1. CONSERVATION OF ENERGY

2. http://www.pbs.org/opb/circus/classroom/cir cus-physics/conservation-energy/

3. A conservative force converts potential energy to other forms of mechanical energy when it does work. In other words, a conservative force does not change the mechanical energy of a system Remember that mechanical energy is potential energy + kinetic energy Conservative Force

4. So, what would be a nonconservative force??? Friction is most common example (air resistance is a form of friction) Work done by friction becomes microscopic internal energy in the object, raising its temperature The internal energy cannot be recovered and turned back into kinetic energy NonConservative Force

5. When is thermal energy a desirable outcome and when is is undesirable? Thermal Energy

6. Energy cannot be created or destoyed, only changed from one form to another E i = E f KE i + PE i = KE f + PE f + HE ½ mv 2 i + mgh i = ½ mv 2 f + mgh f + HE Law of Conservation of Energy

7. Example

8. While jumping over the Great Wall of China an 82 kg skateboarder needs to leave the ramp traveling 21.7 m/s. How much potential energy does he need to start with? And what is the minimum height of ramp he should use? Example

9. A trampoline dunk artist is bounces to a maximum vertical height of 4.8 m before launching himself towards the hoop. At the top of his arc he is 3.2 m above the ground. How fast is he traveling at this point? Example

10. A 65 kg snowboarder starts at rest, travels down a hill into a gulley and back up the other side as shown. Find his speed at top of the 2nd hill. Example

11. A 5.0 kg block of wood is pushed down a ramp with a velocity of 6.0 m/s. The ramp is 1.5 m tall and 3.5 m long. At the bottom of the ramp it is traveling at 7.5 m/s. How much thermal energy is generated due to friction? Determine the force of friction and the coefficient of friction. Example

12. Net work = change in kinetic energy. This means that the net work on a system causes a change in speed of the system Work-Energy Theorem

13. If you know how much energy you want a system or object to have, then you can calculate how much work you need to perform to get it there. Conversely, if you know how much energy a system has, you can calculate how much work that energy can perform. This has literally MILLIONS of real-life examples: The energy of wind movement performs work when it turns a Wind Turbine The chemical energy in gasoline performs work on a piston, which in turn performs work on a vehicle to create kinetic energy. Work is performed on air as it enters a Jet Engine to speed up the air, which results in higher kinetic energy of the air particles, which pushes the airplane Stirring a pot of water performs work in the form of heat transfer, which results in a higher temperature in the water (higher temp = higher energy) When you throw a water balloon at someone’s face, their face performs work on the balloon, which then increases in pressure (higher pressure = higher energy) until it pops. Work-Energy Theorem

14. A 60 kg sprinter exerts a net force of 260 N over a distance of 35 m. What is his change in kinetic energy? If started at rest, what is speed at finish? Example

15. A student pushes a 25 kg crate which is initially at rest with a force of 160 N over a distance of 15 m. If there is 75 N of friction, what is the final speed of the crate? Example