THE CONSTITUTION 0V &AW&& 11 



the velocity, it will generate nine times the heat, and so 

 on. 



Mr. Joule has shown that a pound weight falling from 

 a height of 772 feet, or 772 pounds falling through one 

 foot, will generate by its collision with the earth an 

 amount of heat sufficient to raise a pound of water one de- 

 gree Fahrenheit in temperature. 772 "foot-pounds" 

 constitute the mechanical equivalent of heat. Now, a 

 body falling from a height of 772 feet, has, upon striking 

 the earth, a velocity of 223 feet a second; and if this 

 velocity were imparted to the body, by any other means, 

 the quantity of heat generated by the stoppage of its 

 motion would be that stated above. Six times that 

 velocity, or 1,388 feet, would not be an inordinate one for a 

 cannon-ball as it quits the gun. Hence, a cannon-ball 

 moving with a verocity of 1,338 feet a second, would, by 

 collision, generate an amount of heat competent to raise 

 its own weight of water 36 degrees Fahrenheit in 

 temperature. If composed of iron, and if all the heat 

 generated were concentrated in the ball itself, its tempera- 

 ture would be raised about 360 degrees Fahrenheit; 

 because one degree in the case of water is equivalent to 

 about ten degrees in the case of iron. In artillery prac- 

 tice, the heat generated is usually concentrated upon the 

 front of the bolt, and on the portion of the target first 

 struck. By this concentration the heat developed be- 

 comes sufficiently intense to raise the dust of the metal to 

 incandescence, a flash of light often accompanying colli- 

 sion with the target. 



Let us now fix our attention for a moment on the gun- 

 powder which urges the cannon-ball. This is composed 

 of combustible matter, which if burned in the open air 

 would yield a certain amount of heat. It will not yield 

 this amount if it perform the work of urging a ball. The 

 heat then generated by the gunpowder will fall short 

 of that produced in the open air, by an amount equiva- 

 lent to the vis viva of the ball; and this exact amount 

 is restored by the ball on its collision with the target. 

 In this perfect way are heat and mechanical motion 

 connected. 



Broadly enunciated, the principle of the conservation 

 of force asserts, that the quantity of force in the universe 

 is as unalterable as the quantity 'of matter; that it is alike 



