Page 54 - 4167
P. 54

According  to  the  law  of  conservation  of  energy,  energy  cannot  be
                  created or destroyed, hence this energy cannot disappear. Instead, it is
                  stored  as  potential  energy.  If  the  spring  is  released  or  the  mass  is
                  dropped, this stored energy will be converted into kinetic energy by the

                  restoring force, which is elasticity in the case of the spring, and gravity
                  in  the  case  of  the  mass.  The  more  formal  definition  is  that  potential
                  energy  is  the  energy  difference  between  the  energy  of  an  object  in  a

                  given position and its energy at a reference position.
                             There are various types of potential energy, each associated with
                  a  particular  type  of  force.  More  specifically,  every  conservative  force
                  gives rise to potential energy. For example, the work of an elastic force

                  is called elastic potential energy; work of the gravitational force is called
                  gravitational  potential  energy;  work  of  the  Coulomb  force  is  called
                  electric  potential  energy;  work  of  the  strong  nuclear  force  or  weak

                  nuclear  force  acting  on  the  baryon  charge  is  called  nuclear  potential
                  energy; work of intermolecular forces is called intermolecular potential
                  energy. Chemical potential energy, such as the energy stored in fossil

                  fuels, is the work of the Coulomb force during rearrangement of mutual
                  positions  of  electrons  and  nuclei  in  atoms  and  molecules.  Thermal
                  energy  usually  has  two  components:  the  kinetic  energy  of  random

                  motions of particles and the potential energy of their mutual positions.
                  Returning          back  to  the    question  of  potential  energy    let's  consider
                                                                            motion  of  body  in  the
                                                                            Earth’s  gravity  field.    For

                                                                            example  the  skier  goes
                                                                            downhill  as  shown  in  fig.
                                                                            5.7.

                                                                            So    trajectory  my  be
                                                                            arbitrary,     let's    consider
                                                                            infinite small  displacement
                                                                            dS,    therefore  elementary

                                                                            work  dA  done  by  gravity
                                                                                           
                                Figure 5.7                                  force  F    m  g   is equal to



                                                           dA   mg   dS   cos  .                           (5.18)

                  It’s  easy   to  notice  that   dS  cos       dh, then
                                                                  dA   mg  dh,                                            (5.19)




                                                                53
   49   50   51   52   53   54   55   56   57   58   59