How Can Motion be Described? and Explained?

Similar documents
Torque. Objectives. Assessment. Assessment. Equations. Physics terms 6/2/14

Torque and Static Equilibrium

Chapter 8. Centripetal Force and The Law of Gravity

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10

Turning Forces and Levers. Junior Science

Torque. Physics 6A. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

five moments ELEMENTS OF ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SPRING 2014 lecture ARCH 614

Chapter 8. Rotational Equilibrium and Rotational Dynamics

Chapter 8 Rotational Equilibrium and Rotational Dynamics Force vs. Torque Forces cause accelerations Torques cause angular accelerations Force and

Rotational N.2 nd Law

Rotational N.2 nd Law

Static equilibrium. Objectives. Physics terms. Assessment. Brainstorm. Equations 6/3/14

Application of Forces. Chapter Eight. Torque. Force vs. Torque. Torque, cont. Direction of Torque 4/7/2015

GIANCOLI READING ACTIVITY Lesson 8-4

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

Center of Gravity Pearson Education, Inc.

Chapter 11 Rotational Dynamics and Static Equilibrium. Copyright 2010 Pearson Education, Inc.

Physics 111. Lecture 22 (Walker: ) Torque Rotational Dynamics Static Equilibrium Oct. 28, 2009

Laith Batarseh. internal forces

Cross Product Angular Momentum

Mechatronics. MANE 4490 Fall 2002 Assignment # 1

Torque and Rotational Equilibrium

2008 FXA THREE FORCES IN EQUILIBRIUM 1. Candidates should be able to : TRIANGLE OF FORCES RULE

Simple Biomechanical Models. Introduction to Static Equilibrium F F. Components of Torque. Muscles Create Torques. Torque is a Vector

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

Physics 8 Wednesday, October 28, 2015

Torque and Rotational Equilibrium

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method

Levers of the Musculoskeletal System

Rotational Equilibrium

Torques and Static Equilibrium

Unit 4 Statics. Static Equilibrium Translational Forces Torque

Force in Mechanical Systems. Overview

Static Equilibrium. University of Arizona J. H. Burge

LECTURE 22 EQUILIBRIUM. Instructor: Kazumi Tolich

APPLIED MECHANICS I Resultant of Concurrent Forces Consider a body acted upon by co-planar forces as shown in Fig 1.1(a).

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.

Chapter 8. Rotational Motion

Moments and Torques. M = F d

Static Equilibrium; Torque

Parallel Forces. Forces acting in the same or in opposite directions at different points on an object.

( )( ) ( )( ) Fall 2017 PHYS 131 Week 9 Recitation: Chapter 9: 5, 10, 12, 13, 31, 34

Lecture 14. Rotational dynamics Torque. Give me a lever long enough and a fulcrum on which to place it, and I shall move the world.

P12 Torque Notes.notebook. March 26, Torques

Dynamics. Dynamics of mechanical particle and particle systems (many body systems)

Chapter 12: Rotation of Rigid Bodies. Center of Mass Moment of Inertia Torque Angular Momentum Rolling Statics

Università degli Studi di Bari. mechanics 1. Load system determination. Joint load. Stress-strain distribution. Biological response 2/45 3/45

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

Chapter 8. Rotational Equilibrium and Rotational Dynamics

When the applied force is not perpendicular to the crowbar, for example, the lever arm is found by drawing the perpendicular line from the fulcrum to

Phys101 Lectures 19, 20 Rotational Motion

III. Angular Momentum Conservation (Chap. 10) Rotation. We repeat Chap. 2-8 with rotatiing objects. Eqs. of motion. Energy.

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

CHAPTER 9 ROTATIONAL DYNAMICS

Chap. 10: Rotational Motion

Chapter 9 TORQUE & Rotational Kinematics

Mechanics of Materials

Chapter 12 Static Equilibrium

Equilibrium and Torque

Lecture PowerPoints. Chapter 8 Physics: Principles with Applications, 6 th edition Giancoli

PHY131H1S - Class 20. Pre-class reading quiz on Chapter 12

Physics 101: Lecture 14 Torque and Equilibrium

Recap I. Angular position: Angular displacement: s. Angular velocity: Angular Acceleration:

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS

MATHEMATICAL SKILLS MOMENTS OF FORCE (RATIOS) AND EQUILIBRIUM AND ASSOCIATED EXAMINATION QUESTIONS.

III. Work and Energy

When an object is in translational equilibrium and rotational equilibrium, we say it is in static equilibrium.

Rotational Equilibrium

2/28/2006 Statics ( F.Robilliard) 1

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

Physics A - PHY 2048C

Lab 17 Torques/Moments

Moments, Levers and Centre of Gravity

Equilibrium Notes 1 Translational Equilibrium

Dynamics of Rotational Motion

PHYSICS 220 LAB #3: STATIC EQUILIBRIUM FORCES

The diagram shows the wheel wrench being used without the handle extended.

Equilibrium and Torque

Section 2: Static Equilibrium II- Balancing Torques

Chapter 7 INTERNAL FORCES

Physics 101 Lecture 11 Torque

Lecture Outline Chapter 11. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Methods of Analysis. Force or Flexibility Method

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

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

Torque rotational force which causes a change in rotational motion. This force is defined by linear force multiplied by a radius.

M.S Comprehensive Examination Analysis

21.4 Electric Field and Electric Forces

Study Guide. Physics 3104A. Science. Force, Motion and Energy. Adult Basic Education. Prerequisite: Physics 2104B or Physics 2204.

No Brain Too Small PHYSICS

Rotational Mechanics Part II Torque. Pre AP Physics

ΣF = 0 and Στ = 0 In 2-d: ΣF X = 0 and ΣF Y = 0 Goal: Write expression for Στ and ΣF

Vector Mechanics: Statics

PHYSICS 149: Lecture 21

Chapter 12. Static Equilibrium and Elasticity

Center of Gravity. The location of the center of gravity is defined by: n mgx. APSC 111 Review Page 7

Balancing of Rotating Masses

τ = F d Angular Kinetics Components of Torque (review from Systems FBD lecture Muscles Create Torques Torque is a Vector Work versus Torque

Announcements Oct 16, 2014

(1) (allow e.c.f. for work done in (ii)) = 133 W (1) (allow e.c.f. for incorrect time conversion) 6

Transcription:

How Can Motion be Described? and Explained? Lesson 14: Torque and the Stability of Structures Stable Structures Explain why structures should be stable. What are the conditions for a structure to be stable? Newton's Second Law, F net = ma, gives us a clue. A structure should have. initial velocity and zero. Hence net force on all parts of a structure must equal. A body is in translational when the sum of the forces acting on it is equal to zero. One condition for a stable structure is that it all of its component parts must be in translational equilibrium. 1

Centre of Mass The point in a body where all the can be considered to be concentrated. Centre of mass is a useful concept for analysing structures. Weight forces (mg) should always be drawn from the.. of mass of a structural element. 2

3

Rotational Forces Torque Torque is a force that produces a twisting, turning or rotational effect. Torque Formula 4

Rotational Forces (Continued) How can motion be described and explained? Lesson 14 Semi-notes Calculating Torque when force, F is not. to the lever arm Indicating Direction of Torque 5

6

Rotational Equilibrium A body must be in rotational equilibrium to be A body is in rotational equilibrium when the sum of the acting on it is equal to zero. For a body or structure to be in Static Equilibrium (and hence be stable), it must be in both t equilibrium and r..equilibrium. There is a huge torque acting on this structure. The foundations would need to supply an equal anticlockwise torque to keep the 'cheesestick' stable. Extra Notes 7

8

9

Simple Structural Elements Beams Beam Bridges Why can modern structures span far greater distances? Beam Bridges can be analysed using the conditions for translational and rotational equilibrium. 10

Principle of Moments When analysing situations where more than one acts on a body, the body will be in rotational equilibrium if the net torque about a. (or pivot) point equals zero. Simple Structural Elements (continued) Cantilever A beam that extends beyond its. structure. 11

Analysing the cantilever Draw in all forces acting on the beam as shown below. Cantilever with load. Cantilever Bridge Just place two or more cantilvers together to make a bridge. 12

Cantilever Bridges Can be supported by.. and/or... Cantilever Bridges 13

14

15

Summary Stable Structures What are the conditions for a structure to be stable? Newton's Second Law, F net = ma, gives us a clue. A structure should have zero initial velocity and zero acceleration. Hence net force on all parts of a structure must equal zero. A body is in translational equilibrium when the sum of the forces acting on it is equal to zero. Centre of Mass The point in a body where all the mass can be considered to be concentrated. Rotational Forces Torque Torque is a rotational force that produces a twisting, turning or rotational effect. 16

Rotational Forces (Continued) Alternative Torque Formula When the applied force is not perpendicular to the lever arm Rotational Equilibrium A body must be in rotational equilibrium to be stable A body is in rotational equilibrium when the sum of the torques acting on it is equal to zero. Static Equilibrium For a body or structure to be in Static Equilibrium (and hence be stable), it must be in both translational equilibrium and rotational equilibrium. 17

Simple Structural Elements How can motion be described and explained? Lesson 14 Semi-notes. 18