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Chapter 5

Chapter 5. Energy. Forms of Energy. Mechanical Focus for now May be kinetic (associated with motion) or potential (associated with position) Chemical Electromagnetic Nuclear. Slide 10-3. Slide 10-4. Slide 10-5. Reading Quiz . If a system is isolated , the total energy of the system

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Chapter 5

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  1. Chapter 5 Energy

  2. Forms of Energy • Mechanical • Focus for now • May be kinetic (associated with motion) or potential (associated with position) • Chemical • Electromagnetic • Nuclear

  3. Slide 10-3

  4. Slide 10-4

  5. Slide 10-5

  6. Reading Quiz • If a system is isolated, the total energy of the system • increases constantly. • decreases constantly. • is constant. • depends on work into the system. • depends on work out of the system. Slide 10-6

  7. Answer • If a system is isolated, the total energy of the system • increases constantly. • decreases constantly. • is constant. • depends on work into the system. • depends on work out of the system. Slide 10-7

  8. Reading Quiz • Which of the following is an energy transfer? • Kinetic energy • Heat • Potential energy • Chemical energy • Thermal energy Slide 10-8

  9. Answer • Which of the following is an energy transfer? • Kinetic energy • Heat • Potential energy • Chemical energy • Thermal energy Slide 10-9

  10. Reading Quiz • If you raise an object to a greater height, you are increasing • kinetic energy. • heat. • potential energy. • chemical energy. • thermal energy. Slide 10-10

  11. Answer • If you raise an object to a greater height, you are increasing • kinetic energy. • heat. • potential energy. • chemical energy. • thermal energy. Slide 10-11

  12. Forms of Energy Mechanical Energy Thermal Energy Other forms include Slide 10-12

  13. Some Energy Considerations • Energy can be transformed from one form to another • Essential to the study of physics, chemistry, biology, geology, astronomy • Can be used in place of Newton’s laws to solve certain problems more simply

  14. The Basic Energy Model Slide 10-13

  15. Energy Transformations Kinetic energy K = energy of motion Potential energy U = energy of position Thermal energy Eth = energy associated with temperature System energy E = K + U + Eth + Echem + ... Energy can be transformed within the system without loss. Energy is a property of a system. Slide 10-14

  16. Some Energy Transformations Echem Ug KEth Us KUg Echem Ug Slide 10-15

  17. Checking Understanding • A skier is moving down a slope at a constant speed. What energy transformation is taking place? • A. K  Ug • B. Ug Eth • C. Us Ug • D. Ug K • E. K  Eth Slide 10-16

  18. Answer • A skier is moving down a slope at a constant speed. What energy transformation is taking place? • A. K  Ug • B. Ug Eth • C. Us Ug • D. Ug K • E. K  Eth Slide 10-17

  19. Checking Understanding • A child is on a playground swing, motionless at the highest point of his arc. As he swings back down to the lowest point of his motion, what energy transformation is taking place? • A. K  Ug • B. Ug Eth • C. Us Ug • D. Ug K • E. K  Eth Slide 10-18

  20. Answer • A child is on a playground swing, motionless at the highest point of his arc. As he swings back down to the lowest point of his motion, what energy transformation is taking place? • A. K  Ug • B. Ug Eth • C. Us Ug • D. Ug K • E. K  Eth Slide 10-19

  21. Work • Provides a link between force and energy • The work, W, done by a constant force on an object is defined as the product of the component of the force along the direction of displacement and the magnitude of the displacement

  22. Work, cont. • F is the magnitude of the force • Δ x is the magnitude of the object’s displacement • q is the angle between

  23. Work, cont. • This gives no information about • the time it took for the displacement to occur • the velocity or acceleration of the object • Work is a scalar quantity

  24. Units of Work • SI • Newton • meter = Joule • N • m = J • J = kg • m2 / s2 • US Customary • foot • pound • ft• lb • no special name

  25. More About Work • The work done by a force is zero when the force is perpendicular to the displacement • cos 90° = 0 • If there are multiple forces acting on an object, the total work done is the algebraic sum of the amount of work done by each force

  26. When Work is Zero • Displacement is horizontal • Force is vertical • cos 90° = 0

  27. More About Work, cont. • Work can be positive or negative • Positive if the force and the displacement are in the same direction • Negative if the force and the displacement are in the opposite direction (friction, for instance)

  28. Work Can Be Positive or Negative • Work is positive when lifting the box • Work would be negative if lowering the box • The force would still be upward, but the displacement would be downward

  29. Work and Dissipative Forces • Work can be done by friction • The energy lost to friction by an object goes into heating both the object and its environment • Some energy may be converted into sound • For now, the phrase “Work done by friction” will denote the effect of the friction processes on mechanical energy alone

  30. Energy Transfers These change the energy of the system. Interactions with the environment. Work is the mechanical transfer of energy to or from a system via pushes and pulls. Slide 10-20

  31. Kinetic Energy • Energy associated with the motion of an object • Scalar quantity with the same units as work - joules • Work is related to kinetic energy

  32. Kinetic Energy Example • At rest, KE = ½m(0)2= 0, but with the presence of an instantaneous velocity, the car has KE. • If the velocity is constant, then KE is constant. • If acceleration is present, then the final velocity is determined and used to calculate the KE of the car at the point of time or distance being considered.

  33. Work-Kinetic Energy Theorem • When work is done by a net force on an object and the only change in the object is its speed, the work done is equal to the change in the object’s kinetic energy • Speed will increase if work is positive • Speed will decrease if work is negative

  34. Work and Kinetic Energy • An object’s kinetic energy can also be thought of as the amount of work the moving object could do in coming to rest • The moving hammer has kinetic energy and can do work on the nail

  35. Energy Transfers: Work W K W Eth Slide 10-21 W Us

  36. The Work-Energy Equation Slide 10-22

  37. Types of Forces • There are two general kinds of forces • Conservative • Work and energy associated with the force can be recovered • Examples are gravity, springs, electromagnetism • Non-conservative • The forces are generally dissipative and work done against it cannot easily be recovered • Examples include friction, propulsive forces, and sound

  38. Conservative Forces • A force is conservative if the work it does on an object moving between two points is independent of the path the objects take between the points • The work depends only upon the initial and final positions of the object (displacement) • Any conservative force can have a potential energy function associated with it

  39. More About Conservative Forces • Examples of conservative forces include: • Gravity • Spring force • Electromagnetic forces • Potential energy is another way of looking at the work done by conservative forces

  40. Nonconservative Forces • A force is nonconservative if the work it does on an object depends on the path taken by the object between its final and starting points. • Examples of nonconservative forces • kinetic friction, air drag, propulsive forces, and sound

  41. Friction as a Nonconservative Force • The friction force is transformed from the kinetic energy of the object into a type of energy associated with temperature • The objects are warmer than they were before the movement • Internal Energy is the term used for the energy associated with an object’s temperature

  42. Friction Depends on the Path • The blue path is shorter than the red path • The work required is less on the blue path than on the red path • Friction depends on the path and so is a non-conservative force

  43. Potential Energy • Potential energy is associated with the position of the object within some system • Potential energy is a property of the system, not the object • A system is a collection of objects interacting via forces or processes that are internal to the system

  44. Potential Energy Example • At position A, the elephant has no potential energy, while at B, its mass has been elevated within a system and has PE= mgh

  45. Work and Potential Energy • For every conservative force a potential energy function can be found • Evaluating the difference of the function at any two points in an object’s path gives the negative of the work done by the force between those two points

  46. Gravitational Potential Energy • Gravitational Potential Energy is the energy associated with the relative position of an object in space near the Earth’s surface • Objects interact with the earth through the gravitational force • Actually the potential energy is for the earth-object system

  47. Work and Gravitational Potential Energy • PE = mgy • Units of Potential Energy are the same as those of Work and Kinetic Energy

  48. Work-Energy Theorem, Extended • The work-energy theorem can be extended to include potential energy: • If other conservative forces are present, potential energy functions can be developed for them and their change in that potential energy added to the right side of the equation

  49. The Law of Conservation of Energy Slide 10-23

  50. The Basic Equation • KfUfEthKiUi • A few things to note: • Work can be positive (work in) or negative (work out) • We are, for now, ignoring heat. • Thermal energy is…special. When energy changes to thermal energy, this change is irreversible. Slide 10-24

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