Introduction to the ModelDescription and AssumptionsIf we ignore non-mechanical processes like heat transfer, radiative losses, etc., then we arrive at a model involving only mechanical energy which changes due to the application (or extraction) of the work done by non-conservative forces The non-conservative forces can be external forces exerted on the system or internal forces resulting from the interactions between the elements inside the system. Learning ObjectivesStudents will be assumed to understand this model who can:
Relevant DefinitionsMechanical EnergyKinetic EnergyWorkThe system potential energy is the sum of all the potential energies produced by interactions between system constituents. Even when there are two system constituents involved (for example in a double star) each interaction produces only one potential energy. S.I.M. Structure of the ModelCompatible SystemsOne or more point particles or rigid bodies, plus any conservative interactitons that can be accounted for as potential energies of the system. Relevant InteractionsAny external force that performs that perform work on the system must be considered, and also any internal non-conservative forces that perform work. Any internal conservative forces that are present should have their interaction represented by the associated potential energy rather than by the work. Law of ChangeMathematical RepresentationDifferential FormIntegral FormDiagrammatic RepresentationsRelevant ExamplesExamples Involving Constant Mechanical EnergyExamples Involving Non-Conservative WorkExamples Involving Gravitational Potential EnergyExamples Involving Elastic (Spring) Potential EnergyExamples Involving Rotational Kinetic EnergyAll Examples Using this Model
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