Page 367 - Instant notes
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APPENDIX—
                      MATHEMATICAL RELATIONS



                                          Units

        Dimensional analysis allows the units of the quantities in an equation to predict the units
        of the answer which is obtained. The units in an equation are separated from the
        numerical part of the equation, and treated as variables which may be cancelled out or
                                                                            2
        multiplied. If, for example, the kinetic energy of a ball is calculated from E=½ mυ , the
                                                    −1
        units of mass, m, are kg, the units of speed, υ, are m s , hence the units of kinetic energy
                         2 −2
                 −1 2
        are kg (m s ) =kg m  s .
           This also illustrates the fact that the units of energy (usually given as Joules, J) may
        also be expressed in terms of fundamental (cgs) units. The Joule is known as a derived
        unit. Common examples of derived units are given in Table 1.
                        Table 1. Derived units and their equivalent
                        fundamental units

        Quantity        Derived unit        Fundamental (cgs) units
                                              2
                                                  −2
        Energy          J                   m  kg s
                                             −1
        Frequency       Hz                  s
                                                 −2
        Force           N                   m kg s
                                                   −2
                                              −1
        Pressure        Pa                  m  kg s
        Charge          C                   A s
                                                  −3
                                                     −1
                                              2
        Potential       V                   m  kg s  A
                                                  −3
                                                     −2
                                              2
        Resistance      Ω                   m  kg s  A
                                     Approximations


           ln(N!)=Nln(N)−N     for large values of N (Stirling’s approximation)
           ln(1+x)≈x     as x→0
           x
           e ≈1+x     as x→0
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