Page 141 - Intro to Tensor Calculus
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136



               This equation has two roots λ 1 and λ 2 which satisfy

                                                  Eg − Ge                    Ef − Fe
                                       λ 1 + λ 2 = −          and    λ 1 λ 2 =       ,                (1.5.38)
                                                  Fg − Gf                    Fg − Gf
               where Fg − Gf 6=0. The curvatures κ (1) ,κ (2) corresponding to the roots λ 1 and λ 2 are called the principal
               curvatures at the point P. Several quantities of interest that are related to κ (1) and κ (2) are: (1) the principal
               radii of curvature R i =1/κ i,i =1, 2; (2) H =  1  (κ (1) + κ (2) ) called the mean curvature and K = κ (1) κ (2)
                                                         2
               called the total curvature or Gaussian curvature of the surface. Observe that the roots λ 1 and λ 2 determine
               two directions on the surface

                                          r    ∂~   ∂~               r    ∂~   ∂~ r
                                                r
                                                                           r
                                                     r
                                         d~ 1                       d~ 2
                                            =     +   λ 1   and        =     +   λ 2 .
                                         du    ∂u   ∂v              du    ∂u   ∂v
               If these directions are orthogonal we will have
                                                 r
                                                        r
                                            r
                                                             r
                                           d~ 1  d~ 2  ∂~   ∂~     ∂~ r  ∂~ r
                                               ·    =(    +    λ 1 )(  +  λ 2 )= 0.
                                            du   du    ∂u   ∂v    ∂u    ∂v
               This requires that
                                                 Gλ 1 λ 2 + F(λ 1 + λ 2 )+ E =0.                      (1.5.39)
               It is left as an exercise to verify that this is indeed the case and so the directions determined by the principal
               curvatures must be orthogonal. In the case where Fg − Gf =0 we have that F =0 and f = 0 because the
               coordinate curves are orthogonal and G must be positive. In this special case there are still two directions
               determined by the differential equations (1.5.37) with dv =0, du arbitrary, and du =0, dv arbitrary. From
               the differential equations (1.5.37) we find these directions correspond to

                                                       e                  g
                                                κ (1) =     and     κ (2) =  .
                                                       E                  G
                                                                              α β
                           α
                   We let λ =  du α  denote a unit vector on the surface satisfying a αβ λ λ =1. Then the equation (1.5.34)
                               ds
                                                                           α β
                                          α β
               can be written as κ (n) = b αβ λ λ or we can write (b αβ − κ (n) a αβ )λ λ =0. The maximum and minimum
                                                       α
               normal curvature occurs in those directions λ where
                                                                   α
                                                    (b αβ − κ (n) a αβ )λ =0
               and so κ (n) must be a root of the determinant equation |b αβ − κ (n) a αβ | =0 or


                                                  1           b 1                        b
                                            γ
                                                 b − κ (n)
                              |a αγ b αβ − κ (n) δ | =    1    2      = κ 2  − b αβ a αβ κ (n) +  =0.  (1.5.40)
                                                            2
                                            β       b 2 1  b − κ (n)     (n)            a
                                                            2
               This is a quadratic equation in κ (n) of the form κ 2  − (κ (1) + κ (2) )κ (n) + κ (1) κ (2) =0. In other words the
                                                           (n)
                                                                                       γ
               principal curvatures κ (1) and κ (2) are the eigenvalues of the matrix with elements b = a αγ b αβ . Observe that
                                                                                       β
               from the determinant equation in κ (n) we can directly find the total curvature or Gaussian curvature which
                                                     α
               is an invariant given by K = κ (1) κ (2) = |b | = |a αγ b γβ | = b/a. The mean curvature is also an invariant
                                                     β
               obtained from H =  1 (κ (1) + κ (2) )=  1 αβ b αβ , where a = a 11 a 22 − a 12 a 21 and b = b 11 b 22 − b 12 b 21 are the
                                                  a
                                  2              2
               determinants formed from the surface metric tensor and curvature tensor components.
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