Chapter 12 Equilibrium & Elasticity

Similar documents
Chapter 11: Angular Momentum

PHYS 1443 Section 002 Lecture #20

10/24/2013. PHY 113 C General Physics I 11 AM 12:15 PM TR Olin 101. Plan for Lecture 17: Review of Chapters 9-13, 15-16

Part C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis

Physics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding.

Physics 207: Lecture 20. Today s Agenda Homework for Monday

Study Guide For Exam Two

Chapter 11 Angular Momentum

First Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.

CONDUCTORS AND INSULATORS

10/23/2003 PHY Lecture 14R 1

Physics 207: Lecture 27. Announcements

Module 11 Design of Joints for Special Loading. Version 2 ME, IIT Kharagpur

Spring 2002 Lecture #13

I have not received unauthorized aid in the completion of this exam.

Physics 207 Lecture 6

Week 9 Chapter 10 Section 1-5

Week 6, Chapter 7 Sect 1-5

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

Conservation of Angular Momentum = "Spin"

Angular Momentum and Fixed Axis Rotation. 8.01t Nov 10, 2004

Important Dates: Post Test: Dec during recitations. If you have taken the post test, don t come to recitation!

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

Dynamics of Rotational Motion

Newton s Laws of Motion

Chapter 11 Torque and Angular Momentum

Rotational Dynamics. Physics 1425 Lecture 19. Michael Fowler, UVa

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

One Dimensional Axial Deformations

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Increase Decrease Remain the Same (Circle one) (2 pts)

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Linear Momentum. Center of Mass.

Energy and Energy Transfer

Chapter 8: Potential Energy and The Conservation of Total Energy

TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 2211, Exam 2 Section 1 Version 1 October 18, 2013 Total Weight: 100 points

Physics 111: Mechanics Lecture 11

Physics 141. Lecture 14. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 14, Page 1

Physics 201 Lecture 9

Chapter 07: Kinetic Energy and Work

Physics 181. Particle Systems

THE CURRENT BALANCE Physics 258/259

MECHANICS OF MATERIALS

Physics 207 Lecture 13. Lecture 13

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

PHYSICS 231 Review problems for midterm 2

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

So far: simple (planar) geometries

MEASUREMENT OF MOMENT OF INERTIA

11. Dynamics in Rotating Frames of Reference

Week 8: Chapter 9. Linear Momentum. Newton Law and Momentum. Linear Momentum, cont. Conservation of Linear Momentum. Conservation of Momentum, 2

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 19. Home Page. Title Page. Page 1 of 36.

Error Bars in both X and Y

APPENDIX F A DISPLACEMENT-BASED BEAM ELEMENT WITH SHEAR DEFORMATIONS. Never use a Cubic Function Approximation for a Non-Prismatic Beam

Supplemental Material: Causal Entropic Forces

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

PHYS 1443 Section 004 Lecture #12 Thursday, Oct. 2, 2014

Physics 2A Chapters 6 - Work & Energy Fall 2017

Physics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall

Thermodynamics General

PES 1120 Spring 2014, Spendier Lecture 6/Page 1

Chapter 3. r r. Position, Velocity, and Acceleration Revisited

Problem Points Score Total 100

τ rf = Iα I point = mr 2 L35 F 11/14/14 a*er lecture 1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Chapter 3 and Chapter 4

Problem While being compressed, A) What is the work done on it by gravity? B) What is the work done on it by the spring force?

Mechanics Cycle 3 Chapter 9++ Chapter 9++

Physics 114 Exam 3 Spring Name:

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 2 EXAMINATIONS 2011/2012 DYNAMICS ME247 DR. N.D.D. MICHÉ

Spin-rotation coupling of the angularly accelerated rigid body

EN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics

Moments of Inertia. and reminds us of the analogous equation for linear momentum p= mv, which is of the form. The kinetic energy of the body is.

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics

Conservation of Energy

10/9/2003 PHY Lecture 11 1

EMU Physics Department

Chapter 9. The Dot Product (Scalar Product) The Dot Product use (Scalar Product) The Dot Product (Scalar Product) The Cross Product.

Physics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall

CHAPTER 10 ROTATIONAL MOTION

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

Gravitational Acceleration: A case of constant acceleration (approx. 2 hr.) (6/7/11)

Page 1. SPH4U: Lecture 7. New Topic: Friction. Today s Agenda. Surface Friction... Surface Friction...

Frame element resists external loads or disturbances by developing internal axial forces, shear forces, and bending moments.

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)

MAGNETISM MAGNETIC DIPOLES

In this section is given an overview of the common elasticity models.

PHYS 1443 Section 003 Lecture #17

Page 1. Physics 131: Lecture 14. Today s Agenda. Things that stay the same. Impulse and Momentum Non-constant forces

Rigid body simulation

Chapter 8. Potential Energy and Conservation of Energy

Physics 115. Molecular motion and temperature Phase equilibrium, evaporation

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Lecture Note 3. Eshelby s Inclusion II

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

NEWTON S LAWS. These laws only apply when viewed from an inertial coordinate system (unaccelerated system).

Second Order Analysis

Transcription:

Chapter 12 Equlbrum & Elastcty If there s a net force, an object wll experence a lnear acceleraton. (perod, end of story!) If there s a net torque, an object wll experence an angular acceleraton. (perod, end of story!) How can we keep thngs from movng, then? r r dp r dl r Recall, net and τ dt dt

Chapter 12 Equlbrum & Elastcty Equlbrum: P constant and L constant Statc equlbrum: Objects that are not movng ether n translaton or rotaton. P 0 L 0 Requrements of equlbrum r net r τ r dp dt dl r dt r net 0 (balance of forces) τ 0 (balance of torques)

or the stuatons n whch the forces that act on the body le n the xy plane. Then the only torque that can act on the body s τ z. We have net,x 0 net,y 0 τ net,z 0 τ net,z s the net torque that the external forces produce ether about the z axs or about any axs parallel to t

Center of gravty Center of gravty: gravtatonal force on a body effectvely act at a sngle pont. or everyday objects, the center of gravty concdent wth ts center of mass.

Sample Problem 12-1 A beam of length L and mass m 1.8 kg, s at rest wth ts ends on two scales. A block of M 2.7 kg, s at rest on the beam, wth ts center a dstance L/4 from the beam s left end. What do the scales read ( l and r )?

Sample Problem 12-1 A beam of length L and mass m 1.8 kg, s at rest wth ts ends on two scales. A block of M 2.7 kg, s at rest on the beam, wth ts center a dstance L/4 from the beam s left end. What do the scales read? Sum of all the forces on the beam must equal zero. ŷ : v 0 l Mg mg + r 0

Sample Problem 12-1 A beam of length L and mass m 1.8 kg, s at rest wth ts ends on two scales. A block of M 2.7 kg, s at rest on the beam, wth ts center a dstance L/4 from the beam s left end. What do the scales read? Sum of all the torques about any pont on the beam must equal zero. Choose ths pont to be the left end of the beam. ẑ : v L L τ 0 (0)l Mg mg + (L)r 4 2 0

Sample Problem 12-1 A beam of length L and mass m 1.8 kg, s at rest wth ts ends on two scales. A block of M 2.7 kg, s at rest on the beam, wth ts center a dstance L/4 from the beam s left end. What do the scales read? Whch yelds, r and L 4 Mg + L 2 mg 3L L l Mg + mg r Mg + mg 4 2

Sample problem 12-2: a ladder L 12 m and mass m 45 kg leans aganst a frctonless wall. h 9.3 m. The ladder s c.o.m. s L/3 from the lower end. A frefghter of M 72 kg clmbs the ladder untl her c.o.m. s L/2 from the lower end. What are the magntudes of the forces on the ladder from the wall and the pavement?

Queston 65 N What should 1 be n order to keep the unform rod n statc equlbrum?

Queston ŷ : v 0 20 N 10 N 1 30 N + 65 N 0 1 ẑ : v τ 0 (8d)20 N + (4d)10 N + (2d) 1 + (d)30 N (0d)65 N 0 1 45 N 45 N 65 N What should 1 be n order to keep the unform rod n statc equlbrum? 1) 45 N 2) 0 N 3) 40 N 4) t s ponted n the wrong drecton 5) none of the above

A Quz Suppose that the (unform) horzontal rod s held just barely n statc equlbrum by the rope and the pvot pont. The grey arrow s the weght of the rod at the center of mass and the green arrow s a movable appled downward force. What happens when s moved toward A? 1) nothng 2) the net force ncreases 3) the net torque ncreases 4) the net torque decreases 5) none of the above mg pvot pont

A Quz Suppose that the (unform) horzontal rod s held just barely n statc equlbrum by the rope and the pvot pont. The grey arrow s the weght of the rod at the center of mass and the green arrow s a movable appled downward force. What happens when s moved toward A? 1) nothng 2) the net force ncreases 3) the net torque ncreases 4) the net torque decreases 5) none of the above mg pvot pont

ŷ : xˆ : v v pvot,y pvot,x + T cosθ A Quz mg + Tsn θ v τ l + L 2 mg LTsn θ > L 2 + L 2 mg LTsn θ snce l > L/2, the torque ncreases 1) nothng 2) the net force ncreases 3) the net torque ncreases 4) the net torque decreases 5) none of the above L mg L/2 l pvot pont

Stress and Stran Mcroscopc vew of materals: Materals are made of atoms held n place by electrostatc nteractons wth neghborng atoms. These nteractons are such that the atoms are constantly n harmonc moton about ther equlbrum postons.

Stress and Stran External forces can be exerted on these atoms. The atoms wll react to these forces dependng on ther mcroscopc envronment.

Deformaton Types elongaton (tensle strength) shear hydraulc compresson modulus s a constant depended on how much the materals react (deform) to the appled forces. stress modulus x stran

Elongaton (tensle strength) and compresson Stress s defned as perpendcular force per unt area. Stress /A Stran s defned as the fractonal change n the length of the object. Stran L/L Young s modulus E s the proportonalty constant. A E L L

Shear stress Stress s defned as force n the plane per unt area. Stress /A Stran s defned as the fractonal change n the movement of the object. Stran x/l Shear modulus G s the proportonalty constant. A G x L

Hydraulc Stress or three dmensons we use pressure, whch s also defned as force per unt area. Pressure p /A Stran s defned as the fractonal change n the volume of the object. Stran V/V Bulk modulus B s the proportonalty constant. p A B V V

Materals scence studes cause of specfc shape of ths curve. Elastc Lmt Regon we ll be dscussng ths semester. Addtonal regon of nterest to engneers.