Full text: The collected mathematical papers of Arthur Cayley, Sc.D., F.R.S., late sadlerian professor of pure mathematics in the University of Cambridge (Vol. 8)

148 
ON THE MECHANICAL DESCRIPTION OF A CUBIC CURVE. 
[506 
2 Square ACD, and connected with it by a pin at D, rod DG. 
3. Square ECF ; the two squares being connected by a pin at G. 
4. Rod IJ. 
F .T 
The rod OH rotates about a pin at 0; taking HA = HI, there is a pin at A 
connecting a fixed point of this rod with the extremity A of the square ACD: the 
fixed point B of this square moves along the line Ox. There is a pin at I connecting 
the extremities of the rods HI, IJ; and this slides along the leg AG of the square 
ACD, the rod IJ being always at right angles thereto: finally the legs of the square 
ECF are always parallel to Ox, Oy, and the rod DG at right angles to EC. I have 
omitted from the description the parallel-motion rods or other arrangements necessary 
for giving these fixed directions to the rod IJ, the square ECF, and the rod DG. 
It will be seen that the angles A OB, ABO are variable angles connected by an 
equation of the form above referred to; and that the lines IJ, CF determine by their 
intersection the point P; and the lines CE, DG determine by their intersection the 
point Q; the curve about to be considered is that determined by the relative motion 
of P in regard to Q; or say the curve the coordinates of a point of which are 
x = QC, y = CP. 
I write 
ZA0B = 6, zAB0 = cf>, 
OA = a, AB = b, AC = c, CD — d, 
AH = HI = \h.
	        
Waiting...

Note to user

Dear user,

In response to current developments in the web technology used by the Goobi viewer, the software no longer supports your browser.

Please use one of the following browsers to display this page correctly.

Thank you.