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Physical and Chemical Data  361


                          Newton’s Third Law
                          This lłw in itð most familiar form stateð that for every action,
                          there is an equal and opposite reaction. If F representð a force
                          vector acting on a given body, then the resultant reaction force
                          vector G is related tmF as follows:

                                                          G    F


                          Law of Universal Gravitation
                          Let m and m represent the masseð (in kilogram0 of twm ob-
                                 1         2
                          jectð M and M . Let d be the distance (in meter0 separating
                                            2
                                   1
                          the mass centers. Then a grłvitational force vector           F (whose
                          magnitude is expressed in newton0 actð on          M in the direction
                                                                                1
                          of M , and an equal but opposite grłvitational force vector  F
                                2
                          actð on M in the direction of M , such that:
                                      2                        1
                                                      F    Gm m /d     2
                                                                1
                                                                   2
                          where G is a number known as the gravitational constant, and

                                                    G   6.673   10     11

                          This constant is expressed in newton-meterð squared per kilo-
                          gram squared.



                          CoefficienŁ of static friction
                          Suppose twm objects,M and M , are in physical contact along
                                                      1
                                                               2
                          a common flat surface S. Suppose there is friction caused by the
                          contact. Let F represent the normal (perpendicula? force at S
                                          n
                          (in newton0 wità which      M pusheð against M . Let F represent
                                                                              2
                                                                                      m
                                                        1
                          the maximum force (in newton0 that can be applied tm M rel-
                                                                                             1
                          ative tmM parallel tmS, such that the twm objectð remain sta-
                                      2
                          tionary wità respect tm each other. The coefficient of static fric-
                          tion, denoted   , is defined as follows:
                                            s
                                                            F /F    n
                                                          s
                                                                m
                          CoefficienŁ of kinetic friction

                          Suppose twm objects,M and M , are in physical contact along
                                                      1
                                                               2
                          a common flat surface S, and that the twm objectð are in relative
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