1. Sect. 6-5: Conservative Forces

2. Conservative Force  The work done by that force depends only on initial & final conditions & not on path taken between the initial & final positions of the mass.  A PE CAN be defined for conservative forces Non-Conservative Force  The work done by that force depends on the path taken between the initial & final positions of the mass.  A PE CANNOT be defined for non-conservative forces The most common example of a non-conservative force is FRICTION

3. Definition: A force is conservative if & only if the work done by that force on an object moving from one point to another depends ONLY on the initial & final positions of the object, & is independent of the particular path taken. Example: gravity. ΔyΔy Δℓ

4. Conservative Force: Another definition: A force is conservative if the net work done by the force on an object moving around any closed path is zero.

5. Potential Energy: Can only be defined for Conservative Forces! In other words, If a force is Conservative, a PE CAN be defined. l But, If a force is Non-Conservative, a PE CANNOT be defined!!

6. If friction is present, the work done depends not only on the starting & ending points, but also on the path taken. Friction is a non-conservative force! Friction is non-conservative!!! The work done depends on the path!

7. If several forces act, (conservative & non-conservative), the total work done is: W net = W C + W NC W C ≡ work done by conservative forces W NC ≡ work done by non-conservative forces The work energy principle still holds: W net =  KE For conservative forces (by the definition of PE): W C = -  PE   KE = -  PE + W NC or: W NC =  KE +  PE

8.  In general, W NC =  KE +  PE The total work done by all non-conservative forces ≡ The total change in KE + The total change in PE

9. Sect. 6-6: Mechanical Energy & its Conservation GENERALLY: In any process, total energy is neither created nor destroyed. Energy can be transformed from one form to another & from one object to another, but the Total Amount Remains Constant.  Law of Conservation of Total Energy

10. In general, for mechanical systems, we just found: W NC =  KE +  PE For the Very Special Case of Conservative Forces Only  W NC = 0   KE +  PE = 0  The Principle of Conservation of Mechanical Energy Please Note!! This is NOT (quite) the same as the Law of Conservation of Total Energy! It is a very special case of this law (where all forces are conservative)

11. So, for conservative forces ONLY! In any process  KE +  PE = 0 Conservation of Mechanical Energy It is convenient to Define the Mechanical Energy: E  KE + PE  In any process (conservative forces!):  E = 0 =  KE +  PE Or, E = KE + PE = Constant ≡ Conservation of Mechanical Energy In any process (conservative forces!), the sum of the KE & the PE is unchanged: That is, the mechanical energy may change from PE to KE or from KE to PE, but Their Sum Remains Constant.

12. Principle of Conservation of Mechanical Energy If only conservative forces are doing work, the total mechanical energy of a system neither increases nor decreases in any process. It stays constant—it is conserved.

13. Conservation of Mechanical Energy:   KE +  PE = 0 or E = KE + PE = Constant For conservative forces ONLY (gravity, spring, etc.) Suppose that, initially: E = KE 1 + PE 1, & finally: E = KE 2 + PE 2. But, E = Constant, so  KE 1 + PE 1 = KE 2 + PE 2 A very powerful method of calculation!!

14. Conservation of Mechanical Energy   KE +  PE = 0 or E = KE + PE = Constant For gravitational PE: (PE) grav = mgy E = KE 1 + PE 1 = KE 2 + PE 2  (½)m(v 1 ) 2 + mgy 1 = (½)m(v 2 ) 2 + mgy 2 y 1 = Initial height, v 1 = Initial velocity y 2 = Final height, v 2 = Final velocity

15. PE 1 = mgh, KE 1 = 0 PE 2 = 0 KE 2 = (½)mv 2 KE 3 + PE 3 = KE 2 + PE 2 = KE 1 + PE 1 but their sum remains constant! KE 1 + PE 1 = KE 2 + PE 2 0 + mgh = (½)mv 2 + 0 v 2 = 2gh all PE half KE half U all KE KE 1 + PE 1 = KE 2 + PE 2 = KE 3 + PE 3

16. Example 6-8: Falling Rock PE only part PE part KE KE only v 1 = 0 y 1 = 3.0 m v 2 = ? y 2 = 1.0 m v 3 = ? y 3 = 0 NOTE!! Always use KE 1 + PE 1 = KE 2 + PE 2 = KE 3 + PE 3 NEVER KE 3 = PE 3 !!!! A very common error! WHY???? In general, KE 3 ≠ PE 3 !!! Energy “buckets” are not real!! Speed at y = 1.0 m? Mechanical Energy Conservation! (½)m(v 1 ) 2 + mgy 1 = (½)m(v 2 ) 2 + mgy 2 = (½)m(v 3 ) 2 + mgy 3 (Mass cancels!) y 1 = 3.0 m, v 1 = 0, y 2 = 1.0 m, v 2 = ? Result: v 2 = 6.3 m/s

17. Example 6-9: Roller Coaster Mechanical energy conservation! (Frictionless!)  (½)m(v 1 ) 2 + mgy 1 = (½)m(v 2 ) 2 + mgy 2 (Mass cancels!) Only height differences matter! Horizontal distance doesn’t matter! Speed at the bottom? y 1 = 40 m, v 1 = 0 y 2 = 0 m, v 2 = ? Find: v 2 = 28 m/s What is y when v 3 = 14 m/s? Use: (½)m(v 2 ) 2 + 0 = (½)m(v 3 ) 2 + mgy 3 Find: y 3 = 30 m Height of hill = 40 m. Car starts from rest at top. Calculate: a. Speed of the car at bottom of hill. b. Height at which it will have half this speed. Take y = 0 at bottom of hill. 1 2 3 NOTE!! Always use KE 1 + PE 1 = KE 2 + PE 2 = KE 3 + PE 3 Never KE 3 = PE 3 ! A very common error! WHY???? In general, KE 3 ≠ PE 3 !!!

18. Conceptual Example 6-10: Speeds on 2 Water Slides Frictionless water slides! Both start here! Both get to the bottom here! Who is traveling faster at the bottom? Who reaches the bottom first? Demonstration ! v = 0, y = h y = 0 v = ?