Sample Problem 3.5 A cube is acted on by a force P as shown. Determine the moment of P about A about the edge AB and about the diagonal AG of the cube.

Slides:



Advertisements
Similar presentations
ENGR-1100 Introduction to Engineering Analysis
Advertisements

KULIAH IV MEKANIKA TEKNIK MOMEN GAYA & KOPEL
Rigid Bodies: Equivalent Systems of Forces
Shawn Kenny, Ph.D., P.Eng. Assistant Professor Faculty of Engineering and Applied Science Memorial University of Newfoundland ENGI.
Chapter 2 Resultant of Coplannar Force Systems
Moment of a Force Objects External Effects a particle translation
ME221Lecture 61 ME221 Statics LECTURE # 6 Sections 3.6 – 3.9.
RESULTANTS.
4.6 Moment due to Force Couples
Chapter 3: Force System Resultants
Licensed Electrical & Mechanical Engineer
RESULTANTS.
Engineering Mechanics: Statics
Moment of a force The moment of a force about a point or axis provides a measure of the tendency of the force to cause a body to rotate about the point.
Slide #: 1 Chapter 3 Rigid Bodies : Equivalent Systems of Forces.
An-Najah National University College of Engineering
The Wrench: Let’s suppose that we have already reduced a complicated force system to single (resultant ) force,, and a single couple with the moment,,
In the study of the equilibrium of rigid bodies, i.e. the situation when the external forces acting on a rigid body form a system equivalent to zero, we.
Bellringer Compare and explain in complete sentences and formulas how using the Newton’s three laws of motion find the resultant force.
Chapter 3 Rigid Bodies : Equivalent Systems of Forces Part -2
Overview of Mechanical Engineering for Non-MEs Part 1: Statics 3 Rigid Bodies I: Equivalent Systems of Forces.
RIGID BODIES: EQUIVALENT SYSTEM OF FORCES
4.4 Principles of Moments Also known as Varignon’s Theorem
Equivalent Systems of Forces
College of Engineering CIVE 1150 Summer a = 200mm W = 16Kg*9.8m/s 2 W = 156.9N Find tension in each of the three cords.
1 The scalar product or dot product between two vectors P and Q is defined as Scalar products: -are commutative, -are distributive, -are not associative,
Cont. ERT 146 Engineering Mechanics STATIC. 4.4 Principles of Moments Also known as Varignon ’ s Theorem “ Moment of a force about a point is equal to.
Moment in 3D.
Moment. In addition to the tendency to move a body in the direction of its application, a force can also tend to rotate a body about an axis. The axis.
Lecture #6 Moments, Couples, and Force Couple Systems.
MEC 0011 Statics Lecture 4 Prof. Sanghee Kim Fall_ 2012.
Force System Resultants 4 Engineering Mechanics: Statics in SI Units, 12e Copyright © 2010 Pearson Education South Asia Pte Ltd.
MEC 0011 Statics Lecture 4 Prof. Sanghee Kim Fall_ 2012.
Copyright © 2010 Pearson Education South Asia Pte Ltd
Dr. Baljeet Singh Department of Mathematics
Introduction Treatment of a body as a single particle is not always possible. In general, the size of the body and the specific points of application.
Licensed Electrical & Mechanical Engineer
Introduction Treatment of a body as a single particle is not always possible. In general, the size of the body and the specific points of application.
GOVERNMENT ENGINEERING COLLEGE, DAHOD CIVIL ENGINEERING DEPARTMENT
Rigid Bodies: Equivalent Systems of Forces
Sample Problem 3.6 Alternatively, compute the sum of the moments of the four forces about D. Only the forces at C and E contribute to the moment about.
Sample Problem 3.1 e) Although each of the forces in parts b), c), and d) produces the same moment as the 100 lb force, none are of the same magnitude.
SUB:-MOS ( ) Guided By:- Prof. Megha Patel.
ES2501: Statics/Unit 8-1: Moment of Force (2D cases)
Sakalchand Patel College
Chp 4: Moment Mathematics
Moments of the forces Mo = F x d A moment is a turning force.
Lecture 4.
X, Y axis (Horizontal & Vertical) Triangle Force (Sine Law)
Copyright © 2010 Pearson Education South Asia Pte Ltd
Chapter 4 EQUILIBRIUM OF RIGID BODIES
Lecture# 12: Rigid Bodies
MOMENT OF A FORCE ABOUT A POINT
The moment of F about O is defined as
STATICS (ENGINEERING MECHANICS-I)
Statics Course Code: CIVL211 Dr. Aeid A. Abdulrazeg
Chapter Objectives Concept of moment of a force in two and three dimensions Method for finding the moment of a force about a specified axis. Define the.
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
KNUS&T Kumasi-Ghana Instructor: Dr. Joshua Ampofo
ENGINEERING MECHANICS
Students will be able to a) define a couple, and,
Moment of a Force.
Moment of a Force.
Moment of a Force.
Bölüm 4 Rijit Cisimlerin Dengesi
Force-Couple Systems.
CE Statics Lecture 13.
Presentation transcript:

Sample Problem 3.5 A cube is acted on by a force P as shown. Determine the moment of P about A about the edge AB and about the diagonal AG of the cube. Determine the perpendicular distance between AG and FC. 3 - 1

Sample Problem 3.5 Moment of P about A, List an alternative to the position vector , and discuss your answer with a neighbor. Moment of P about AB, 3 - 2

Sample Problem 3.5 Moment of P about the diagonal AG, What if, for , you had chosen instead? How would that change the answer? 3 - 3

Sample Problem 3.5 Perpendicular distance between AG and FC, Therefore, P is perpendicular to AG. 3 - 4

Moment of a Couple Two forces F and -F having the same magnitude, parallel lines of action, and opposite sense are said to form a couple. Moment of the couple, The moment vector of the couple is independent of the choice of the origin of the coordinate axes, i.e., it is a free vector that can be applied at any point with the same effect. 3 - 5

Moment of a Couple Two couples will have equal moments if the two couples lie in parallel planes, and the two couples have the same sense or the tendency to cause rotation in the same direction. 3 - 6

Addition of Couples Consider two intersecting planes P1 and P2 with each containing a couple Resultants of the vectors also form a couple Sum of two couples is also a couple that is equal to the vector sum of the two couples By Varignon’s theorem 3 - 7

Couples Can Be Represented by Vectors A couple can be represented by a vector with magnitude and direction equal to the moment of the couple. Couple vectors obey the law of addition of vectors. Couple vectors are free vectors, i.e., there is no point of application – it simply acts on the body. Couple vectors may be resolved into component vectors. 3 - 8

Resolution of a Force Into a Force at O and a Couple Force vector F can not be simply moved to O without modifying its action on the body. Attaching equal and opposite force vectors at O produces no net effect on the body. The three forces may be replaced by an equivalent force vector and couple vector, i.e, a force-couple system. 3 - 9

Resolution of a Force Into a Force at O and a Couple Moving F from A to a different point O’ requires the addition of a different couple vector MO’ The moments of F about O and O’ are related, Moving the force-couple system from O to O’ requires the addition of the moment of the force at O about O’. 3 - 10

Sample Problem 3.6 SOLUTION: Attach equal and opposite 20 lb forces in the ±x direction at A, thereby producing 3 couples for which the moment components are easily computed. Alternatively, compute the sum of the moments of the four forces about an arbitrary single point. The point D is a good choice as only two of the forces will produce non-zero moment contributions.. Determine the components of the single couple equivalent to the couples shown. 3 - 11

Sample Problem 3.6 Attach equal and opposite 20 lb forces in the ±x direction at A The three couples may be represented by three couple vectors, 3 - 12