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Conservation of Mechanical Energy. Introduction “The laws of conservation are the cornerstone of physics.”

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Presentation on theme: "Conservation of Mechanical Energy. Introduction “The laws of conservation are the cornerstone of physics.”"— Presentation transcript:

1 Conservation of Mechanical Energy

2 Introduction “The laws of conservation are the cornerstone of physics.”

3 Definition  When a physical quantity is conserved, the numeric value of the quantity remains the same throughout the physical process.  Although the form of the quantity may change, the final and initial value is consistent.

4 Example

5 Let’s Explain  The kinetic energy of an object falling solely under the influence of gravity is constantly changing.  During this time the gravitational potential energy is also changing.

6 Individually?  These quantities are not conserved individually; however, as a system, they are.

7 Recall that  A system is defined as a definite quantity of matter enclosed by boundaries.  In general the amount of energy remains constant when no mechanical work is done on or by the system, and no energy is transmitted to or from the system.

8 Example

9 The Law of Conservation of Energy The total energy of an isolated system is always conserved!

10 Conversions  Within an isolated system, energy may be converted from one form to another.  However, the total amount of all forms of energy is not going to change!

11 Random Thought  Did you know that total energy can neither be created nor destroyed?  This means that energy as a whole, (taking the entire universe as our system) is conserved and constantly being changed from one form to another.

12 Conservation of Energy  We can say that because: W = ΔKE + ΔPE and the net work done on the system is to be 0 Then, ΔKE = - ΔPE

13 We can expand…  We can expand this equation and say that: KE i + PE i = KE f + PE f According to this equation, the sum of the kinetic and potential energy remains the same before and after.

14 Example

15 Example continued  With the absence of non-conservative forces such as air resistance and friction, the trading of energy is exactly even.  Fortunately for the skydivers, this is not the case. They have their parachutes which create resistive forces that slow them down.

16  Allowing for a nice, smooth landing!

17 So, the rule is  In any isolated system of objects interacting only through conservative forces, the total mechanical energy is: E = KE + PE

18 Example  A diver of mass m drops from a board 10.0 meters above the waters surface. (a) Use conservation of mechanical energy to find the divers speed 5 meters above the surface. (b) his speed when he hits the water. (Neglect air resistance)

19 Example  Suppose the same diver vaults off the springboard, leaving it with an initial speed of 3.50 m/s upwards. Use the law of conservation of energy to find his speed when he strikes the water.

20 Example  A waterslide is 21.9 meters high. With what speed will a 60 kg woman be travelling when she reaches the bottom?


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