# Spiral

**SPIRAL**, in mathematics, the locus of the extremity of a line (01 radius vector) which varies in length as it revolves about a fixed
point (or origin). Here we consider some of the more important plane spirals. Obviously such curves are conveniently expressed by polar equations, i.e.
equations which directly state a relation existing between the radius vector and the vector angle; another form is the " p, r " equation, wherein r is the
radius vector of a point, and p the length of the perpendicular from the origin to the tangent at that point.

The equiangular or logarithmic spiral (fig. l) is such that as the vector angle increases arithmetically, the radius vector increases F/C3.

F/G4.

geometrically; this definition laads to an equation of the form r = AB, where e is the base of natural logarithms and A, B are constants. Another definition is that the tangent makes a constant angle (a, say) with the radius vector; this leads to p = r sin a. This curve has the property that its positive pedals, inverse, polar reciprocal and evolutes are all equal equiangular spirals. A group of spirals are included in the " parabolic spirals " given by the equation r = a8"; the more important are the Archimedean spiral, r = a8 (fig.2); the hyperbolic or reciprocal spiral, r = o~i (fig.3);and the lituus, r = af>~i (fig. 4). The first-named was discovered byConon, whose studies were completed by Archimedes. Its " p, r " equation is = r 2 /V (<I 2 +'' 2 ), and the angle between the radius vector and the tangent equals the vector angle. The second, called hyperbolic on account of the analogy of its equation (polar) to that (Cartesian) of a hyperbola between the asymptotes, is the inverse of the Archimedean. Its p, r equation is p~2 = r~2+a~2, and it has an asymptote at the distance a above the initial line. The lituus has the initial line as asymptote. Another group of spirals termed Cotes's spirals appear as the path of a particle moving under the influence of a central force varying as the inverse cube of the distance (see M ECHANICS). Their general equation is p~2 = A.r~i + B, in which A and B can have any values. If B =o, we have p = rVA, and the locus is the equiangular spiral. If A = i we have p~'=*r~? + B, which leads to the polar equation r0 = i/VB, i.e. the reciprocal spiral. The more general investigation is as follows : Writing u = f~i we have p-* = Au 2 + B, and since p- 2 = u? + (du/d8)'' (see INFINITESIMAL CALCULUS), then Au' + B='u?+(du/d0)*, i.e. (du/M)* = (A-i)u* + B. The right-hand side may be written as C 2 ( 2 + D 2 ), C 2 (M 2 -D 2 ), C 2 (D 2 M 2 ) according as A I and B are both positive, A I positive and B negative, and as A I negative and B positive. On integration these three forms yield the polar equations = C sin hD8, = C cos hDff, and u = C sin D0. Of interest is the spiral r = o0 2 /(0 2 i), which has the circle r=a as an asymptote in addition to a linear asymptote.

*Note - this article incorporates content from Encyclopaedia Britannica, Eleventh Edition, (1910-1911)*