Leonhard Euler · 1748 · Internet Archive
Introductio in analysin infinitorum
All 320 leaves · leaf 68
Transcription
40 DE TRANSFORMATIONE FUNCTIONUM
LIB. I. neque vicissim $z$ per $y$ exhiberi potest. Quo igitur huic incommodo remedium afferatur; ponatur $y = x^m z^n$, eritque $ax^{am} z^{an} + bz^\zeta + cx^{\gamma m} z^{\gamma n + \delta} = 0$. Determinetur nunc exponens $n$ ita ut ex hac aequatione valor ipsius $z$ definiri queat: quod tribus modis praestari potest.
I. Sit $an = \zeta$; ideoque $n = \frac{\zeta}{a}$; erit, aequatione per $z^\zeta$ divisa, $ax^{am} + b + cx^{\gamma m} z^{\gamma n - \zeta + \delta} = 0$; unde oritur $z = (\frac{-ax^{am}-b}{cx^{\gamma m}})^{\frac{1}{\gamma n - \zeta + \delta}}$, sive
$z = (\frac{-ax^{am}-b}{cx^{\gamma m}})^{\frac{\alpha}{\alpha\gamma n - \alpha\zeta + \alpha\delta}}, \&$
$y = x^m (\frac{-ax^{am}-b}{cx^{\gamma m}})^{\frac{an}{\alpha\gamma n - \alpha\zeta + \alpha\delta}}$
II. Sit $\zeta = \gamma n + \delta$ seu $n = \frac
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