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Potential Energy Height Work is a process. When a box is lifted, work is done on the box. At the end, the box is resting – no kinetic energy. Where did the work go? y2 F = -mg h y1 W -mg( y2 - y1 ) -mgh Path Dependence What happens to work as a rollercoaster goes down hill then up again? What if the roller coaster took a less steep path? Reversible Process If an object is acted on by a force has its path reversed the work done is the opposite sign. This represents a reversible process. y2 F = -mg h y1 W F d -mg ( y2 - y1 ) -mgh Closed Path If the work done by a force doesn’t depend on the path it is a conservative force. Conservative forces do no work on a closed path. From 1 to 2, the path A or B doesn’t matter From 1 to 2 and back to 1, the path A then the reverse path B gives no work Nonconservative Force Not all forces are conservative. In particular, friction and drag are not conservative. d Negative work is done by friction to get here F = -mFN -d F = mFN Negative work is also done returning the box Net Work The work-energy principle is DK = Wnet. The work can be divided into parts due to conservative and non-conservative forces. • Kinetic energy DK = Wcon + Wnon d Ff Fg Kinetic and Potential Energy Potential energy is the negative of the work done by conservative forces. • Potential energy DU = -Wcon The kinetic energy is related to the potential energy. • Kinetic energy DK = -DU + Wnon The energy of velocity and position make up the mechanical energy. • Mechanical energy Emech = K + U Conservation of Energy Certain problems assume only conservative forces. • No friction, no air resistance • The change in energy, DE = DK + DU = 0 If the change is zero then the total is constant. • Total energy, E = K + U = constant Energy is not created or destroyed – it is conserved. Solving Problems There are some general techniques to solve energy conservation problems. • Make sure there are only conservative forces and kinetic energy in the problem • Identify all the potential and kinetic energy at the beginning • Identify all the potential and kinetic energy at the end • Set the initial and final energy equal to one another next