160 ON FARADAY'S LINES OP FORCE. 



I. Theory of the Motion of an incompressible FluiJ. 



(1) The substance here treated of must not be assumed to possess any of 

 the properties of ordinary fluids except those of freedom of motion and resistance 

 to compression. It is not even a hypothetical fluid which is introduced to 

 explain actual phenomena. It is merely a collection of imaginary properties 

 which may be employed for establishing certain theorems in pure mathematics in 

 a way more intelligible to many minds and more applicable to physical problems 

 than that in which algebraic symbols alone are used. The use of the word 

 " Fluid " will not lead us into error, if we remember that it denotes a purely 

 imaginary substance with the following property : 



T7ie portion of fluid which at any instant occupied a given volume, will at 

 any succeeding instant occupy an equal volume. 



This law expresses the incompressibility of the fluid, and furnishes us with 

 a convenient measure of its quantity, namely its volume. The unit of quantity 

 of the fluid will therefore be the unit of volume. 



(2) The direction of motion of the fluid will in general be different at 

 different points of the space which it occupies, but since the direction is deter- 

 minate for every such point, we may conceive a line to begin at any point and 

 to be continued so that every element of the line indicates by its direction the 

 direction of motion at that point of space. Lines drawn in such a manner that 

 their direction always indicates the direction of fluid motion are called lines of 

 fluid motion. 



If the motion of the fluid be what is called steady motion, that is, if the 

 direction and velocity of the motion at any fixed point be independent of the 

 tune, these curves will represent the paths of individual particles of the fluid, 

 but if the motion be variable this will not generally be the case. The cases 

 of motion which will come under our notice will be those of steady motion. 



(3) If upon any surface which cuts the lines of fluid motion we draw a 

 closed curve, and if from every point of this curve we draw a line of motion, 

 these lines of motion will generate a tubular surface which we may call a tube 

 of fluid motion. Since this surface is generated by lines in the direction of fluid 



