Equilibrium. Lecture 8 Physics 106 Spring Equilibrium. Equilibrium. Equilibrium. Balance of Forces: Balance of Forces: Balance of Torques:

Similar documents
Equilibrium: Forces and Torques

EQUILIBRIUM and ELASTICITY

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

τ net l = r p L = Iω = d L dt = I α ΔL Angular momentum (one) Angular momentum (system, fixed axis) Newton s second law (system)

HATZIC SECONDARY SCHOOL

Physics 2101, Final Exam, Spring 2007

PHYSICS - CLUTCH CH 13: ROTATIONAL EQUILIBRIUM.

Chapter 9- Static Equilibrium

is the study of and. We study objects. is the study of and. We study objects.

Equilibrium & Elasticity

Upthrust and Archimedes Principle

Physics Mechanics. Lecture 11 Newton s Laws - part 2

TEST REPORT. Question file: P Copyright:

Static Equilibrium; Torque

Definition. is a measure of how much a force acting on an object causes that object to rotate, symbol is, (Greek letter tau)

4.1.1 Extra Practice 4.1 Analyze the effects of a uniform force (magnitude and direction.)

Lecture 13 REVIEW. Physics 106 Spring What should we know? What should we know? Newton s Laws

PY205N Spring The vectors a, b, and c. are related by c = a b. The diagram below that best illustrates this relationship is (a) I

Angular Momentum L = I ω

Angular Speed and Angular Acceleration Relations between Angular and Linear Quantities

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

Chapter 9 TORQUE & Rotational Kinematics

Angular Momentum L = I ω

Equilibrium Notes 1 Translational Equilibrium

Statics. Phys101 Lectures 19,20. Key points: The Conditions for static equilibrium Solving statics problems Stress and strain. Ref: 9-1,2,3,4,5.

Problem Set x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. 1. Moment of Inertia: Disc and Washer

Phys101 Second Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Sunday, November 03, 2013 Page: 1

LECTURE 22 EQUILIBRIUM. Instructor: Kazumi Tolich

Unit 4 Statics. Static Equilibrium Translational Forces Torque

Physics 12 Final Exam Review Booklet # 1

AP Physics 1 Multiple Choice Questions - Chapter 4

Your Comments. That s the plan

ROTATIONAL DYNAMICS AND STATIC EQUILIBRIUM

Physics 2514 Lecture 13

SPH3U1 - Dynamics Problems Set 3

Sample Physics Placement Exam

(1) +0.2 m/s (2) +0.4 m/s (3) +0.6 m/s (4) +1 m/s (5) +0.8 m/s

AP Mechanics Summer Assignment

Lecture 6 Physics 106 Spring 2006

What is a Force? Free-Body diagrams. Contact vs. At-a-Distance 11/28/2016. Forces and Newton s Laws of Motion

Physics 101 Lecture 12 Equilibrium

PHYSICS 221, FALL 2011 EXAM #2 SOLUTIONS WEDNESDAY, NOVEMBER 2, 2011

Consider two students pushing with equal force on opposite sides of a desk. Looking top-down on the desk:

1. An object is fired with an initial velocity of 23 m/s [R30 U]. What are the initial components of its velocity?

Physics 2210 Fall smartphysics Rotational Statics 11/18/2015

CHAPTER 12 STATIC EQUILIBRIUM AND ELASTICITY. Conditions for static equilibrium Center of gravity (weight) Examples of static equilibrium

PHYS 185 Practice Final Exam Fall You may answer the questions in the space provided here, or if you prefer, on your own notebook paper.

Equilibrium. the linear momentum,, of the center of mass is constant

Work and energy. 15 m. c. Find the work done by the normal force exerted by the incline on the crate.

1 MR SAMPLE EXAM 3 FALL 2013

AP Physics Multiple Choice Practice Torque

Chapter 11. Today. Last Wednesday. Precession from Pre- lecture. Solving problems with torque

King Fahd University of Petroleum and Minerals Department of Physics. Final Exam 041. Answer key - First choice is the correct answer

EXAM 3 MECHANICS 40% of the final grade

Physics 2211 ABC Quiz #3 Solutions Spring 2017

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

= v 0 x. / t = 1.75m / s 2.25s = 0.778m / s 2 nd law taking left as positive. net. F x ! F

4.0 m s 2. 2 A submarine descends vertically at constant velocity. The three forces acting on the submarine are viscous drag, upthrust and weight.

Unit 2 ~ Learning Guide Name:

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

Lecture 8. Torque. and Equilibrium. Pre-reading: KJF 8.1 and 8.2

is acting on a body of mass m = 3.0 kg and changes its velocity from an initial

PHYSICS 8A, Lecture 2 Spring 2017 Midterm 2, C. Bordel Thursday, April 6 th, 7pm-9pm

Chapter 12 Static Equilibrium

Chapter 4 Dynamics: Newton s Laws of Motion

Practice. Newton s 3 Laws of Motion. Recall. Forces a push or pull acting on an object; a vector quantity measured in Newtons (kg m/s²)

Physics 101 Lecture 5 Newton`s Laws

We define angular displacement, θ, and angular velocity, ω. What's a radian?

Phys 1401: General Physics I

5.2 Rigid Bodies and Two-Dimensional Force Systems

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

Static Equilibrium. Lecture 22. Chapter 12. Physics I Department of Physics and Applied Physics

The Laws of Motion. Newton s first law Force Mass Newton s second law Gravitational Force Newton s third law Examples

Multiple Choice Practice

Chapter 4 Dynamics: Newton s Laws of Motion

Section 2: Static Equilibrium II- Balancing Torques

Concept of Force Challenge Problem Solutions

Dynamic equilibrium: object moves with constant velocity in a straight line. = 0, a x = i

Static Equilibrium and Torque

α f k θ y N m mg Figure 1 Solution 1: (a) From Newton s 2 nd law: From (1), (2), and (3) Free-body diagram (b) 0 tan 0 then

General Physics I Forces

Physics 1A, Summer 2011, Summer Session 1 Quiz 3, Version A 1

Chapter 8. Rotational Equilibrium and Rotational Dynamics. 1. Torque. 2. Torque and Equilibrium. 3. Center of Mass and Center of Gravity

4.2. Visualize: Assess: Note that the climber does not touch the sides of the crevasse so there are no forces from the crevasse walls.

Last-night s Midterm Test. Last-night s Midterm Test. PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity

Fr h mg rh h. h 2( m)( m) ( (0.800 kg)(9.80 m/s )

Physics 111 Lecture 4 Newton`s Laws

PHYS 101 Previous Exam Problems. Force & Motion I

2.1 Force. Net Force. Net Force. Net Force

AP Physics First Nine Weeks Review

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Chapter 4: Newton s Second Law F = m a. F = m a (4.2)

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.

CHAPTER 8: ROTATIONAL OF RIGID BODY PHYSICS. 1. Define Torque

Static Equilibrium. Lecture 24. Chapter 12. Physics I. Department of Physics and Applied Physics

Dynamics: Forces and Newton s Laws of Motion

Lecture Presentation Chapter 8 Equilibrium and Elasticity

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Wiley Plus. Final Assignment (5) Is Due Today: Before 11 pm!

2 Mechanical Equilibrium. An object in mechanical equilibrium is stable, without changes in motion.

Transcription:

Lecture 8 Physics 106 Spring 2006 http://web.njit.edu/~sirenko/ 3/8/2006 Andrei Sirenko, JIT 1 3/8/2006 Andrei Sirenko, JIT 2 3/8/2006 Andrei Sirenko, JIT 3 3/8/2006 Andrei Sirenko, JIT 4

3/8/2006 Andrei Sirenko, JIT 5 3/8/2006 Andrei Sirenko, JIT 6 inside a Star 1. The vector sum of all the external forces that act on the body must be zero. 2. The vector sum of all the external torques that act on the body, measured about any possible point, must be zero. 3. The linear momentum P of the body must be zero. 4. The gravitational force F g on a body effectively acts on a single point, called the center of gravity (cog) of the body. If g is the same for all elements of the body, then the body s cog is coincident with the body s center of mass. 3/8/2006 Andrei Sirenko, JIT 7 3/8/2006 Andrei Sirenko, JIT 8

of the tower of Piza Is it really stable? Static Back to Eq. Away from Eq. 3/8/2006 Andrei Sirenko, JIT 9 3/8/2006 Andrei Sirenko, JIT 10 for fun for fun Unstable Equil. Unstable Equil. COG Stable Equil. 3/8/2006 Andrei Sirenko, JIT 11 Stable Equil. 3/8/2006 Andrei Sirenko, JIT 12

; Stable vs. Unstable Two Forces Unstable Equil. Stable Equil. Bridge of Mechanical Constructions Tower: Roof Torque is in the direction of the Torque is opposite angular to the direction of displacement the angular displacement 3/8/2006 Andrei Sirenko, JIT 13 3/8/2006 Andrei Sirenko, JIT 14 Sample Problem XIII 1 A uniform beam of length L and mass m = 1.8 kg is at rest with its ends on two scales. A uniform block with mass M = 2.7 kg is at rest on the beam, with its center a distance L/4 from the beam s left end. What do the scales read? From the force balance we have Two unknowns 3/8/2006 Andrei Sirenko, JIT 15 3/8/2006 Andrei Sirenko, JIT 16

Is this rotating wheel stable? Dynamic and Static s are different! 3/8/2006 Andrei Sirenko, JIT 17 Sample Problem XIII 2 A ladder of length L = 12 m and mass m = 45 kg leans against a slick (frictionless) wall. Its upper end is at height h = 9.3 m above the pavement on which the lower end rests (the pavement is not frictionless). The ladder s center of mass is L/3 from the lower end. A firefighter of mass M = 72 kg climbs the ladder until her center of mass is L/2 from the lower end. What the are the magnitudes of the forces of the ladder from the wall and the pavement? 3/8/2006 Andrei Sirenko, JIT 18 Sample Problem XIII 3 A safe of mass M = 430 kg is hanging by a rope from a boom with dimensions a = 1.9 m and b = 2.5 m. The boom consists of a hinged beam and a horizontal cable that connects the beam to a wall. The uniform beam has a mass m = 85 kg. The masses of the cable and the rope are negligible. Torque balance for the point O 3/8/2006 Andrei Sirenko, JIT 19 a) What are the tension T c in the cable? In other words, what is the magnitude of the force T c on the beam from the cable? b) Find the magnitude F of the net force on the beam from the hinge. 3/8/2006 Andrei Sirenko, JIT 20

3/8/2006 Andrei Sirenko, JIT 21 3/8/2006 Andrei Sirenko, JIT 22 m m M QZ#8 d d 1.5d m = 5 kg d = 2 m Show all forces acting on the beam. Mass of the beam is zero Write the force and torque balances Calculate M to keep the whole system in equilibrium 3/8/2006 Andrei Sirenko, JIT 23 Sample Problem XIII 4 A rock climber with mass m = 55 kg rests during a chimney climb, pressing only with her shoulders and feet against the walls of a fissure of width w = 1.0 m. Her center of mass is is a horizontal distance d = 0.2 m from the wall against which her shoulders are pressed. The coefficient of static friction between her shoes and the wall is µ 1 = 1.1, and between her shoulders and the wall it is µ 2 = 0.7. a) What is the minimum horizontal push To rest, the climber wants to on the walls? minimize her horizontal push on the walls. The minimum occurs when b) For that push, what must be the her feet and her shoulders are on the vertical distance h between her feet verge of sliding. and her shoulders if she is to be stable? 3/8/2006 Andrei Sirenko, JIT 24