chapter general principles - assakkaf 302/lectures/chapter0a.pdf · 4 chapter 1. general principles...

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1 •College of Engineering •Department of Mechanical Engineering Tenth Edition CHAPTER 1 Engineering Mechanics: Statics GENERAL PRINCIPLES by Dr. Ibrahim A. Assakkaf SPRING 2007 ENES 110 – Statics Department of Mechanical Engineering University of Maryland Baltimore County Slide No. 1 Chapter 1. GENERAL PRINCIPLES ENES110 ©Assakkaf_SP07 Statics, Units, Calculations & problem Solving Students will be able to: – Use Law of Sines and Cosines – Solve system of simultaneous equations – Round the final answer appropriately

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Page 1: CHAPTER GENERAL PRINCIPLES - assakkaf 302/Lectures/Chapter0a.pdf · 4 Chapter 1. GENERAL PRINCIPLES Slide No. 6 ENES110 ©Assakkaf_SP07 Rigid-Body Mechanics Statics – Deals with

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•College of Engineering •Department of Mechanical Engineering

Tenth EditionCHAPTER

1

Engineering Mechanics: Statics

GENERAL PRINCIPLES

byDr. Ibrahim A. Assakkaf

SPRING 2007ENES 110 – Statics

Department of Mechanical EngineeringUniversity of Maryland Baltimore County

Slide No. 1Chapter 1. GENERAL PRINCIPLES

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Statics, Units, Calculations & problem Solving

Students will be able to:– Use Law of Sines and Cosines– Solve system of simultaneous equations– Round the final answer appropriately

Page 2: CHAPTER GENERAL PRINCIPLES - assakkaf 302/Lectures/Chapter0a.pdf · 4 Chapter 1. GENERAL PRINCIPLES Slide No. 6 ENES110 ©Assakkaf_SP07 Rigid-Body Mechanics Statics – Deals with

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Slide No. 2Chapter 1. GENERAL PRINCIPLES

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Mechanics

Mechanics can be defined as that branchof the physical sciences concerned withthe state of rest or motion of bodies thatare subjected to the action of forces.

Slide No. 3Chapter 1. GENERAL PRINCIPLES

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Mechanics

Page 3: CHAPTER GENERAL PRINCIPLES - assakkaf 302/Lectures/Chapter0a.pdf · 4 Chapter 1. GENERAL PRINCIPLES Slide No. 6 ENES110 ©Assakkaf_SP07 Rigid-Body Mechanics Statics – Deals with

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Slide No. 4Chapter 1. GENERAL PRINCIPLES

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Mechanics

Slide No. 5Chapter 1. GENERAL PRINCIPLES

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MechanicsWHAT MAY HAPPEN IF STATICS IS NOT

APPLIED PROPERLY?

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Slide No. 6Chapter 1. GENERAL PRINCIPLES

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Rigid-Body Mechanics

Statics– Deals with the equilibrium of bodies, that is,

those that are either at rest or move with a constant velocity.

Dynamics– Is concerned with the accelerated motion of

bodies.

Slide No. 7Chapter 1. GENERAL PRINCIPLES

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Fundamental Concepts

Basic Quantities– Length (m, ft)– Time (h, s, min)– Mass (Kg, slug)– Force (N, lb)

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Slide No. 8Chapter 1. GENERAL PRINCIPLES

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Fundamental ConceptsIdealization– Particle

• A particle has a mass but a size that can be neglected.

– Rigid Body• A rigid body can be considered as a combination

of a large umber of particles in which all the particles remain at fixed distance from one another both before and after applying a load.

– Concentrated Force• Represents the effect of a loading which is

assumed to act at a point on a body.

Slide No. 9Chapter 1. GENERAL PRINCIPLES

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Fundamental Concepts

Newton’s Three Laws of Motion– First Law

• A particle originally at rest, or moving in a straight line with constant velocity, will remain in this state.

– Second Law• A particle acted upon by an unbalanced force F

experiences an acceleration a that has the same direction as the force and a magnitude that is directly proportional to the force.

aF m= (1-1)

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Slide No. 10Chapter 1. GENERAL PRINCIPLES

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Fundamental Concepts

Newton’s Three Laws of Motion (cont’d)– Third Law

• The mutual forces of action and reaction between two particles are equal, opposite, and collinear.

Slide No. 11Chapter 1. GENERAL PRINCIPLES

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Fundamental Concepts

Newton’s Law of Gravitational Attraction

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rmmGF = (1-2)

F = force of gravitation between the two particlesG = universal constant of gravitation (= 66.73 × 10-12 m3/kg⋅s2)

m1 m2 = mass of each of the particlesr = distance between the two particles

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Slide No. 12Chapter 1. GENERAL PRINCIPLES

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Fundamental Concepts

Newton’s Law of Gravitational Attraction– Weight

• The weight of a particle having a mass m1 = m ( assuming that the mass of the earth m2 = Me) can be given as

• Or

• where

2rmMGFW e==

mgW =

2rMGg e=

(1-3)

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Units of Measurements

SI Units– The international System of Units,

abbreviated SI after French “System International d’Unites.”

– The unit of force F or W is called newton (N).– It is derived from F = ma.– Thus

)m/s 9.81( 2== gmgW (1-4)

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Slide No. 14Chapter 1. GENERAL PRINCIPLES

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Units of Measurements

U.S. Customary Units– In the U.S. Customary systems of units (FPS)

length is measured in feet (ft), force in pounds (lb), and time in seconds (s).

– The unit of mass is called slug.– It is derived from F = ma.– Therefore,

)ft/s 32.2( 2== gg

Wm (1-5)

Slide No. 15Chapter 1. GENERAL PRINCIPLES

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Units of Measurements

System of Units

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Slide No. 16Chapter 1. GENERAL PRINCIPLES

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Units of MeasurementsConversion of Units– In FPS system,

• 1 ft = 12 in. (inches)• 5280 ft = 1 mi (mile)• 1000 lb = 1 kip (kilo-pound)• 2000 lb = 1 ton

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Units of Measurements

Prefixes

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Slide No. 18Chapter 1. GENERAL PRINCIPLES

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Units of Measurements

International System of Units (SI)– No Plurals (e.g., m = 5 kg not kgs )– Separate Units with a • (e.g., meter second = m • s )– Most symbols are in lowercase.– Some exceptions are N, Pa, M and G.– Exponential powers apply to units, e.g., cm • cm = cm2

– Compound prefixes should not be used.– Other rules are given in your textbook

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Numerical Calculations

Must have dimensional “homogeneity.”Dimensions have to be the same on both sides of the equal sign, (e.g. distance = speed × time.)Use an appropriate number of significant figures (3 for answer, at least 4 for intermediate calculations). Why?

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Slide No. 20Chapter 1. GENERAL PRINCIPLES

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Numerical Calculations

Be consistent when rounding off– greater than or equal to 5, round up (3528 →

3530).– smaller than 5, round down (0.03521 →

0.0352).

Slide No. 21Chapter 1. GENERAL PRINCIPLES

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Numerical CalculationsExample 1

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Slide No. 22Chapter 1. GENERAL PRINCIPLES

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Numerical CalculationsExample 2

Slide No. 23Chapter 1. GENERAL PRINCIPLES

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Numerical CalculationsExample 3

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Numerical Calculations

Example 3 (cont’d)

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Numerical CalculationsExample 3 (cont’d)

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Slide No. 26Chapter 1. GENERAL PRINCIPLES

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Law of Sines and Cosines

Law of Sines

A

B

C

α

β

γ

sin(α)A

sin(β)B

sin(γ)C

= =

C = A2 + B2 -2ABcos(γ)

Law of Cosines

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Properties of Right Triangles

A

B

C

α

β

Remember – SOH-CAH-TOAsin is opposite/hypotenuse, cosine is adjacent/hypotenuse, and tangent is opposite/adjacent.

sin(α) = AC

cos(α) = BC

tan(α) = AB

A2 + B2 = C2 (Pythagorean Theorem)

cos(β) = AC

sin(β) = BC

tan(β) = BA

Hypotenuse

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Slide No. 28Chapter 1. GENERAL PRINCIPLES

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Simultaneous EquationsMost calculators can do this or can be programmed to do this.Many different methods available.Beyond scope of class – examples in text.