Chapter 12 Static Equilibrium and Elasticity. Introduction Equilibrium- a condition where an object is at rest OR its center of mass moves with a constant.

Slides:



Advertisements
Similar presentations
Equilibrium and Elasticity
Advertisements

PHYS 1441 – Section 002 Lecture #23 Monday, April 29, 2013 Dr. Jaehoon Yu Conditions for Equilibrium Elastic Properties of Solids –Young’s Modulus –Bulk.
Physics Montwood High School R. Casao
Chapter 12: (Static) Equilibrium and Elasticity
Equilibrium and Elasticity Equilibrium Center of gravity Static Equilibrium Indeterminate Structures Elasticity Tension, Compression and Shearing pps by.
Equilibrium and Elasticity
Statics & Elasiticity.
Deformation of Solids Stress is proportional to Strain stress = elastic modulus * strain The SI unit for stress is the Newton per meter squared (N/m 2.
Static Equilibrium and Elasticity
Chapter 12: Static Equilibrium and Elasticity
Chapter 11 Equilibrium and Elasticity. Equilibrium.
Static Equilibrium And Elasticity (Keseimbangan Statik dan Kekenyalan)
Static Equilibrium and Elasticity
Copyright © 2009 Pearson Education, Inc. Chapter 12 Elasticity.
Chapter 12: Equilibrium and Elasticity  Conditions Under Which a Rigid Object is in Equilibrium  Problem-Solving Strategy  Elasticity.
Chapter 12 Equilibrium and Elasticity Key contents Conditions for mechanical equilibrium Indeterminate structure Stress, strain, modulus of elasticity.
Chapter 9 Solids and Fluids. Solids Has definite volume Has definite volume Has definite shape Has definite shape Molecules are held in specific locations.
Objectives  Understand how elasticity is related to Hooke’s Law for springs.  Know that the change in length of an object is proportional to the force.
10 Pure Bending.
Spring Forces and Simple Harmonic Motion
Chapter 7 Energy of a System.
Elasticity and Strength of Materials
Chapter 9 Static Equilibrium; Elasticity and Fracture
PHYSICS PROJECT WORK FOR ANNUAL EXAM
Objects in static equilibrium don’t move, F net = 0,  net = 0 Important for posture of human body, biomechanics. Important civil and mechanical engineers.
Equilibrium and Elasticity
Stress and Strain Unit 8, Presentation 1. States of Matter  Solid  Liquid  Gas  Plasma.
Equilibrium and Elasticity
1 Physics for Scientists & Engineers, with Modern Physics, 4 th edition Giancoli Piri Reis University / Physics -I.
Static Equilibrium; Elasticity and Fracture
Physics Notes Ch 9 Statics Statics – The study of forces in equilibrium. The net force and the net torque on an object (or on a system) are zero. The.
Examples of Rigid Objects in Static Equilibrium.
Strengths Chapter 10 Strains. 1-1 Intro Structural materials deform under the action of forces Three kinds of deformation Increase in length called an.
Chapter 7 Energy of a System. Introduction to Energy A variety of problems can be solved with Newton’s Laws and associated principles. Some problems that.
Wednesday, Nov. 12, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #19 Wednesday, Nov. 12, 2003 Dr. Jaehoon Yu 1.Conditions.
Chapter 12: Equilibrium and Elasticity
Chapter 12 Static Equilibrium and Elasticity. Static Equilibrium Equilibrium implies that the object moves with both constant velocity and constant angular.
Dynamics: Newton’s Laws of Motion. Concepts Force Newton’s First Law of Motion Mass Newton’s Second Law of Motion Newton’s Third Law of Motion Weight.
Chapter 12 Equilibrium and elasticity. Equilibrium We already introduced the concept of equilibrium in Chapter 8: dU(x)/dx = 0 More general definition.
Copyright © 2009 Pearson Education, Inc. An object with forces acting on it, but with zero net force, is said to be in equilibrium. The Conditions for.
Physics 201: Lecture 22, Pg 1 Lecture 21 Goals: Use Free Body Diagrams prior to problem solving Introduce Young’s, Shear and Bulk modulus Exam 3: Wednesday,
Static Equilibrium and Elasticity
Rotational Kinetic Energy An object rotating about some axis with an angular speed, , has rotational kinetic energy even though it may not have.
Elasticity I Ali K. Abdel-Fattah. Elasticity In physics, elasticity is a physical property of materials which return to their original shape after they.
Equilibrium and Elasticity
Chapter 11 Angular Momentum. Introduction When studying angular motion, angular momentum plays a key role. Newton’s 2 nd for rotation can be expressed.
Monday, Nov. 18, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #18 Monday, Nov. 18, 2002 Dr. Jaehoon Yu 1.Elastic Properties.
Equilibrium and Elasticity Ch 12 (all). Equilibrium An object is in equilibrium when: - The vector sum of all the external forces that act the body must.
ENGR 107 – Introduction to Engineering Static Equilibrium, and Stress and Strain (Lecture #8)
Spring 2002 Lecture #17 Dr. Jaehoon Yu 1.Conditions for Equilibrium 2.Center of Gravity 3.Elastic Properties of Solids Young’s Modulus Shear Modulus.
Chapter 12 Equilibrium and elasticity. Equilibrium We already introduced the concept of equilibrium in Chapter 8: dU(x)/dx = 0 More general definition.
Tuesday, June 27, 2006PHYS , Summer 2006 Dr. Jaehoon Yu 1 PHYS 1443 – Section 001 Lecture #15 Tuesday, June 27, 2006 Dr. Jaehoon Yu Angular Momentum.
Wednesday, Nov. 17, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Conditions for Equilibrium 2.Mechanical Equilibrium 3.How to solve equilibrium problems?
Advanced Physics Chapter 9—Bodies in Equilibrium.
Chapter 12 Lecture 22: Static Equilibrium and Elasticity: II.
Wednesday, Nov. 13, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #17 Wednesday, Nov. 13, 2002 Dr. Jaehoon Yu 1.Conditions.
Material Properties and Forces. Centroid Principles Object’s center of gravity or center of mass. Graphically labeled as.
PHYS 1443 – Section 003 Lecture #19
Stress – Strain Relationships Credit: Modified from:
PHYS 1443 – Section 002 Lecture #22
Material Properties and Forces
PHYS 1443 – Section 003 Lecture #17
PHYS 1443 – Section 501 Lecture #22
3 Torsion.
Announcements: Midterm 2 coming up Monday Nov. 12 , (two evening times, 5-6 pm or 6-7 pm), Olin 101. Material: Chapters 6 – 14 (through HW 14.1 (pressure)).
Section 9-4: Stability & Balance
12.1 Static equilibrium Static equilibrium: No net torque, no net force and no motion. Static equilibrium 12.2 Sample problem: a witch and a duck balance.
When all the forces that act upon an object are balanced, then the object is said to be in a state of equilibrium. Consider these objects: (1) a book.
Figure 12.1  A single force F acts on a rigid object at the point P.
Equilibrium and Elasticity
Presentation transcript:

Chapter 12 Static Equilibrium and Elasticity

Introduction Equilibrium- a condition where an object is at rest OR its center of mass moves with a constant velocity. Static Equilibrium (former def.) is a common practice in engineering disciplines, critical for civil, arch, and mech eng. Elasticity- we will look at how objects deform under load conditions

12.1 The conditions for Equilibrium – Translation Eq. (from Ch 5) Only works (by itself) for objects modeled as particles (point masses) – Rotational Eq- now that we can deal with extended objects… (about ANY axis) Implies that the object is either not rotating or rotating with a constant speed.

12.1 We will be looking at Static Equilibrium only, which implies both Quick Quizzes p 364

12.1 The vector expressions result in six scalar expressions (three for each axis for both Force and Torque) We will keep motion limited to a single 2D plane for practical purposes.

12.1 If the object is in translational equilibrium and the net torque is zero about one axis, then the net torque is zero about any axis. In other words, when problem solving, any location can be chosen for the axis of rotation.

12.2 More on Center of Gravity The location of a force’s application is critical in evaluating equilibrium conditions. The force of gravity on a given object (assuming a constant gravitational field) acts at the center of mass. One single gravitational force at the center of mass is equivalent to the sum of all the individual gravitational forces on each particle.

12.2

The center of gravity can be located via a number of methods both experimental and calculated. Be careful not to confuse an object’s center of gravity and a system’s center of gravity. A system will balance so long as the support is underneath the center of gravity of the system. Quick Quiz p 366

12.3 Examples of Static Equilibrium Remember Examples

12.4 Elastic Properties of Solids Up to this point we have assumed solid objects remain rigid under external forces. In reality solid objects deform under external forces. Two Key Ideas – Stress- the amount of force acting on an object per unit area – Strain- the result of stress, a measure of deformation.

12.4 Materials can be rated with an Elastic Modulus, a constant of proportionality between stress and strain. – Depends on the material, and type of deformation – Generally determined by – Relates what is done to an object, to how the object responds.

12.4 Different Types of Deformation result in unique elastic moduli. – Young’s Modulus- resistance of a solid to changes in length. – Shear Modulus- resistance of a solid to a shift in parallel planes. – Bulk Modulus- resistance of a solids or fluids to changes in volume (opposite of compressibility)/

12.4 Young’s Modulus- (Tensile Modulus) – The bar is stretch from an initial length Li by a change in length Δ L. – The Stress on the bar is the ratio of the tension force and the cross sectional area of the bar.

12.4 – The strain on the bar is the ratio of the change in length and the initial length. Youngs Modulus also applies to compression forces.

12.4 Objects can be stressed to their elastic limit, at which point it will be permanently deformed, and beyond to their breaking point.

12.4 Shear Modulus – When a force acts on the face of an object parallel to a another face held fixed by an opposite force. – The stress is the ratio of force and parallel surface area.

12.4 – The strain the is ratio of displacement of the sheared face, and the height of the object.

12.4 Bulk Modulus – When a force of uniform magnitude is applied perpendicularly to all surfaces. – The object will undergo a change in volume but not shape. – The volume stress is the ratio of the Force to the surface area of the object. (Also known as pressure).

12.4 – The volume strain is the ratio of the change in volume and the initial volume. – The negative indicates that an increase in pressure, will result in a decrease volume. The inverse of Bulk Modulus is compressibility, and is more commonly used.

12.4 Prestressed Concrete Quick Quizzes p 375 Examples