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EPICYCLOID , the See also:curve traced out by a point on the circumference of a circle See also:rolling externally on another circle. If the moving circle rolls internally on the fixed circle, a point on the circumference describes a " hypocycloid " (from inro, under). The See also:locus of any other carried point is an " epitrochoid " when the circle rolls externally, and a "hypotrochoid " when the circle rolls internally. The epicycloid was so named by Ole Romer in 1674, who also demonstrated that See also:cog-wheels having epicycloidal See also:teeth revolved with minimum See also:friction (see See also:MECHANICS: Applied); this was also proved by See also:Girard Desargues, Philippe de la Hire and See also: It may be shown that if the distance of the carried point from the centre of the rolling circle be mb, the equation to the epitrochoid is x = (a+b) cos B – mb cos (a+b/b)B, y = (a+b) sin o – mb sin (a+b/b)9. The equations to the hypocycloid and its corresponding trochoidal curves are derived from the two preceding equations by changing the sign of b. Leonhard See also:Euler (Acta Petrop. 1784) showed that the same hypocycloid can be generated by circles having radii of a (a+b) rolling on a circle of radius a; and also that the hypocycloid formed when the radius of the rolling circle is greater than that of the fixed circle is the same as the epicycloid formed by the rolling of a circle whose radius is the difference of the original radii. These See also:pro-positions may be derived from the formulae given above, or proved directly by purely geometrical methods. The tangential polar equation to the epicycloid, as given above, is p=(a+2b) sin (a a+2b)+,G, while the See also:intrinsic equation is s=4(bla)(a+b) cos (a/aa--2b)p and the pedal equation is See also:r2=See also:a2+ (4b.a+b)p1/(a+2b)2, Therefore any epicycloid or hypocycloid may be represented by the equations p =A sin or p =A cos B,', s=A sin B¢ or s =A cos BC or r2=A+Bpi, the constants A and B being readily determined by the above considerations. If the radius of the rolling circle be one-See also:half of the fixed circle, the hypocycloid becomes a See also:diameter of this circle; this may be See also:con-firmed from the equation to the hypocycloid. If the ratio of the radii be as 1 to 4, we obtain the four-cusped hypocycloid, which has the See also:simple cartesian equation x213+yE13=a213. This curve is the envelope of a line of constant length, which moves so that its extremities are always on two fixed lines at right angles to each other, i.e.. of the line x/a+y/a=1, with the See also:condition a2+(32 =1/a, a constant. The epicycloid when the radii of the circles are equal is the See also:cardioid (q.v ), and the corresponding trochoidal curves are limagons (q.v.). Epicycloids are also examples of certain caustics (q.v.). For the methods of determining the formulae and results stated above see J. See also:Edwards, See also:Differential Calculus, and for geometrical constructions see T. H. Eagles, Plane Curves. Additional information and Commentscan you please explain why the Epicycloid of Cremona was called that in the first place?
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