1. Chapter 6 Work and Energy

4. So far : Motion analysis with forces . NOW : An alternative analysis using the concepts of Work & Energy . Work : Precisely defined in physics. Describes what is accomplished by a force in moving an object through a distance.

5. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component of the force in the direction of displacement: (6-1)

6. W = Fd cos θ Simple special case : F & d are parallel: θ = 0, cos θ = 1  W = Fd Example: d = 50 m, F = 30 N W = (30N)(50m) = 1500 N m Work units: Newton - meter = Joule 1 N m = 1 Joule = 1 J θ F d

9. W = F || d = Fd cos θ m = 50 kg, F p = 100 N, F fr = 50 N, θ = 37º W net = W G + W N +W P + W fr = 1200 J W net = (F net ) x x = (F P cos θ – F fr )x = 1200 J Example 6-1

10. Example 6-1 Σ F =ma F H = mg W H = F H (d cos θ ) = mgh F G = mg W G = F G (d cos(180- θ )) = -mgh W net = W H + W G = 0

11. 6-1 Work Done by a Constant Force Work done by forces that oppose the direction of motion, such as friction, will be negative . Centripetal forces do no work, as they are always perpendicular to the direction of motion.

12. 6-3 Kinetic Energy, and the Work-Energy Principle Energy was traditionally defined as the ability to do work . We now know that not all forces are able to do work; however, we are dealing in these chapters with mechanical energy, which does follow this definition. Energy  The ability to do work Kinetic Energy  The energy of motion “ Kinetic”  Greek word for motion An object in motion has the ability to do work

13. Consider an object moving in straight line. Starts at speed v1 . Due to presence of a net force F net , accelerates (uniform) to speed v2 , over distance d . 6-3 Kinetic Energy, and the Work-Energy Principle

14. Newton’s 2nd Law: F net = ma (1) 1d motion, constant a  (v 2 ) 2 = (v 1 ) 2 + 2ad  a = [(v 2 ) 2 - (v 1 ) 2 ]/(2d) (2) Work done: W net = F net d (3) Combine (1), (2), (3):  W net = mad = md [(v 2 ) 2 - (v 1 ) 2 ]/(2d) OR W net = (½)m(v 2 ) 2 – (½)m(v 1 ) 2 6-3 Kinetic Energy, and the Work-Energy Principle

15. 6-3 Kinetic Energy, and the Work-Energy Principle If we write the acceleration in terms of the velocity and the distance , we find that the work done here is We define the translational kinetic energy : (6-2) (6-3)

18. 6-3 Kinetic Energy, and the Work-Energy Principle Because work and kinetic energy can be equated, they must have the same units : kinetic energy is measured in joules . Work done on hammer: W h =  KE h = -Fd = 0 – (½)m h (v h ) 2 Work done on nail: W n =  KE n = Fd = (½)m n (v n ) 2 - 0

20. 6-4 Potential Energy In raising a mass m to a height h , the work done by the external force is We therefore define the gravitational potential energy: (6-5a) (6-6) W G = -mg(y 2 –y 1 ) = -(PE 2 – PE 1 ) = -  PE

21. W ext =  PE The Work done by an external force to move the object of mass m from point 1 to point 2 (without acceleration) is equal to the change in potential energy between positions 1 and 2 W G = -  PE 6-4 Potential Energy

22. 6-4 Potential Energy This potential energy can become kinetic energy if the object is dropped. Potential energy is a property of a system as a whole, not just of the object (because it depends on external forces). If , where do we measure y from? It turns out not to matter, as long as we are consistent about where we choose y = 0. Only changes in potential energy can be measured.

23. 6-4 Potential Energy Potential energy can also be stored in a spring when it is compressed ; the figure below shows potential energy yielding kinetic energy.

24. 6-4 Potential Energy Restoring force “ Spring equation or Hook’s law” where k is called the spring constant , and needs to be measured for each spring. (6-8) The force required to compress or stretch a spring is : F P = kx

25. 6-4 Potential Energy The force increases as the spring is stretched or compressed further (elastic) (not constant) . We find that the potential energy of the compressed or stretched spring, measured from its equilibrium position, can be written: (6-9)

26. 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 CAN’T be defined for non-conservative forces The most common example of a non-conservative force is FRICTION 6-5 Conservative and Nonconservative Forces

27. 6-5 Conservative and Nonconservative Forces If friction is present, the work done depends not only on the starting and ending points, but also on the path taken. Friction is called a nonconservative force.

28. 6-5 Conservative and Nonconservative Forces Potential energy can only be defined for conservative forces.

29. 6-5 Conservative and Nonconservative Forces Therefore, we distinguish between the work done by conservative forces and the work done by nonconservative forces. We find that the work done by nonconservative forces is equal to the total change in kinetic and potential energies: W net = W c + W nc W net = Δ KE = W c + W nc W nc = Δ KE - W c = Δ KE – (– Δ PE) (6-10)

30. 6-6 Mechanical Energy and Its Conservation If there are no nonconservative forces, the sum of the changes in the kinetic energy and in the potential energy is zero – the kinetic and potential energy changes are equal but opposite in sign.  KE +  PE = 0 This allows us to define the total mechanical energy : And its conservation : (6-12b)

31.  PE 2 = 0 KE 2 = (½)mv 2 KE 1 + PE 1 = KE 2 + PE 2 0 + mgh = (½)mv 2 + 0 v 2 = 2gh  KE + PE = same as at points 1 & 2 The sum remains constant  PE 1 = mgh KE 1 = 0

32. 6-7 Problem Solving Using Conservation of Mechanical Energy In the image on the left, the total mechanical energy is: The energy buckets (right) show how the energy moves from all potential to all kinetic.

33. 6-7 Problem Solving Using Conservation of Mechanical Energy If there is no friction , the speed of a roller coaster will depend only on its height compared to its starting point.

34. 6-7 Problem Solving Using Conservation of Mechanical Energy For an elastic force , conservation of energy tells us: (6-14)

35. 6-8 Other Forms of Energy; Energy Transformations and the Conservation of Energy Some other forms of energy: Electric energy, nuclear energy, thermal energy, chemical energy. Work is done when energy is transferred from one object to another. Accounting for all forms of energy, we find that the total energy neither increases nor decreases. Energy as a whole is conserved .

36. 6-9 Energy Conservation with Dissipative Processes; Solving Problems If there is a nonconservative force such as friction, where do the kinetic and potential energies go? They become heat ; the actual temperature rise of the materials involved can be calculated.

41. 6-10 Power Power is also needed for acceleration and for moving against the force of gravity. The average power can be written in terms of the force and the average velocity : (6-17)

42. Part a) constant speed a = 0 ∑F x = 0 F – F R – mg sin θ = 0 F = F R + mg sin θ F = 3100 N P = F v = 91 hp Part b) constant acceleration Now, θ = 0 ∑ F x = ma F – F R = ma v = v 0 + at a = 0.93 m/s 2 F = ma + F R = 2000 N P = Fv = 82 hp Example 6-15