The whole theory of angular sections, and all the various relations between the trigonometrical functions of an angle and its multiples, may be derived from two remarkable formulæ established by Euler, by which the sine and cosine of an angle are expressed as exponential functions of the angle itself. These formulæ we propose, in the first instance, to establish, and from them to derive all the theorems which form the subject of this part. They will thus hold the same relation to the analysis of angular sections as the formula for the sine of the sum of two angles does to plane trigonometry, and as the formulæ established in (25.) do to spherical trigonemetry. Were it not that the principles upon which these exponential formulæ are established are not sufficiently elementary, the original formula for the sine of the sum of two angles itself might be deduced from them, and these celebrated theorems might thus be made the foundation of the whole superstructure of trigonometry. The exponential formula for the sine and cosine which we are now to establish are and ... no constant is added, since both sides become equal when x 0. = If the sign of x be changed, this becomes cos.x—✓✓ — 1 sin.x = e−√—1 ̧ which being added to and subtracted from the former, gives cos.x=} (e*√/−1 + e ̄2√ −1) √=] sin.æ=}(e®+x√—1_ e ̄®√—1) [1]. m ✓lsin. m 2(m−1)*+x Of the Development of Sines and Cosines, of Multiple Arcs in Powers of the Sines and Cosines of the Simple Arcs. The developments respecting multiple arcs may be divided into two distinct classes. The first includes all series in which the sine or cosine of a -1)*+*) multiple arc is expressed in powers of those of the m simple arc, and the second those in which a power of the sine or cosine of a simple arc is expressed in a series of sines or cosines of its multiples; to the former we shall devote the present section, reserving the latter for the following one. The series in powers of the sine, cosine, &c. may be either ascending or descending, and accordingly the several problems into which our analysis resolves itself may be enumerated as follow: To develope, 1o. cos.mx in ascending powers of sin.mx S cos.x. 2o. sin.mx in ascending powers of cos.mx S sin.x. 3o. sin.mx in ascending powers of 4o. cos.mx in descending powers of sin.mx S COS.X. 5o. sin.mx in descending powers of cos.mx S sin.x. +1) To develope cos.mx in a series of ascending powers of 0, 1, 2, 3, being substituted for n in cos.m(4n+1), it will Since S and S' involve no functions of x except cos.m(2n'x+x) = cos.m(4n17). S. +cos. 1(m-1) (4n + 1)π . mS', 73 where both members have the same number of values, and where the values of the indeterminate integers, n', n are supposed to be less than the denominator of m. It still remains, however, to show the values of each member which correspond respectively to those of the other. Since the value of each member changes by ascribing different values to the integers n' and n, this question only amounts to the determination of the relation between any two cor Let x = , and therefore S = 1, S' = 0. Hence responding values of these integers. cos.m(2n+1)= cos.m(4n+1)*, or cos.m(4n' + 1) = cos.im(4n+1)x, Since n and n' are not supposed to receive any value greater than the denominator of m (for all the values of the cosine after that would only be repetitions of former values), this last condition can only be satisfied by n = n'. Hence the formula becomes* cos.m(2n+x) = cos.m(4n+1). S [3]. To develope sin.mx in ascending powers of cos.x. By subtracting the value of z-m from that of zm, the result being disengaged from the imaginary symbols becomes sin.m(2n+x) = sin.}m(4n+1)′′S + sin.}(m — 1) (4n+1). mS'. [4]. All the observations in the last proposition are equally applicable here. When the denominator of m is an odd integer there are always two values of an angle x whose cosine is given, which are such that sin.mx will be expressed by only one of the two series in [4]. Another form for the development of sin.mx in ascending powers of the cos. may be established by differentiating the series found for cos.mx. By this process we obtain msin.m(2n+x)=cos.m(4n+1). ds dx * In clearing the formula [1] of imaginary quantities, Lagrange has fallen into an error which was lately detected by Poinsot, and the difficulty explained as above. Lagrange's mistake arose from assuming that which is evidently erroneous, since the it does produce a change on (√— 1)m)=cos.mπ+/-1 sin.¿mæ, first member has as many different values as there are units in the denominator of m, and He forgot to take into account, that while the change of x into 2n+x produces no (cos.x+1 sinx)m, cos.mx+-1 sin.mx. In fact, without this consideration, Moivre's formula itself is involved in the absurdity of one member having a greater number of different values than the other. VOL. XVIII. PART I. M* To develope the sine and cosine of a multiple arc in the problem will be solved by obtaining the develop a series of ascending powers of the tangent of the ment of zm in ascending powers of y. simple arc. Lagrange, and all the mathematicians after him, have fallen into an error in the determination of these coefficients. Poinsot has lately corrected it. † Poinsot, 1825. |