«GÂLCÓS»に関連するルーマニア語の本
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1
Debris Flows/avalanches: Process, Recognition, and Mitigation
Inclusion of c in the derivation of the criteria using equations 66 and 67 necessitates the addition of c ctn 111/ g a L cos 0 in the numerator on the right-hand side of equation 69 and c ctn (75/ g k ha cos 0 in the numerator on the left-hand side of ...
John E. Costa, Gerald F. Wieczorek,
1987
2
Report of the American Home Missionary Society
•if d ^j"» s c "'3 ^ •3 tn • 1 £ c 'C o • a a * «• □g a >-l cos .— 0-i . •? . a . . s . □ . S3 . > 2 > • > > j t • l"1!^ >• 8858 «!B5 ft! QJ U 1 j aj '£ 5 v^ S <2S<2° =2 rtft! « m ftl CM s c4 CO □* in CO r^ m CTi O 'D CD GO CO C/. 00 UJ UJ UJ CD en UJ CO CD ...
American Home Missionary Society,
1841
3
System der analytischen Geometrie: Erster Band - Pagina 175
(1.x) : —E—- si 2 1 +a2_|;ala G.a L.cos.(_'l.y) : -‚ ' ___.___. __ s‚; 1+a'+aß L.cos.(1.z) : 11€2'_:_'a_2. :s„ö ' l Aus diesen Gleichungen folgt unmittelbar die Relation: _ G : gs+lbs‚+ars„i 9 O 0 ' 0 o Die Projektionen dieses Lothes in den coordinirten ...
4
Archiv der Mathematik und Physik - Volumul 1 - Pagina 149
__ cosesin d._sin 98m a cos J {x— —r(cos9 s|ng>--sin9 cosq: sin 10 T1}. Setzt man der Kürze wegen 14 Czcos 9 sin öi-sin 9 sin a cos d', I A, =cos «p cos. 15 T, A'..-=:‚cos a cos d, B=sin 9 sin ä-l-cos 9 sin a cos d', B‚=sin 9 sin ga-l-cos 9 cos g> ...
Johann August Grunert,
1841
5
Technische Mechanik 2: Elastostatik - Pagina 238
Die Vertikalverschiebung folgt dann zu MM„ 1 EI ds : Ü / —
Ga(l — cos (‚0)[— a(1 — cos <p)]adcp 0 4a 1 +E /(—2aG)(—2a)dm 7 Ga3 (l 2 + 2 )d J74Ga24 7 EI cosgo cos 90 <p EI a 0 7 Ga3 37T+16 N20 7Ga3 ' EI 2 N ' EI' Zur Ermittlung der ...
Dietmar Gross, Werner Hauger, Jörg Schröder,
2014
6
Report of the Superintendent of the U.S. Coast and ... - Pagina 283
_%:.41. cos. (al—lxl—l—a)—-%A”l"x'. sin. 2(al—lx'-{-a). I T205 291:1? +39 _ —-A'l"- 2 g-A'l' cos 2(al—lx'+a) + 2A,! cos 2(al— lx'+ a!) + A21” .I_+Ls_2(g;v_slfffll_ Q. :A/. cos(al-—lx'+a). {2.421%. sin. 2(al—lx'+a). +'3A'l' cos 2(al—lx'+a)+2 A'! cos ...
U.S. Coast and Geodetic Survey,
1907
7
Dynamics ...: A Text-book for the Use of the Higher ...
But the latter equation might have been obtained directly as the equation of energy, beginning in the form bm (u2 + v*) + \mk* (o^* + <o,2 + <o,2) = ga(l— cos 8) + const. Equations (13) and (14) determine the motion. The reactions at the point ...
Arthur Stanley Ramsey,
1941
8
Classical and modern mechanics - Pagina 76
point is U = ga(l-cos 9) = 2ga sin2 (9/2) Since this does not contain the time explicitly, energy is conserved, i.e. j a2 92 + 2ga sin2 | = h (3.21) Solving mg (3.22) where u,2 = g/a (3.23) In order for any motion to be possible, h must be positive, ...
James Holley Bartlett,
1975
9
Trattato analitico di trigonometria e poligonometria ... - Pagina 98
che un poligono piano regolare di 11. lati è iscrittibile al circolo. Sia x=cos.3a-l-cos 5a-+cos. 7a-l-cos. n a z=cos. a-l-cos.ga-l-cos. 13a-l-cos. 15a Sarò. (m. 22.') x...z=f ed xz=z(cos.2a+cos4a+cos 6a...+003.16a) ovvero xz=-2(ws.15a+coi~I3a.
10
Historiae progressuum instrumentorum, mensurae angulorum ...
ιιτιd·σ, pσtestatἱσus altἱοτὶσns ipsius y neglectis, x znocnss . a sιuἔΔ Μιι ίΩ-ὲ-ἑ-θἔἐἔδ cosp cos cl cos φ ξ sin z i quem terruinumposteriorem ob parvitatem ipsius Δ ρanΠnlσπι κ:σntrahere licet. list sin fli-f- gai z sin h cos ga -l- cos iz sin i Δ ...
Enno Heeren Dirksen,
1819