Today: Work, Kinetic Energy, Potential Energy. No Recitation Quiz this week

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1 Today: Work, Kinetic Energy, Potential Energy HW #4 due Thursday, 11:59 p.m. pm No Recitation Quiz this week 1

2 What is Energy? Mechanical Electromagnetic PHY 11 PHY 13 Chemical CHE 105 Nuclear PHY 555 E = mc!!

3 Work in Physics By applying a force F, you have moved the car through a displacement Δx!! That was a lot of work!! 3

4 Work in Physics Δ x F x The work W done on an object by a constant force F during a linear displacement is given by: W = F Δx > 0 (scalar quantity) where F is the magnitude of the force, Δx is the magnitude of the displacement, and F and Δx point in the same direction. If F and Δx point in opposite SI Unit : directions, then W < 0. Joule = N m= kg m /s 4

5 Work in Physics What if the force is NOT in the same direction as the displacement? θ F F cosθ y x Δ x The work W done on an object by a constant force F during a linear displacement Δx is given (in general) by W = (F cos θ) Δx (scalar quantity) F = magnitude of force Δx = magnitude of displacement θ = angle between F and Δx 5

6 Sign (+ or ) of the Work Work can be either positive (> 0) or negative (< 0). W = (F cos θ) Δx F and Δx are magnitudes (so both > 0) cos θ determines the sign of W (+ or ) [ direction of F relative to Δx ] Lifting i : upward force exerted by woman mg Δx Work done by the woman is > 0. Work done by gravity is < 0. 6

7 Sign (+ or ) of the Work Work can be either positive (> 0) or negative (< 0). W = (F cos θ) Δx F and Δx are magnitudes (so both > 0) cos θ determines the sign of W (+ or ) [ direction of F relative to Δx ] Lowering : upward force exerted by woman mg Δx Work done by the woman is < 0. Work done by gravity is > 0. 7

8 Work and Dissipative Forces Recall example worked in class of hockey puck sliding across ice : f k x f k In this example, the work done by the force of kinetic friction is NEGATIVE (θ = 180 ). Frictional work is (usually) negative. Negative work by friction results in the DISSIPATION of mechanical energy. The lost energy is primarily dissipated as HEAT. 8

9 Example A worker pushes a wheelbarrow 5.0 m along a level surface, exerting a constant horizontal force of N. If a frictional force of 43 N acts on the wheelbarrow while it is moving, what is the NET WORK done on the wheelbarrow? 5.0 m 43 N 50 N 9

10 Example: 5.5 Starting from rest, a 5.0 kg block slides.50 m down a 30 ramp. The coefficient of kinetic friction between the block and ramp is μ k = Determine the : (a) Work done by the force of gravity. (b) Work done by the frictional force. (c) Work done by the normal force. 10

11 Kinetic Energy The kinetic energy of an object of mass m moving with a speed v is : 1 mv KE SI unit : Joule = kg m /s (scalar quantity) Work Energy Theorem : The net work done on an object is equal to the change in the object s kinetic energy W net KE f KE i 1 mv 1 f mv i KE If W net > 0, the object s speed increases If W net < 0, the object s speed decreases 11

12 Kinetic Energy On previous slide, we thought of work as causing an increase or decrease in an object s speed. Conversely, we can think of the kinetic energy as being equivalent to the amount of work a moving object can do in coming to rest. 1

13 Example: 5.15 A 7.8 gram bullet moving at 575 m/s penetrates a tree trunk to a depth of 5.50 cm. ()U (a) Use work and energy considerations to find the average frictional force that stops the bullet. (b) Assuming the frictional force is constant, determine how much time elapses between the moment the bullet enters the tree and the moment it stops moving. 13

14 Example A 1000 kg car slams on the brakes, leaving 7.0 m long skid marks. Suppose a constant friction force of 8000 N acts on the car while it is skidding. What was the car s minimum speed? 14

15 Conservative vs. Non Conservative Forces In general, there are two kinds of forces : Conservative Forces Non Conservative Forces Energy can be Energy cannot be recovered recovered Eg E.g., Gravity Eg E.g., Friction Generally: Dissipative 15

16 Gravitational Potential Energy Suppose an object falls from some height to a lower height. How much work has been done by gravity? y W g mg y y (cos0) f i 0 F Δy cos θ y i mg Δy y f If an object is raised to some height, there is the potential for gravity to do positive work. Positive work means an increase in the object s kinetic energy. 16

17 Gravitational Potential Energy So we then define the gravitational potential energy y : vertical position Gravitational Potential Energy relative to Earth s PE = mgy surface (or another reference point) SI unit: Joule The gravitational potential energy quantifies the magnitude of work that can be done by gravity. By the Work Energy Theorem, the gravitational potential energy is then equal to the change in the object s kinetic energy if it falls a distance y. 17

18 Reference Level for Potential Energy We have defined the gravitational potential energy to be: PE mgy Q: Does it matter where we define y = 0? A: No, it doesn t matter. All that matters is the difference in the potential energy, ΔPE = mg Δy. It doesn t matter where we define zero to be. 100 m 5 m 95 m 0 m In both of these, the object falls 5 m. 18

19 Gravity and Conservation of Energy Conservation Law : If a physical quantity is conserved, the numerical value of the physicalquantity remains unchanged. Conservation of Mechanical Energy : KE i PE i KE f PE f Sum of kinetic energy and gravitational potential energy remains constant at all times. It is a conserved quantity. If we denote the total mechanical energy as E = KE + PE, the total mechanical energy E is conserved at all times. 19

20 Conservation of Energy Ignoring dissipative forces (air resistance), at all times KE i PE i KE f PE f Sum of the kinetic and gravitational potential energy remains constant at all times. 1 mv 1 mgy 1 1 mv mgy initial total mechanical energy final total mechanical energy 0

21 Example A 5 kg object is dropped from a height of 15.0 m above the ground. Assuming air resistance is negligible (a) What is its speed m above the ground? (b) What is its speed when it hits the ground? 1

22 Example A skier starts from rest at the top of a frictionless ramp of height 0.0 m. 0 At the bottom of the ramp, the skier encounters a horizontal surface where the coefficient of kinetic friction is μ k = Neglect air resistance. (a) () Find the skier s speed at the bottom of the ramp. (b) How far does the skier travel on the horizontal surface before coming to rest?

23 Next Class Spring Potential Energy, Energy Conservation, Power We will NOT cover 5.7 3

= 1 2 kx2 dw =! F! d! r = Fdr cosθ. T.E. initial. = T.E. Final. = P.E. final. + K.E. initial. + P.E. initial. K.E. initial =

= 1 2 kx2 dw =! F! d! r = Fdr cosθ. T.E. initial. = T.E. Final. = P.E. final. + K.E. initial. + P.E. initial. K.E. initial = Practice Template K.E. = 1 2 mv2 P.E. height = mgh P.E. spring = 1 2 kx2 dw =! F! d! r = Fdr cosθ Energy Conservation T.E. initial = T.E. Final (1) Isolated system P.E. initial (2) Energy added E added

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