Statics. Introductions Review Course Outline and Class Schedule Course Expectations Chapter 1

Similar documents
Statics. Today Introductions Review Course Outline and Class Schedule Course Expectations Chapter 1 ENGR 1205 ENGR 1205

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati

Introduction to Engineering Mechanics

Fundamental Principles

CE 201 Statics. 2 Physical Sciences. Rigid-Body Deformable-Body Fluid Mechanics Mechanics Mechanics

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

MECHANICS. Prepared by Engr. John Paul Timola

MECHANICS, UNITS, NUMERICAL CALCULATIONS & GENERAL PROCEDURE FOR ANALYSIS

Physics 2A Chapters 4 & 5 - Newton s Laws of Motion Fall Newton s Second Law, F = ma, is the only new equation for Chapter 4 and 5.

ARC241 Structural Analysis I Lecture 1, Sections ST1.1 ST2.4

Tenth Edition STATICS 1 Ferdinand P. Beer E. Russell Johnston, Jr. David F. Mazurek Lecture Notes: John Chen California Polytechnic State University

Physics 141 Dynamics 1 Page 1. Dynamics 1

STATICS. Introduction Lecture Notes: J. Walt Oler Texas Tech University. Vector Mechanics for Engineers: Statics VECTOR MECHANICS FOR ENGINEERS:

General Physics I, Spring Vectors

CHAPTER 1 INTRODUCTION

PHYSICS - CLUTCH CH 01: UNITS & VECTORS.

Forces. A force is a push or a pull on an object

two forces and moments Structural Math Physics for Structures Structural Math

1). To introduce and define the subject of mechanics. 2). To introduce Newton's Laws, and to understand the significance of these laws.

ME 201 Engineering Mechanics: Statics. Unit 1.1 Mechanics Fundamentals Newton s Laws of Motion Units

Chapter 5 Newton s Laws of Motion

Unit 3: Force and Laws of Motion

Quiz No. 1: Tuesday Jan. 31. Assignment No. 2, due Thursday Feb 2: Problems 8.4, 8.13, 3.10, 3.28 Conceptual questions: 8.1, 3.6, 3.12, 3.

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Vectors 1. The METRIC Project, Imperial College. Imperial College of Science Technology and Medicine, 1996.

General Physics (PHY 2130)

Chapter 2: Statics of Particles

Newton s Laws Review

Introduction to Engineering Mechanics

Physics 2514 Lecture 2

Chapter 4. The Laws of Motion. Dr. Armen Kocharian

Chapter 3. Vectors and. Two-Dimensional Motion Vector vs. Scalar Review

Chapter 4 Dynamics: Newton s Laws of Motion

You know the drill: Turn in hw Pick up graded hw Name tags up Grab white boards and markers for your group

Chapter 4. The Laws of Motion

Physics General Physics. Lecture 3 Newtonian Mechanics. Fall 2016 Semester. Prof. Matthew Jones

VECTORS. Given two vectors! and! we can express the law of vector addition geometrically. + = Fig. 1 Geometrical definition of vector addition

FORCE TABLE INTRODUCTION

POGIL: Newton s First Law of Motion and Statics. Part 1: Net Force Model: Read the following carefully and study the diagrams that follow.

Physics 1A Lecture 4B. "Fig Newton: The force required to accelerate a fig inches per second. --J. Hart

Mathematical review trigonometry vectors Motion in one dimension

Chapter 4 Dynamics: Newton s Laws of Motion

Newton s Law of Motion

Mechanics of Material 11/29/2017. General Information

If there is nothing pushing on an object, it will not move. If there is nothing pushing on an object, it will not stop. The List:

Vectors and Equilibrium Lecture 3

AP Physics 1 Summer Assignment

Chapter 2. Forces & Newton s Laws

Teacher Content Brief

The Essentials to the Mathematical world

Force Vectors and Static Equilibrium

Main topics for the First Midterm Exam

FORCES. Force. Combining Forces

AP Physics Math Review Packet

DISPLACEMENT AND FORCE IN TWO DIMENSIONS

INTRODUCTION AND KINEMATICS. Physics Unit 1 Chapters 1-3

Monday, September 22 nd

Vector Basics, with Exercises

MITOCW ocw-18_02-f07-lec02_220k

Statics and Mechanics of Materials

*Definition of Mechanics *Basic Concepts *Newton s Laws *Units

Physics 121 for Majors

Newton s Law of Motion

Review of Lectures 1, 2 and 3

Force a push or a pull exerted on some object the cause of an acceleration, or the change in an objects velocity

The History of Motion. Ms. Thibodeau

Dynamics: Newton s Laws of Motion

CHAPTER 2. FORCE and Motion. CHAPTER s Objectives

1.1 WHAT IS MECHANICS?

Vectors Part 1: Two Dimensions

Part I: Mechanics. Chapter 2 Inertia & Newton s First Law of Motion. Aristotle & Galileo. Lecture 2

ME101: Engineering Mechanics ( )

Unit 1: Equilibrium and Center of Mass

Newton s Laws of Motion

Section 8: 8: Statics Statics - Basics 8-1

NEWTON S LAWS OF MOTION (EQUATION OF MOTION) (Sections )

Chapter 5. The Laws of Motion

A N D. c h a p t e r 1 2 M O T I O N F O R C E S

Clickers Registration Roll Call

(arrows denote positive direction)

Announcements. Atom Energy Levels

Physics Chapter 3 Notes. Section 3-1: Introduction to Vectors (pages 80-83)

ADVANCED PLACEMENT PHYSICS 1

THE LAWS OF MOTION. Mr. Banks 7 th Grade Science

Vectors a vector is a quantity that has both a magnitude (size) and a direction

Forces and Motion. Holt Book Chapter 4

ENGINEERING MECHANICS STATIC. Mechanic s is the oldest of the physical sciences which deals with the effects of forces on objects.

Today. Clickers Registration Roll Call. Announcements: Loose ends from lecture 2 Law of Inertia (Newton s 1st Law) What is Force?

Newton s Laws. A force is simply a push or a pull. Forces are vectors; they have both size and direction.

Physics Knowledge Organiser P8 - Forces in balance

Physics 141 Energy 1 Page 1. Energy 1

Newton s Laws and Free-Body Diagrams General Physics I

Chapter 5. Force and Motion I

Engineering Mechanics I. Phongsaen PITAKWATCHARA

Module 3: Cartesian Coordinates and Vectors

A. Incorrect. Solve for a variable on the bottom by first moving it to the top. D. Incorrect. This answer has too many significant figures.

Lab: Vectors. You are required to finish this section before coming to the lab. It will be checked by one of the lab instructors when the lab begins.

Chapter 5. The Laws of Motion

Vector components and motion

Goals: Equipment: Introduction:

Transcription:

Statics ENGR 1205 Kaitlin Ford kford@mtroyal.ca B175 Today Introductions Review Course Outline and Class Schedule Course Expectations Chapter 1 1 Review the Course Outline and Class Schedule Go through Handout Also posted on Blackboard Course Format 2 1

Lectures fill-in-the-blank notes posted on Blackboard Read the text and try to fill them in before class I will use the completed slides during lectures (I will not post the completed slides) Tutorials will happen whenever Time for YOU to practice (with help) Assignments Due every Thursday We will mark 2 questions in class (one self 25%, one peer-25%) I will mark one other question (50% of the mark) Quizzes on Tuesdays format will vary 3 My Expectations fair, but I expect a lot tough course, work hard or else need to fairly good at math and physics (vectors) bring text to class read the textbook do all assigned homework 4 2

Keep up with the material. Review math fundamentals. (vectors, trig) Devise and practice problem-solving techniques. Do the recommended practice problems and understand them (don t try to memorize!) Participate. 5 Ask questions WRONG WAY I don t know how to do this question. RIGHT WAY I tried this problem and I think this part is correct, but I m not sure about the next step because 6 3

Leave your cell phone on during class. Request more marks on an assignment when you haven t figured out what you did wrong yet. Send me an e-mail saying I wasn t in class. What did I miss? Fall behind (stay healthy, etc.) 7 the goal of this course is to develop your ability to analyze and solve basic problems we will use vector analysis We will solve two-dimensional (2D) and threedimensional (3D) problems we will use SI units 8 4

Mechanics is a branch of the physical sciences that is concerned with the motion of bodies that are subjected to the action of FORCES (including statics - the special case in which bodies remain at rest) The general principles were first enunciated by Sir Isaac Newton in his Philosophiae Naturalis Principia Mathematica (1687), commonly known as the Principia 9 Mechanics can be subdivided into 3 parts... 1) Rigid Body Mechanics (generally an unrealistic portrayal of situations) - statics (rest) ΣF = 0 (a = 0), ΣM = 0 - dynamics (motion) ΣF 0 (a 0) 2) Deformable-Body Mechanics - includes the mechanics of materials 3) Fluid Mechanics - study of gas and liquids Mechanics is an applied physical science and a key foundation in the engineering sciences 10 5

Historical Development Aristotle Archimedes Galileo NEWTON Euler, d Alembert, Lagrange, g Hamilton then Einstein (quantum or relativistic mechanics) 4 Basic Quantities in Mechanics: SPACE - the position of a point given in terms of three coordinates (x, y, z) measured from a reference point or origin TIME necessary to define an event in addition to spatial coordinates MASS - characterizes and compares bodies e.g. 2 bodies of the same mass are attracted the same amount by the Earth and offer the same resistance to a change in their state of motion 11 The Fourth Basic Quantity is: FORCE a push or pull ; the action of one body on another, either by contact or at a distance (characterized by a point of application, a magnitude, a sense and a line of action; it s a vector) The first 3 quantities are absolute concepts, independent of each other (in Newtonian mechanics) Force is not an independent quantity. It is related to the mass of the body and the variation of its velocity with time (acceleration). d v t F ma m m t t 12 6

We ll study PARTICLES and RIGID BODIES (RB) PARTICLES small amounts of matter occupying one point in space, have mass but size is ignored RIGID BODIES combinations of particles occupying fixed positions in space with respect to one another, positions don t change with added force 13 Scalar quantities those which have only a magnitude Examples: time volume density speed mass Vector quantities those which have magnitude and direction and obey the parallelogram l law of addition i Examples: displacement velocity force 14 7

Free vector one whose action is not confined to or associated with a unique line in space Examples: displacement of a rigid body which is moving without rotation; force couple Sliding vector has a unique line of action in space but not a unique point of application Example: external force on a rigid body Fixed vector a unique point of application is specified Example: force on a deformable body 15 Represent vectors with a representative letter with an arrow above it. E.g. F (or be consistent) For magnitude of vectors, use absolute value notation. E.g. F equal vectors have the same magnitude and direction (but maybe not the same point of application) a negative vector simply has the opposite sense of its positive P P 0 16 8

the parallelogram law for the addition of vectors: the resultant sum of two vectors is the diagonal of the parallelogram formed using the two vectors as adjacent sides 17 parallelogram law note that, in general, P Q P Q since P+ Q= Q+ P (from the parallelogram law), we can conclude that vector addition is commutative R Or, use the triangle rule (arrange vectors tip to tail) and resultant goes from first tail to last tip Find R with scale diagram R Find R using geometry (trigonometry) 18 9

BASIC TRIGONOMETRY RATIOS (for right angle triangles): SINE LAW: COSINE LAW: 19 subtraction is the addition of a negative sense vector e.g. - = + = to sum 3 or more coplanar vectors, add the first and second, and then keep adding one vector at a time (repetitively applying the triangle rule) i.e. P Q S P Q S P Q S i e vector addition is associative (grouping doesn t matter) 20 10

OR, apply the tip to tail method in one fast step this extension of the parallelogram law is called the polygon rule e.g. P P 2P such that the direction of 2P is the direction of P and the magnitude of is 2P 2 P For kp, the direction of kp is the same as P if k>0 and it s the opposite of P if k<0, while the magnitude is always kp 21 Vectors can be mathematically represented in two ways: Rectangular components - a sum of vectors along perpendicular axes - generally along x, y, z axes Magnitude and direction - direction in reference to some origin 22 11

Newton s First Law: if ΣF = 0, a body stays at rest or doesn t accelerate (constant velocity or constant speed with unchanging direction) 23 Newton s Second Law: if ΣF 0, F = ma The acceleration of a particle is proportional to the vector sum of the forces acting on it, and is in the same direction of this vector sum. 24 12

Newton s Third Law: the forces of action and reaction between interacting bodies are equal in magnitude and opposite in direction (same line of action, but opposite sense) 25 We will use S.I. Units (Système International d Unités) SI units are absolute i.e. they mean the same thing everywhere The base units are length (m), mass (kg) and time (s). the 3 are independent units, defined arbitrarily Force (newtons, N) is a derived unit Defined as the force that gives an acceleration of 1 m/s 2 to a mass of 1 kg. N = kg*m/s 2 (F = ma = kg (m/s 2 )) 26 13

know metric prefixes (m, µ, n) and (k, M, G) for time: s, min, hr for area: m 2 (1 m x 1 m) for volume: m 3 (1 m x 1 m x 1 m) -for liquids, dm 3 = 1 L note the SI unit conversions in front cover of text note 200 000 has no comma since commas mean decimal points in Europe 27 Mm F G r Newton s Law of Gravitation: 2 where: F = the Force exerted by one object (M) on another (m) G = the universal gravitational constant r = the distance between the masses The Force of Gravitation exerted by the Earth on an object (at the surface) is: M W mg g G r earth, 2 earth g varies by location on the Earth we will use g = 9.81 m/s 2 28 14

The mathematical formulation of a physical problem represents an ideal description, or model, which approximates but never quite matches the actual physical condition. Examples of assumptions/simplifications: neglect small distances, angles, and forces Rigid bodies, force distribution area 29 The accuracy of a solution depends on: accuracy of the given data, and accuracy of the computations performed. The solution cannot be more accurate than the less accurate (worst) of these two. The use of calculators generally makes the accuracy of the computations much greater than the accuracy of the data. Hence, the solution accuracy is usually limited by the data accuracy. e.g. given 75 000 ± 100 N ± 0.13% so an answer of 14 322 N, is really 14 322 ± 20 N 30 15

As a general rule for engineering problems, the data are seldom known with an accuracy greater than 0.2%. As a practical rule, use 4 significant digits if the lead digit is 1 and 3 significant digits, e.g. 27.0 and 15.00 DON T WRITE DOWN EVERY DIGIT YOUR CALCULATOR GIVES YOU! 31 The ability to clearly communicate a solution is vital Your solutions must be clear (presentation, layout, handwriting, logical progression) as well as complete and correct Include (mandatory minimum): Problem Statement: Includes given data, specification of what is to be determined, and a figure showing all quantities involved. Free-Body Diagrams: Create separate diagrams for each of the bodies involved with a clear indication of all forces acting on each body. 32 16

Fundamental Principles: Newton s Laws (and relevant equations) are applied to express the conditions of rest or motion of each body. The rules of algebra are applied to solve the equations for the unknown quantities. Could be an equation or a statement. Solution Check: -Test for errors in reasoning by verifying that the units of the computed results are correct, -test for errors in computation by substituting i given data and computed results into previously unused equations based on the six principles, -always apply experience and physical intuition to assess whether results seem reasonable. 33 The screw is subjected to two forces F 1 and F 2. Determine the magnitude and direction of the resultant force. a) Using a scale diagram b) Using trigonometry c) Using components 10 o F 2 = 150 N 15 o F 1 = 100 N 34 17

35 18