Druckschrift 
Theoria motvs corporvm coelestivm in sectionibvs conicis solem ambientivm
Entstehung
Seite
72
Einzelbild herunterladen
 

n m Libe. I. Sect. II.

/ ^

JjL pro sin(Z/' L). Ita faciendo N L , formulae praecedentes assumuntformam sequentem:

I. /ul = RB -f 7 t sin b ) cotang fi

II. R' R-\- 7 z cos b cos (l L) fj, cos (A L)

n cos b sin (l L) u sin (AIII. L'L =--- ~r- -

-L)

Proprie quidem hic B , : r, UL in partibus radii exprimendi sunt; sed patet, siilli anguli in minutis secundis exprimantur, aequationes I, III sine mutatione reti-neri posse, pro II autem substitui debere

7t cos b cos (/ L/) u cos (A L)

R' = R +

Ceterum in formula III pro denominatore R' absque errore sensibili semper adhiberelicebit R. Reductio temporis autem, angulis in minutis secundis expressis, fiet

__ 495 ".^

206265". COSy 3

r*

70.

Exemplum. Sit A 554 ° 44 ' 54 ", fi = 4 ° 5 g , 52 ", /= 24*29', b = 46 ° 55 ',28'54", H = + o" 4 g, 72 = 0,9988839, tt 8"60. Ecce iam calculum:

Jog-S. 9^99951 log.T.o, g 545 o

log B .9,69020 log sin 6.g, 8653 o

logBR .9,68971 log^rsinfe.0,79780

Ilinc log (fBR -f- Tt sin 5 ).o, 8 oo 4 o

log cotang fi ...1,05875 n

log/t.1,88913 n

log ( « ...;.i,88910 n

log 1". 4,68557

logcos (A Z/)...9,97886

6,55556 nnumerus 0,0003577

log^r.o,g545o

logcos b .9,85475

logi".4,6855 7

logcos (7 IS) .g,ggo4o

5,44520numerus -f - 0,0000279