FREE BOOKS

Author's List




PREV.   NEXT  
|<   377   378   379   380   381   382   383   384   385   386   387   388   389   390   391   392   393   394   395   396   397   398   399   400   401  
402   403   404   405   406   407   408   409   410   411   412   413   >>  
f a pyrometer placed in a furnace are hard to interpret and such temperature measurements can be of little value. If the furnace gases absorb the radiations from the fire and from the brickwork of the side walls and in their turn radiate heat to the boiler surface, it is scientifically correct to assume that the actual or sensible temperature of the gas would be measured by a pyrometer and the amount of radiation could be calculated from this temperature by Stefan's law, which is to the effect that the rate of radiation is proportional to the fourth power of the absolute temperature, using the constant with the resulting formula that has been determined from direct experiment and other phenomena. With this understanding of the matter, the radiations absorbed by a boiler can be taken as equal to that absorbed by a flat surface, covering the portion of the boiler tubes exposed to the furnace and at the temperature of the tube surface, when completely exposed on one side to the radiations from an atmosphere at the temperature in the furnace. With this assumption, if S^{1} is the area of the surface, T the absolute temperature of the furnace gases, t the absolute temperature of the tube surface of the boiler, the heat absorbed per hour measured in B. t. u.'s is equal to _ _ | / T \ / t \ | 1600 | |----|^{4} - |----|^{4}| S^{1} |_\1000/ \1000/ _| In using this formula, or in any work connected with heat transfer, the external temperature of the boiler heating surface can be taken as that of saturated steam at the pressure under which the boiler is working, with an almost negligible error, since experiments have shown that with a surface clean internally, the external surface is only a few degrees hotter than the water in contact with the inner surface, even at the highest rates of evaporation. Further than this, it is not conceivable that in a modern boiler there can be much difference in the temperature of the boiler in the different parts, or much difference between the temperature of the water and the temperature of the steam in the drums which is in contact with it. If the total evaporation of a boiler measured in B. t. u.'s per hour is represented by E, the furnace temperature by T_{1}, the temperature of the gas leaving the boiler by T_{2}, the weight of gas leaving the furnace and passing through the setting per hour by W, the specific heat of the gas by C
PREV.   NEXT  
|<   377   378   379   380   381   382   383   384   385   386   387   388   389   390   391   392   393   394   395   396   397   398   399   400   401  
402   403   404   405   406   407   408   409   410   411   412   413   >>  



Top keywords:
temperature
 

boiler

 
surface
 

furnace

 

absolute

 

measured

 
absorbed
 

radiations

 
contact
 
formula

leaving

 

difference

 

evaporation

 

external

 

exposed

 
radiation
 

pyrometer

 

interpret

 

internally

 

degrees


hotter

 

measurements

 
pressure
 

saturated

 
heating
 

working

 
negligible
 

experiments

 

highest

 
represented

weight
 

passing

 

specific

 

setting

 

Further

 

transfer

 

conceivable

 

modern

 

phenomena

 

amount


experiment

 

direct

 

understanding

 
matter
 
actual
 

determined

 

fourth

 

proportional

 

effect

 
Stefan