ENGR-1100 Introduction to Engineering Analysis. Lecture 9

Similar documents
Chapter 4 Force System Resultant Moment of a Force

MOMENT OF A FORCE SCALAR FORMULATION, CROSS PRODUCT, MOMENT OF A FORCE VECTOR FORMULATION, & PRINCIPLE OF MOMENTS

Force System Resultants. Engineering Mechanics: Statics

Mengetahui dan memahami maksud dari momen gaya, momen kopel, dan cara. Apa yang dipelajari sekarang? memindah gaya MOMEN DAN KOPEL

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

MOMENT OF A COUPLE. Today s Objectives: Students will be able to. a) define a couple, and, b) determine the moment of a couple.

ENGR-1100 Introduction to Engineering Analysis. Lecture 23

Lecture 23. ENGR-1100 Introduction to Engineering Analysis FRAMES S 1

Moment of a force (scalar, vector ) Cross product Principle of Moments Couples Force and Couple Systems Simple Distributed Loading

ENGINEERING MECHANICS BAA1113. Chapter 4: Force System Resultants (Static)

MOMENT OF A FORCE ABOUT A POINT

MOMENT OF A COUPLE. Today s Objectives: Students will be able to a) define a couple, and, b) determine the moment of a couple.

MOMENT ABOUT AN AXIS

P12 Torque Notes.notebook. March 26, Torques

Moments and Torques. M = F d

SIMPLIFICATION OF FORCE AND COUPLE SYSTEMS & THEIR FURTHER SIMPLIFICATION

DOT PRODUCT Objective:

EQUIVALENT SYSTEMS, RESULTANTS OF FORCE AND COUPLE SYSTEM, & FURTHER REDUCTION OF A FORCE AND COUPLE SYSTEM

APPLICATIONS. CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.4 7. IMPACT (Section 15.4) APPLICATIONS (continued) IMPACT READING QUIZ

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

Center of Mass. A baseball thrown into the air follows a smooth parabolic path. A baseball bat thrown into the air does not follow a smooth path.

INTERNAL FORCES Today s Objective: Students will be able to: 1. Use the method of sections for determining internal forces in 2-D load cases.

Chapter -4- Force System Resultant

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS

Announcements. Trusses Method of Joints

EQUIVALENT SYSTEMS, RESULTANTS OF FORCE AND COUPLE SYSTEM, & FURTHER REDUCTION OF A FORCE AND COUPLE SYSTEM

EQUATIONS OF EQUILIBRIUM & TWO-AND THREE-FORCE MEMEBERS

ENGR-1100 Introduction to Engineering Analysis. Lecture 20

Lecture 20. ENGR-1100 Introduction to Engineering Analysis THE METHOD OF SECTIONS

6.6 FRAMES AND MACHINES APPLICATIONS. Frames are commonly used to support various external loads.

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS

RELATIVE MOTION ANALYSIS: VELOCITY (Section 16.5)

ENGR-1100 Introduction to Engineering Analysis. Lecture 13

CEE 271: Applied Mechanics II, Dynamics Lecture 14: Ch.15, Sec.1-3

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

Equilibrium Notes 1 Translational Equilibrium

Rotational N.2 nd Law

EQUATIONS OF MOTION: CYLINDRICAL COORDINATES

Rotational N.2 nd Law

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

ENGR-1100 Introduction to Engineering Analysis. Lecture 3

F A C U L T Y O F E D U C A T I O N. Physics Electromagnetism: Induced Currents Science and Mathematics Education Research Group

UNIT - I. Review of the three laws of motion and vector algebra

Cross Product Angular Momentum

Sports biomechanics explores the relationship between the body motion, internal forces and external forces to optimize the sport performance.

Ishik University / Sulaimani Architecture Department Structure ARCH 214 Chapter -4- Force System Resultant

Chapter 7 INTERNAL FORCES

ARC241 Structural Analysis I Lecture 5, Sections ST4.5 ST4.10

Equilibrium Notes 1 Translational Equilibrium

EQUATIONS OF MOTION: RECTANGULAR COORDINATES

two forces and moments Structural Math Physics for Structures Structural Math

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

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

CIV100: Mechanics. Lecture Notes. Module 1: Force & Moment in 2D. You Know What to Do!

EQUATIONS OF MOTION: CYLINDRICAL COORDINATES (Section 13.6)

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

Chapter 5: Forces in Equilibrium

Chapter 12 Static Equilibrium

POSITION VECTORS & FORCE VECTORS

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

Forces and Newton s Laws Notes

ENGR-1100 Introduction to Engineering Analysis. Lecture 19

LECTURE 22 MAGNETIC TORQUE & MAGNETIC FIELDS. Instructor: Kazumi Tolich

Chapter 4 Kinetics of Particle: Impulse and Momentum

Vector Mechanics: Statics

If the pull is downward (Fig. 1), we want C to point into the page. If the pull is upward (Fig. 2), we want C to point out of the page.

Figure Two. Then the two vector equations of equilibrium are equivalent to three scalar equations:

DOT PRODUCT. Statics, Fourteenth Edition in SI Units R.C. Hibbeler. Copyright 2017 by Pearson Education, Ltd. All rights reserved.

The student will learn about the main purposes and the basic components of all machines. SIMPLE MACHINES. SPH4C Findlay

STATICS. Equivalent Systems of Forces. Vector Mechanics for Engineers: Statics VECTOR MECHANICS FOR ENGINEERS: Contents & Objectives.

Rotational Equilibrium

LECTURE 15 TORQUE AND CENTER OF GRAVITY

Review session for Exam 2 Monday 3/25 6:00 PM in Loomis 151 (here) Print out/bring Exam 2, Fall 2005

Force in Mechanical Systems. Overview

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia):

Static Equilibrium; Torque

Statics: Lecture Notes for Sections

two structural analysis (statics & mechanics) APPLIED ACHITECTURAL STRUCTURES: DR. ANNE NICHOLS SPRING 2017 lecture STRUCTURAL ANALYSIS AND SYSTEMS

Rotational Kinetic Energy

Engineering Mechanics Statics

PLANAR RIGID BODY MOTION: TRANSLATION &

Force System Resultants Distributed Loads. A hole has been found in the nudist camp wall. The police are looking into it.

Physics 111. Lecture 23 (Walker: 10.6, 11.1) Conservation of Energy in Rotation Torque March 30, Kinetic Energy of Rolling Object

Forces of Friction Contact between bodies with a relative velocity produces friction opposite

Check out course website for: Link to practice problems & old/sample exams Link to HW website Lecture notes

REDUCTION OF A SIMPLE DISTRIBUTED LOADING. Today s Objectives: Students will be able to determine an equivalent force for a distributed load.

Lenz s Law (Section 22.5)

Physics 8 Wednesday, October 28, 2015

Review of Lectures 1, 2 and 3

ENGR-1100 Introduction to Engineering Analysis. Lecture 17

EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS

Chapter 3, Problem 28. Agenda. Forces. Contact and Field Forces. Fundamental Forces. External and Internal Forces 2/6/14

Engineering Mechanics Statics

Rotational Mechanics Part II Torque. Pre AP Physics

Equivalent Systems of Forces

ENGR DYNAMICS. Rigid-body Lecture 4. Relative motion analysis: acceleration. Acknowledgements

FE Sta'cs Review. Torch Ellio0 (801) MCE room 2016 (through 2000B door)

Physics 8 Wednesday, October 25, 2017

Welcome back to PHYS 3305

Transcription:

ENGR-1100 Introduction to Engineering Analysis Lecture 9

MOMENT OF A FORCE (SCALAR FORMULATION), CROSS PRODUCT, MOMENT OF A FORCE (VECTOR FORMULATION), & PRINCIPLE OF MOMENTS Today s Objectives : Students will be able to: a) understand and define moment, and, b) determine moments of a force in 2-D and 3-D cases. In-Class Activities : Reading Quiz Applications Moment in 2-D Moment in 3-D Concept Quiz Group Problem Solving Attention Quiz

APPLICATIONS Beams are often used to bridge gaps in walls. We have to know what the effect of the force on the beam will have on the supports of the beam. What do you think is happening at points A and B?

APPLICATIONS (continued) Carpenters often use a hammer in this way to pull a stubborn nail. Through what sort of action does the force F H at the handle pull the nail? How can you mathematically model the effect of force F H at point O?

MOMENT OF A FORCE - SCALAR FORMULATION (Section 4.1) The moment of a force about a point provides a measure of the tendency for rotation (sometimes called a torque).

MOMENT OF A FORCE - SCALAR FORMULATION (continued) In a 2-D case, the magnitude of the moment is M o = F d As shown, d is the perpendicular distance from point O to the line of action of the force. In 2-D, the direction of M O is either clockwise (CW) or counter-clockwise (CCW), depending on the tendency for rotation.

MOMENT OF A FORCE - SCALAR FORMULATION (continued) a F For example, M O = F d and the b direction is counter-clockwise. O d Often it is easier to determine M O by using the components of F as shown. Then M O = (F Y a) (F X b). Note the different signs on the terms! The typical sign convention for a moment in 2-D is that counterclockwise is considered positive. We can determine the direction of rotation by imagining the body pinned at O and deciding which way the body would rotate because of the force. b O a F y F F x

VECTOR CROSS PRODUCT (Section 4.2) While finding the moment of a force in 2-D is straightforward when you know the perpendicular distance d, finding the perpendicular distances can be hard especially when you are working with forces in three dimensions. So a more general approach to finding the moment of a force exists. This more general approach is usually used when dealing with three dimensional forces but can be used in the two dimensional case as well. This more general method of finding the moment of a force uses a vector operation called the cross product of two vectors.

CROSS PRODUCT (Section 4.2) In general, the cross product of two vectors A and B results in another vector, C, i.e., C = A B. The magnitude and direction of the resulting vector can be written as C = A B = A B sin u C As shown, u C is the unit vector perpendicular to both A and B vectors (or to the plane containing the A and B vectors).

CROSS PRODUCT (continued) The right-hand rule is a useful tool for determining the direction of the vector resulting from a cross product. For example: i j = k Note that a vector crossed into itself is zero, e.g., i i = 0

CROSS PRODUCT (continued) Also, the cross product can be written as a determinant. Each component can be determined using 2 2 determinants.

MOMENT OF A FORCE VECTOR FORMULATION (Section 4.3) Moments in 3-D can be calculated using scalar (2-D) approach, but it can be difficult and time consuming. Thus, it is often easier to use a mathematical approach called the vector cross product. Using the vector cross product, M O = r F. Here r is the position vector from point O to any point on the line of action of F.

MOMENT OF A FORCE VECTOR FORMULATION (continued) So, using the cross product, a moment can be expressed as By expanding the above equation using 2 2 determinants (see Section 4.2), we get (sample units are N - m or lb - ft) M O = (r y F Z - r Z F y ) i (r x F z - r z F x ) j + (r x F y - r y F x ) k The physical meaning of the above equation becomes evident by considering the force components separately and using a 2-D formulation.

EXAMPLE I Given: A 100 N force is applied to the frame. Find: The moment of the force at point O. Plan: 1) Resolve the 100 N force along x and y-axes. 2) Determine M O using a scalar analysis for the two force components and then add those two moments together..

EXAMPLE I (continued) Solution + F y = 100 (3/5) N + F x = 100 (4/5) N + M O = { 100 (3/5)N (5 m) (100)(4/5)N (2 m)} N m = 460 N m or 460 N m CW

EXAMPLE II Given: F 1 ={100 i - 120 j + 75 k}lb F 2 ={-200 i +250 j + 100 k}lb o Find: Plan: Resultant moment by the forces about point O. 1) Find F = F 1 + F 2 and r OA. 2) Determine M O = r OA F.

Solution: EXAMPLE II (continued) First, find the resultant force vector F F = F 1 + F 2 = { (100-200) i + (-120 + 250) j + (75 + 100) k} lb = {-100 i +130 j + 175 k} lb Find the position vector r OA r OA = {4 i + 5 j + 3 k} ft Then find the moment by using the vector cross product. i j k 4 5 3-100 130 175 M O = = [{5(175) 3(130)} i {4(175) 3(-100)} j + {4(130) 5(-100)} k] ft lb = {485 i 1000 j + 1020 k} ft lb

READING QUIZ 1. What is the moment of the 12 N force about point A (M A )? F = 12 N A) 3 N m B) 36 N m C) 12 N m D) (12/3) N m E) 7 N m A d = 3 m 2. The moment of force F about point O is defined as M O =. A) r x F B) F x r C) r F D) r * F

CONCEPT QUIZ 1. If a force of magnitude F can be applied in four different 2-D configurations (P,Q,R, & S), select the cases resulting in the maximum and minimum torque values on the nut. (Max, Min). A) (Q, P) B) (R, S) C) (P, R) D) (Q, S) P Q S R

y GROUP PROBLEM SOLVING I x Given: A 20 lb force is applied to the hammer. Find: Plan: The moment of the force at A. Since this is a 2-D problem: 1) Resolve the 20 lb force along the handle s x and y axes. 2) Determine M A using a scalar analysis.

y GROUP PROBLEM SOLVING I (continued) x Solution: + F y = 20 sin 30 lb + F x = 20 cos 30 lb + M A = { (20 cos 30 )lb (18 in) (20 sin 30 )lb (5 in)} = 361.77 lb in = 362 lb in (clockwise or CW)

GROUP PROBLEM SOLVING II Given: The force and geometry shown. Find: Moment of F about point A Plan: 1) Find F and r AC. 2) Determine M A = r AC F

GROUP PROBLEM SOLVING II (continued) Solution: F ={ (80 cos30) sin 40 i + (80 cos30) cos 40 j 80 sin30 k} N ={44.53 i + 53.07 j 40 k } N r AC ={0.55 i + 0.4 j 0.2 k } m Find the moment by using the cross product. M A = i j k 0.55 0.4 0.2 44.53 53.07 40 = { -5.39 i + 13.1 j +11.4 k } N m

ATTENTION QUIZ 10 N 3 m P 2 m 5 N 1. Using the CCW direction as positive, the net moment of the two forces about point P is A) 10 N m B) 20 N m C) - 20 N m D) 40 N m E) - 40 N m 2. If r = { 5 j } m and F = { 10 k } N, the moment r x F equals { } N m. A) 50 i B) 50 j C) 50 i D) 50 j E) 0