Chapter 6 Conservation of Energy MFMc Graw Ch

  • Slides: 43
Download presentation
Chapter 6 Conservation of Energy MFMc. Graw Ch 06 - Energy - Revised: 2/20/10

Chapter 6 Conservation of Energy MFMc. Graw Ch 06 - Energy - Revised: 2/20/10

Conservation of Energy • Work by a Constant Force • Kinetic Energy • Potential

Conservation of Energy • Work by a Constant Force • Kinetic Energy • Potential Energy • Work by a Variable Force • Springs and Hooke’s Law • Conservation of Energy • Power MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 2

The Law of Conservation of Energy The total energy of the Universe is unchanged

The Law of Conservation of Energy The total energy of the Universe is unchanged by any physical process. The three kinds of energy are: kinetic energy, potential energy, and rest energy. Energy may be converted from one form to another or transferred between bodies. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 3

MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 4

MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 4

Work by a Constant Force Work is an energy transfer by the application of

Work by a Constant Force Work is an energy transfer by the application of a force. For work to be done there must be a nonzero displacement. The unit of work and energy is the joule (J). 1 J = 1 Nm = 1 kg m 2/s 2. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 5

Work - Example Only the force in the direction of the displacement that does

Work - Example Only the force in the direction of the displacement that does work. F An FBD for the box at left: rx y rx N w x F The work done by the force F is: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 6

Work - Example The work done by the normal force N is: The normal

Work - Example The work done by the normal force N is: The normal force is perpendicular to the displacement. The work done by gravity (w) is: The force of gravity is perpendicular to the displacement. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 7

Work - Example The net work done on the box is: MFMc. Graw Ch

Work - Example The net work done on the box is: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 8

Work Done In general, the work done by a force F is defined as

Work Done In general, the work done by a force F is defined as where F is the magnitude of the force, r is the magnitude of the object’s displacement, and is the angle between F and r (drawn tail-to-tail). MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 9

Work - Example: A ball is tossed straight up. What is the work done

Work - Example: A ball is tossed straight up. What is the work done by the force of gravity on the ball as it rises? y r FBD for rising ball: x w MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 10

Inclined Plane-V Constant A box of mass m is towed up a frictionless incline

Inclined Plane-V Constant A box of mass m is towed up a frictionless incline at constant speed. The applied force F is parallel to the incline. y Question: What is the net work done on the box? F x N F An FBD for the box: w Apply Newton’s 2 nd Law: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 11

Inclined Plane-V Constant Example continued: The magnitude of F is: If the box travels

Inclined Plane-V Constant Example continued: The magnitude of F is: If the box travels along the ramp a distance of x the work by the force F is The work by gravity is MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 12

Inclined Plane-V Constant Example continued: The work by the normal force is: The net

Inclined Plane-V Constant Example continued: The work by the normal force is: The net work done on the box is: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 13

Inclined Plane-Acceleration Example: What is the net work done on the box in the

Inclined Plane-Acceleration Example: What is the net work done on the box in the previous example if the box is not pulled at constant speed? Proceeding as before: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 New Term 14

Kinetic Energy is an object’s translational kinetic energy. This is the energy an object

Kinetic Energy is an object’s translational kinetic energy. This is the energy an object has because of its state of motion. It can be shown that, in general Net Work = Change in K MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 15

Kinetic Energy Example: The extinction of the dinosaurs and the majority of species on

Kinetic Energy Example: The extinction of the dinosaurs and the majority of species on Earth in the Cretaceous Period (65 Myr ago) is thought to have been caused by an asteroid striking the Earth near the Yucatan Peninsula. The resulting ejecta caused widespread global climate change. If the mass of the asteroid was 1016 kg (diameter in the range of 49 miles) and had a speed of 30. 0 km/sec, what was the asteroid’s kinetic energy? This is equivalent to ~109 Megatons of TNT. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 16

Gravitational Potential Energy Part 1 - Close to Earth’s Surface Potential energy is an

Gravitational Potential Energy Part 1 - Close to Earth’s Surface Potential energy is an energy of position. There are potential energies associated with different forces. Forces that have a potential energy associated with them are called conservative forces. In general Not all forces are conservative, i. e. Friction. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 17

Gravitational Potential Energy The change in gravitational potential energy (only near the surface of

Gravitational Potential Energy The change in gravitational potential energy (only near the surface of the Earth) is where y is the change in the object’s vertical position with respect to some reference point. You are free to choose to location of this where ever it is convenient. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 18

GPE Problem The table is 1. 0 m tall and the mass of the

GPE Problem The table is 1. 0 m tall and the mass of the box is 1. 0 kg. Ques: What is the change in gravitational potential energy of the box if it is placed on the table? U=0 First: Choose the reference level at the floor. U = 0 here. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 19

GPE Problem Example continued: Now take the reference level (U = 0) to be

GPE Problem Example continued: Now take the reference level (U = 0) to be on top of the table so that yi = 1. 0 m and yf = 0. 0 m. The results do not depend on the location of U = 0. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 20

Total Mechanical Energy Mechanical energy is The total mechanical energy of a system is

Total Mechanical Energy Mechanical energy is The total mechanical energy of a system is conserved whenever nonconservative forces do no work. That is E i = Ef or K = U. Then if K increases U decreases and vice versa MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 21

Mechanical Energy Problem A cart starts from position 4 with v = 15. 0

Mechanical Energy Problem A cart starts from position 4 with v = 15. 0 m/s to the left. Find the speed of the cart at positions 1, 2, and 3. Ignore friction. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 22

Mechanical Energy Problem Or use E 3=E 2 Or use E 3=E 1 E

Mechanical Energy Problem Or use E 3=E 2 Or use E 3=E 1 E 2=E 1 MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 23

Roller Coaster Problem A roller coaster car is about to roll down a track.

Roller Coaster Problem A roller coaster car is about to roll down a track. Ignore friction and air resistance. m = 988 kg 40 m 20 m y=0 (a) At what speed does the car reach the top of the loop? MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 24

Roller Coaster Problem Example continued: (b) What is the force exerted on the car

Roller Coaster Problem Example continued: (b) What is the force exerted on the car by the track at the top of the loop? Apply Newton’s Second Law: FBD for the car: y x N MFMc. Graw w Ch 06 - Energy - Revised: 2/20/10 25

Roller Coaster Problem Example continued: (c) From what minimum height above the bottom of

Roller Coaster Problem Example continued: (c) From what minimum height above the bottom of the track can the car be released so that it does not lose contact with the track at the top of the loop? Using conservation of mechanical energy: Solve for the starting height MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 26

Roller Coaster Problem Example continued: What is vmin? v = vmin when N =

Roller Coaster Problem Example continued: What is vmin? v = vmin when N = 0. This means that The initial height must be MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 27

Nonconservative Forces What do you do when there are nonconservative forces? For example, if

Nonconservative Forces What do you do when there are nonconservative forces? For example, if friction is present The work done by friction. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 28

Gravitational Potential Energy Part 2 - Away from Earth’s Surface The general expression for

Gravitational Potential Energy Part 2 - Away from Earth’s Surface The general expression for gravitational potential energy is: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 29

Gravitational Potential Energy Example: What is the gravitational potential energy of a body of

Gravitational Potential Energy Example: What is the gravitational potential energy of a body of mass m on the surface of the Earth? MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 30

Planetary Motion A planet of mass m has an elliptical orbit around the Sun.

Planetary Motion A planet of mass m has an elliptical orbit around the Sun. The elliptical nature of the orbit means that the distance between the planet and Sun varies as the planet follows its orbital path. Take the planet to move counterclockwise from its initial location. QUES: How does the speed of a planet vary as it orbits the Sun once? The mechanical energy of the planet-sun system is: B MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 r A 31

Planetary Motion B r A At point “B” the planet is the farthest from

Planetary Motion B r A At point “B” the planet is the farthest from the Sun. At point “A” the planet is at its closest approach to the sun. Starting from point “B” (where the planet moves the slowest), as the planet moves in its orbit r begins to decrease. As it decreases the planet moves faster. At point “A” the planet reaches its fastest speed. As the planet moves past point A in its orbit, r begins to increase and the planet moves slower. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 32

Work by a Variable Force Work can be calculated by finding the area underneath

Work by a Variable Force Work can be calculated by finding the area underneath a plot of the applied force in the direction of the displacement versus the displacement. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 33

Example: What is the work done by the variable force shown below? Fx (N)

Example: What is the work done by the variable force shown below? Fx (N) F 3 The net work is then W 1+W 2+W 3. F 2 F 1 x 2 x 3 x (m) The work done by F 1 is The work done by F 2 is The work done by F 3 is MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 34

Spring Force By hanging masses on a spring we find that stretch applied force.

Spring Force By hanging masses on a spring we find that stretch applied force. This is Hooke’s law. For an ideal spring: Fx = kx Fx is the magnitude of the force exerted by the free end of the spring, x is the measured stretch of the spring, and k is the spring constant (a constant of proportionality; its units are N/m). A larger value of k implies a stiffer spring. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 35

Spring Force (a) A force of 5. 0 N applied to the end of

Spring Force (a) A force of 5. 0 N applied to the end of a spring cause the spring to stretch 3. 5 cm from its relaxed length. Ques: How far does a force of 7. 0 N cause the same spring to stretch? For springs F x. This allows us to write Solving for x 2: MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 36

Spring Force Example continued: (b) What is the spring constant of this spring? Or

Spring Force Example continued: (b) What is the spring constant of this spring? Or MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 37

Spring Force An ideal spring has k = 20. 0 N/m. What is the

Spring Force An ideal spring has k = 20. 0 N/m. What is the amount of work done (by an external agent) to stretch the spring 0. 40 m from its relaxed length? MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 38

Elastic Potential Energy The work done in stretching or compressing a spring transfers energy

Elastic Potential Energy The work done in stretching or compressing a spring transfers energy to the spring. Below is the equation of the spring potential energy. The spring is considered the system MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 39

Elastic Potential Energy A box of mass 0. 25 kg slides along a horizontal,

Elastic Potential Energy A box of mass 0. 25 kg slides along a horizontal, frictionless surface with a speed of 3. 0 m/s. The box encounters a spring with k = 200 N/m. Ques: How far is the spring compressed when the box is brought to rest? MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 40

Power is the rate of energy transfer. Average Power Instantaneous Power The unit of

Power is the rate of energy transfer. Average Power Instantaneous Power The unit of power is the watt. 1 watt = 1 J/s = 1 W. MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 41

Power - Car Example A race car with a mass of 500. 0 kg

Power - Car Example A race car with a mass of 500. 0 kg completes a quarter-mile (402 m) race in a time of 4. 2 s starting from rest. The car’s final speed is 125 m/s. (Neglect friction and air resistance. ) Ques: What is the engine’s average power output? MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 42

Summary • Conservation of Energy • Calculation of Work Done by a Constant or

Summary • Conservation of Energy • Calculation of Work Done by a Constant or Variable Force • Kinetic Energy • Potential Energy (gravitational, elastic) • Power MFMc. Graw Ch 06 - Energy - Revised: 2/20/10 43