Elastic Force: A Force Balance: Elastic & Gravitational Force: Force Example: Determining Spring Constant. Some Other Forces

Size: px
Start display at page:

Download "Elastic Force: A Force Balance: Elastic & Gravitational Force: Force Example: Determining Spring Constant. Some Other Forces"

Transcription

1 Energy Balance, Units & Proble Solving: Mechanical Energy Balance ABET Course Outcoes: 1. solve and docuent the solution of probles involving eleents or configurations not previously encountered (e) (e.g. a new geoetric arrangeent, a new ter to include in an analysis, a new type of starting condition). solve probles using ultiple approaches including varied analytic approaches, diagras, foral solution steps or siple coputer progras (e) By the end of today you should be able to: Calculate the force of a spring and coplete spring force balances Calculate elastic potential energies Solve probles balancing kinetic, gravitational potential, and elastic potential energies Class Plan Handout: eg fro slides 5 8 and worksheet (possibly) Lecture Outline: 1. Elastic Force a) Background: Equations and Balances b) Exaple : Deterining k (force balance) c) Proble: Final position of a bungee cord. Elastic Potential Energy a) Background: Equations and Balances b) Proble 1: Mass stopped by spring (finding k) c) Exaple : Deterining ax height of a spring launched ass d) Exaple 3: Roller coaster with KE, PE & Spring E 3. Wrap/Review a) Energy Balance Suary b) Proble Solving Lessons/Concepts (ephasize proble solving approach as well conservation balances.) Slides will be posted (& therefore these exaples). F s Δx Spring at rest: x = 0, where F s = 0 Elastic Force Elastic Force: Soe Other Forces Hooke s Law Constant k [=] force/length Kineatic: F = a Weight: F g = g (also frictional, drag, agnetic ) F s = k Δx A Force Balance: Elastic & Gravitational Force: Force Exaple: Deterining Spring Constant An 8 kg weight copresses a spring 10 c. What is the Hook s Law Constant (k)? 8 kg 10 c Proble Setup Diagra: Given: = 8 kg x = 10 c (copression, fro rest) Find: k Known: F (spring) = k Δx F (gravity) = a = g g = 9.8 /s Balance: g = k x / /

2 Elastic Force Balance: Force Proble: Bungee Juping Proble (Hooke s Law) A 100 kg bungee juper jups fro a bridge 00 above the river. His bungee cord has a Hooke s Law Constant of 00 N/ and is 100 long at rest (i.e., with no load). When he stops otion (no ore bouncing) how high above the river is he? Hint: Balance the Hooke s Law force & the gravitational force Unweighted 100 Weighted, = 100 kg L f 00 Have students work on Bungee proble on previous slide Ask for setup, Then solve proble (worksheet?) Length at Rest Proble Setup Given: = 100 kg, k = 00 N/ L o (no load) = 100 Find: Final Loaded Length, L f Known: F s = k(l f L o ) F g = ( g) F s = F g (when otion stops) Assuptions: no losses (friction and drag) Solution: k(l f L o ) = g + L o = Distance above river = = / / Diagra: Unweighted 100 Weighted, = 100 kg L f =? Gravitational Potential Energy & Kinetic Energy (Review): Equations and a Siple Energy Balance Gravitational Potential Energy (U ) Kinetic Energy (K) K = ½ v v g U g = (g) h In a closed syste the total energy change is zero: E = 0 K + U g = 0 ½ (v ) + g h = 0 or ½ v + g h = constant h Previous Slide: Quick Review of KE & PE. 1. Forula: Review forula for KE and PE (but on board?). Units Work K = ½ v [=] kg = kg /s Energy units Ug = (g) h [=] kg = kg /s Energy units 3. Signs: need to ake sure signs ake sense 4. Balance Equations: Review 5. Syste: this is a balance on an object (the syste) Now add spring energy (next slide)

3 F s x Elastic Potential Energy x = 0, where F s = 0 Hook s Law Constant Elastic PE: U s = ½ k Δx Adding this into the Energy Balance K + U g + U s = 0 ½ (v ) + g h + ½ k (x) = 0 or ½ v + g h + ½ k x = constant Elastic Potential Energy: Energy Exaple 1: Ball launcher (an energy balance) The earlier spring/ass syste (k = 784 ) is copressed 40 c and then released. What is the resulting axiu height of the ass? Proble Setup Diagra: Given: = 8 kg Δx = 40 c (copression, fro rest) k = 784 N/ (previous calc.) Find: Maxiu height of the ass Known: U s = ½ k Δx U g = ( g) h Copress Release 8 kg 10 c 8 kg 30 c h =? Elastic Potential Energy Exaple 4: Spring Launcher Energy at the beginning (E 0 ) Energy at axiu height (E ax ) Elastic Potential Energy Exaple 4: Spring Launcher Calculation Spring copressed x = 40 c = 0.4 Spring relaxed (x = 0) U s,ax = 0 No otion K o = 0 Take this to be h = 0 U go = 0 No otion K ax = 0 Find: Height =? h ax = /.. / E o = U so = ½ k x o E ax = U g = gh ax Conservation of Energy: E o = E ax ½ k x o = g h ax

4 Elastic Potential Energy: Energy Exaple : Stopping a Sliding Block A.5 kg block slides on a frictionless surface into a spring. It coes to rest when the spring has been copressed 7.5 c. The spring constant is 30 N/. What was the velocity of the block before it contacted the spring? Hint: Use a before & after energy balance. Energy Exaple 1: Stopping a Sliding Block Proble Setup Diagra: on previous page Given: =.5 kg, k = 30 N/ x f = 7.5 c = Find: V 0 =? Known: U sf = ½ k x f K 0 = ½ v 0 K 0 = U sf Assuptions: frictionless, no drag Have students try this proble Ask the for proble setup Possible steps Equation developed The answer V 0 =? k = 30 N/ Δx f = 7.5 c Solution: ½ v 0 = ½ k x f v 0 = k x f /.5 kg.5 kg / / Exaple 5: Launched Roller Coaster 3 Spring Constant k = 5000 N/ Cart Mass, = 1000 kg 5 Work with neighbors 1. Select the datu (h =0). Describe Energy coponents at tie 0 (t 0 ) 3. Proble Restateent (diagra, given, find) 4. Solution V =? 1 Exaple 5: Launched Roller Coaster Questions (possible answers) have groups discuss, then ask class 1. Select the datu (h = 0) could be any places: At ground would be logical At height of position B siplifies calc.. Describe Energy coponents at t 0 Need to define t 0 t 0 = when spring is copressed Syste: entire roller coaster (cart & spring) Energy Coponents of Cart: Es = Us = ½ k x U g = g h (with h = 5 1 = 13 ) 3. Proble Restateent Given: Cart Mass = 1000 kg Spring Const., k = 5000 N/ x = 3 h 1 = 5, h = 1 (h = 13 ) Find: V B =? Diagra (on slide) 4. Proble Steps 1. Calculate Initial Energy (E 0 = U s0 ). Conservation of Energy E B = E 0 3. Calculate Velocity at B E B = K + Ug + Us h = 0, no spring Ug and Us = 0, E B = K B = ½ v

5 Exaple 5: Launched Roller Coaster Calculations Given: Cart Mass = 1000 kg Spring Const., k = 5000 N/ x = 3 h 1 = 5, h = 1 (h = 13 ) Find: V B =? Diagra: (below 3 Datu (h = 0) 5 V B =? 1 1. Calculate Initial Energy (= U g + U s ) U so = ½ k x = ½ 5000 N/ (3 ) =,500 N or J U go = g h = 1000 kg (9.8 /s) (13 ) = 17,400 kg /s or J E 0 = U so + U go = 149,900 J. Conservation of Energy E B = E 0 3. Calculate Velocity at B E B = Ug + K + Us = 0 + ½ V + 0 E 0 =E B = ½ V conservation of E v = ( E o /) ½ = ( 150 kj/1000 kg) ½ v = 17.3 /s Units [=] / = ( /s ) ½ = /s Could define spring as out of the syste in which case it would act on the syste (work) Energy in a Closed Syste Syste (of fixed ass) Energy = a property Previous Slide Suarize energy balances in general, this proble in particular Note energy crossed a boundary (springs can also be inside a syste (e.g. a wind up toy) Heat will be treated later. Next Slide Quickly note that this sections key goals have been proble solving. If tie, ask students in sall groups coe up with a list of key considerations for solving probles particularly involving energy Review the next slide as appropriate. Soe Proble Solving Keys Understand Circustances (Principles, Assuptions, Units ) conservation! Break into parts/steps (setup, initial conditions, solution steps ) Units: Pay attention throughout (ake sure they work, use to understand) Nubers & Signs: Do they ake sense at each step? Discipline: Take tie and care throughout (easy to ake accounting errors) Reread/reevaluate the proble any ties

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10 There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference

More information

Chapter 11 Simple Harmonic Motion

Chapter 11 Simple Harmonic Motion Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion

More information

In the session you will be divided into groups and perform four separate experiments:

In the session you will be divided into groups and perform four separate experiments: Mechanics Lab (Civil Engineers) Nae (please print): Tutor (please print): Lab group: Date of lab: Experients In the session you will be divided into groups and perfor four separate experients: (1) air-track

More information

Flipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions

Flipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions 2015 FRQ #1 Free Response Question #1 - AP Physics 1-2015 Exa Solutions (a) First off, we know both blocks have a force of gravity acting downward on the. et s label the F & F. We also know there is a

More information

m potential kinetic forms of energy.

m potential kinetic forms of energy. Spring, Chapter : A. near the surface of the earth. The forces of gravity and an ideal spring are conservative forces. With only the forces of an ideal spring and gravity acting on a ass, energy F F will

More information

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Experient 9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Objectives 1. Verify Hoo s law,. Measure the force constant of a spring, and 3. Measure the period of oscillation of a spring-ass syste and copare it

More information

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1 PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic

More information

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω =

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω = Thur Oct 9 Assignent 10 Mass-Spring Kineatics (x, v, a, t) Dynaics (F,, a) Tie dependence Energy Pendulu Daping and Resonances x Acos( ωt) = v = Aω sin( ωt) a = Aω cos( ωt) ω = spring k f spring = 1 k

More information

Tactics Box 2.1 Interpreting Position-versus-Time Graphs

Tactics Box 2.1 Interpreting Position-versus-Time Graphs 1D kineatic Retake Assignent Due: 4:32p on Friday, October 31, 2014 You will receive no credit for ites you coplete after the assignent is due. Grading Policy Tactics Box 2.1 Interpreting Position-versus-Tie

More information

5.1 m is therefore the maximum height of the ball above the window. This is 25.1 m above the ground. (b)

5.1 m is therefore the maximum height of the ball above the window. This is 25.1 m above the ground. (b) .6. Model: This is a case of free fall, so the su of the kinetic and gravitational potential energy does not change as the ball rises and falls. The figure shows a ball s before-and-after pictorial representation

More information

Page 1. Physics 131: Lecture 16. Today s Agenda. Collisions. Elastic Collision

Page 1. Physics 131: Lecture 16. Today s Agenda. Collisions. Elastic Collision Physics 131: Lecture 16 Today s Agenda Elastic Collisions Definition Exaples Work and Energy Definition of work Exaples Physics 01: Lecture 10, Pg 1 Collisions Moentu is alost always consered during as

More information

4.7. Springs and Conservation of Energy. Conservation of Mechanical Energy

4.7. Springs and Conservation of Energy. Conservation of Mechanical Energy Springs and Conservation of Energy Most drivers try to avoid collisions, but not at a deolition derby like the one shown in Figure 1. The point of a deolition derby is to crash your car into as any other

More information

Physics 120. Exam #2. May 23, 2014

Physics 120. Exam #2. May 23, 2014 Physics 10 Exa # May 3, 014 Nae Please read and follow these instructions carefully: ead all probles carefully before attepting to solve the. Your work ust be legible, and the organization clear. You ust

More information

Energy and Momentum: The Ballistic Pendulum

Energy and Momentum: The Ballistic Pendulum Physics Departent Handout -10 Energy and Moentu: The Ballistic Pendulu The ballistic pendulu, first described in the id-eighteenth century, applies principles of echanics to the proble of easuring the

More information

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016 NB1140: Physics 1A - Classical echanics and Therodynaics Proble set 2 - Forces and energy Week 2: 21-25 Noveber 2016 Proble 1. Why force is transitted uniforly through a assless string, a assless spring,

More information

Lecture 6. Announcements. Conservation Laws: The Most Powerful Laws of Physics. Conservation Laws Why they are so powerful

Lecture 6. Announcements. Conservation Laws: The Most Powerful Laws of Physics. Conservation Laws Why they are so powerful Conseration Laws: The Most Powerful Laws of Physics Potential Energy gh Moentu p = + +. Energy E = PE + KE +. Kinetic Energy / Announceents Mon., Sept. : Second Law of Therodynaics Gie out Hoework 4 Wed.,

More information

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich TUTORIAL 1 SIMPLE HARMONIC MOTION Instructor: Kazui Tolich About tutorials 2 Tutorials are conceptual exercises that should be worked on in groups. Each slide will consist of a series of questions that

More information

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015 Physics 2210 Fall 2015 sartphysics 20 Conservation of Angular Moentu 21 Siple Haronic Motion 11/23/2015 Exa 4: sartphysics units 14-20 Midter Exa 2: Day: Fri Dec. 04, 2015 Tie: regular class tie Section

More information

We last left off by talking about how the area under a force vs. time curve is impulse.

We last left off by talking about how the area under a force vs. time curve is impulse. Lecture 11 Ipulse and Moentu We last left off by talking about how the area under a force vs. tie curve is ipulse. Recall that for our golf ball we had a strongly peaked force curve: F F avg t You have

More information

8.012 Physics I: Classical Mechanics Fall 2008

8.012 Physics I: Classical Mechanics Fall 2008 MIT OpenCourseWare http://ocw.it.edu 8.012 Physics I: Classical Mechanics Fall 2008 For inforation about citing these aterials or our Ters of Use, isit: http://ocw.it.edu/ters. MASSACHUSETTS INSTITUTE

More information

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact Physically Based Modeling CS 15-863 Notes Spring 1997 Particle Collision and Contact 1 Collisions with Springs Suppose we wanted to ipleent a particle siulator with a floor : a solid horizontal plane which

More information

Particle dynamics Physics 1A, UNSW

Particle dynamics Physics 1A, UNSW 1 Particle dynaics Physics 1A, UNSW Newton's laws: S & J: Ch 5.1 5.9, 6.1 force, ass, acceleration also weight Physclips Chapter 5 Friction - coefficients of friction Physclips Chapter 6 Hooke's Law Dynaics

More information

Take-Home Midterm Exam #2, Part A

Take-Home Midterm Exam #2, Part A Physics 151 Due: Friday, March 20, 2009 Take-Hoe Midter Exa #2, Part A Roster No.: Score: NO exa tie liit. Calculator required. All books and notes are allowed, and you ay obtain help fro others. Coplete

More information

Unit 14 Harmonic Motion. Your Comments

Unit 14 Harmonic Motion. Your Comments Today s Concepts: Periodic Motion Siple - Mass on spring Daped Forced Resonance Siple - Pendulu Unit 1, Slide 1 Your Coents Please go through the three equations for siple haronic otion and phase angle

More information

Description: Conceptual: A bullet embeds in a stationary, frictionless block: type of collision? what is conserved? v_final?

Description: Conceptual: A bullet embeds in a stationary, frictionless block: type of collision? what is conserved? v_final? Chapter 8 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 8 Due: 11:59p on Sunday, October 23, 2016 To understand how points are awarded, read the Grading Policy for this

More information

Lesson 27 Conservation of Energy

Lesson 27 Conservation of Energy Physics 0 Lesson 7 Conservation o nergy In this lesson we will learn about one o the ost powerul tools or solving physics probles utilizing the Law o Conservation o nergy. I. Law o Conservation o nergy

More information

Physics 201, Lecture 15

Physics 201, Lecture 15 Physics 0, Lecture 5 Today s Topics q More on Linear Moentu And Collisions Elastic and Perfect Inelastic Collision (D) Two Diensional Elastic Collisions Exercise: Billiards Board Explosion q Multi-Particle

More information

Name Period. What force did your partner s exert on yours? Write your answer in the blank below:

Name Period. What force did your partner s exert on yours? Write your answer in the blank below: Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:

More information

2. Which of the following best describes the relationship between force and potential energy?

2. Which of the following best describes the relationship between force and potential energy? Work/Energy with Calculus 1. An object oves according to the function x = t 5/ where x is the distance traveled and t is the tie. Its kinetic energy is proportional to (A) t (B) t 5/ (C) t 3 (D) t 3/ (E)

More information

BALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass

BALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the

More information

The ballistic pendulum

The ballistic pendulum (ta initials) first nae (print) last nae (print) brock id (ab17cd) (lab date) Experient 3 The ballistic pendulu Prelab preparation Print a copy of this experient to bring to your scheduled lab session.

More information

PS 11 GeneralPhysics I for the Life Sciences

PS 11 GeneralPhysics I for the Life Sciences PS GeneralPhysics I for the Life Sciences W O R K N D E N E R G Y D R. E N J M I N C H N S S O C I T E P R O F E S S O R P H Y S I C S D E P R T M E N T J N U R Y 0 4 Questions and Probles for Conteplation

More information

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2! Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In

More information

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we

More information

WileyPLUS Assignment 3. Next Week

WileyPLUS Assignment 3. Next Week WileyPLUS Assignent 3 Chapters 6 & 7 Due Wednesday, Noveber 11 at 11 p Next Wee No labs of tutorials Reebrance Day holiday on Wednesday (no classes) 24 Displaceent, x Mass on a spring ωt = 2π x = A cos

More information

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4.

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4. PHYSICS 151 Notes for Online Lecture.4 Springs, Strings, Pulleys, and Connected Objects Hook s Law F = 0 F = -k x 1 x = 0 x = x 1 Let s start with a horizontal spring, resting on a frictionless table.

More information

Question 1. [14 Marks]

Question 1. [14 Marks] 6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is

More information

OSCILLATIONS AND WAVES

OSCILLATIONS AND WAVES OSCILLATIONS AND WAVES OSCILLATION IS AN EXAMPLE OF PERIODIC MOTION No stories this tie, we are going to get straight to the topic. We say that an event is Periodic in nature when it repeats itself in

More information

Problem Set 7: Potential Energy and Conservation of Energy AP Physics C Supplementary Problems

Problem Set 7: Potential Energy and Conservation of Energy AP Physics C Supplementary Problems Proble Set 7: Potential Energy and Conservation of Energy AP Pysics C Suppleentary Probles 1. Approxiately 5.5 x 10 6 kg of water drops 50 over Niagara Falls every second. (a) Calculate te aount of potential

More information

P235 Midterm Examination Prof. Cline

P235 Midterm Examination Prof. Cline P235 Mier Exaination Prof. Cline THIS IS A CLOSED BOOK EXAMINATION. Do all parts of all four questions. Show all steps to get full credit. 7:00-10.00p, 30 October 2009 1:(20pts) Consider a rocket fired

More information

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.

More information

LAB MECH8.COMP From Physics with Computers, Vernier Software & Technology, 2003.

LAB MECH8.COMP From Physics with Computers, Vernier Software & Technology, 2003. LAB MECH8.COMP Fro Physics with Coputers, Vernier Software & Technology, 003. INTRODUCTION You have probably watched a ball roll off a table and strike the floor. What deterines where it will land? Could

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

Today s s topics are: Collisions and Momentum Conservation. Momentum Conservation

Today s s topics are: Collisions and Momentum Conservation. Momentum Conservation Today s s topics are: Collisions and P (&E) Conservation Ipulsive Force Energy Conservation How can we treat such an ipulsive force? Energy Conservation Ipulsive Force and Ipulse [Exaple] an ipulsive force

More information

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ). Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D

More information

Chapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant

Chapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant Chapter 7 Ipulse and Moentu So far we considered only constant force/s BUT There are any situations when the force on an object is not constant JUST IN TIME TEACHING E-ail or bring e your questions prior

More information

Systems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39.

Systems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39. Systes of Masses. Ignoring friction, calculate the acceleration of the syste below and the tension in the rope. Drawing individual free body diagras we get 4.0kg 7.0kg g 9.80 / s a?? g and g (4.0)(9.80)

More information

PHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS.

PHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS. !! www.clutchprep.co INTRO TO FRICTION Friction happens when two surfaces are in contact f = μ =. KINETIC FRICTION (v 0 *): STATIC FRICTION (v 0 *): - Happens when ANY object slides/skids/slips. * = Point

More information

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta 1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve

More information

Student Book pages

Student Book pages Chapter 7 Review Student Boo pages 390 39 Knowledge. Oscillatory otion is otion that repeats itself at regular intervals. For exaple, a ass oscillating on a spring and a pendulu swinging bac and forth..

More information

8.1 Force Laws Hooke s Law

8.1 Force Laws Hooke s Law 8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which

More information

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces

More information

The ballistic pendulum

The ballistic pendulum (ta initials) first nae (print) last nae (print) brock id (ab17cd) (lab date) Experient 4 The ballistic pendulu In this Experient you will learn how to deterine the speed of a projectile as well as the

More information

Physics 11 HW #6 Solutions

Physics 11 HW #6 Solutions Physics HW #6 Solutions Chapter 6: Focus On Concepts:,,, Probles: 8, 4, 4, 43, 5, 54, 66, 8, 85 Focus On Concepts 6- (b) Work is positive when the orce has a coponent in the direction o the displaceent.

More information

Problem Set 14: Oscillations AP Physics C Supplementary Problems

Problem Set 14: Oscillations AP Physics C Supplementary Problems Proble Set 14: Oscillations AP Physics C Suppleentary Probles 1 An oscillator consists of a bloc of ass 050 g connected to a spring When set into oscillation with aplitude 35 c, it is observed to repeat

More information

2.003 Engineering Dynamics Problem Set 2 Solutions

2.003 Engineering Dynamics Problem Set 2 Solutions .003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study

More information

Problem Solving & Energy Balances 4: Those Pesky US Units ABET Course Outcomes: Important Resource: Class Plan distance Velocity time acceleration

Problem Solving & Energy Balances 4: Those Pesky US Units ABET Course Outcomes: Important Resource: Class Plan distance Velocity time acceleration Problem Solving & Energy Balances 4: Those Pesky US Units ABET Course Outcomes: 1. solve and document the solution of problems involving elements or configurations not previously encountered (e) 2. solve

More information

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of Chapter 14 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 14 Due: 11:59p on Sunday, Noveber 27, 2016 To understand how points are awarded, read the Grading Policy for this

More information

Pearson Physics Level 20 Unit IV Oscillatory Motion and Mechanical Waves: Chapter 7 Solutions

Pearson Physics Level 20 Unit IV Oscillatory Motion and Mechanical Waves: Chapter 7 Solutions Pearson Physics Level 0 Unit IV Oscillatory Motion and Mechanical Waves: Chapter 7 Solutions Student Boo page 345 Exaple 7. Practice Probles. 60 s T 5.00 in in 300 s f T 300 s 3 3.33 0 Hz The frequency

More information

Definition of Work, The basics

Definition of Work, The basics Physics 07 Lecture 16 Lecture 16 Chapter 11 (Work) v Eploy conservative and non-conservative forces v Relate force to potential energy v Use the concept of power (i.e., energy per tie) Chapter 1 v Define

More information

SPH4U. Conservation of Energy. Review: Springs. More Spring Review. 1-D Variable Force Example: Spring. Page 1. For a spring we recall that F x = -kx.

SPH4U. Conservation of Energy. Review: Springs. More Spring Review. 1-D Variable Force Example: Spring. Page 1. For a spring we recall that F x = -kx. -D Variable Force Exaple: Spring SPH4U Conseration of Energ For a spring we recall that F x = -kx. F(x) x x x relaxe position -kx F = - k x the ass F = - k x Reiew: Springs Hooke s Law: The force exerte

More information

Physics 139B Solutions to Homework Set 3 Fall 2009

Physics 139B Solutions to Homework Set 3 Fall 2009 Physics 139B Solutions to Hoework Set 3 Fall 009 1. Consider a particle of ass attached to a rigid assless rod of fixed length R whose other end is fixed at the origin. The rod is free to rotate about

More information

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START Laboratory Section: Last Revised on Deceber 15, 2014 Partners Naes: Grade: EXPERIMENT 8 Electron Beas 0. Pre-Laboratory Work [2 pts] 1. Nae the 2 forces that are equated in order to derive the charge to

More information

- Conservation of Energy Notes Teacher Key -

- Conservation of Energy Notes Teacher Key - NAME: DATE: PERIOD: PHYSICS - Conservation of Energy Notes Teacher Key - - Is Energy Conserved? - Determine the max height that a 5kg cannonball will reach if fired vertically with an initial velocity

More information

Curious Bounds for Floor Function Sums

Curious Bounds for Floor Function Sums 1 47 6 11 Journal of Integer Sequences, Vol. 1 (018), Article 18.1.8 Curious Bounds for Floor Function Sus Thotsaporn Thanatipanonda and Elaine Wong 1 Science Division Mahidol University International

More information

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along (40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass

More information

Chapter 1: Basics of Vibrations for Simple Mechanical Systems

Chapter 1: Basics of Vibrations for Simple Mechanical Systems Chapter 1: Basics of Vibrations for Siple Mechanical Systes Introduction: The fundaentals of Sound and Vibrations are part of the broader field of echanics, with strong connections to classical echanics,

More information

Simple and Compound Harmonic Motion

Simple and Compound Harmonic Motion Siple Copound Haronic Motion Prelab: visit this site: http://en.wiipedia.org/wii/noral_odes Purpose To deterine the noral ode frequencies of two systes:. a single ass - two springs syste (Figure );. two

More information

Momentum. Conservation of Linear Momentum. Slide 1 / 140 Slide 2 / 140. Slide 3 / 140. Slide 4 / 140. Slide 6 / 140. Slide 5 / 140.

Momentum. Conservation of Linear Momentum. Slide 1 / 140 Slide 2 / 140. Slide 3 / 140. Slide 4 / 140. Slide 6 / 140. Slide 5 / 140. Slide 1 / 140 Slide 2 / 140 Moentu www.njctl.org Slide 3 / 140 Slide 4 / 140 Table of Contents Click on the topic to go to that section Conservation of Linear Moentu Ipulse - Moentu Equation Collisions

More information

Experiment 2: Hooke s Law

Experiment 2: Hooke s Law COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance

More information

Work, Energy and Momentum

Work, Energy and Momentum Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered

More information

Chapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant

Chapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant Chapter 7 Ipulse and Moentu So far we considered only constant force/s BUT There are any situations when the force on an object is not constant Force varies with tie 7. The Ipulse-Moentu Theore DEFINITION

More information

Periodic Motion is everywhere

Periodic Motion is everywhere Lecture 19 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand and use energy conservation

More information

Chapter 5, Conceptual Questions

Chapter 5, Conceptual Questions Chapter 5, Conceptual Questions 5.1. Two forces are present, tension T in the cable and gravitational force 5.. F G as seen in the figure. Four forces act on the block: the push of the spring F, sp gravitational

More information

+ 1 2 mv 2. Since no forces act on the system in the x-direction, linear momentum in x-direction is conserved: (2) 0 = mv A2. + Rω 2.

+ 1 2 mv 2. Since no forces act on the system in the x-direction, linear momentum in x-direction is conserved: (2) 0 = mv A2. + Rω 2. ME 74 Spring 018 Final Exaination Proble 1 Given: hoogeneous dis of ass and outer radius R is able to roll without slipping on the curved upper surface of a cart. art (of ass ) is able to ove along a sooth,

More information

UNIT 2 REVIEW. (Pages ) mv = 2 2 mv = p =

UNIT 2 REVIEW. (Pages ) mv = 2 2 mv = p = UNI REVIEW (Pages 07 Understanding Concepts. One situation is a person carrying a book at a constant height across a level floor. A satellite in circular orbit or pushing on a brick wall are two other

More information

PH 221-1D Spring Oscillations. Lectures Chapter 15 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-1D Spring Oscillations. Lectures Chapter 15 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-1D Spring 013 Oscillations Lectures 35-37 Chapter 15 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 15 Oscillations In this chapter we will cover the following topics: Displaceent,

More information

Some Perspective. Forces and Newton s Laws

Some Perspective. Forces and Newton s Laws Soe Perspective The language of Kineatics provides us with an efficient ethod for describing the otion of aterial objects, and we ll continue to ake refineents to it as we introduce additional types of

More information

Tutorial Exercises: Incorporating constraints

Tutorial Exercises: Incorporating constraints Tutorial Exercises: Incorporating constraints 1. A siple pendulu of length l ass is suspended fro a pivot of ass M that is free to slide on a frictionless wire frae in the shape of a parabola y = ax. The

More information

HW 6 - Solutions Due November 20, 2017

HW 6 - Solutions Due November 20, 2017 Conteporary Physics I HW 6 HW 6 - Solutions Due Noveber 20, 2017 1. A 4 kg block is attached to a spring with a spring constant k 200N/, and is stretched an aount 0.2 [5 pts each]. (a) Sketch the potential

More information

Simple Harmonic Motion

Simple Harmonic Motion Reading: Chapter 15 Siple Haronic Motion Siple Haronic Motion Frequency f Period T T 1. f Siple haronic otion x ( t) x cos( t ). Aplitude x Phase Angular frequency Since the otion returns to its initial

More information

Introduction to Robotics (CS223A) (Winter 2006/2007) Homework #5 solutions

Introduction to Robotics (CS223A) (Winter 2006/2007) Homework #5 solutions Introduction to Robotics (CS3A) Handout (Winter 6/7) Hoework #5 solutions. (a) Derive a forula that transfors an inertia tensor given in soe frae {C} into a new frae {A}. The frae {A} can differ fro frae

More information

Department of Physics Preliminary Exam January 3 6, 2006

Department of Physics Preliminary Exam January 3 6, 2006 Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.

More information

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis.

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis. Instructor(s): Acosta, inzler PHYSICS DEPATMENT PHY 048, Spring 04 Final Exa March 4, 04 Nae (print, last first): Signature: On y honor, I have neither given nor received unauthorized aid on this exaination.

More information

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE)

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE) The Lagrangian ethod vs. other ethods () This aterial written by Jozef HANC, jozef.hanc@tuke.sk Technical University, Kosice, Slovakia For Edwin Taylor s website http://www.eftaylor.co/ 6 January 003 The

More information

3. In the figure below, the coefficient of friction between the center mass and the surface is

3. In the figure below, the coefficient of friction between the center mass and the surface is Physics 04A Exa October 9, 05 Short-answer probles: Do any seven probles in your exa book. Start each proble on a new page and and clearly indicate the proble nuber for each. If you attept ore than seven

More information

Honors Lab 4.5 Freefall, Apparent Weight, and Friction

Honors Lab 4.5 Freefall, Apparent Weight, and Friction Nae School Date Honors Lab 4.5 Freefall, Apparent Weight, and Friction Purpose To investigate the vector nature of forces To practice the use free-body diagras (FBDs) To learn to apply Newton s Second

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please

More information

2. What would happen to his acceleration if his speed were half? Energy The ability to do work

2. What would happen to his acceleration if his speed were half? Energy The ability to do work 1. A 40 kilogram boy is traveling around a carousel with radius 0.5 meters at a constant speed of 1.7 meters per second. Calculate his centripetal acceleration. 2. What would happen to his acceleration

More information

CHAPTER 15: Vibratory Motion

CHAPTER 15: Vibratory Motion CHAPTER 15: Vibratory Motion courtesy of Richard White courtesy of Richard White 2.) 1.) Two glaring observations can be ade fro the graphic on the previous slide: 1.) The PROJECTION of a point on a circle

More information

Conservation of Energy

Conservation of Energy Lecture 3 Chapter 8 Physics I 03.0.04 Conservation of Energy Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Lecture Capture: http://echo360.uml.edu/danylov03/physicsspring.html

More information

26 Impulse and Momentum

26 Impulse and Momentum 6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction

More information

Kinetic Theory of Gases: Elementary Ideas

Kinetic Theory of Gases: Elementary Ideas Kinetic Theory of Gases: Eleentary Ideas 17th February 2010 1 Kinetic Theory: A Discussion Based on a Siplified iew of the Motion of Gases 1.1 Pressure: Consul Engel and Reid Ch. 33.1) for a discussion

More information

Monitoring and system identification of suspension bridges: An alternative approach

Monitoring and system identification of suspension bridges: An alternative approach Monitoring and syste identification of suspension bridges: An alternative approach Erdal Şafak Boğaziçi University, Kandilli Observatory and Earthquake Reseach Institute, Istanbul, Turkey Abstract This

More information

Momentum Balances & Quadratic Equations

Momentum Balances & Quadratic Equations Momentum Balances & Quadratic Equations ABET Course Outcomes: C.1 formulate and solve engineering problems using linear and quadratic equations By the end of this class you should be able to: Solve problems

More information

Waves Unit I Activity: Kinematic Equations for SHM

Waves Unit I Activity: Kinematic Equations for SHM Nae Date Period Waves Unit I Activity: Kineatic Equations for SHM You have seen four different graphs in the wor you have done on ass-spring systes oscillating in siple haronic otion (SHM). Now we will

More information

Oscillations: Review (Chapter 12)

Oscillations: Review (Chapter 12) Oscillations: Review (Chapter 1) Oscillations: otions that are periodic in tie (i.e. repetitive) o Swinging object (pendulu) o Vibrating object (spring, guitar string, etc.) o Part of ediu (i.e. string,

More information

Physics Circular Motion: Energy and Momentum Conservation. Science and Mathematics Education Research Group

Physics Circular Motion: Energy and Momentum Conservation. Science and Mathematics Education Research Group F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Departent of Curriculu and Pedagogy Physics Circular Motion: Energy and Moentu Conservation Science and Matheatics Education Research Group Supported

More information

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14 Physics 07, Lecture 18, Nov. 3 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand

More information

More Oscillations! (Today: Harmonic Oscillators)

More Oscillations! (Today: Harmonic Oscillators) More Oscillations! (oday: Haronic Oscillators) Movie assignent reinder! Final due HURSDAY April 20 Subit through ecapus Different rubric; reeber to chec it even if you got 00% on your draft: http://sarahspolaor.faculty.wvu.edu/hoe/physics-0

More information