Blaga P. Lectures on the differential geometry of - tiera.ru
Blaga P. Lectures on the differential geometry of - tiera.ru
Blaga P. Lectures on the differential geometry of - tiera.ru
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4.9. The spherical map and <strong>the</strong> shape operator <strong>of</strong> an oriented surface 137<br />
Theorem 4.9.1. The spherical map Γ : S → S 2 <strong>of</strong> an oriented surface S into <strong>the</strong> unit<br />
sphere S 2 is a smooth map between surfaces.<br />
Pro<strong>of</strong>. Let a ∈ S . We choose a local parameterizati<strong>on</strong> (U, r) <strong>of</strong> <strong>the</strong> surface S around a,<br />
compatible with <strong>the</strong> orientati<strong>on</strong>. Clearly, since S is orientable, such a parameterizati<strong>on</strong><br />
always exists. Indeed, if we choose a parameterizati<strong>on</strong> (U1, r1) which is not compatible<br />
with <strong>the</strong> orientati<strong>on</strong>, i.e. we have<br />
r ′ 1u × r′ 1v<br />
�r ′ 1u × r′ = − n(u, v),<br />
� 1v<br />
<strong>the</strong>n we replace <strong>the</strong> domain U1 by U− 1 , <strong>the</strong> symmetric <strong>of</strong> U1 with respect to <strong>the</strong> Ov-axis,<br />
and <strong>the</strong> map r1(u, v) by r− 1 (u, v) = r1(−u, v). It is easy to see that <strong>the</strong> pair (U− 1 , r− 1 ) is a<br />
parameterizati<strong>on</strong> <strong>of</strong> <strong>the</strong> surface, compatible with <strong>the</strong> orientati<strong>on</strong>.<br />
Now we have<br />
(Γ ◦ r)(u, v) = Γ(r(u, v)) = Γr(u, v) = n(u, v) = r′ u × r ′<br />
v<br />
�r ′<br />
u × r ′<br />
v� .<br />
Thus, <strong>the</strong> local representati<strong>on</strong> <strong>of</strong> Γ is smooth, <strong>the</strong>refore Γ itself is smooth. �<br />
Examples. (i) For a plane Π <strong>the</strong> spherical map is c<strong>on</strong>stant.<br />
(ii) For <strong>the</strong> sphere S 2 R <strong>the</strong> map Γ : S 2 R<br />
with x2 + y2 + z2 = R2 .<br />
1<br />
→ S has <strong>the</strong> expressi<strong>on</strong> Γ(x, y, z) = R (x, y, z),<br />
As we saw, <strong>the</strong> tangent space to <strong>the</strong> sphere, TΓ(a)S 2 , is orthog<strong>on</strong>al to <strong>the</strong> radius<br />
vector n(a) <strong>of</strong> <strong>the</strong> point Γ(a). On <strong>the</strong> o<strong>the</strong>r hand, n(a) is orthog<strong>on</strong>al to TaS . Thus, if we<br />
identify R 3 a and R 3 Γ(a) to R3 , <strong>the</strong>n <strong>the</strong> subspaces, TaS and TΓ(a)S 2 coincide. Therefore,<br />
we may think <strong>of</strong> <strong>the</strong> <strong>differential</strong> daΓ : TaS → TΓ(a)S 2 as being, in fact, a linear operator<br />
TaS → TaS .<br />
Definiti<strong>on</strong> 4.9.1. The linear operator daΓ : TaS → TaS is called <strong>the</strong> shape operator <strong>of</strong><br />
<strong>the</strong> oriented surface S at <strong>the</strong> point a and it is denoted by A or Aa.<br />
Remark. There is no general agreement regarding <strong>the</strong> definiti<strong>on</strong>, nor <strong>the</strong> name <strong>of</strong> <strong>the</strong><br />
shape operator. In some books, <strong>the</strong> shape operator carries an extra minus sign. Sometimes<br />
it is called <strong>the</strong> Weingarten mapping, or, also <strong>the</strong> principal, or fundamental operator.<br />
Historically, it is t<strong>ru</strong>e, indeed, that Weingarten was <strong>the</strong> first to write down <strong>the</strong><br />
formulae for <strong>the</strong> differentiati<strong>on</strong> <strong>of</strong> <strong>the</strong> spherical map (in o<strong>the</strong>r words, he was <strong>the</strong> <strong>on</strong>e to<br />
find <strong>the</strong> partial derivatives <strong>of</strong> <strong>the</strong> unit normal vectors in terms <strong>of</strong> <strong>the</strong> derivatives <strong>of</strong> <strong>the</strong>