A family decides to create a tire swing in their backyard for their son Ryan. They tie a nylon rope to a branch that is located 16 m above the earth, and.

Slides:



Advertisements
Similar presentations
“I wonder what the tension is in each of those massless strings.”
Advertisements

Forces.
Physics 111: Mechanics Lecture 5
Section 4-7 Solving Problems with Newton’s Laws; Free Body Diagrams
Circular Motion What is Circular Motion? Uniform Circular Motion is motion along a circular path in which there is no change in speed, only a change.
Sect. 8-3: Mechanical Energy & It’s Conservation.
Work, Energy, And Power m Honors Physics Lecture Notes.
Physics Circular Motion Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund Department of.
Question Title Superhero Physics v r. Question Title A superhero is designing a new rope-like gadget that will allow him to swing from building to building.
Examples and Hints in Chapter 7. Wild Monkey III Tarzan (m =100 kg) grabs a vine to swing to cross a chasm. He starts a from a cliff face that is 10 m.
Circular Motion Newton’s Second Law and circular motion
As the ball revolves faster, the angle increases
Fall Final Review WKS: WORD PROBLEMS Part II. 1. A car travels at a constant speed of 15 m/s for 10 seconds. How far did it go?
A ladder with length L weighing 400 N rests against a vertical frictionless wall as shown below. The center of gravity of the ladder is at the center of.
Phy100: More on Energy conservation Mechanical energy (review); Goals: Work done by external forces; Understand conservation law for isolated systems.
Lecture 4 Monday: 26 January 2004 Newton’s Laws of Motion.
Newton’s Laws of Motion three laws of motion: fundamental laws of mechanics describe the motion of all macroscopic objects (i.e., everyday size objects)
NEWTON'S LAWS OF MOTION There are three of them.
Gravitational Potential energy Mr. Burns
Discussions Feb 26 Work Conservation of energy. Work and conservation of energy.
Newton’s Third Law of Motion
Chapter 11 Angular Momentum.
Introduction to Work Monday, September 14, 2015 Work Work tells us how much a force or combination of forces changes the energy of a system. Work is.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Demo spin stopper Is it accelerating? Does it have F net ? Direction of F net ? What causes F net ? Direction of F net ? Is tension doing work?
Newton’s Laws of Motion 1. If the sum of all external forces on an object is zero, then its speed and direction will not change. Inertia 2. If a nonzero.
Newton’s 2 nd law problems ΣF = ma Or F net = ma.
Energy m m Physics 2053 Lecture Notes Energy.
Chapter 7 Energy of a System. Introduction to Energy A variety of problems can be solved with Newton’s Laws and associated principles. Some problems that.
Chapter 4 Dynamics: Newton’s Laws of Motion. Units of Chapter 4 Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law.
Chapter 4 Dynamics: Newton’s Laws of Motion. Units of Chapter 4 Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law.
Two small spheres of putty, A and B, of equal mass m, hang from the ceiling on massless strings of equal length. Sphere A is raised to a height h 0 as.
Chapter 8 Rotational Motion.
Projectile Motion An object may move in both the x and y directions simultaneously The form of two-dimensional motion we will deal with is called projectile.
Uniform Circular Motion
Lecture 10 Employ Newton’s Laws in 2D problems with circular motion 1.
Two blocks (m 1 =2.5kg, m 2 =1.8kg) are hanging from a pulley as shown in the figure below. The moment of inertia through the axis of rotation passing.
A series of blocks is connected to a pulley in the manner depicted below. Find the minimum mass that block C must have in order to keep block A from sliding.
Chapter 6 Work and Energy. Units of Chapter 6 Work Done by a Constant Force Work Done by a Varying Force Kinetic Energy, and the Work-Energy Principle.
Monday, Mar. 24, 2008 PHYS , Spring 2008 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #16 Monday, Mar. 24, 2008 Dr. Jaehoon Yu Potential Energy.
Work and Energy.
Physics 207: Lecture 10, Pg 1 Lecture 10 l Goals:  Exploit Newton’s 3 rd Law in problems with friction  Employ Newton’s Laws in 2D problems with circular.
Systems and energy. Equations For any closed system that undergoes a change, the total energy before the change is the same as the total energy after.
Dynamics: Newton’s Laws of Motion
Dynamics: Newton’s Laws of Motion
A certain pendulum consists of a 2
Circular Motion. Rotating Turning about an internal axis Revolving Turning about an external axis.
Conservation of Energy. Equations For any closed system that undergoes a change, the total energy before the change is the same as the total energy after.
Work Readings: Chapter 11.
Wednesday June 15, PHYS , Summer I 2005 Dr. Andrew Brandt PHYS 1443 – Section 001 Lecture #9 Wednesday June 15, 2005 Dr. Andrew Brandt Lightning.
Dynamics: Newton’s Laws of Motion. Force A force is a push or pull. An object at rest needs a force to get it moving; a moving object needs a force to.
Force and Motion Jeopardy Review
Chapter 4 Dynamics: Newton’s Laws of Motion. Units of Chapter 4 Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law.
Work and Energy 5. What is a force? a. change in speed over time b. the tendency to resist change in motion c. a push or pull d. apparent weightlessness.
Forces In One Dimension
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Two blocks (m1 = 5kg, m2 = 2.5kg) are in contact on a frictionless table. A constant horizontal force FA = 3N is applied to the larger block as shown.
Today: (Ch. 3) Tomorrow: (Ch. 4) Apparent weight Friction Free Fall Air Drag and Terminal Velocity Forces and Motion in Two and Three Dimensions.
What is a force? An interaction between TWO objects. For example, pushes and pulls are forces. We must be careful to think about a force as acting on one.
EnergyDefinitions 1 Different kinds of energy Kinetic energy Kinetic energy is motion energy. The faster it moves the more kinetic energy it possesses.
Uniform circular motion Uniform circular motion is motion along a circular path in which there is no change in speed, only a change in direction. v.
Force and Motion–I Chapter 5. Newton's First and Second Laws A force: o Is a “push or pull” acting on an object o Causes acceleration We will focus on.
Different kinds of energy
Gravitational Potential energy Mr. Burns
Force and Motion Jeopardy Review
Force and Motion Vocabulary
Force and Motion Vocabulary
NEWTON'S LAWS OF MOTION There are three of them.
Force and Motion Jeopardy Review
NEWTON'S LAWS OF MOTION There are three of them.
Presentation transcript:

A family decides to create a tire swing in their backyard for their son Ryan. They tie a nylon rope to a branch that is located 16 m above the earth, and adjust it so that the tire swings 1 meter above the ground. To make the swing more exciting, and so they don't have to push Ryan all the time, they construct a launch point that is 13 m above the ground. You are their neighbor, and you are concerned that the swing might not be safe, so you calculate the maximum tension (T max ) in the rope to see if it will hold. Calculate the maximum tension in the rope, assuming that Ryan starts from rest from his launch pad. Is it greater than the rated value of the rope (1500 N)? y x 16m 1m h 0 =13m Ryan’s mass: m R =30kg Mass of tire: m T =5kg Neglect the mass of the rope. Ryan’s mass: m R =30kg Mass of tire: m T =5kg Neglect the mass of the rope.

Question 1 Question 2 Question 3 Question 4 Question 5 Question 6 Question 7 Question 8 Reflection

1. At what point of the swinging motion will the tension in the rope be at it’s maximum. AA) On the way down BB) At the lowest point CC) On the way back up

At the bottom of the trajectory, all forces acting on Ryan are vertical. The sum of the tension (up) and weight (down) produce a centripetal force (up). The more the force of weight pulls down on the rope, the greater the tension will be. Only a component of the force of weight pulls on the rope on the way up or down. Choice A Incorrect

Choice B Correct y x At the bottom of the trajectory, all forces acting on Ryan are vertical. The sum of the tension (up) and weight (down) produce a centripetal force (up). The more the force of weight pulls down on the rope, the greater the tension will be. Only a component of the force of weight pulls on the rope on the way up or down. The tension is at a maximum at the bottom of the trajectory. At the bottom of the trajectory, all forces acting on Ryan are vertical. The sum of the tension (up) and weight (down) produce a centripetal force (up). The more the force of weight pulls down on the rope, the greater the tension will be. Only a component of the force of weight pulls on the rope on the way up or down. The tension is at a maximum at the bottom of the trajectory.

Choice C Incorrect At the bottom of the trajectory, all forces acting on Ryan are vertical. The sum of the tension (up) and weight (down) produce a centripetal force (up). The more the force of weight pulls down on the rope, the greater the tension will be. Only a component of the force of weight pulls on the rope on the way up or down.

2. Which physics principle should we use to solve this problem. AA) Conservation of Mechanical Energy BB) Newton’s 2nd Law CC) Both A and B

Choice A It’s a good choice, but only part of the story. Since we know that the maximum tension is when the swing reaches the bottom of its trajectory, we can use the conservation of energy law to find the speed of the tire at this point. But, once we find the speed we will need to use Newton’s 2nd Law to find the solution.

We need to use Newton’s 2nd Law, but we must also apply the law of conservation of energy to find important information first. Choice B It’s a good choice, but only part of the story. There are no forces acting on the tire in the x-direction at the instant when the tire is at the bottom of its trajectory.

Choice C Correct We can use the conservation of energy law to find the speed of the tire at the point of maximum tension: Once we find the speed we will need to use the vertical component of Newton’s 2nd Law to find the solution:

3. Applying the law of conservation of energy, which of the following simplified expressions do we find for Ryan’s speed when the swing is at its lowest point. A)B)C)A)B)C) V B = Ryan’s speed at the bottom Subscripts 0 and f stand for initial and final. V B = Ryan’s speed at the bottom Subscripts 0 and f stand for initial and final.

Choice A Incorrect You must take the initial gravitational energy into consideration. Ryan swings from rest atop the launch pad. Please try again.

Choice B Correct Setting the initial energy equal to the final energy we find: At the bottom point, the swing is moving with a velocity v B, so there is kinetic energy. There is also gravitational potential energy, because the swing is still above the ground in our coordinate system. There is only gravitational potential energy at the initial point, because the swing is not moving yet.

Since the tire swings 1 meter above the ground at its lowest point, the system has gravitational potential energy at this point. Please try again. Choice C Incorrect

4. What value do we get for Ryan’s speed at the point of maximum tension? AA) v B =17.1m/s BB) v B =15.3 m/s CC) v B =7.7m/s

h 0 =13m This is the height from which Ryan is released from rest. h f =1m This is the height that Ryan will still have when he reaches the lowest point in the swing’s motion. g=9.8m/s 2 Choice A Incorrect Please try again, make sure you are using the correct values:

Choice B Correct

Choice C Incorrect h 0 =13m This is the height from which Ryan is released from rest. h f =1m This is the height that Ryan will still have when he reaches the lowest point in the swing’s motion. g=9.8m/s 2 Please try again, make sure you are using the correct values:

5. Which of the following freebody diagrams correctly depicts all of the forces acting on Ryan and the tire at the lowest point? A)B)C)A)B)C) (m R +m T )g T max FcFc FcFc T max =Maximum Tension m r =Ryan’s mass m T =Tire’s mass g=9.8m/s 2 F c = Centripetal Force T max =Maximum Tension m r =Ryan’s mass m T =Tire’s mass g=9.8m/s 2 F c = Centripetal Force

Choice A Correct This diagram correctly depicts the only forces acting on the tire and rider.

Choice B Incorrect The centripetal force is not a new force, but only the name of the component of the net force acting towards the center of curvature when the path is not straight. When we use Newton’s 2nd Law we will set the right hand side equal to the centripetal force (ma c ), because this expresses the response of the system to the forces acting upon it.

Choice C Incorrect The centripetal force is not a new force, but only the name of the component of the net force acting towards the center of curvature when the path is not straight. When we use Newton’s 2nd Law we will set the right hand side equal to the centripetal force (ma c ), because this expresses the response of the system to the forces acting upon it.

Note: Centripetal force is generally expressed as: This is a statement of the “radial” or ”centripetal” component of the net force. Note: Centripetal force is generally expressed as: This is a statement of the “radial” or ”centripetal” component of the net force. 6. Apply Newton’s 2nd Law to find an expression for T max. Which one of the following expressions is correct? A)B)C)A)B)C)

Choice A Correct Since this is a non-equilibrium problem, our net force is not zero.

Choice B Incorrect Since this is a non-equilibrium problem, our net force is not zero. Correct expression:

Choice C Incorrect This sign should be negative, because the weight of Ryan and the tire acts in the opposite direction of the tension force.

7. Find an expression for T max in terms of v B and other given quantities. Which of the following expressions is correct? A)B)C)A)B)C) Hint Centripetal acceleration: R is the radius of the curve that is being traveled. Hint Centripetal acceleration: R is the radius of the curve that is being traveled.

Choice A Incorrect Be careful with your signs. Correct reasoning:

Choice B Correct

Choice C Incorrect Correct reasoning: Be careful with your signs.

8. What is the value of T max ? Is the swing safe for Ryan if the rope will break at a tension of 1500N? Answer

Reflection Problems 16m 1m 15m R=15m The swing is safe for Ryan!

Reflection Questions What is the maximum mass that a rider can have and swing safely? If the launch pad was lowered to 10m, would T max become higher or lower for Ryan?