FREE BOOKS

Author's List




PREV.   NEXT  
|<   286   287   288   289   290   291   292   293   294   295   296   297   298   299   300   301   302   303   304   305   306   307   308   309   310  
311   312   313   314   315   316   317   318   319   320   321   322   323   324   325   326   327   328   329   330   331   332   333   334   335   >>   >|  
t state of the art, arising in the conversion of the heat energy of the coal to the heat energy in the steam. These losses may be classified as follows: 1st. Loss due to fuel dropped through the grate. 2nd. Loss due to unburned fuel which is carried by the draft, as small particles, beyond the bridge wall into the setting or up the stack. 3rd. Loss due to the utilization of a portion of the heat in heating the moisture contained in the fuel from the temperature of the atmosphere to 212 degrees; to evaporate it at that temperature and to superheat the steam thus formed to the temperature of the flue gases. This steam, of course, is first heated to the temperature of the furnace but as it gives up a portion of this heat in passing through the boiler, the superheating to the temperature of the exit gases is the correct degree to be considered. 4th. Loss due to the water formed and by the burning of the hydrogen in the fuel which must be evaporated and superheated as in item 3. 5th. Loss due to the superheating of the moisture in the air supplied from the atmospheric temperature to the temperature of the flue gases. 6th. Loss due to the heating of the dry products of combustion to the temperature of the flue gases. 7th. Loss due to the incomplete combustion of the fuel when the carbon is not completely consumed but burns to CO instead of CO_{2}. The CO passes out of the stack unburned as a volatile gas capable of further combustion. 8th. Loss due to radiation of heat from the boiler and furnace settings. Obviously a very elaborate test would have to be made were all of the above items to be determined accurately. In ordinary practice it has become customary to summarize these losses as follows, the methods of computing the losses being given in each instance by a typical example: (A) Loss due to the heating of moisture in the fuel from the atmospheric temperature to 212 degrees, evaporate it at that temperature and superheat it to the temperature of the flue gases. This in reality is the total heat above the temperature of the air in the boiler room, in one pound of superheated steam at atmospheric pressure at the temperature of the flue gases, multiplied by the percentage of moisture in the fuel. As the total heat above the temperature of the air would have to be computed in each instance, this loss is best expressed by: Loss in B. t. u. per pound = W(212-t+970.4+.47(T-212)) (33) Where W =
PREV.   NEXT  
|<   286   287   288   289   290   291   292   293   294   295   296   297   298   299   300   301   302   303   304   305   306   307   308   309   310  
311   312   313   314   315   316   317   318   319   320   321   322   323   324   325   326   327   328   329   330   331   332   333   334   335   >>   >|  



Top keywords:

temperature

 

moisture

 

combustion

 

boiler

 
losses
 
heating
 

atmospheric

 

superheated

 

degrees

 

portion


instance

 

superheating

 

furnace

 

formed

 

superheat

 

evaporate

 

energy

 
unburned
 

accurately

 

ordinary


practice
 
volatile
 

determined

 

capable

 

Obviously

 

elaborate

 

radiation

 
settings
 

typical

 

expressed


computed

 
percentage
 

multiplied

 
computing
 

methods

 

summarize

 
pressure
 
reality
 

customary

 

hydrogen


setting

 

bridge

 

particles

 

atmosphere

 

utilization

 

contained

 
conversion
 

arising

 
classified
 

carried