University of Virginia Library

Search this document 
  
  
  
  

expand section1. 
expand section2. 
expand section3. 
expand section4. 
expand section5. 
expand section6. 
expand section7. 
expand section8. 
expand section9. 
expand section10. 
expand section11. 
expand section12. 
expand section13. 
expand section14. 
expand section15. 
expand section16. 
expand section17. 
expand section18. 
expand section19. 
expand section20. 
expand section21. 
collapse section22. 
  
  
  
  
  
  
  
Weight of Lightest Motors.
  
  
  
  
  
expand section23. 
expand section24. 
expand section25. 
expand section26. 
expand section27. 
 28. 

Weight of Lightest Motors.

As shown in the first lecture of his course, the resistance to motion was nearly independent of the velocity, so that the total work done in transporting a given weight was nearly constant. Hence the question of fuel economy was not a bar to high velocities of flight, though should these become excessive, the body resistance might constitute a large proportion of the total. The horsepower required varied as the velocity, so the factor governing the maximum velocity of flight was the horsepower that could be developed on a given weight. At present the weight per horsepower of feather-weight motors appeared to range from 2 1/4 pounds up to 7 pounds per brake horsepower, some actual figures being as follows:

      
Antoinette 5 lbs. 
Fiat 3 lbs. 
Gnome Under 3 lbs. 
Metallurgic 8 lbs. 
Renault 7 lbs. 
Wright 6 lbs. 


202

Automobile engines, on the other hand, commonly weighed 12 pounds to 13 pounds per brake horsepower.

For short flights fuel economy was of less importance than a saving in the weight of the engine. For long flights, however, the case was different. Thus, if the gasolene consumption was 1/2 pound per horsepower hour, and the engine weighed 3 pounds per brake horsepower, the fuel needed for a six-hour flight would weigh as much as the engine, but for half an hour's flight its weight would be unimportant.