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FUNDAMENTALS OF ENERGY BALANCES
                     Energy can exist in many forms and this, to some extent, makes an energy balance
                   more complex than a material balance.                                   61
                       3.3. FORMS OF ENERGY (PER UNIT MASS OF MATERIAL)

                   3.3.1. Potential energy
                   Energy due to position:
                                               Potential energy D gz                      3.1
                   where z D height above some arbitrary datum, m,
                                                          2
                         g D gravitational acceleration (9.81 m/s ).


                   3.3.2. Kinetic energy
                   Energy due to motion:
                                                               u 2
                                                Kinetic energy D                          3.2
                                                               2
                   where u D velocity, m/s.


                   3.3.3. Internal energy

                   The energy associated with molecular motion. The temperature T of a material is a
                   measure of its internal energy U:
                                                    U D f T                               3.3


                   3.3.4. Work
                   Work is done when a force acts through a distance:
                                                         1

                                                  W D     F dx                            3.4
                                                        0
                   where F D force, N,
                         x and l D distance, m.
                     Work done on a system by its surroundings is conventionally taken as negative; work
                   done by the system on the surroundings as positive.
                     Where the work arises from a change in pressure or volume:
                                                          2
                                                   W D    P dv                            3.5
                                                        1
                                            2
                   where P D pressure, Pa (N/m ),
                                                  3
                         v D volume per unit mass, m /kg.
                     To integrate this function the relationship between pressure and volume must be known.
                   In process design an estimate of the work done in compressing or expanding a gas is
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