FREE BOOKS

Author's List




PREV.   NEXT  
|<   85   86   87   88   89   90   91   92   93   94   95   96   97   98   99   100   101   102   103   104   105   106   107   108   109  
110   111   112   113   114   115   116   117   118   119   120   121   122   123   124   125   126   127   128   129   130   131   132   133   134   >>   >|  
to translate the extraordinary compounds in which K.C.F. Krause expounds his theory of the categories. Notices of the changes introduced by Antonio Rosmini-Serbati, and of Vincenzo Gioberti's remarkable theory, will be found in Ragnisco's work referred to below. [10] _System der Metaphysik_ (1844). [11] _Logische Untersuchungen_, i. 376-377. [12] _Essais de critique generale_ (2nd ed.), _La Logique_, i. pp. 184, 190, 207-225. [13] _Discussions_, p. 577. [14] _Logic_, i. 83; cf. Bain, _Ded. Log._, App. C. CATENARY (from Lat. _catena_, a chain), in mathematics, the curve assumed by a uniform chain or string hanging freely between two supports. It was investigated by Galileo, who erroneously determined it to be a parabola; Jungius detected Galileo's error, but the true form was not discovered until 1691, when James Bernoulli published it as a problem in the _Acta Eruditorum_. Bernoulli also considered the cases when (1) the chain was of variable density, (2) extensible, (3) acted upon at each point by a force directed to a fixed centre. These curves attracted much attention and were discussed by John Bernoulli, Leibnitz, Huygens, David Gregory and others. The mechanical properties of the curves are treated in the article MECHANICS, where various forms are illustrated. The simple catenary is shown in the figure. The cartesian equation referred to the axis and directrix is y = c cosh (x/c) or y = 1/2c[e^(x/c) + e^(-x/c)]; other forms are s = c sinh (x/c) and y^2 = c^2 + s^2, s being the arc measured from the vertex; the intrinsic equation is s = c tan [psi]. The radius of curvature and normal are each equal to c sec^2 [psi]. [Illustration] The surface formed by revolving the catenary about its directrix is named the _alysseide_. It is a minimal surface, i.e. the catenary solves the problem: to find a curve joining two given points, which when revolved about a line co-planar with the points traces a surface of minimum area (see VARIATIONS, CALCULUS OF). The involute of the catenary is called the _tractory_, _tractrix_ or _antifriction_ curve; it has a cusp at the vertex of the catenary, and is asymptotic to the directrix. The cartesian equation is _ _ | c - [root](c^2 - y^2) | x = [root](c^2 - y^2) + 1/2c log |-----------------------|
PREV.   NEXT  
|<   85   86   87   88   89   90   91   92   93   94   95   96   97   98   99   100   101   102   103   104   105   106   107   108   109  
110   111   112   113   114   115   116   117   118   119   120   121   122   123   124   125   126   127   128   129   130   131   132   133   134   >>   >|  



Top keywords:
catenary
 

directrix

 

surface

 
equation
 

Bernoulli

 

vertex

 
Galileo
 

theory

 

cartesian

 
problem

points

 

referred

 

curves

 
Krause
 
expounds
 

illustrated

 

simple

 

compounds

 
figure
 

attention


discussed

 

attracted

 

directed

 

centre

 

Leibnitz

 

Huygens

 

treated

 

article

 

MECHANICS

 

properties


mechanical

 

Gregory

 
traces
 

minimum

 

planar

 
revolved
 

VARIATIONS

 

CALCULUS

 

asymptotic

 

antifriction


tractrix

 

involute

 
called
 

tractory

 

joining

 
radius
 

curvature

 
normal
 
intrinsic
 
measured