Full text: Einleitung in die Theorie der Gammafunktion und der Euler'schen Integrale

T 
x (1 — x) = — [1 — (2 x — l) 2 ], wenn 2 x — 1 = y. 
— [1 — y 2 ], Grenzen — 1 und -f- 1, 
4 
(1 — y 2 )' • — dy. Wir brechen das Integral, 
u 
(1 — y 2 ) • dy. Es sei y 2 
= 2 Vs j z-' /! (l - z)- ,4 dz. 
1 — z = (1 — s 3 )‘ 
(1 — z)' ,, ‘ = (1 — s 2 )' 
dz = 4 (1 — s 2 ).sds, Weg von 0 bis 1, 
(Kt))’ .f 
y V/l—s«v/l— 4s 2 ei 
4 K. (K = Normalform 
eines elliptischen Integ 
rals 1. Art.) 
2 K = \/ 2 rt k 
y 
Q=1-f-2 q -f- 2 q 4 —|— 2 q 9 —(—..., woq=e" 
rGj-i =V2«' / ‘q «■ /2 f*> ¿e Z- 
— \J~2 st’ , ‘ (1 + 2q -f- 2 q 4 + 2q 9 + J 
(28)
	        
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