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Fall 2011 PHYS 172: Modern Mechanics Lecture 9 – The Energy Principle Read 6.1 – 6.7.

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Presentation on theme: "Fall 2011 PHYS 172: Modern Mechanics Lecture 9 – The Energy Principle Read 6.1 – 6.7."— Presentation transcript:

1 Fall 2011 PHYS 172: Modern Mechanics Lecture 9 – The Energy Principle Read 6.1 – 6.7

2 TODAY The Energy Principle Energy is Conserved Rest Energy and Kinetic Energy Work =

3 What Is Energy? Energy is just some number you can compute that obeys a conservation law. It’s helpful book-keeping. (See Feynman Lectures on Physics, Vol. 1, Sec. 4-1) Why Introduce Energy? say something about initial and final states of a system predict whether some process CAN occur Without following the details of a complicated process, we can: Basically, for some problems, using energy is much simpler than using the momentum principle. Often, however, we’ll use both principles in combination.

4 The Energy Principle “effect” “cause” (due to interactions) Compare With Momentum Principle: “effect”“cause” (due to interactions) NOTE: Momentum is a vector. Energy is a scalar (no direction). * We mean the Work done ON a System by a Force in the Surroundings*

5 Energy is A Conserved Quantity Compare with Conservation of Momentum: Reminder: Momentum is a vector. Energy is a scalar (no direction). Energy is a useful thing to consider because energy can’t be destroyed: it can only change forms.

6 Energy of a Single Particle System Experimentally, this is the expression that works in a conservation law

7 Rest Energy A particle at rest has some energy just because it exists! Rest energy = mc 2.

8 Kinetic Energy Excess energy above rest energy (mc 2 ) is due to motion (ignoring internal degrees of freedom): mc 2

9 Kinetic Energy What?? What happened to ? At low velocities, Use a Taylor expansion (power series):

10 Energy And Momentum Use ALWAYS TRUE. EVERY REFERENCE FRAME.

11 It takes twice as much energy to raise a heavy box a distance 2h, compared to lifting it only h. Thus, it is distance that seems to matter, not time. Energy and Force Does this match your real-world experience?

12 It takes twice as much energy to raise a heavy box a distance 2h, compared to lifting it only h. Thus, it is distance that seems to matter, not time. In more general vector notation, this is: * We mean the Work done ON a System by a Force in the Surroundings* Energy and Force WORK due to mechanical energy transfer:

13 Force at an angle y x Only x -component of force “works”! Definition of work Force component along the path of motion

14 14 Work as a dot product x y Dot product:

15 Sun does work on comet, speeding it up. Earth does no work on the Moon. Circular orbit Sign of Work

16 Game: What’s the Sign of the Work? * We mean the Work done ON a System by a Force in the Surroundings*

17 What Causes The Energy of A System to Change? Reminder: Momentum Principle Interactions: some P surroundings transforms into P system. Forces transfer momentum from one object to another. Energy can be transferred from the surroundings to a system in two ways: Energy transfer by heat (next chapter) Energy transfer by work set = 0 for now

18 Example You hold a ball of mass 0.5 kg at rest in your hand and throw it forward so that it leaves your hand at speed 20 m/s. How much work did you do on the ball? v f = 20 m/s v i = 0 m/s Rest energy did not change

19 Change of identity – change of rest energy Neutron decay An electron-volt (eV) unit: 1 eV = 1.6  10 -19 J 1 MeV = 10 6 eV 1 Volt How much kinetic energy do the products have? =0 Mass of products is smaller than mass of reactant! Mass is converted into kinetic energy >0

20 WHAT WE DID TODAY The Energy Principle Energy is Conserved Rest Energy and Kinetic Energy Work =


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