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                   Продовження таблиці 2.2
             8    lg( 1   sin( m ))   ln( 1   sin( n ))    3  83 0   2     16 0      4.6035    5.1546e-2

                                                 7                    3
             9    3   2            2             5       0.3       12 0      220 0     4.875e-1+   7.3715e-1
                   sin  ( m   ) n   sin  ( m   ) n
                                                 7                                      8.4448e-1i
            10        log  n (    ) 4 . 1    3  4     3.56   e 0.316   2   2.16410 -2   1.1790   1.6630
                          m
            11           2 3  1 2  3         ln3        lg3      0.013     1.410 2    5.7737    6.6559e+1
                     m      n    m  n 
                                
            12         2                       364.85       –         24         –      1.5880e+4   5.4516e-1
                        m   m  3  m 4  m
                       3                                              37

            13         8    m      n          e 1.11     7       5.403       28 0      2.8187    3.7879e-3
                        m     sin  6   
                       3          2                     11
                                                                                   0
            14          m            n         1         5        ln7       1.34       -6.6313   5.0346e-6
                     2    tg  ) n (  sin  2    
                                    2         . 0  03    7

            15       1      m  3  cos(  ) n    -20.1       20 0     lg13.6     1.48     -3.0201e-2   8.5792e-3
                       
                    12  (sin(  ) n   cos( n )) 3
            16        3                         0.28       41 0     e 0.415    237 0     8.1284e-2    4.9334
                   3 m
                        sin( n   30 ) sin( n   30 )
                 cos 2  ) n (

                                                             0            -2
            17       n                 2       6.178       20      -2.2410    1.146     3.5028e-2    1.4003
                       lg( m   ) 2   tg   ) n (
                     3
            18      3         4        4        10.6       50 0      e 2.3       1      4.1645e+2   4.1101e+2
                 m  ctg  ) n (  sin  ) n (    cos  ) n (

            19    m  2  3                       5.08       25 0     ln1.37      12     1.6193e+3   3.5238e+3
                                          4
                        (sec(  ) n   cos ec  n (  ))
                    4                                                           25
                                                   0         0
            20                 1               51         39       0.643               1.4132e-1   5.0772e-2
                       
                     3  ( ctg ( m )   ctg  n (  ))  2                           7
            21             2      8          e 1.648      –       tg1.21       –        6.1109    -5.1927e-1
                      lg 3 m  m 9    
                                  27  

            22       5  e 5  4 m  ( m   12 . 36 ) 2  2.17510 2   –   cos17 0   –      8.5511e+75    4.0272

                          ln( m   ) 7

                                                                          -1
            23                  27  m 1     e 2.145      –      2.46810      –      -2.0936e+3   1.7858e-1
                       lg  2  m   
                            
                                8 
            24                     1           e -0.37   ln2.1517    37 0         7     3.4445e-1   2.6745e-1
                     5 m(    ) n  2  3                                       cos
                                 n (   m )                                       24
            25          sin( m )   tg  ) n (   5.6       lg25        8                 4.4466    5.2145e-1

                         5        2                                   9         10
                          ( m   3  ) n
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