Accueil
Au hasard
Se connecter
Configuration
Faire un don
À propos de Wikisource
Avertissements
Rechercher
Page
:
Lagrange - Œuvres (1867) vol. 1.djvu/686
Langue
Suivre
Modifier
Le texte de cette page a été
corrigé
et est conforme au fac-similé.
et par conséquent
r
′
u
′
3
cos
θ
=
1
a
′
2
cos
θ
−
2
i
y
′
1
a
′
2
cos
θ
.
{\displaystyle {\frac {r'}{u'^{3}}}\cos \theta ={\frac {1}{a'^{2}}}\cos \theta -2iy'{\frac {1}{a'^{2}}}\cos \theta .}
Donc si l’on fait
A
2
=
a
3
A
1
−
a
2
a
′
B
1
2
,
B
2
=
a
3
B
1
−
a
2
a
′
2
A
1
+
C
1
2
+
a
2
a
′
2
,
C
2
=
a
3
C
1
−
a
2
a
′
B
1
+
D
1
2
,
D
2
=
a
3
D
1
−
a
2
a
′
C
1
+
E
1
2
,
…
…
…
…
…
…
…
…
…
;
P
4
=
a
3
(
A
1
+
P
2
)
−
a
2
a
′
Q
2
2
,
Q
4
=
a
3
(
B
1
+
Q
2
)
−
a
2
a
′
2
P
2
+
R
2
2
,
R
4
=
a
3
(
C
1
+
R
2
)
−
a
2
a
′
Q
2
+
S
2
2
,
S
4
=
a
3
(
D
1
+
S
2
)
−
a
2
a
′
R
2
+
T
2
2
,
…
…
…
…
…
…
…
…
…
…
…
;
P
3
=
a
3
P
3
−
a
2
a
′
(
B
1
2
+
Q
3
2
)
,
Q
3
=
a
3
Q
3
−
a
2
a
′
(
2
A
1
+
C
1
2
+
2
P
3
+
R
3
2
)
−
2
a
a
′
2
,
R
3
=
a
3
R
3
−
a
2
a
′
(
B
1
+
D
1
2
+
Q
3
+
S
3
2
)
,
S
3
=
a
3
S
3
−
a
2
a
′
(
C
1
+
E
1
2
+
R
3
+
T
3
2
)
,
…
…
…
…
…
…
…
…
…
…
…
…
…
.
{\displaystyle {\begin{aligned}{\mathfrak {A}}_{2}&=a^{3}{\mathfrak {A}}_{1}-a^{2}a'{\frac {{\mathfrak {B}}_{1}}{2}},\\{\mathfrak {B}}_{2}&=a^{3}{\mathfrak {B}}_{1}-a^{2}a'{\frac {2{\mathfrak {A_{1}+C_{1}}}}{2}}+{\frac {a^{2}}{a'^{2}}},\\{\mathfrak {C}}_{2}&=a^{3}{\mathfrak {C}}_{1}-a^{2}a'{\frac {\mathfrak {B_{1}+D_{1}}}{2}},\\{\mathfrak {D}}_{2}&=a^{3}{\mathfrak {D}}_{1}-a^{2}a'{\frac {\mathfrak {C_{1}+E_{1}}}{2}},\\\ldots &\ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \,;\\{\mathfrak {P}}_{4}&=a^{3}({\mathfrak {A_{1}+P_{2}}})-a^{2}a'{\frac {{\mathfrak {Q}}_{2}}{2}},\\{\mathfrak {Q}}_{4}&=a^{3}({\mathfrak {B_{1}+Q_{2}}})-a^{2}a'{\frac {2{\mathfrak {P_{2}+R_{2}}}}{2}},\\{\mathfrak {R}}_{4}&=a^{3}({\mathfrak {C_{1}+R_{2}}})-a^{2}a'{\frac {\mathfrak {Q_{2}+S_{2}}}{2}},\\{\mathfrak {S}}_{4}&=a^{3}({\mathfrak {D_{1}+S_{2}}})-a^{2}a'{\frac {\mathfrak {R_{2}+T_{2}}}{2}},\\\ldots &\ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \,;\\{\mathfrak {P}}_{3}&=a^{3}{\mathfrak {P}}_{3}-a^{2}a'\left({\frac {{\mathfrak {B}}_{1}}{2}}+{\frac {{\mathfrak {Q}}_{3}}{2}}\right),\\{\mathfrak {Q}}_{3}&=a^{3}{\mathfrak {Q}}_{3}-a^{2}a'\left({\frac {2{\mathfrak {A_{1}+C_{1}}}}{2}}+{\frac {2{\mathfrak {P_{3}+R_{3}}}}{2}}\right)-{\frac {2a}{a'^{2}}},\\{\mathfrak {R}}_{3}&=a^{3}{\mathfrak {R}}_{3}-a^{2}a'\left({\frac {\mathfrak {B_{1}+D_{1}}}{2}}+{\frac {\mathfrak {Q_{3}+S_{3}}}{2}}\right),\\{\mathfrak {S}}_{3}&=a^{3}{\mathfrak {S}}_{3}-a^{2}a'\left({\frac {\mathfrak {C_{1}+E_{1}}}{2}}+{\frac {\mathfrak {R_{3}+T_{3}}}{2}}\right),\\\ldots &\ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots \ldots .\end{aligned}}}
on aura (n
o
67
R
=
J
′
a
2
(
A
2
+
B
2
cos
θ
+
C
2
cos
2
θ
+
D
2
cos
3
θ
+
…
)
+
i
J
′
a
2
y
(
P
4
+
Q
4
cos
θ
+
R
4
cos
2
θ
+
S
4
cos
3
θ
+
…
)
+
i
J
′
a
2
y
′
(
P
5
+
Q
5
cos
θ
+
R
5
cos
2
θ
+
S
5
cos
3
θ
+
…
)
,
{\displaystyle {\begin{aligned}\mathrm {R} =&{\frac {\mathrm {J} '}{a^{2}}}\left({\mathfrak {A_{2}+B_{2}}}\cos \theta +{\mathfrak {C}}_{2}\cos 2\theta +{\mathfrak {D}}_{2}\cos 3\theta +\ldots \right)\\&+i{\frac {\mathrm {J} '}{a^{2}}}y\ \left({\mathfrak {P_{4}+Q_{4}}}\cos \theta +{\mathfrak {R}}_{4}\cos 2\theta +{\mathfrak {S}}_{4}\cos 3\theta +\ldots \right)\\&+i{\frac {\mathrm {J} '}{a^{2}}}y'\left({\mathfrak {P_{5}+Q_{5}}}\cos \theta +{\mathfrak {R}}_{5}\cos 2\theta +{\mathfrak {S}}_{5}\cos 3\theta +\ldots \right),\end{aligned}}}