Page 202 - Intro to Tensor Calculus
P. 202

197

































                                            Figure 2.2-5. Motion along curves c and c


               where
                                                                       i
                                                                     i
                                                    L = T − V = L(t, x , ˙ x )
               is the Lagrangian evaluated along the curve c. We ask the question, “What conditions must be satisfied by
               the curve c in order that the integral I( ) have an extremum value when   is zero?”If the integral I( )has
               a minimum value when   is zero it follows that its derivative with respect to   will be zero at this value and
               we will have
                                                        dI( )
                                                                 =0.
                                                         d
                                                              =0
               Employing the definition

                                              dI          I( ) − I(0)
                                                                        0
                                                     = lim           = I (0) = 0
                                               d        →0
                                                  =0
               we expand the Lagrangian in equation (2.2.30) in a series about the point   =0. Substituting the expansion

                                                                   ∂L  i   ∂L  i    2
                                                          i
                                                             i
                                            i
                                         i
                                    i
                                                 i
                                L(t, x +  η , ˙x +   ˙η )= L(t, x , ˙x )+    η +  ˙ η  +   [] + ···
                                                                   ∂x i    ∂ ˙x i
               into equation (2.2.30) we calculate the derivative
                                                       Z  t 1
                                       I( ) − I(0)          ∂L  i     ∂L  i
                             I (0) = lim         = lim         η (t)+    ˙ η (t) dt +   [] + ··· =0,
                              0
                                    →0              →0  t 0  ∂x i     ∂ ˙x i
               where we have neglected higher order powers of   since   is approaching zero. Analysis of this equation
               informs us that the integral I has a minimum value at   = 0 provided that the integral
                                                  Z  t 1     ∂L  ∂L
                                                                     i
                                                           i
                                             δI =         η (t)+    ˙ η (t) dt =0                     (2.2.31)
                                                       ∂x i      ∂ ˙x i
                                                   t 0
   197   198   199   200   201   202   203   204   205   206   207