Convection Heat Treating (2)

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By Robert N. Britz,
President

Part II:  Furnace Considerations

    The growth in the use of forced convected heat in heat treating processes, such as baking, tempering, normalizing, surface hardening, annealing of ferrous and non-ferrous metals and alloys, precipitation hardening of aluminum alloys, stress relieving, vacuum furnace cooling cycles and numerous other applications, indicate the need for discussion of the major requirements of successful convection furnace equipment.
    While it is impossible to reduce every problem of convection furnace or oven heating to a simple formula or chart, an attempt will be made to explain the elementary principles of this heating method to approximate the requirements of such equipment and appraise the factors which are of prime importance in this method of furnace design.

Air Circulation Most Important
   
The success of a forced convected heat application depends mainly upon two factors - the volume of air circulation and velocity past the work required for a given heat transfer and temperature uniformity.
    To a technician observing the progress of recirculative convection heating of ovens and furnaces, it is quite apparent that the above mentioned factors are the most abused ones, as most of the failures of convection type furnaces to produce rapid enough heating and desired temperature uniformity or cooling can be traced to the underestimation of the importance of these factors and most of such installations are lacking in sufficient air circulation and uniformity.
    In the forced convection method of heating, air, products of combustion and various protective atmospheres, serve as the heating media which supply the heat for heating of the charges as well as for maintaining the enclosures at a desired temperature with given limitations of temperature fluctuations.

High Velocity Air
   
The ideal way of heating a metal object by convection would be to immerse it in a stream of air of high velocity and constant temperature.  The air velocity would then govern the rate of heat transfer between the heating medium and the object heated, the amount of fluctuation in the temperature of the air stream governing the degree of uniformity to which such heating could be held.  A good forced convection type furnace design will duplicate these ideal heating conditions, as  far as practical and economical limitations will permit, and the closer the approach to these ideal conditions, the better will be the performance of the equipment.

Economy
   
Very close uniformities of heating, with permissible variations of plus or minus 15° F or even plus or minus 5° F (Fig.1), are sought for modern processes and as these can be attained, economically, only by forced convection heating, it will be well to point out the requisites of a successful furnace equipment of this type.
    Equipment well designed for given conditions may approach very closely the condition of absolute uniformities and no thermal heads of heating regardless of temperatures of furnace loads.  A number of installations were observed in which attempts were made to obtain uniformity of heating as close as plus or minus 2 or 5 degrees Fahrenheit with heated air 100 to 200° F higher in temperature than the desired maximum temperature of the heated load blown directly against the furnace loads.  While fairly uniform temperature measurements may have been obtained at certain locations in the furnace interiors, this was not the case throughout the furnace, unless large volumes of forced convection and some type of heat input regulation was used.
    What is the ideal maximum allowable temperature of the air or any other heating medium circulated in a furnace which is to operate at a  given temperature - say at 1000° F, with a desired temperature uniformity of plus or minus 15 degrees Fahrenheit?  With the heating medium blown at a high velocity directly at the furnace load, there is only one ideal answer to this question - 1015° F.  Thus, with a recirculative convection type furnace, operating under the above desired condition, the maximum temperature of the incoming heating medium will be 1015° F and when heat equilibrium has been established the temperature of the recirculated heating medium will be not lower than 985° F.  Under such conditions,  uniformity of plus or minus 15° F at 1000° F would be established throughout the furnace cycle.

How Much Air?
   
Consider an empty furnace of the box type which is to be maintained by forced convection method of heating at 1200° F with a uniformity of plus or minus 10° F throughout the interior.  No matter how well insulated, a certain amount of heat loss will occur through the furnace walls and if a given volume of air at 1200 is introduced into the furnace and withdrawn, the temperature of the outgoing air will be somewhat lower, due to the heat which was abstracted from it and lost through the walls of the furnace, Fig. 2.  Thus the air forced through the furnace will be lowered in temperature along its path from the inlet to outlet, the reduction in temperature being directly proportional to the heat loss through the furnace walls as well as to the weight of the air.

Conclusions
   
In practical applications, where furnace and oven loads are not located close to the walls, the volumes of circulation may be somewhat lower.  This is especially true of furnaces and ovens with built in fans and those with ducts, which surround the loads.  With equipment of such design the heat losses through the walls affect the interior and load temperatures to a lesser extent, and consequently, the circulation volume requirements are lower.
    It is evident that the best fans for furnace and oven applications are those having large inlets and outlets, and consequently, low inlet and outlet velocities.  It also follows that these fans operate at the lowest speeds and have lower wheel stresses for the high temperatures required.

 

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