backwards through the angle JOT, so that T. S. fall into the positions J, S'. D and E then coincide upon / D, OF becomes perpendicular to J/2, b – 3 remains unchanged in value but merges into ‘p, and the new modulus becomes p/1/X*-Hoo, or p / A cos @, its former value with the factor cis 3 omitted; while no change in A, p. and a need take place. Thus the path of P remains intact, and the new Q moves with its former speed in a straight line passing through S' and through a point on O/ at a distance to the left of O equal to OE. Hence the values of 2 in the two systems are identical, while w, of the original gonic system, in virtue of the backward rotation through the angle /OZ’, is transferred to the new or agonic system, by being multiplied by cis (– 3), so that the original w and its transformed value, here denoted by w”, bear to one another the relation The agonic system above described obviously has for its equations of definition (Art. 68) in which m = p s A cos q, and b is the value of 2 for which logo, 2 = 1. The formula connecting logarithms in the two systems therefore is Finally, if in this equation 2 = B, the resulting relation between 3 and B is cis (–3) = logm B, or in the inverse form it is B = expo, ; cis (–3):= }cis-É). 71. Special Constructions. A further specialization is obtained by making q = 3 = O. Q then moves upon a line parallel to O/, and since tan (q – 3) is now zero, w is also zero, R remains fixed at A, and P moves upon a straight line passing through O and A. This is a convenient construction for logarithms and exponentials of complex quantities with respect to a real modulus. The base is here also real (Art. 70). In particular, if Q moves upon the real axis itself, A coincides with /, P also moves upon the real axis, and the resulting construction is that described in Art. 23 for logarithms of real quantities. Returning to the general case in which 3 is not zero, we are at liberty, by our original hypothesis concerning the motion of Q, to permit Q to move upon any straight line in the plane, provided we assign to P such a motion as shall consist with the definition that OQ shall be the logarithm, to modulus k, of OP. Accordingly, let Q be supposed to move parallel to EM’; p – 3 is then zero, o is likewise zero, and P moves upon a straight line passing through O and A. Or again, let Q move parallel to OF; q – 3 is then T / 2, A is zero, and P moves in a circumference concentric with the unit circle. Such constructions are possible to every logarithmic system and enable us to simplify the graphical representation of the relative motions of P and Q.” Expressions of the form logs +, for which no interpretation could be found in terms of real quantities unless a were real and positive (Art. 57), will henceforth be susceptible of definite geometrical representation for all possible values of ar. See the examples of Art. 86. *We might, in fact, propose to assign, as the path of Pin the first instance, any straight line passing through the origin, define OP as the exponential of O.Q., and then determine the modulus by the appropriate auxiliary construction. 72. Relative Positions of A and C in Fig. 36. We have by definition, c= OC, a = /A -- a possible multiple of 27, m = p, / A 'cos (q – 3), o = A tan (q – 3). The product of the last two of these equations gives m o – p sin ($ – 3). But o and p sin (b – 3) are the rates of change of 6 and v' respectively, and 6 = O, v’= O are simultaneous values (Art. 68), m 6 = z'; and since 6= a, v'- care also simultaneous values (Art. 68), Thus A has always a definite position depending upon the modulus and the distance from the origin at which Q crosses the modular normal. Since a is the length of arc over which R passes while Q passes from E to C, it is evident that when c s m lies between 2 & T and 2 (A + 1) tr, say where k is an integer, the part of P's path that corresponds to EC encircles the origin & times before it intersects the circumference of the unit circle, and the point upon the real axis that corresponds to E is its (k+ 1)" intersection with the path of P, counting from / to the left. . It is required to find / and 6 as functions of u and v. Since the speed of M" in OT is p cos (q – 3) and that of P in OR is Ap, and since by definition m = p, / A cos (q – 3), the relation between OM", == u’ and OP, -p, two real quantities, is that of an exponential to its logarithm, with respect to the modulus m (Art. 23); that is, if b = base corresponding to modulus m, Or since & = e^* (Art. 24), this formula may be written and when m = 1 and therefore b = e, it assumes the more * Introductio in Analysin Infinitorum, ed. Nov., 1797, Lib. I, p. 104. for all real values of n. This equation is known as Demoivre's theorem.* 75. Relations between Base and Modulus. Let the lines EAV’, EQ and OF be regarded for the moment as rigidly connected with one another and be turned conjointly in the plane about the fixed point O through an arbitrary angle, whose arc-ratio may here be denoted by y. OM’, in the new position thus given it, then forms with O/ an angle whose arc-ratio is 3 + y, the modulus k, = m cis 3, by virtue of this change, becomes and since OQ, in common with the other lines with which it is connected, is turned about O through the angle of arcratio y, w is hereby transformed into w cis y; while the locus of P is in no way disturbed by any of these changes. In a second transformation, let the motion of P still remain undisturbed, while the speed of Q is changed from p to mp (n = a real quantity). By this change the modulus kcisy becomes no cis y, the distance of Q from the origin becomes no instead of 7, and w cis y is transformed into may cis y. Hence, writing m cis y = y, we have * Demoivre: Miscellamea Analytica (Lond., 1730), p. 1. |