Lecture 19. Friction

Similar documents
16. Friction Mechanics of Manipulation

27. Impact Mechanics of Manipulation

Chapter 10: Dynamics of Rotational Motion

dt 2 x = r cos(θ) y = r sin(θ) r = x 2 + y 2 tan(θ) = y x A circle = πr 2

Unit 1: Equilibrium and Center of Mass

LECTURE 11 FRICTION AND DRAG

Lecture 20. Planar Sliding

Physics 111: Mechanics Lecture 5

12. Foundations of Statics Mechanics of Manipulation

Physics B Newton s Laws AP Review Packet

O Which force produces the greatest torque about the point O (marked by the blue dot)?

Robot Autonomy Notes

E X P E R I M E N T 6

= F 4. O Which force produces the greatest torque about the point O (marked by the blue dot)? E. not enough information given to decide

However, the friction forces are limited in magnitude and will not prevent motion if sufficiently large forces are applied.

STATICS. Friction VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Please circle the name of your instructor: EB01: Beamish EB02: Fenrich EB03: Ruhl. EB04: Rahman EB05: Nedie EB06: Ropchan LAST NAME: FIRST NAME: ID#:

Physics 207: Lecture 24. Announcements. No labs next week, May 2 5 Exam 3 review session: Wed, May 4 from 8:00 9:30 pm; here.

How Do Objects Move? Describing Motion. Different Kinds of Motion

24/06/13 Forces ( F.Robilliard) 1

PHYSICS 220. Lecture 15. Textbook Sections Lecture 15 Purdue University, Physics 220 1

Chapter 6 Dynamics I: Motion Along a Line

Review of Lectures 1, 2 and 3

Things going in circles

STEP Support Programme. Mechanics STEP Questions

Last 6 lectures are easier

Physics 211 Week 10. Statics: Walking the Plank (Solution)

Lecture 8: Friction Part 1 Friction Phenomena

Physics 8 Wednesday, October 19, Troublesome questions for HW4 (5 or more people got 0 or 1 points on them): 1, 14, 15, 16, 17, 18, 19. Yikes!

Physics 211 Test 2 Practice August 31, 2011

HATZIC SECONDARY SCHOOL

Engineering Problem Solving ENG1101. Physics 101 For The Design Project Mathematical Model

Kinematics vs. Dynamics

Physics 8 Friday, November 4, 2011

PH 2213 : Chapter 05 Homework Solutions

Physics 101 Lecture 5 Newton`s Laws

Physics 2211 ABC Quiz #3 Solutions Spring 2017

Dynamics Test K/U 28 T/I 16 C 26 A 30

5. Nonholonomic constraint Mechanics of Manipulation

NCSP 2 nd Ed Chapter 4 Solutions Forces

March 10, P12 Inclined Planes.notebook. Physics 12. Inclined Planes. Push it Up Song

Rigid Body Equilibrium Grasps

PHYSICS 149: Lecture 21

How things move and the forces that act on them.

Engineering Problem Solving ENG1101. Physics 101 For The Design Project Mathematical Model

*************************************************************************

Announcements 23 Sep 2014

Forces and Newton s Laws Notes

Friction. Objectives. Assessment. Assessment. Physics terms. Equations 5/20/14. Models for friction

PHY131H1F - Class 9. Today, finishing Chapter 5: Kinetic Friction Static Friction Rolling without slipping (intro) Drag

11. (7 points: Choose up to 3 answers) What is the tension,!, in the string? a.! = 0.10 N b.! = 0.21 N c.! = 0.29 N d.! = N e.! = 0.

Newton and Real Life. Newton and Real Life 9/13/12. Friction, Springs and Scales. Summary

Galileo & Friction 2000 yrs prior to inertia idea, the popular belief was that all objects want to come to a rest. BUT 1600's: Galileo reasoned that

Chapter 4. The Laws of Motion

l Every object in a state of uniform motion tends to remain in that state of motion unless an

Problem Solving Day and Movie Project Introduction

End-of-Chapter Exercises

Chapter 9-10 Test Review

You know the drill: Turn in hw Pick up graded hw Name tags up Grab white boards and markers for your group

Or why this won t work very well

Lecture III. Introduction to Mechanics, Heat, and Sound /FIC 318

Page 1. Name: 1) The diagram below represents two concurrent forces.

Midterm 3 Review (Ch 9-14)

Announcements 24 Sep 2013

Chapter 4. Forces and Newton s Laws of Motion. continued

preap Physics Exploratory Lab Weight = 1 DIRECTIONS: Do the activities below and fill the blanks/spaces provided. 50 points available.

Physics 211 Week 5. Work and Kinetic Energy: Block on Ramp

Unit 4 Statics. Static Equilibrium Translational Forces Torque

SPH4U Sample Test Dynamics

Force, Friction & Gravity Notes

Simple Practical Mechanics. Lesley Swarbrick FMSP associate

Work and kinetic Energy

Overview The Laws of Motion

Chapter 6, Problem 18. Agenda. Rotational Inertia. Rotational Inertia. Calculating Moment of Inertia. Example: Hoop vs.

PHYSICS 220 Lecture 04 Forces and Motion in 1 D Textbook Sections

9/20/11. Physics 101 Tuesday 9/20/11 Class 8" Chapter " Weight and Normal forces" Frictional Forces"

SPH 4C Unit 2 Mechanical Systems

VISUAL PHYSICS ONLINE DYNAMICS TYPES OF FORCES FRICTION

PHY131 Summer 2011 Class 5 Notes

Dry Friction Static vs. Kinetic Angles

Unit 08 Work and Kinetic Energy. Stuff you asked about:

= o + t = ot + ½ t 2 = o + 2

Assignment 9. to roll without slipping, how large must F be? Ans: F = R d mgsinθ.

5. A car moves with a constant speed in a clockwise direction around a circular path of radius r, as represented in the diagram above.

Chapter 4 Force and Motion

Isaac Newton ( ) 1687 Published Principia Invented Calculus 3 Laws of Motion Universal Law of Gravity

A hockey puck slides on ice at constant velocity. What is the net force acting on the puck?

Contents. Concept Map

Name: School Name: PHYSICS CONTEST EXAMINATION

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

I pt mass = mr 2 I sphere = (2/5) mr 2 I hoop = mr 2 I disk = (1/2) mr 2 I rod (center) = (1/12) ml 2 I rod (end) = (1/3) ml 2

Static Equilibrium and Torque

The net force on a moving object is suddenly reduced to zero. As a consequence, the object

Study Questions/Problems Week 4

Whenever these forces act on an object (make it move), we can classify the force as being either attractive or repulsive by the way the objects move:

Overview. Dry Friction Wedges Flatbelts Screws Bearings Rolling Resistance

Introduction to Friction YouTube is a wonderful resource for physics videos

SPH3U1 - Dynamics Problems Set 3

SPH3U Practice Test. True/False Indicate whether the statement is true or false.

Mechanisms Simple Machines. Lever, Wheel and Axle, & Pulley

Transcription:

Matthew T. Mason angle, Mechanics of Manipulation

Today s outline angle, angle,

How do you move things around? angle, Kinematics, kinematic constraint. Force. Force of constraint; Gravity; ; Momentum.

How do you know where things are? You put them somewhere, or you look at them. And then, they stay put. Theorem (Liouville s theorem) In a Hamiltonian system (including an energy-conserving passive mechanical system) the uncertainty, measured as a probability distribution in phase space, remains constant as the system evolves. angle, Energy loss is essential. and plastic impact are essential.

An alternative reality What would it be like to live in a world without friction? Grabbing anything would be like grabbing a bar of soap. No tables. Bowls? Tables with edges? Walking wouldn t work. Drill footholds everywhere? (You re stranded in the middle of a frozen pond, perfectly flat and frictionless. Q: How do you get to shore? A: Throw one of your shoes to the opposite shore.) What would feet and hands look like? With no gravity? Where do you look for lost items? On the space shuttle, they find lost articles at the AC intake grille. angle,

Overview is complex and difficult to model. We will focus on simple approximations: generally, Coulomb s law of sliding friction, with known uniform coefficient of friction. Applied with common sense, this model is good enough to explore problems, and perform useful manipulation. But, know the limits. angle,

An experiment, in the style of Coulomb Clean surfaces, but not too clean dry, unlubricated. Pull on string with force f a, ramping up from 0. force f f will balance f a, up to a point. Max f f when not moving: µ s mg. f f µ smg µ dmg f f mg f a angle, Max f f when moving: µ d mg. From now on we will assume µ s = µ d = µ. f a

Coulomb s observations Coulomb conducted hundreds of experiments, and over a broad range of conditions he observed: al force is approximately independent of contact area. al force is approximately independent of velocity magnitude. Coefficient of friction depends on pairs of materials. angle, Materials µ metal on metal 0.15 0.6 rubber on concrete 0.6 0.9? 1.0 2.0? plastic wrap on lettuce Leonardo s number 0.25 (Do not believe these numbers!)

Apply Coulomb s law with care angle, It holds over a broad range, but not nearly everywhere. It is approximate. Coefficients of friction tables are terrible. How can you use something so unreliable? But, how can you not use it?

Contact modes We can write Coulomb s law: ẋ ẍ < 0 f t = µf n left sliding f n > 0 f t = µf n right sliding x = 0 < 0 f t = µf n left sliding = 0 > 0 f t = µf n right sliding = 0 = 0 f t µf n rest and define contact mode to be the right column left sliding, etc. f t angle,

angle Block at rest on plane with angle α: f n = mg cos α angle, f t = mg sin α At rest f t µf n. Maximum α: f t = µf n f n f t Substituting, mg sin α = µmg cos α α = tan 1 µ mg Sometimes called the friction angle or the angle of repose.

cone Definition Define the friction cone to be the set of all wrenches satisfying Coulomb s law for an object at rest, i.e. satisfying f t µ f n 2tan 1 µ f n f t angle, The friction cone is a polyhedral convex cone in wrench space. We can restate Coulomb s law using contact modes Left sliding: f n + f t right edge of friction cone Right sliding: f n + f t left edge of friction cone Rest: f n + f t friction cone

friction cone angle, cone is positive linear span of left edge unit vector and right edge unit vector. Moment labeling

Given a mobile body, several frictional contacts, and an applied force, is equilibrium possible? Approach: use moment labelling to identify all feasible contact wrenches; test whether one of them balances the applied force. Caveat A: Presence of balancing wrench in the cone does not imply nature will select that wrench. See the wedged plank example (static indeterminacy). Caveat B: Even if equilibrium is attained, stability may not be. Stability requires more careful analysis, depending on hypothesized disturbances. angle,

Pipe clamp design problem Why does pipe clamp work? Let diameter be 2 cm. Let length be 2 cm. Assume µ of 0.25. Find min moment arm. Extend to woodpecker toy? angle, fc1 f1 fa f2 fc2

Block on table angle,

Wedged plank and piranha angle,

Triangle and three fingers. angle,

tricks Measuring the coefficient of friction. Driving Coulomb s law doesn t work so well for rubber on concrete; Theory suggests you don t spin your wheels. Almost always spinning is bad. But sometimes, in snow or mud, spinning is a good idea. You can push a car sideways, if the wheels are spinning, turning sliding friction into viscous friction. Reducing imprecision due to friction: dithering. Reducing imprecision due to friction: impact. angle, In theory, there is no difference between theory and practice. In practice, there is. Anonymous