Announcements CAPA #11 due this Friday at 10 pm Reading: Chapter 9 Section – this week Lab #4, next week Lab #5 (no prelab) Midterm Exam #3 on Tuesday.

Slides:



Advertisements
Similar presentations
Physics 111: Mechanics Lecture 12
Advertisements

Equilibrium An object is in “Equilibrium” when:
ℓ Torque τ = F·ℓ F and ℓ must be perpendicular. F Axis
It’s gravy n I got it all smothered, like make-up I got it all covered
Torque and Equilibrium
Physics 101: Lecture 14 Torque and Equilibrium
Quiz * Vector A has a magnitude of 4 units and makes an angle of 37°
Chapter 9 Torque.
12. Static Equilibrium.
Short Version : 12. Static Equilibrium Conditions for Equilibrium (Mechanical) equilibrium = zero net external force & torque. Static equilibrium.
Classical Mechanics Lecture 18
PHYS16 – Lecture 26 Ch. 12 Static Equilibrium. Static Equil. Pre-question If ball 2 has twice the mass of ball 1 and the system is in static equilibrium.
Statics & Elasiticity.
Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Rolling Objects l Today’s lecture will cover Textbook Chapter Exam III.
Chapter 11 Statics In this chapter we will study the conditions under which a rigid body does not move. This part of Mechanics is called “Statics”. Even.
Torque and Equilibrium Lecture 8 Pre-reading : KJF §8.1 and 8.2.
Chapter 12: Static Equilibrium Conditions for equilibrium  First condition for equilibrium When a particle is in equilibrium (no acceleration), in an.
12. Static Equilibrium Conditions for Equilibrium Center of Gravity
Physics 106: Mechanics Lecture 07
Physics 106: Mechanics Lecture 08
Equilibrium of Particles Free-body Diagram Equilibrium of Rigid Bodies
Statics. Static Equilibrium  There are three conditions for static equilibrium. 1.The object is at rest 2.There is no net force 3.There is no net torque.
Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback.
Physics 101: Lecture 9, Pg 1 Physics 101: Application of Newton's Laws l Review of the different types of forces discussed in Chapter 4: Gravitational,
Equilibrium Lecturer: Professor Stephen T. Thornton.
T082 Q1. A uniform horizontal beam of length 6
Warm-Up: February 17, 2015 Write down a definition for equilibrium.
Announcements CAPA Set #5 due today (Friday) at 10 pm CAPA Set #6 now available, due next Friday Next week in Section  Lab 2: Acceleration due to gravity.
MedAdvance Internship Program MedAdvance is an internship program based out of the Scientific Education and Research Institute in Thornton, CO. As a member.
Announcements CAPA Set #6 due Friday at 10 pm This week in Section  Lab 2: Acceleration due to gravity Make sure to do the pre-lab and print materials.
Announcements CAPA #11 due this Friday at 10 pm Reading: Finish Chapter 8, Start Chapter Section – this week Lab #4: Rotations Midterm Exam #3.
Chapter 8: Torque and Angular Momentum
Chapter 9 Torque.
ROTATIONAL MOTION AND EQUILIBRIUM
Torque and Equilibrium
Static Equilibrium (Serway ) Physics 1D03.
Rotational Dynamics General Physics I Mechanics Physics 140 Racquetball Striking a Wall Mt. Etna Stewart Hall.
Chapter 8 Statics Statics. Equilibrium An object either at rest or moving with a constant velocity is said to be in equilibrium An object either at rest.
What forces act upon the meter stick? Where should the force of gravity be considered to act? Center of Gravity – the single point on a body where the.
1© Manhattan Press (H.K.) Ltd. 1.7 Stability 2 © Manhattan Press (H.K.) Ltd. Stability 1.7 Stability (SB p. 75) What makes objects more stable than others?
1 In the problem about finding the tension in a support wire for a beam and sign in static equilibrium, where is the correct point to use as the axis of.
Chapter 8: Equilibrium and Mechanical Advantage
Physics 101: Lecture 27, Pg 1 Forces: Equilibrium Examples Physics 101: Lecture 02 l Today’s lecture will cover Textbook Sections No LAB preflights.
Copyright © 2009 Pearson Education, Inc. An object with forces acting on it, but with zero net force, is said to be in equilibrium. The Conditions for.
Lecture What is the sign of cos(225 o )? Sign of sin(225 o )? Don’t use a calculator! A) cos(225 o ) = (+), sin(225 o ) = (–) B) cos(225 o ) =
Chapter 5 Two Dimensional Forces Equilibrium An object either at rest or moving with a constant velocity is said to be in equilibrium The net force acting.
Announcements CAPA Assignment #12 due this Friday at 10 pm Section: Lab #5, Springs and Things (note no prelab) Nagle’s office hours 2-3 pm cancelled Exam.
Velocity is constant, thus acceleration is zero.
Physics 101: Lecture 14, Pg 1 Physics 101: Lecture 14 Torque and Equilibrium Today’s lecture will cover Textbook Chapter Exam II.
Chapter 11 Equilibrium. If an object is in equilibrium then its motion is not changing. Therefore, according to Newton's second law, the net force must.
Topic 2.2 Extended F – Torque, equilibrium, and stability
Physics 101: Lecture 14, Pg 1 Physics 101: Lecture 14 Torque and Equilibrium Today’s lecture will cover Textbook Chapter Exam II.
Physics 101: Lecture 14, Pg 1 Physics 101: Lecture 14 Torque and Equilibrium Today’s lecture will cover Textbook Chapter Exam II.
Two-Dimensional Rotational Dynamics 8.01 W09D2 Young and Freedman: 1.10 (Vector Product), , 10.4, ;
Monday, Dec. 6, 2010PHYS , Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #23 Monday, Dec. 6, 2010 Dr. Jaehoon Yu Similarities Between.
Equilibrium. The First Condition of Equilibrium In a situation involving equilibrium, there is no acceleration (no change in velocity). Thus the net force.
“ Friendship is like peeing on yourself; everyone can see it, but only you get the warm feeling it brings.” Funnyquotes.com Course web page
4-8 Applications Involving Friction, Inclines
Chapter 12 Lecture 21: Static Equilibrium and Elasticity: I HW8 (problems):11.7, 11.25, 11.39, 11.58, 12.5, 12.24, 12.35, Due on Friday, April 1.
Wednesday, Nov. 13, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #17 Wednesday, Nov. 13, 2002 Dr. Jaehoon Yu 1.Conditions.
1 Rotational Dynamics The Action of Forces and Torques on Rigid Objects Chapter 9 Lesson 2 (a) Translation (b) Combined translation and rotation.
Mechanics Lecture 17, Slide 1 Physics 211 Lecture 17 Today’s Concepts: a) Torque Due to Gravity b) Static Equilibrium Next Monday 1:30-2:20pm, here: Hour.
Chapter 12. Rotation of a Rigid Body
PHY131H1F - Class 19 Today, Chapter 12:
Wednesday, May 9 noon-1:50PM
PHYS 1443 – Section 003 Lecture #17
Collisions and Rotations
Announcements: Midterm 2 coming up Monday Nov. 12 , (two evening times, 5-6 pm or 6-7 pm), Olin 101. Material: Chapters 6 – 14 (through HW 14.1 (pressure)).
Chapter 9 Torque.
Presentation transcript:

Announcements CAPA #11 due this Friday at 10 pm Reading: Chapter 9 Section – this week Lab #4, next week Lab #5 (no prelab) Midterm Exam #3 on Tuesday November 8 th, 2011  details given on course web page “exam info”  practice exam and solutions on CULearn  formula sheet and info. posted on web page Fraction of all clicker questions answered posted on CULearn. me with your clicker ID, name, student ID if you believe it is incorrect.

Static Equilibrium

A mass m is hanging (statically) from two strings. The mass m, and the angles α and β are known. What are the tensions T 1 and T 2 ? Note: No lever arm. Thus no torques. Two equations with two unknowns, can solve for T 1 and T 2 after some algebra.

Static Equilibrium Problem: 4 Step Process #1 – Draw the free body diagram identifying all forces and exactly where they act. Mgmg N #2 – Label the coordinate axis and axis of rotation being considered (and the sign convention) x y Axis of rotation CCW= +

Static Equilibrium Problem: 4 Step Process Mgmg N x y Axis of rotation CCW= + #3 – Write out F net = ma and  net = I  equations… F net,x = (M+m)a x = 0 (no forces in this direction) F net,y = (M+m)a y = 0 = +N – Mg – mg  net = I  = 0 = +(Mg)D 1 – (mg)D 2 #4 – Solve…

Clicker QuestionRoom Frequency BA Assume pencil of length L and mass M and with  =60 degrees. We treat the force of gravity (Mg) as if it acts only on the center-of-mass position of the object. Approximately in the middle of the pencil.  What is the torque around the tip of the pencil at this time? A)-(N-Mg) sin(60) L B)-Mg cos(60) L/2 – N cos(60) L C)-Mg sin(60) L/2 D)-Mg cos(60) L/2 E)-Mg sin(60) L Mg N Mgcos(60) Mgsin(60) L/2  net = r F perp = -(L/2) (Mgcos(60))

Stability and Balance If only the gravitational force and the Normal force are acting (as shown), if the center-of-mass is not directly over the point of contact, the system is unstable (will fall over). System is in static equilibrium. Called neutral equilibrium. System is in static equilibrium. Called unstable equilibrium (slightest change and it falls)

Clicker QuestionRoom Frequency BA Case 1Case 2 Which of the following are correct (assume in both cases the sphere is at rest at this moment)? A)Case 1 and Case 2 are in neutral equilibrium B)Case 1 is in unstable equilibrium and Case 2 is just unstable C)Case 1 is in neutral equilibrium and Case 2 is in neutral eq. D)Case 1 is in neutral equilibrium and Case 2 is just unstable E)None of the above

Tipping Point If force of gravity applied at the center-of-gravity (CG) points outside the point of balance, the object will fall (unstable). U.S. Consumer Product Safety Commission finds approximately 2.18 deaths per year from vending machine tipovers.

7 m 55 m 4.0 m CM The leaning tower of Pisa is 55 m high and leans 4 m off vertical at the top. Its base is 7 m wide. How much further could it lean horizontally (at the top) before it would fall over? A) 1.5 m B) 2 m C) 3 m D) 4 m E) 6 m Clicker QuestionRoom Frequency BA Ignoring any small forces holding it to the ground.

A sign with mass m s is hung from a uniform bar of mass m b and length L. The sign is suspended ¾ of the way from the pivot. The sign is held up with a cable at an angle θ. How strong a cable is required (i.e. what is tension T)?

Step #1: Force Diagram Step #2: Coordinate System x y CCW= +

A sign of mass m s is hung from a uniform horizontal bar of mass m B as shown. What is the sign of the x-component of the force exerted on the bar by the wall? A)Positive B)Negative C)F wx = 0. Using Σ F x = 0, the hinge force must have a positive x-component, in order to cancel the negative x-component of the tension force. Clicker QuestionRoom Frequency BA

x y CCW= + Step #3: Static Equilibrium condition F=ma=0 and  =I  =0 Not enough information to solve for T, F wx, F wy (2 constraint equations and 3 unknowns)