Chapter 8 Equilibrium and Elasticity.

Slides:



Advertisements
Similar presentations
Elasticity Hooke's Law : the extension in an elastic string is proportional to the applied force . T = x = extension l = natural length =
Advertisements

GRAVITY (also known as Weight) F grav The force of gravity is the force with which the earth, moon, or other massively large object attracts another object.
Q12. Static Equilibrium.
Applying Newton’s Laws
Foundations of Physics
Equilibrium and Elasticity
Statics & Elasiticity.
Physics for Scientists and Engineers, 6e
Dr. Jie Zou PHY 1151 Department of Physics1 Chapter 6 Application of Newton’s Laws.
Instructor: Dr. Tatiana Erukhimova
Chapter 12: Static Equilibrium and Elasticity
Reading Quiz 1. Viscous friction is
Instructor: Dr. Tatiana Erukhimova
Physics 151 Week 12 Day Topics: Hooke’s Law and Oscillations (Chs. 8 & 14)  Springs  Hooke’s Law  Applications  Oscillations  Period & Frequency.
Application of Newton’s Laws
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Equilibrium Using Newton’s second law Mass, weight, and apparent weight.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 818, 819, 820, 821 Lecture 10.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Torque and static equilibrium The spring force Hooke’s law Elastic materials.
Equilibrium Lecturer: Professor Stephen T. Thornton.
AP Physics Review Ch 10 – Oscillatory Motion
Spring Force. Compression and Extension  It takes force to press a spring together.  More compression requires stronger force.  It takes force to extend.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Important forms of energy How energy can be transformed and transferred.
Lecture 8 Applications of Newton’s Laws (Chapter 6)
Springs. Hooke’s Law Any spring has a natural length at which it exerts no net force on the mass m. This length, or position, is called the equilibrium.
Forces in Two Dimension
Springs and Hooke’s Law
Static Conditions of Equilibrium: Static Equilibrium:
Work. Work is the product of the magnitude of the __________________ moved times the component of a ________________ in the direction of the ________________.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
Mechanics 105 Work done by a constant force Scalar product Work done by a varying force Kinetic energy, Work-kinetic energy theorem Nonisolated systems.
Jw Physics 2111 Understanding Physics Chapter 12 1 Fundamentals of Physics Chapter 12 Equilibrium & Elasticity 1.Equilibrium 2.The Requirements of Equilibrium.
Springs and Hooke’s Law Physics 11. Newton’s Cradle  Explain this…  0HZ9N9yvcU.
Springs We are used to dealing with constant forces. Springs are more complicated - not only does the magnitude of the spring force vary, the direction.
Work-2 & Power. Work and Area If the force is constant, we can graphically interpret the work done ( W = F d ) as the area of a rectangle F tall and d.
1© Manhattan Press (H.K.) Ltd. 1.7 Stability 2 © Manhattan Press (H.K.) Ltd. Stability 1.7 Stability (SB p. 75) What makes objects more stable than others?
Equilibrium Static Equilibrium.
Chapter 12 Equilibrium and elasticity. Equilibrium We already introduced the concept of equilibrium in Chapter 8: dU(x)/dx = 0 More general definition.
Chapter 5 THE LAWS OF MOTION. Force, net force : Force as that which causes an object to accelerate. The net force acting on an object is defined as.
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.
A certain pendulum consists of a 2
Lecture 7 Newton’s Laws of Motion. Midterm Test #1 - Thursday!  21 multiple-choice problems - A calculator will be needed. - CHECK YOUR BATTERIES! -
332 – UNIT 6 WORK & ENERGY.
Describe moment of force or torque as moment = force × perpendicular distance from pivot to the line of action of force;
Chapter 12. Equilibrium 1. Introduction 2. Equilibrium 3. The Conditions for Equilibrium.
Static Equilibrium. 1. Identify the object of interest. 2. Draw a free-body diagram. 3. Choose a coordinate system. 4. Write out Newton's 2nd law for.
1 7/29/2004 Midterm 2 – Tomorrow (7/30/04)  Material from Chapters 7-12  Room where recitation meets Practice Exam available on-line or in Davey library.
Hour Exam 2 Review 9:00 Exam is Tomorrow (Wednesday) at 7:00 pm.
Potential Energy and Conservation of Energy
Module 1.1 – Displacement and Velocity Vectors
Springs and Hooke’s Law Physics 11. Springs A mass-spring system is given below. As mass is added to the end of the spring, what happens to the spring?
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Important forms of energy How energy can be transformed and transferred.
Physics Fall Practice Final Exam 25 Questions Time = Less than 30 minutes.
Chapter 5 Work and Energy. Question A crate of mass 10 kg is on a ramp that is inclined at an angle of 30⁰ from the horizontal. A force with a magnitude.
Physics and Forces Dynamics Newton’s Laws of Motion  Newton's laws are only valid in inertial reference frames:  This excludes rotating and accelerating.
6.3 Equilibrium of Forces and Hooke’s Law
Spring Force. Compression and Extension  It takes force to press a spring together.  More compression requires stronger force.  It takes force to extend.
Chapter 5 Work and Energy.
Lecture 5Purdue University, Physics 2201 Lecture 05 Forces and Motion beyond 1 D Textbook Sections 3.7, 4.1 PHYSICS 220.
Torque & Equilibrium AP Physics.
Exam – Curve and Some Statistics
Instructor: Dr. Tatiana Erukhimova
PHYSICS 197 Section 1 Chapter N4 Statics
Elastic Forces Hooke’s Law.
Purdue University, Physics 220
6 Circular Motion, Orbits, and Gravity
PHY131H1F - Class 19 Today, Chapter 12:
Springs and Hooke’s Law
Simple Harmonic Motion
Applying Newton’s Laws
Presentation transcript:

Chapter 8 Equilibrium and Elasticity

Reading Quiz An object is in equilibrium if Fnet = 0. net = 0. either A or B. both A and B.     Answer: D Slide 8-5

Answer An object is in equilibrium if Fnet = 0. net = 0. either A or B. both A and B.     Answer: D Slide 8-6

Reading Quiz An object will be stable if its center of gravity is below its highest point. its center of gravity lies over its base of support. its center of gravity lies outside its base of support. the height of its center of gravity is less than 1/2 its total height. Answer: B Slide 8-7

Answer An object will be stable if its center of gravity is below its highest point. its center of gravity lies over its base of support. its center of gravity lies outside its base of support. the height of its center of gravity is less than 1/2 its total height. Answer: B Slide 8-8

Reading Quiz Hooke’s law describes the force of gravity. a spring. collisions. tension. none of the above. Answer: B Slide 8-9

Answer Hooke’s law describes the force of gravity. a spring. collisions. tension. none of the above. Answer: B Slide 8-10

Torque and Static Equilibrium For an extended object to be in equilibrium, the net force and the net torque must be zero. Slide 8-11

Choosing the Pivot Point Slide 8-12

Solving Static Equilibrium Problems Slide 8-13

Checking Understanding What does the scale read? 500 N 1000 N 2000 N 4000 N Answer: C Slide 8-14

Answer What does the scale read? 500 N 1000 N 2000 N 4000 N Slide 8-15 Answer: C Slide 8-15

Example Problem A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? 2m 𝐹 𝑟 𝐹 𝑙 Slide 8-16

A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? .6m .4m 𝐹 𝑐 𝐹 𝑟 𝐹 𝑙 𝐹 𝑐 Slide 8-16

𝜏 =.3m∙ 𝐹 𝑙 +.2m∙ 𝐹 𝑟 +𝑟∙ 𝐹 𝑐 =0 .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 𝜏 =.3m∙ 𝐹 𝑙 +.2m∙ 𝐹 𝑟 +𝑟∙ 𝐹 𝑐 =0 Slide 8-16

A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 𝐹 𝑟 =.4∙50N 𝐹 𝑙 =.6∙50N 𝜏 =.3m∙ 𝐹 𝑙 +.2m∙ 𝐹 𝑟 +𝑟∙ 𝐹 𝑐 =0 Slide 8-16

.3m∙.6∙50N+.2m∙.4∙50N+𝑟∙25N=0 .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 .3m∙.6∙50N+.2m∙.4∙50N+𝑟∙25N=0 Slide 8-16

9N−4N−𝑟∙25N=0 𝑟= 9N∙m−4N∙m 25N = 1 5 m .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 A 2-m-long board weighing 50 N extends out over the edge of a table, with 40% of the board’s length off the table. How far beyond the table edge can a 25 N cat walk before the board begins to tilt? .3m .2m 𝐹 𝑙 𝐹 𝑐 𝐹 𝑟 9N−4N−𝑟∙25N=0 𝑟= 9N∙m−4N∙m 25N = 1 5 m Slide 8-16

Stability of a Car Slide 8-19

The Spring Force Fsp = k ∆x The magnitude of the spring force is proportional to the displacement of its end: Fsp = k ∆x Slide 8-21

Hooke’s Law (Fsp)x = –k ∆x The spring force is directed oppositely to the displacement. We can then write Hooke’s law as (Fsp)x = –k ∆x Slide 8-22

Checking Understanding Which spring has the largest spring constant? Answer: A Slide 8-23

A Answer Which spring has the largest spring constant? Slide 8-24 Answer: A Slide 8-24

Checking Understanding The same spring is stretched or compressed as shown below. In which case does the force exerted by the spring have the largest magnitude? Answer: E. The idea is that the force is determined by the displacement from the spring’s equilibrium length, which is not given. Slide 8-25

Answer The same spring is stretched or compressed as shown below. In which case does the force exerted by the spring have the largest magnitude? Answer: E. The idea is that the force is determined by the displacement from the spring’s equilibrium length, which is not given. E. Not enough information to tell. Slide 8-26

𝐹 =𝑘 𝑥 𝑘= 𝐹 𝑥 = 100N .22m 100N Example Problem A 20-cm-long spring is attached to a wall. When pulled horizontally with a force of 100 N, the spring stretches to a length of 22 cm. What is the value of the spring constant? 𝐹 =𝑘 𝑥 𝑘= 𝐹 𝑥 = 100N .22m 100N Slide 8-27

Example Problem The same spring is now used in a tug-of-war. Two people pull on the ends, each with a force of 100 N. How long is the spring while it is being pulled? 100N 100N 22 cm Slide 8-28

Example Problem The same spring is now suspended from a hook and a 10.2 kg block is attached to the bottom end. How long is the stretched spring? 10.2kg Slide 8-29

The Springiness of Materials: Young’s Modulus The force exerted by a stretched or compressed rod has the same form as Hooke’s law: F = L L YA Y is Young’s modulus, which depends on the material that the rod is made of. Slide 8-30

Beyond the Elastic Limit Slide 8-31

Summary Slide 8-32

Summary Slide 8-33

Additional Example Problem A spring with spring constant k = 125 N/m is used to pull a 25 N wooden block horizontally across a tabletop. The coefficient of friction between the block and the table is µk = 0.20. By how much does this spring stretch from its equilibrium length? Slide 8-34