AP Physics C - Mechanics. Energy and Work. Slide 1 / 125 Slide 2 / 125. Slide 4 / 125. Slide 3 / 125. Slide 6 / 125. Slide 5 / 125.

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1 Slide 1 / 125 Slide 2 / 125 AP Physics C - Mechanics Work and nergy Slide 3 / 125 Slide 4 / 125 Table of Contents Click on the topic to go to that section nergy and Work Conservative and Non-Conservative Forces Conservation of Total Mechanical nergy Two imensional Forces and Work Work done by a Position ependent Force Position ependent Potential nergy Power nergy and Work Return to Table of Contents Slide 5 / 125 nergy The concept of energy is so fundamental, like space and time, that there is no real good definition of what it "is." However, just like space and time, that doesn't stop us from doing very useful calculations with energy. There are some things we can say about it: It is the ability to do work. It can be stored. It can be changed from one form to another (light to thermal energy, mechanical to thermal energy, gravitational potential energy to kinetic energy). It can be measured and compared. Slide 6 / 125 Work Work has the ability to increase or decrease the amount of nergy at a certain position and time in space. Work has the same units as energy - Joules. What is Work? It is not what is talked about in common language. It is unfortunate that sometimes Physics uses words that are used everyday - in a quite different fashion. For example - if you're holding up a heavy box, do you think you're doing work? id you notice a term in the bullet list above that hasn't been defined yet?

2 You're not! Slide 7 / 125 Work Work, in physics terms, is defined as the exertion of a force over a displacement where only the component of the force in the direction of the motion is relevant. For now, we'll assume a constant force. If you're just holding a box, you are certainly exerting an upward force on the box (to keep gravity from pulling it to the ground), but it's not moving, so there is no displacement. Therefore, there is no work. You learned the following equation: W = Fd parallel = Fdcosθ Slide 8 / 125 Work A more elegant way to represent this is by using vector notation and a specific type of vector multiplication called the vector dot product, or just dot product. The result of the dot product of two vectors is a scalar - and is the length of one vector projected on the other - so this achieves the goal of just using the component of force along the direction of the displacement. ut where is the work being done? Where is the energy being increased or decreased? The entire universe? We need two more definitions to bound these questions. where θ is the angle between the Force and the displacement. Slide 9 / 125 System and nvironment The system and the environment. A system is a small segment of the universe that will be considered in solving a specific problem, and we will erect a boundary around it. Any force or object outside this boundary will not be considered. The environment is everything outside the system boundary. The system can be a particle, a group of particles, an object, an area of space, and its size and shape is totally determined by how you want to solve the problem. Slide 10 / 125 System and nvironment So we can make the problem solvable. y defining an appropriate system, we can isolate the forces that are within the system from the forces that act on the system from the environment. If the forces are internal to the system, then there is no change in the energy of the system (as long as we don't consider thermal energy - which we won't for now). If the forces are external, then there will be a change in the energy of the system. Why are we defining a system and its environment? Slide 11 / Which of the following are characteristics of energy? A Thermal energy can be changed to mechanical energy. Slide 11 () / Which of the following are characteristics of energy? A Thermal energy can be changed to mechanical energy. Mechanical energy can be changed to thermal energy. Mechanical energy can be changed to thermal energy. C nergy can be stored. nergy has the ability to do work. C nergy can be stored. nergy has the ability to do work. All of the above. All of the above.

3 2 A system is defined as: Slide 12 / 125 A All the forces that are external to the boundary between it and the rest of the universe. 2 A system is defined as: Slide 12 () / 125 A All the forces that are external to the boundary between it and the rest of the universe. A small segment of the universe that has no internal forces. A small segment of the universe that has no internal forces. C A small segment of the universe that is chosen to solve a problem. Forces internal to the system can change its total mechanical energy. A small segment of the universe that is chosen to solve a problem. Forces internal to the system cannot change its total mechanical energy. C A small segment of the universe that is chosen to solve a problem. Forces internal to the system can change its total mechanical energy. A small segment of the universe that is chosen to solve a problem. Forces internal to the system cannot change its total mechanical energy. Uniquely for a problem. Only one specific system can be used to solve a problem. Uniquely for a problem. Only one specific system can be used to solve a problem. Slide 13 / 125 Slide 13 () / In solving an energy problem, the environment is defined as: A An area that contains no forces. An area that is partially in, and partially outside the system. C The source of the external forces on the system. The source of the internal forces on the system. 3 In solving an energy problem, the environment is defined as: A An area that contains no forces. An area that is partially in, and partially outside the system. C The source of the external forces on C the system. The source of the internal forces on the system. A small area within the system. A small area within the system. Slide 14 / 125 Slide 15 / 125 Work Units of Work and nergy If the force acts in the same direction as the object's motion, then the work done is positive, and the energy of the object increases. If the force acts in the opposite direction as the object's motion, then the work done is negative and the energy of the object decreases. If the object does not move, then zero work is done. Work is a scalar - it has magnitude, but not direction. The unit of work is the Joule - just like energy. This equation gives us the units of work. Since force is measured in Newtons (N) and distance is measured in meters (m) the unit of work is the Newton-meter (N-m). And since N = kg-m/s 2 ; a N-m also equals a kg-m 2 /s 2. In honor of James Joule, who made critical contributions in developing the idea of energy, the unit of work and energy is also known as the Joule (J). 1 Joule = 1 Newton-meter = 1 kilogram-meter 2 /second 2 1 J = 1 N-m = 1 kg-m 2 /s 2

4 Slide 16 / 125 James Prescott Joule Joule was instrumental in showing that different forms of energy can be converted into other forms - most notably mechanical to thermal energy. efore Joule, it was commonly accepted that thermal energy is conserved. This was disproved by Joule's extremely accurate and precise measurements showing how thermal energy is just another form of energy. This was made possible by his experience as a brewer which relied on very accurate measurements of temperature, time and volume! Slide 17 / Which is a valid unit for work? A N/m N-s C W J/s J Slide 17 () / Which is a valid unit for work? A N/m N-s F v Slide 18 / 125 Force and Work C W J/s v #x F J F v #x #x Slide 19 / 125 Slide 19 () / A 36.0 N force is applied to an object that moves 11.0 m in the same direction as the applied force on a frictionless surface. How much work is done on the object? F 5 A 36.0 N force is applied to an object that moves 11.0 m in the same direction as the applied force on a frictionless surface. How much work is done on the object? F

5 Slide 20 / A 36.0 N force is applied to an object that moves 11.0 m in the opposite direction of the applied force on a frictionless surface. How much work is done on the object? Slide 20 () / A 36.0 N force is applied to an object that moves 11.0 m in the opposite direction of the applied force on a frictionless surface. How much work is done on the object? F v F v Slide 21 / A 36 N force is applied to an object that remains stationary. How much work is done on the object by the applied force? Slide 21 () / A 36 N force is applied to an object that remains stationary. How much work is done on the object by the applied force? F F Slide 22 / 125 Work Slide 23 / In which of the following cases is positive work done by an external force? You have to very specific about using work. The system or environment that the work is acting on needs to be specified. For example: "An applied force does 12 J of work on a box." "Gravity does -5 J of work on a box that is being raised up." This next sentence is not a complete statement. What's missing? "An external force does 6 J of work." The system or the environment that the work is acting on must be described. A A softball player catches a ball in her glove. A home owner is pushing a lawnmower from rest. C A drive applies the break to his car. A student holds her textbook and is not moving. A ball falls from a height. The ground applies a force to stop the ball.

6 Slide 23 () / In which of the following cases is positive work done by an external force? A A softball player catches a ball in her glove. Slide 24 / A 2 kg block slides 4.5 m to the right on a frictionless table with a constant velocity of 5 m/s. What is the net work on the block? A home owner is pushing a lawnmower from rest. C A drive applies the break to his car. A student holds her textbook and is not moving. A ball falls from a height. The ground applies a force to stop the ball. Slide 24 () / A 2 kg block slides 4.5 m to the right on a frictionless table with a constant velocity of 5 m/s. What is the net work on the block? Slide 25 / A book is held at a height of 2.0 m for 20 s. How much work is done on the book? A 400 J Since the block is moving with a constant velocity, there is zero net force on the block. 200 J C 40 J 20 J 0 J Slide 25 () / A book is held at a height of 2.0 m for 20 s. How much work is done on the book? A 400 J Slide 26 / An athlete is holding a football. He then throws it to a teammate who catches it. escribe the work done on the football by both players starting from when the football is Students type their answers here at rest before it is thrown and after it is caught. 200 J C 40 J 20 J 0 J

7 Slide 26 () / 125 Slide 27 / An athlete is holding a football. He then throws it to a teammate who catches it. escribe the work done on the football by both players starting from when the football is Students type their answers here at rest before it is thrown and after it is caught. When the ball is at rest before it is thrown and after it is caught, there is no work done as there is no displacement. Positive work is done as it is thrown since the force is in the same direction as the displacement of the ball. Negative work is done by the receiver in catching the ball as the force is opposite the displacement. Conservative and Non-Conservative Forces Slide 28 / 125 Slide 29 / 125 Return to Table of Contents Work - nergy quation When a net external force acts on an object in the same direction of its displacement, positive work is done - just think of pushing a ball on the floor by applying a constant force. Δx parallel to a constant force enables us to use kinematics equation 3 solving for aδx Recognize anything? substituting into W equation Work - nergy quation y applying a constant force over a displacement, we've derived both the Work - nergy quation and found the expression for kinetic energy. Net positive work applied to a system increases its kinetic energy. What if an object is moving in the positive x direction with a velocity, v 0, and a force is applied opposite its displacement? Slide 30 / 125 Work - nergy quation Slide 31 / How much net external force must be applied to an object such that it gains J of kinetic energy over a displacement of 20.0 m, parallel to the direction of the external force? Negative work is done on the object, so its kinetic energy, and velocity decreases; v f < v 0

8 Slide 31 () / How much net external force must be applied to an object such that it gains J of kinetic energy over a displacement of 20.0 m, parallel to the direction of the external force? Slide 32 / A net external force of 5.00 N is applied to a 5.10 kg object and it moves parallel to the force application a displacement of 20.0 m. What is the object's final velocity if it started at rest? Slide 32 () / A net external force of 5.00 N is applied to a 5.10 kg object and it moves parallel to the force application a displacement of 20.0 m. What is the object's final velocity if it started at rest? (F parallel to Δx) Slide 33 / Over what displacement must a N net external force be applied, in parallel with the displacement to an object such that it gains 1600 J of kinetic energy? Slide 33 () / Over what displacement must a N net external force be applied, in parallel with the displacement to an object such that it gains 1600 J of kinetic energy? (F parallel to Δx) Slide 34 / 125 Gravitational Potential nergy Kinetic energy is the energy of motion. Gravitational potential energy is the energy of an object due to its position. This is derived by examining the work done by the gravitational force on an object that is changing its distance from the center of the earth. Caution - this will only apply for objects near the surface of the earth (or other celestial bodies). This restriction will be lifted in the Universal Gravitation unit. a = 0 F app F g = mg An object of mass m, is being lifted at a constant velocity near the surface of the earth by an external force, F app = F. It starts at height h 0, with v 0 = 0 and finishes at h f, with v f = 0.

9 Slide 35 / 125 Gravitational Potential nergy Slide 36 / 125 Gravitational Potential nergy hf h0 a = 0 F app = F F g = mg The Work done by gravity is negative (h f > h 0). Negative sign because Fg points down and Δy is in the up direction efine the gravitational potential energy as the negative of the work done by the gravitational force on the object. This will give us a positive potential energy for an object at a height above the earth - which you've seen in your previous physics course. Gravitational Potential nergy depends on the change in height, not the absolute value of the height - an object will have a different value of GP depending on where h 0 is chosen. If h 0 = 0, and an object is at height, h, then the familiar expression for GP shows up: Can potential energies be defined for other forces? Yes - they will be covered soon... Slide 37 / 125 Slide 37 () / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much work does the external force do on the book? A mg 15 A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much work does the external force do on the book? A mg -mg C 0 -mg C 0 mgh mgh -mgh -mgh Slide 38 / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much work does the gravitational force do on the book? A mg -mg Slide 38 () / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much work does the gravitational force do on the book? A mg -mg C 0 mgh C 0 mgh -mgh -mgh

10 Slide 39 / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much net work is done on the book by the external force and the gravitational force? A mg -mg Slide 39 () / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. How much net work is done on the book by the external force and the gravitational force? A mg -mg C 0 mgh C 0 mgh C -mgh -mgh Slide 40 / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. What is the gravitational potential energy of the mass when it is lifted to the height, h? A mg Slide 40 () / A book of mass, m, is lifted upwards at a constant velocity, a displacement, h, by an external force. What is the gravitational potential energy of the mass when it is lifted to the height, h? A mg -mg C 0 -mg C 0 mgh mgh -mgh -mgh Slide 41 / What is the change of GP for a 5.0 kg object which is raised from an initial height of 1.0 m above the floor to a final height of 8.0 m above the floor? Slide 41 () / What is the change of GP for a 5.0 kg object which is raised from an initial height of 1.0 m above the floor to a final height of 8.0 m above the floor?

11 Slide 42 / What is the change of GP for an 8.0 kg object which is lowered from an initial height of 2.1 m above the floor to a final height of 1.5 m above the floor? Slide 42 () / What is the change of GP for an 8.0 kg object which is lowered from an initial height of 2.1 m above the floor to a final height of 1.5 m above the floor? Slide 43 / What is the change in height of a 2.0 kg object which gained 16 J of GP? Slide 43 () / What is the change in height of a 2.0 kg object which gained 16 J of GP? Slide 44 / A librarian takes a book off a high shelf and refiles it on a lower shelf. Which of the following are correct about the work done on the book by the librarian and the earth's gravitational field as the book is lowered? Librarian A Positive Negative C Positive Gravitational Field Positive Negative Negative Slide 44 () / A librarian takes a book off a high shelf and refiles it on a lower shelf. Which of the following are correct about the work done on the book by the librarian and the earth's gravitational field as the book is lowered? Librarian A Positive Negative C Positive Gravitational Field Positive Negative Negative Negative Positive Negative Positive Zero Zero Zero Zero

12 Slide 45 / 125 Slide 46 / 125 Conservative and Non Conservative Forces The gravitational force is a conservative force. The path that an object takes has no bearing on its potential energy - GP depends only on the initial and final heights. Work has a non zero value only for the force components in the same direction as the motion. The gravitational force always points down, so lateral motion requires zero work by the gravitational force. The only impact on potential energy is the vertical component of the motion. h h0=0 ach path results in the same GP for an object moving from h 0 to h. Slide 47 / 125 Conservative and Non Conservative Forces h h0=0 Slide 48 / 125 Conservative Forces A conservative force has two properties: The work done by a conservative force on an object depends only on its initial and final position - it is path independent. The work done by a conservative force on an object is zero on a closed path (initial and final position are the same). As the object goes up, the gravitational force does negative work, decreasing the object's kinetic energy (and speed). On the way down, positive work is done by the gravitational force, increasing its kinetic energy (and speed). The sum of the work done over the closed path is zero. Slide 49 / A vacuum cleaner is moved from the ground floor to the second floor of an apartment building. In which of the following cases is the most work done by the person moving the vacuum? A The vacuum cleaner is pushed up an inclined plane set over the stairs. The person carries the cleaner up the stairs. C The person brings the cleaner to the third floor, by mistake, then back to the second floor. The work is the same in each case. A pulley is set up outside the building and the vacuum is hoisted up to the second floor by a rope. Slide 49 () / A vacuum cleaner is moved from the ground floor to the second floor of an apartment building. In which of the following cases is the most work done by the person moving the vacuum? A The vacuum cleaner is pushed up an inclined plane set over the stairs. The person carries the cleaner up the stairs. C The person brings the cleaner to the third floor, by mistake, then back to the second floor. The work is the same in each case. A pulley is set up outside the building and the vacuum is hoisted up to the second floor by a rope.

13 Slide 50 / 125 Non - Conservative Forces Slide 51 / 125 Non - Conservative Forces A non - conservative force does not follow the two properties of a conservative force. The path taken does impact the work done, and the work done on a closed path is not equal to zero. Think about this and please do two things: 1.Propose a force that is non-conservative and show how it doesn't follow the two properties. 2.iscuss what impact this has on deriving a potential energy from the force. Friction is the most common example of a non-conservative force. Friction force always opposes motion. The longer the path taken by an object, the greater the work done. An easy demonstration is to move your hand over a smooth surface - like your desk. Movement in a straight line may warm your hand a little. ut if you move your hand back and forth and take a longer path to get to the final position - it heats up more - your hand experieces more frictional force - more work. You cannot derive a potential energy function for this force - as the energy difference between two points will not always be the same - it depends on the path taken. Slide 52 / Which of the following is an example of a conservative force? A Kinetic friction Gravitational force Slide 52 () / Which of the following is an example of a conservative force? A Kinetic friction Gravitational force C Static friction Air resistance Water resistance C Static friction Air resistance Water resistance Slide 53 / Which of the following is a property of a non conservative force? A The net work done by this force over a closed path is zero. The net work done by this force over a closed path is a non zero value. C The work done by this force on an object moving from point A to is independent of the path taken. The work done by this force on an object moving from point A to is always positive. A potential energy can be associated with a nonconservative force. Slide 53 () / Which of the following is a property of a non conservative force? A The net work done by this force over a closed path is zero. The net work done by this force over a closed path is a non zero value. C The work done by this force on an object moving from point A to is independent of the path taken. The work done by this force on an object moving from point A to is always positive. A potential energy can be associated with a nonconservative force.

14 Slide 54 / 125 Slide 55 / 125 Conservation of Total Mechanical nergy Conservation of Total Mechanical nergy We're now going to derive a conservation law - the Conservation of Total Mechanical nergy which is defined as the total potential energy plus the kinetic energy of an object. In earlier physics courses, you learned the conservation of energy, the conservation of mass, and maybe the conservation of massenergy. Here, we're just going to look at the energy of objects moving around the surface of the earth, and not worry about their thermal or nuclear or sound or light energy. Return to Table of Contents Start with the Work-nergy equation, and assume an object is being elevated from h 0 to h f. Slide 56 / 125 Slide 57 / 125 Conservation of Total Mechanical nergy Work-nergy quation Split the net work on the system into the work done by external non conservative forces (such as friction) and conservative forces. This is done because the work done by a conservative force can be replaced by its potential energy. The only conservative force is the gravitational force. Negative sign as gravitational force is opposite the displacement as the object is raised from h 0 to h f. Slide 58 / 125 Conservation of Total Mechanical nergy In the absence of a net external non conservative force, we have W NC = 0 and f = 0. The initial total mechanical energy equals the final total mechanical energy - it is conserved. If there are other forms of potential energy in the system - like elastic potential energy (spring), then those terms would be added to the total mechanical energy (we will do this a little later). Slide 59 / 125 Internal forces Net non-zero work can only be done to a system by an external force; a force from the environment outside the system. So if our system is a box sitting on a table and I come along and push the box, I can increase the kinetic energy of the box - I am doing net non-zero work on the box. Why are none of the internal forces (forces within the box, such as the box molecules moving about and colliding with each other) involved in increasing the energy of the system? The molecules are certainly exerting forces on each other, and they are causing each other to move.

15 Newton's Third Law! Slide 60 / 125 Internal forces very time a molecule in the box strikes another molecule, it exerts a force on it, and moves it. However, the second molecule exerts an equal and opposite force on the first one. Thus, assuming equal masses for the molecules, the work done internal to the system equals zero - it all cancels out. Thermal nergy increases as the molecules vibrate and move faster, but this type of energy is not included in TM by definition. Slide 61 / Which law explains why internal forces of a system do not change its total mechanical energy? A Newtons First Law Newton's Second Law C Newton's Third Law Newton's Law of Universal Gravitation Conservation of Angular Momentum Slide 61 () / Which law explains why internal forces of a system do not change its total mechanical energy? A Newtons First Law Newton's Second Law C Newton's Third Law Newton's Law of Universal Gravitation Conservation of Angular Momentum C Slide 62 / 125 lastic Potential nergy We have analyzed two types of energy, kinetic energy (K) and gravitational potential energy (GP). In your previous physics classes, you studied elastic potential energy (P). Hooke's Law tells us that. The equation for GP was calculated using the definition of work and the fact that the potential energy resulting from a conservative force is the negative of the work done by the force. The spring force is a conservative force. This allows us to calculate a potential energy. ut, what makes this a little trickier than when GP was derived? Slide 63 / 125 lastic Potential nergy Slide 64 / 125 lastic Potential nergy The gravitational force (near the surface of the earth) is assumed to be constant (it doesn't vary much). The spring force is a function of position - it is not constant. At each point of the spring's motion, the force is different. In order to calculate work, the motion must be analyzed at infinitesimal displacements which are multiplied by the force at each infinitesimal point, and then summed up. What does that sound like? Calculus - specifically, integration. Rewrite the Work equation to take into account the position varying force, where F(x) is the force in the x direction: For motion in three dimensions, work is expressed as follows: or in Cartesian coordinates:

16 Slide 65 / 125 lastic Potential nergy Slide 66 / 125 Total Mechanical nergy (adding a spring) Start at the equilibrium point, x 0 = 0, and stretch the spring to x f. P has been used in this course, but U is generally the symbol for potential energy. We'll use both. Work-nergy quation Split the net work on the system into the work done by external non conservative forces (such as friction) and conservative forces. This is done because the work done by a conservative force can be replaced by its potential energy. Two conservative forces: elastic and gravitational. Let's go back to the Work - nergy equation and see how to fit this new potential energy in. Taking the general case where the spring is stretched from x 0 to x f. Slide 67 / 125 Slide 68 / 125 Advantages of using Conservation of Mechanical nergy When trying to solve motion problems, you were first taught to use Newton's Laws and the Kinematics equations. That can get problematic if the forces are not constant, are acting in multiple dimensions, very complex or numerous. Conservation laws enable you to just work with the initial and final conditions - you don't care how or why the object gets to where it is, you just need a snapshot of where it was and where it is now. In addition, energy is a scalar, so you don't have to worry about vectors, and the solutions are typically easier. Slide 69 / When using the Conservation of Total Mechanical nergy to solve a system problem, what needs to be considered? A The initial and final energy of the system. The initial and final forces on the system. C Only the initial energy of the system. Only the final energy of the system. The magnitude and direction of the internal forces on the system. Slide 69 () / When using the Conservation of Total Mechanical nergy to solve a system problem, what needs to be considered? A The initial and final energy of the system. The initial and final forces on the system. C Only the initial energy of the system. A Only the final energy of the system. The magnitude and direction of the internal forces on the system.

17 Slide 70 / A ball is swung around on a string, in a circle, traveling a displacement of 2.0 m in 5.0 s. What is the work done on the ball by the string? A 0 J Slide 70 () / A ball is swung around on a string, in a circle, traveling a displacement of 2.0 m in 5.0 s. What is the work done on the ball by the string? A 0 J 2.5 J C 5.0 J 2.5 J C 5.0 J A 10 J 10 J 25 J 25 J Slide 71 / Assume the earth moves around the sun in a perfect circular orbit (a good approximation). Use the direction of the gravitational force between the two celestial objects Students and type describe their answers here the work done by the sun on the earth and how that impacts the earth's orbital speed. How does your answer change if you don't make the circular orbit assumption? Slide 71 () / Assume the earth moves around the sun in a perfect circular orbit (a good approximation). Use the direction of the gravitational force between the two celestial objects Students and type describe their answers The here the gravitational work force done is in by a line the sun on the connecting the earth and the sun, and is earth and how that impacts the earth's orbital speed. How does your answer no work change on the earth. if The you earth's don't total make the circular orbit assumption? perpendicular to the earth's displacement at all times. The sun does mechanical energy is conserved. The earth is the same distance from the sun in its circular orbit, its potential energy is constant. Its kinetic energy is constant and its speed is constant. Since the earth's orbit is not a perfect circle, Fg has a component in the direction of the earth's motion, so work is done by the sun on the earth and the earth's speed changes. Slide 72 / 125 Slide 73 / 125 Two imensional Forces and Work Two imensional Forces and Work In the previous section, we learned that the amount of work done to a system, and therefore the amount of energy increase that the system experiences, is given by We have only dealt with one dimensional movement, and will now generalize to two dimensions. We will actually go backwards a little - we won't use the scalar dot product, but will show how it arises from trigonometry. Return to Table of Contents

18 Slide 74 / 125 Two imensional Forces and Work Slide 75 / 125 Two imensional Forces and Work Instead of pulling the object horizontally, what if it is pulled at an angle to the horizontal? How would we interpret: v F APP #x After breaking F APP into components that are parallel and perpendicular to the direction of motion, we can see that no work is done by the perpendicular component; work is only done by the parallel component. v F # perpendicular F parallel #x W = Fdparallel for this case? Using trigonometry, we find that F parallel = F APPcosθ Slide 76 / 125 Two imensional Forces and Work Slide 77 / 125 Two imensional Forces and Work W = F paralleld becomes: W = (F APPcosθ)Δx = F APPΔxcosθ v F # perpendicular F parallel Instead of pulling the object at an angle to the horizontal, what if it is pushed? In words, the work done on an object by a force is the product of the magnitude of the force and the magnitude of the displacement times the cosine of the angle between them. Which is exactly what the scalar dot product shows: #x This is really no more difficult a case. We just have to find the component of force that is parallel to the object's displacement. Slide 78 / 125 Slide 79 / 125 Two imensional Forces and Work 30 A 40.0 N force pulls an object at an angle of θ = to its direction of motion. Its displacement is Δx = 8.00 m. How much work is done by the force on the object? The interpretation is the same, just determine the angle between the force and displacement and use: # F parallel F APP F perpendicular v # W = F APPΔxcosθ #x #x ven though F perpendicular is in the negative direction (it was positive when the object was pulled), it does not affect the work - as only the parallel component contributes to the work.

19 Slide 79 () / A 40.0 N force pulls an object at an angle of θ = to its direction of motion. Its displacement is Δx = 8.00 m. How much work is done by the force on the object? Slide 80 / An object is pushed with an applied force of 36.0 N at an angle of θ = to the horizontal and it moves Δx = 3.40 m. What work does the force do on the object? v # #x # F APP #x Slide 80 () / 125 Slide 81 / An object is pushed with an applied force of 36.0 N at an angle of θ = to the horizontal and it moves Δx = 3.40 m. What work does the force do on the object? # F APP #x Work done by a Position ependent Force Return to Table of Contents Slide 82 / 125 Position ependent Force Slide 83 / 125 Position ependent Force We've already seen one example of a position dependent force - the spring. Let's generalize. F(x) N F(x) = Cx 1/2 x(m) I, KSmrq [GFL ( CC-Y-SA-3.0 ( creativecommons.org/licenses/by-sa/3.0/) or CC Y-SA 2.5 ( creativecommons.org/licenses/by-sa/2.5)], via Wikimedia Commons To find Work on a Force/position diagram, you take the area under the force function. When the force is constant or increases linearly, it is a simple geometry problem. F(x) N F(x) = Cx 1/2 x(m) I, KSmrq [GFL ( CC-Y-SA-3.0 ( creativecommons.org/licenses/by-sa/3.0/) or CC Y-SA 2.5 ( creativecommons.org/licenses/by-sa/2.5)], via Wikimedia Commons The Force plotted to the left is proportional to the square root of the position; hence integration techniques are used to solve for the work performed by the force on this system. Where have you done this before? In the Kinematics unit of this course with position-time, velocity-time and accelerationtime graphs.

20 Slide 84 / 125 Position ependent Force For the spring problem (where F = -kx), we assumed that the spring was stretched from x = 0 to a given x to find W e and then U e. Slide 85 / 125 Position ependent Force y decreasing the width of the boxes to be infinitesimally small - the integration branch of calculus. F(x) N F(x) = Cx 1/2 x(m) I, KSmrq [GFL ( CC-Y-SA-3.0 ( creativecommons.org/licenses/by-sa/3.0/) or CC Y-SA 2.5 ( creativecommons.org/licenses/by-sa/2.5)], via Wikimedia Commons Using the same technique, but changing the limits of integration, enables you to find the work done between any two points in the object's motion. The yellow boxes show an approximate area below the force curve. y decreasing the width of the boxes (green), you get closer to the real area. How is a more exact answer achieved? F(x) N F(x) = Cx 1/2 x0 x(m) I, KSmrq [GFL ( CC-Y-SA-3.0 ( creativecommons.org/licenses/by-sa/3.0/) or CC Y-SA 2.5 ( creativecommons.org/licenses/by-sa/2.5)], via Wikimedia Commons xf Try this problem: Given where C is a constant, find the work done by the force when the object is moved from x 0 to x f. Slide 86 / 125 Position ependent Force Slide 87 / 125 Position ependent Force F(x) N F(x) = Cx 1/2 For conservative forces moving in one dimension, the potential energy is found: Use a bit of calculus and take the derivative of both sides with respect to x: x0 x(m) xf The potential energy due to this force (if it is conservative) would be the negative of the work. I, KSmrq [GFL ( CC-Y-SA-3.0 ( creativecommons.org/licenses/by-sa/3.0/) or CC Y-SA 2.5 ( creativecommons.org/licenses/by-sa/2.5)], via Wikimedia Commons Slide 88 / The potential energy (in Joules) of a block as it moves in the x direction is U(x) = 3x 3 + 4x Find the general expression for the force exerted on the block. What is the force, in Newtons, on the block at x = 2.0 m? Students type their answers here Slide 88 () / The potential energy (in Joules) of a block as it moves in the x direction is U(x) = 3x 3 + 4x Find the general expression for the force exerted on the block. What is the force, in Newtons, on the block at x = 2.0 m? Students type their answers here

21 Slide 89 / 125 Slide 89 () / 125 Slide 90 / The force exerted by a non-linear spring on a mass is F = -kx 2 /2. If k = 200 N/m, find the work done by the spring on a mass from x = 0.08 m to x = 0.10 m. What is the change in potential energy of the spring? Slide 90 () / The force exerted by a non-linear spring on a mass is F = -kx 2 /2. If k = 200 N/m, find the work done by the spring on a mass from x = 0.08 m to x = 0.10 m. What is the change in potential energy of the spring? because Fspring(x) is in the opposite direction of dx Slide 91 / 125 Slide 92 / 125 Position ependent Potential nergy Position ependent Potential nergy A particle's potential energy, U, is plotted with respect to its displacement, as shown to the left. The equation below will be used to determine the motion of a particle with this potential energy: Return to Table of Contents

22 Slide 93 / 125 Position ependent Potential nergy Slide 94 / 125 Position ependent Potential nergy First, let's find where this particle is at an equilibrium position. A particle is at equilibrium when the net force on it is zero. Where can you see equilibrium points on the graph using the equation below? is the slope of the curve. The slope is zero at the four points indicated by the arrows. If the particle is placed at any of those points at rest, it will not move, since there is no force acting on it. ut what if the particle is momentarily pushed by an external force when it is at those points? How will it move? Slide 95 / 125 Position ependent Potential nergy Slide 96 / 125 Unstable quilibrium Slide 97 / 125 At the two arrowed points - where the curve is concave down, points on the curve to the left of the peak have a positive slope; points to the right have a negative slope. What does that tell you about the direction of the force that the particle after it is pushed? Position ependent Potential nergy A particle pushed to the left experiences a negative force, moving it to the left - sliding down the potential energyposition curve. A particle pushed to the right experiences a positive force, moving it to the right - sliding down the potential energy - position curve. This is called unstable equilibrium - the particle is stationary, but if an external force is applied, it moves and doesn't come back to the same equilibrium point. Slide 98 / 125 Stable quilibrium At the two arrowed points - where the curve is concave up, points on the curve to the left of the peak have a negative slope; points to the right have a positive slope. What does that tell you about the direction of the force that the particle feels from the potential energy after it is pushed? A particle pushed to the left experiences a positive force, moving it to the right - back in the direction of the equilibrium point. A particle pushed to the right experiences a negative force, moving it to the left - back in the direction of the equilibrium point. This is stable equilibrium - the particle is stationary in the potential energy well, and if an external force is applied, it moves, but comes back to the equilibrium point. Will it stay there?

23 Slide 99 / 125 Simple Harmonic Motion Simple Harmonic Motion! Slide 101 / 125 No. If it is moving on a frictionless surface, it will reach the equilibrium point with a velocity and continue past it - until the restoring force stops it and turns it around. It will continue this oscillatory motion. Just like a spring. If friction were present, it would eventually come to rest at the bottom of the potential energy well after the oscillations. 35 A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which points is the particle not in equilibrium? Slide 100 / 125 Position ependent Potential nergy What's nice about the graph is that you can visualize a particle on the curve and get the same result as the math. If the graph was a drawing of a roller coaster track, a ball put at the top of the curves would move away from the peaks and not come back. A ball pushed from the wells would go up the track, and then return, and oscillate about the bottom of the well. Slide 101 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which points is the particle not in equilibrium? A A,, A,, C A A,, A,, C A C, C, C, C, C,, F A,, C,, F A,, Slide 102 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which points is the particle in equilibrium? A A,, Slide 102 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which points is the particle in equilibrium? A A,, A,, C C, C, A,, C C, C, C,, F C,, F A,, A,,

24 Slide 103 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the particle in stable equilibrium? A, Slide 103 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the particle in stable equilibrium? A, C, F C C, C, F C C, A A Slide 104 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the particle in unstable equilibrium? A A, Slide 104 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the particle in unstable equilibrium? A A, C, F C C, C, F C C, A A Slide 105 / 125 Position ependent Potential nergy Four more curve segments to analyze. Slide 106 / 125 Position ependent Potential nergy Points A and C are on straight lines with constant positive (but different) slopes. A C The segments at points A and C will be looked at first. What kind of segments are they? What is the sign of their slopes? A C The force on those points is negative - so if a particle is placed at points A or C with zero velocity, it will move down the curve and to the left. If the particle has an initial velocity to the right, the force will accelerate it to the left and slow it down.

25 Slide 107 / 125 Position ependent Potential nergy Point is on a straight line with a negative slope. What is the direction of the force on the particle? What would be the motion of a particle placed at point with a negative velocity, zero velocity and positive velocity? Slide 108 / 125 Position ependent Potential nergy A particle with zero velocity would increase its speed in the positive x direction. A particle with negative velocity would slow down and a particle with positive velocity would speed up. The acceleration would be the same in each case since the slope of a straight line is constant, thus the Force is constant. Last one - what about point, which is on a parabola? Slide 109 / 125 Position ependent Potential nergy The potential energy at point is proportional to x 2, hence the slope, or force, is proportional to x. Sound familiar? That's a spring. The slope at point is negative, so the force is to the right. Let's add one more point - point which is symmetric to point with respect to the bottom of the well. Slide 110 / 125 Position ependent Potential nergy The particle would oscillate between points and. The force at point (and that side of the parabola) is to the left - a restoring force. escribe the motion of an object that is released at point with zero velocity. Slide 111 / 125 Position ependent Potential nergy Slide 112 / 125 Position ependent Potential nergy A C As the particle moves along the potential energy curve, what can be said about the kinetic and total mechanical energy? A C The total mechanical energy stays constant, and as the potential energy decreases, the kinetic energy will increase. As the potential energy increases, the kinetic energy will decrease.

26 Slide 113 / 125 Position ependent Potential nergy A 1 C 2 3 e careful with the sign of the potential energy - it can be negative or positive. Kinetic energy can only be positive. A particle moving from point 1 to point 2 is speeding up as the potential energy decreases. A particle moving from point 2 to point 3 is slowing down as the potential energy increases. Slide 114 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. What is the force on the particle when at point C? A -2.0 N -1.0 N C 0 N 1.0 N 2.0 N The roller coaster analogy also works for determining the speed behavior! Slide 114 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. What is the force on the particle when at point C? A -2.0 N -1.0 N C 0 N 1.0 N 2.0 N C Slide 115 / A conservative force parallel to the x-axis moves a particle is released at rest at point. What is the largest value of x reached by the particle during this motion? A 2.9 m 4.0 m C 5.5 m 6.7 m 8.0 m Slide 115 () / A conservative force parallel to the x-axis moves a particle is released at rest at point. What is the largest value of x reached by the particle during this motion? A 2.9 m Slide 116 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the force on the particle positive? A, F 4.0 m C 5.5 m C C, 6.7 m 8.0 m A,

27 Slide 116 () / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the force on the particle positive? Slide 117 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the force on the particle negative? A, F A, F C C, C C, A, A, Slide 117 () / 125 Slide 118 / A conservative force parallel to the x-axis moves a particle is released at rest at point A. At which point or points is the force on the particle negative? A, F C C, Power A, Return to Table of Contents Slide 119 / 125 Power It is often important to know not only if there is enough energy available to perform a task but also how much time will the energy be used. Average Power is defined as the rate that work is done: Slide 120 / 125 Power Instantaneous power is found by using the same method we found instantaneous velocity and acceleration: Since work is measured in Joules (J) and time is measured in seconds (s) the unit of power is Joules per second (J/s). In honor of James Watt, who made critical contributions in developing efficient steam engines, the unit of power is known as a Watt (W). Using a little non rigorous calculus in one dimension (don't show this to your calculus teacher): Substitute this into the instantaneous power equation above.

28 Slide 121 / 125 Power Slide 122 / 125 Power A third useful expression for power can be derived from the work energy equation when only the K changes: For a constant force acting in the x direction, the instantaneous power generated is equal to the magnitude of the force times the velocity. This is quite a handy equation. The power absorbed by a system can be thought of as the rate at which the kinetic energy in the system is changing. In vector notation, allowing for a non parallel force: Slide 123 / A steam engine does 52 J of work in 12 s. What is the power supplied by the engine? A 3.4 W 3.9 W Slide 123 () / A steam engine does 52 J of work in 12 s. What is the power supplied by the engine? A 3.4 W 3.9 W C 4.3 W 4.9 W C 4.3 W 4.9 W C 5.7 W 5.7 W Slide 124 / How long must a W engine run in order to produce kj of work? A 1987 s 2057 s Slide 124 () / How long must a W engine run in order to produce kj of work? A 1987 s 2057 s C 2146 s 2305 s C 2146 s 2305 s 2861 s 2861 s

29 Slide 125 / A 12.0 kw motor runs a vehicle at a speed of 8.00 m/s. What is the force supplied by the motor (assume all of the power is delivered in the direction of the vehicle's motion). A 1000 N 1250N Slide 125 () / A 12.0 kw motor runs a vehicle at a speed of 8.00 m/s. What is the force supplied by the motor (assume all of the power is delivered in the direction of the vehicle's motion). A 1000 N 1250N C 1400 N 1450 N C 1400 N 1450 N 1500 N 1500 N