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10             σV                                                                          7           Eδ
               FL                                                                                      σL
        Wp  =                                                                                 ∆  p  =                                 ∆≈π −2 L
                                                                                                                                             4H
9

                                                                                           6

  8         b et h constants                                                                                                          b constant
                                                                                                                                      h variable
  7         Wp  =  3  L                                                                                    ∆≈1 L
                   4  H                                                                    5                    4H
  6
                                                              WM , p     =       1    L
  5                                                                              2    H
                                                                                                           b variable
  4                                                                                        4               h constant

  3                                                                    b constant
                                                                       h variable
  2
                                                                           ,  P  =  3π  L  3
3 34                                                                                16  H
                                                                       WM
  1
                                              Wp  =  3  π − arctan  3H L +3 3
3 38                                                 8  2             LH 8

  0                                    b variable                                          2
     0                                 h constant

                                 Wp =  3 +1   L 2+3     H2          3+4  L       2      3
                                       16 4   H 16      L
                                                                         H         −

                                                                                           1               b et h constants ∆ ≈ 5 L
                                                                                                                                  24 H
                                                                                      L                                                           L
                                                                                      H
                                                                                                                                                  H

                                                                                           0

            2 3 6 9 12 15 18                                                                  0 3 6 9 12 15 18
                      Figure 2.1.4.1.
                                                                                                           Figure 2.1.4.2.

20          σV                                                                             7           Eδ
            FL                                                                                         σL
    WP  =                                                                                     ∆P    =                                 ∆≈π −2 L
                                                                                                                                             4H
18

                                                                                           6

16                                                                                                         ∆≈1 L                      b constant
                                                                                                                4H                    h variable
               b et h constants

14                                                                                         5

            WP     =  3  L
                      2  H

12                                                                                                                        b variable

                                                                                           4 h constant

10                                                b constant                               3
 8                                                h variable
 6
 4                                            WM ,P     = 3π        L                      2
 2                                                         8        H
 0
                                       b variable
    0                                  h constant

                                                                                           1               b et h constants ∆ ≈ 5 L
                                                                                                                                 24 H
                                                  L                                 L                                                             L
                                                  H                                 H
                                       WM ,P  =                                                                                                   H

                                                                                           0

               3 6 9 12 15 18                                                                 0 3 6 9 12 15 18

                       Figure 2.1.4.3.                                                                     Figure 2.1.4.4.
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