ENGINEERING MECHANICS

Slides:



Advertisements
Similar presentations
Calculating the “actual” internal force in truss bridge members
Advertisements

PHYS 218 sec Review Chap. 4 Newton’s laws of motion.
Physics Montwood High School R. Casao
Rotational Equilibrium and Rotational Dynamics
Introduction to Statics
Rotational Equilibrium and Rotational Dynamics
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Rotational Dynamics Chapter 9.
Torque and Rotational Equilibrium
ME 221 Statics (Angel). ME221Lecture 22 Vectors; Vector Addition Define scalars and vectors Vector addition, scalar multiplication 2-D.
Solution of Simultaneous Linear Equations (AX=B)
Chapter 2 Statics of Particles
Copyright © 2010 Pearson Education South Asia Pte Ltd
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Newton’s First Law Mathematical Statement of Newton’s 1st Law:
Physics Chapter 4: Forces and the Laws of Motion
ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS
Chapter 4 Preview Objectives Force Force Diagrams
Rotational Equilibrium and Rotational Dynamics
NEWTON’S FIRST LAW Definition- An object at rest will remain at rest, or if it is moving, it will continue to move with constant velocity, unless acted.
Fundamental Concepts and Principles
Overview of Mechanical Engineering for Non-MEs Part 1: Statics 2 Statics of Particles Concurrent Forces.
MAE 242 Dynamics – Section I Dr. Kostas Sierros. Problem.
Engineering Mechanics: Statics Chapter 1 General Principles Chapter 1 General Principles.
CHAPTER 10: TERMINOLOGY AND MEASUREMENT IN BIOMECHANICS
© Houghton Mifflin Harcourt Publishing Company The student is expected to: Chapter 4 Section 1 Changes in Motion TEKS 4E develop and interpret free-body.
1 MPA104 Mechanical Design Engineering Statics Duncan Price IPTME, Loughborough University © Copyright: (2006)
Forces and Newton’s Laws of Motion. 4.1 The Concepts of Force and Mass A force is a push or a pull. Arrows are used to represent forces. The length of.
Copyright © 2010 Pearson Education South Asia Pte Ltd
Copyright © 2015 Chris J Jewell 1 Mechanics M1 (Slide Set 11) Core Mathematics for Mechanics M1 Mechanics M1.
Chapter 4 Forces and Newton’s Laws of Motion. 4.1 The Concepts of Force and Mass A force is a push or a pull. Contact forces arise from physical contact.
Engineering Mechanics: Statics
ENGINEERING STATICS COURSE INTRODUCTION.
Principle of Engineering ENG2301 F Mechanics Section F Textbook: F A Foundation Course in Statics and Dynamics F Addison Wesley Longman 1997.
BB101 ENGINEERING SCIENCE
Chapter 3 Equilibrium of a Particle. 3.1 Condition for the Equilibrium of a Particle o "static equilibrium" is used to describe an object at rest. o To.
Thursday, Oct. 30, 2014PHYS , Fall 2014 Dr. Jaehoon Yu 1 PHYS 1443 – Section 004 Lecture #19 Thursday, Oct. 30, 2014 Dr. Jaehoon Yu Rolling Kinetic.
Chapter 14 Systems of Particles.
General Principles 1 Engineering Mechanics: Statics in SI Units, 12e Copyright © 2010 Pearson Education South Asia Pte Ltd.
MECHANICS Ms. Peace Introduction. Sequence 1.1 What is Mechanics? 1.1 What is Mechanics? 1.2 Fundamental Concepts and Principles 1.2 Fundamental Concepts.
Equilibrium of a Particle 3 Engineering Mechanics: Statics in SI Units, 12e Copyright © 2010 Pearson Education South Asia Pte Ltd.
AP Chapter 4. Force - a push or pull Contact Force – Noncontact Force – mass.
Forces Chapter 6.1. What You Already Learned Velocity is the ratio of the change in position of an object over a period of time. Acceleration describes.
SCALARS & VECTORS. Physical Quantities All those quantities which can be measured are called physical quantities. Physical Quantities can be measured.
Understand the principles of statics Graphical vectors Triangle of forces theorem Parallelogram of forces theorem Concept of equilibrium
ERT 146 Engineering Mechanics Ms Siti Kamariah Md Sa’at School of Bioprocess Engineering, UniMAP
Dr. Baljeet Singh Department of Mathematics
Introduction.
Statics of Particles.
Kinetics of Particles: Newton’s Second Law
Statics of Particles.
Statics of Particles.
Statics of Particles.
CE 102 Statics Chapter 1 Introduction.
Introduction.
Statics of rigid bodies
Statics of Particles.
Static and Dynamic Chapter 1 : Introduction
Introduction.
By : Amit Phogat (lecturer in M.E.)
Introduction.
POWER POINT PRESENTATION OF
Vectors & Equilibrium Sara sultan 07/04/2019.
Statics of Particles.
1. Introduction to Statics
Applying Forces AP Physics 1.
Applying Forces AP Physics C.
Introduction.
CHAPTER 1: INTRODUCTION & STATICS OF PARTICLES
Presentation transcript:

ENGINEERING MECHANICS CHAPTER TOPIC 1 INTRODUCTION AND REVIEW OF MATHEMATICS      2 FORCES AND RESULTANTS 3 MOMENTS AND COUPLES 4 EQUILIBRIUM 5 FRICTION 6     KINEMATICS OF LINEAR & ROTATIONAL MOTION 7 KINETICS OF LINEAR MOTION 8 KINETICS OF ROTATIONAL MOTION Click on VIEW and select SLIDE SHOW to view the presentation. Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 1 of 19 EE31102005

CHAPTER 1 :Introduction And Review of Mathematics Basic mechanics involves the study of two principal areas – statics and dynamics. Statics is the study of forces on objects or bodies which are at rest or moving at a constant velocity, and the forces are in balance, or in static equilibrium. A ball at rest may have several forces acting on it, such as gravitational force (weight) and a force opposing that gravity (reaction). The ball is at rest or static, has forces in balance or EQUILIBRIUM Dynamics is the study of forces on moving bodies, and the forces are in dynamic equilibrium. Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 2 of 19 EE31102005

The concept of applied mechanics is useful when it comes to analyzing stress, designing of machine structures and hydraulics, etc. There are only seven basic units in the SI system but only three are frequently used in statics and dynamics: Physical Quantity Unit Symbol 1. Length meter m 2. Mass kilogram kg 3. Time second s Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 3 of 19 EE31102005

Multiples Submultiples 1 kilogram is 1 kg or 103 g. 1 millimeter is 1 For large or small figures, multiples or submultiples are used. For example: Multiples Submultiples 1 kilogram is 1 kg or 103 g. 1 millimeter is 1 mm or 10-3 m. 1 megagram is 1 Mg or 106 g. 1 micrometer is 1 m or 10-6m. 1 gigagram is 1 Gg or 109g. 1 nanometer is 1 nm or 10-9m. Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 4 of 19 EE31102005

The following SI derived units are frequently used in this course: Force – The unit of force is the newton (N) . 1 newton is the force applied to a 1 kg mass to give it an acceleration of 1 m/s2 (i.e 1 N = 1 kg.m/s2). Or : Force = mass x acceleration = kg x m/s2 = kg m/s2 Hence a 1 kg mass has a force or weight due to gravity, equal to (1 kg x 9.81 m/s2) = 9.81 N, where g = 9.81 m/s2 . Moment – It is the product of a force and its perpendicular distance, and the unit is newton-meter or N-m. Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 5 of 19 EE31102005

Simultaneous equations 1.2 Mathematics Required The followings are the mathematics skills that are important for this module : Quadratic equations Simultaneous equations Trigonometry functions of a right-angle triangle Sine and cosine rules Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 6 of 19 EE31102005

1.2.1 Quadratic Equations The equation has the standard form as follows ax2 + bx + c = 0 (1.1) The standard solution to this equation is x = – b   ( b2 – 4ac) (1.2) 2a Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 7 of 19 EE31102005

Example 1 Solve for x in the equation 5x2 + 12x – 2 = 0. Comparing equation 1.1 above, and substitute a=5, b=12 and c= –2 into equation 1.2, the solution is : X = – 12   [(12)2 – 4(5)( – 2)] 2(5) = – 12  13.56 10 = +0.156 or – 2.56 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 8 of 19 EE31102005

1.2.2 Simultaneous Equation The equation has two unknowns x and y in the form of ax + by + c = 0 (1.3) px + qy + r = 0 (1.4) Example 2 Find the values of x and y satisfying the given equations: 4x + 3y + 10 = 0 (1) 20x + 30y + 5 = 0 (2) There are 2 methods of solving these equations Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 9 of 19 EE31102005

Method of Substitution We can start by expressing x in terms of y, or y in terms of x. Let us choose to express x in terms of y, thus from (1) x = -3y -10 (3) 4 Substituting (3) into (2) , yielding 20( -3y -10) + 30y + 5 = 0 4 -15y -50 + 30y + 5 = 0 15y – 45 = 0 y = 45 = 3 15 To find x, substitute the value of y into (3) x = (-3 x 3 - 10) = -19 4 4 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 10 of 19 EE31102005

Method of Elimination This method looks for a way to eliminate one of the unknowns. This can be done by making the constant factor of that unknown or variable the same in both equations by multiplying or dividing one equation by a selected constant: Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 11 of 19 EE31102005

Substitute the value of y into (1) or (2) 4x + 3(3) + 10 = 0 4x + 3y + 10 = 0 (1) 20x + 30y + 5 = 0 (2) Divide (2) by 5 4x + 6y + 1 = 0 (3) Subtract (3) by (1) 3y - 9 = 0 y = 3 Substitute the value of y into (1) or (2) 4x + 3(3) + 10 = 0 4x = - 9 - 10 x = - 19 4 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 12 of 19 EE31102005

1.2.3 Trigonometry Functions Of A Right-Angle Triangle  sine  = opposite side = o = cosine  (1.5) hypotenuse h cosine  = adjacent side = a = sine  (1.6) tangent  = opposite side = o (1.7) adjacent side a tangent  = sin  cos o  a h  Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 13 of 19 EE31102005

1.2.4 Sine And Cosine Rules For triangles that are not right-angle, the following two laws are important in vector algebra introduced in chapter two later: Cosine Rule a2 = b2 + c2 – 2bc cos  (1.8) b2 = a2 + c2 – 2ac cos  c2 = a2 + b2 – 2ab cos  Sine Rule a = b = c sin  sin  sin  Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 14 of 19 EE31102005

If the cosine rule is applied to a right-angle triangle where  = 90 0 , and applying to equation (1.8), c a 90 0 b i.e. a2 = b2 + c2 – 2bc cos 90 0 since cos 90 0 = 0 a2 = b2 + c2 (Pythagoras Theorem) Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 15 of 19 EE31102005

Example 3 Find the length of the unknown side a and the angle . Cosine rule : a2 = b2+c2-2bccos 200 6m 4m  i.e. a2 = 62+42-2x6x4cos200 = 36 +16-6x4xcos200 = 6.9 a = 2.63m Sine rule : 2.63 = 6 sin 200 sin  a sine  = 6 x sin 200 2.63 = 51.30 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 16 of 19 EE31102005

But we know this to be in the second quadrant, Hence  = 180 – 51 Check : 62 = 2.632 - 42 - 2x2.63x4 cos  cos  = 2.632 + 42 – 62 2x2.63x4 = - 0.634  = 128.6 0 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 17 of 19 EE31102005

1.2.5 Geometry Some of the basic rules are shown below: Sum of supplementary angles = 180 0  +  = 180 0   A straight line intersecting two parallel lines  = ,  =   = ,  =      Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 18 of 19 EE31102005

Similar triangles ABC and ADE, by proportion AB = BC = AC AD DE AE Hence if AB = 6, AD = 3 and BC = 4, Then, 6 = 4 3 DE DE = (3 x 4) 3 = 2 B D A C E End of Chapter 1 Engineering Mechanics – Chapter 1: Introduction & Review of Mathematics Slide 19 of 19 EE31102005