In the mathematical field of differential geometry a Liouville surface (named after Joseph Liouville) is a type of surface which in local coordinates may be written as a graph in R3
z=f(x,y)
such that the first fundamental form is of the form
ds2=(f1(x)+
2+dy | |
f | |
2(y))\left(dx |
2\right).
Sometimes a metric of this form is called a Liouville metric. Every surface of revolution is a Liouville surface.
Darboux[1] gives a general treatment of such surfaces considering a two-dimensionalspace
(u,v)
ds2=
2du | |
(U-V)(U | |
1 |
2+
2dv | |
V | |
1 |
2),
U
U1
u
V
V1
v
U1du | |
\sqrt{U-\alpha |
ds=
UU1du | |
\sqrt{U-\alpha |
\alpha
\alpha=U\sin2\omega+V\cos2\omega,
\omega
v
. Jean-Gaston Darboux . Leçons sur la théorie générale des surfaces . fr . Lessons on the General Theory of Surfaces . 3 . Gauthier-Villars . 1894 .