (usually sand) to improve the transfer of heat to the waste streams to be incinerated. Air is blown through the granular bed materials until they are "suspended" and able to move and mix in a manner similar to a fluid, i.e., they are "fluidized".In this manner, the heated bed particles come in intimate contact with the wastes being burned. The process requires that the waste be fed into multiple injection ports for successful treatment. Advantages... [Pg.163]

The overall heat transfer eoeffieient U is determined from a series of resistanees to the transfer of heat, namely... [Pg.619]

This is the state equation of an ideal gas, where p is pressure, v is specific volume, p is density, R is the gas constant, and T is absolute temperature. In an airflow there is a transfer of heat from one layer to another. This change of... [Pg.49]

The transfer of heat from one molecule to an adjaeent molecule while the particles remain in fixed positions relative to each other is conduction. For example, if a piece of pipe has a hot fluid on the inside and a eold fluid on the outside, heat is transferred through the wall of the pipe by conduc tion. This is illustrated in Figure 2-1. The molecules stay intact, relative to each other, but the heat is transferred from molecule to molecule by the process of conduetion. This type of heat transfer occurs in solids or, to a much lesser extent, within fluids that are relatively stagnant. [Pg.8]

The transfer of heat within a fluid as the result of mixing of the warmer and cooler portions of the fluid is convection. For example, air in contact with the hot plates of a radiator in a room rises and cold air is drawn off the floor of the room. The room is heated by convection. It is the mixing of the warmer and cooler portions of the fluid that conducts the heat from the radiator on one side of a room to the other side. Another example is a bucket of water placed over a flame. The water at the bottom of the bucket becomes heated and less dense than before due to thermal expansion. It rises through the colder upper portion of the bucket transferring its heat by mixing as it rises. [Pg.9]

The transfer of heat from a source to a receiver by radiant energy is radiation. The sun transfers its energy to the earth by radiation. A fire in a fireplace is another example of radiation. The fire in the fireplace heats the air in the room and by convection heats up the room. At the same time, when you stand within line of sight of the fireplace, the radiant energy coming from the flame of the fire itself makes you feel warmer than when you are shielded from the line of sight of the flame. Heat is being transferred both by convection and by radiation from the fireplace... [Pg.10]

Most heat transfer processes used in production facilities involve combinations of conduction and convection ti ansfer processes. For example, in heat exchangers the transfer of heat energy from the hot fluid to the coLl fluid involves tliree steps. First, the heat energy is transferred from the luH fluid to the exchanger tube, then through the exchanger tube wall, ctud finally from the tube wall to the cold fluid. The first and third steps are convection transfer processes, while the second step is conduction process. [Pg.11]

The transfer of heat to and from process fluids is an essential part of most chemical processes. The most commonly used type of heat transfer equipment is the shell and tube heat exchanger. The chemical process industries use four principal types of heat exchanger. [Pg.136]

The addidon of a second bank of similar coils for additional heat transfer area, either outside or inside the first bank of coils will not provide twice the transfer of heat but the effecdveness is estimated to be 70%-90% of the first bank of duplicate coils (assuming the same heat transfer area per bank) [29]. The additional coils will provide additional baffling therefore, the need for the dimension of the vertical baffles is reduced, or they might be removed entirely. [Pg.330]


See other pages where Heats of transfer is mentioned: [Pg.66]    [Pg.4]    [Pg.59]    [Pg.402]    [Pg.481]    [Pg.883]    [Pg.1547]    [Pg.2370]    [Pg.249]    [Pg.508]    [Pg.714]    [Pg.1059]    [Pg.7]    [Pg.14]    [Pg.160]    [Pg.49]    [Pg.605]    [Pg.674]    [Pg.1034]    [Pg.1137]    [Pg.1137]    [Pg.1227]   
See also in sourсe #XX -- [ Pg.69 ]

See also in sourсe #XX -- [ Pg.36 ]




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Addition of New Heat Transfer Area in Retrofit

Axial distribution, of heat transfer coefficient

Balances, Kinetics of Heat and Mass Transfer

Basic Equations for Transfer of Heat, Mass, and Momentum

Basic Models of Heat Transfer in Packed Beds

Bypassing around heat transfer devices photograph of bypass

Calculation of heat transfer

Calculation of heat transfer coefficients for boiling in free flow

Calorimetry Measurement of Heat Transfer

Coefficient of convection heat transfer

Coefficient of heat transfer

Combined Heat and Mass Transfer in Tapered Capillaries with Bubbles under the Action of a Temperature Gradient

Combined Influence of External Mass and Heat Transfer on the Effective Rate

Combined modes of heat transfer

Computation of the Heat Transfer Coefficient for External Flow

Computation of the Heat Transfer Coefficient for Given qw

Computer Solution of Heat-Transfer Problems

Correlations of heat transfer

Correlations of heat transfer coefficients

Definition of Heat Transfer Coefficients

Different Forms of Heat Transfer

Effect of Fluid Properties on Heat Transfer

Effect of Noncondensables on Heat Transfer

Effect of external mass and heat transfer

Effect of temperature-dependent physical properties on heat transfer

Energy Transfer by Use of Trim Heat Exchangers

Enhancement of heat transfer

Enthalpy transfers after assumption of no heat loss

Equation of heat transfer

Estimation of Heat- and Mass-Transfer Coefficients

Evaluation of Heat and Mass Transfers in Bi-Layer Films

Evaluation of Heat and Mass Transfers in Tri-Layer Film

Exact Solutions of Linear Heat and Mass Transfer Equations

Experimental Studies of Heat Transfer

FOUNDATIONS OF HEAT TRANSFER

Film Coefficients of Heat and Mass Transfer

Formulation of Heat Transfer

Fouling Factor. Variable Coefficient of Heat Transfer. Closure

Fourier’s law of heat transfer

General Concepts of Heat Transfer

Heat Transfer Between the Bulk Fluid and External Surfaces of Solid Catalysts

Heat Transfer Coefficients for Radiation in the Freeboard of a Rotary Kiln

Heat Transfer Properties of Optically Thin Aerogels

Heat Transfer in Channel. Account of Dissipation

Heat Transfer in Channels and Tubes. Account of Dissipation

Heat Transfer in a Series of Tanks, dsolve

Heat Transfer of Non-Newtonian Fluids

Heat and Work Two Forms of Energy Transfer

Heat transfer coefficients, overall range of values

Heat transfer in laminar flow of a power-law fluid over an isothermal plane surface

Heat transfer, units of quantities

History of Thermodynamics and Heat Transfer

Importance of Mass and Heat Transfer Processes

Individual and overall coefficients of heat transfer

Influence of Heating Rates on Decomposition and Mass Transfer

Influence of turbulence on heat and mass transfer

Introduction and Mechanisms of Heat Transfer

Main heat transfer data of the

Margin for Fouling of Heat Transfer Surfaces

Mean overall coefficient of heat transfer

Modes of heat transfer

Modes of heat transfer conduction

Origin of Heat Transfer. Particular Laws

Overall coefficient of heat transfer

Physical fundamentals of heat transfer

Place of Heat Transfer in Engineering

Practical Determination of Heat Transfer Coefficients

Principles of Steady-State Heat Transfer

Principles of Unidirectional Heat Transfer

Properties of Heat Transfer Fluids

Qualitative Features of Heat Transfer in Highly Viscous Liquids

Radial and Axial Distributions of Heat Transfer Coefficient

Rate of heat transfer

Related Field (II) Fundamentals of Computational Heat Transfer

Representation of Heat-Transfer Coefficients

Reversible Heat of Polymer Transfer Between Sol and Gel

Reversible transfer of heat

Role of mass and heat transfer

Simple form of analogy between momentum, heat and mass transfer

Skill 11.1b-Discuss how the transfer of energy as heat is related to changes in temperature

Solution of Parabolic Partial Differential Equations for Heat Transfer

Summary of Tests for Mass and Heat Transfer Effects

Surface coefficient of heat transfer

Temperature and Transfer of Heat

The Equations of Convective Heat Transfer

The different types of heat transfer

The reversible transfer of heat

Theoretical Study of Heat and Mass Transfers

Thermal design of heat-transfer equipment

Three modes of heat transfer

Time constant of heat transfer

Types of heat transfer

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