Alexander Campbell Fraser. a -- e = e --y x e --y= y-+ a y -- a = a -- e Cuspis decima tertia. a -- e = e +b b- e y-+ b b-y b-+ e e-b b-+ y y-b se-+y= y-b b+ya - b b+ a b-y y+b b-a a+b y-+ a= a +bb- a e-+b b- e b+ a a-b b-+ e e-b a + e= e +b b- e y+ b b -y b+ e e-b .24-3 Farther, suppose the stars, being still in the ecliptic, to appear in one line, when the earth is in any other part of its orbit between O and E ; then will the parallax still be expressed by the same algebraic formula, and one of the maxima will still lie at O, the other at E; but the whole effect will be divided into two parts, which .To investigate these differences, and to discover Harmony, the reason for which they happen, we shall begin by forming a new diatonic scale of the minor mode, simitiga- - o lar to the second scale of the major mode, these differ- 'c, d, e; f, g; g, a, b ', C. ences and That last series, as we have seen, was formed by their rea- .Let the lines AD, DE, EB, BF, FG, GH lie in the same plane, and let them be placed perpendicular to the horizon. From the points D, E, B, c. draw the vertical lines D d, Ee, B b, c. and taking D p of any length, make E r equal to D p, c. and complete the parallelograms p c, q r. Again, make B sqe, and complete the .
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