THE BICYCLE RACE ALBERT SCHUELLER

Size: px
Start display at page:

Download "THE BICYCLE RACE ALBERT SCHUELLER"

Transcription

1 THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The cyclit ride at a contant velocity with her ditance in eter fro the refrehent tation given by where i tie in econd after paing the tation. The puruing upport car ditance in eter fro the tation i given by. There are everal apect of the ituation we will analyze. We are given the poition of the cyclit relative to the location of the refrehent tation a a function of tie. We denote by the poition of the cyclit at tie. Denote by the poition function of the auto. Fro the dicuion in. of Calculu, Stewart rd ed, we know that the velocity of the cyclit i and the velocity of the auto i. In of thi article we copute the cyclit velocity and the tie at which the chae car catche the cyclit. In we explore the effect of different cyclit velocitie on eeting tie. In we attept to illutrate the variou cenario graphically. Finally, in we connect a theortical reult about cubic polynoial with the ituation of the cyclit and the chae car.. VELOCITY AND MEETING TIME In thi ection we deterine the peed of the cyclit and how long it take the chae car to catch her. We have the additional inforation that when the chae car catche the cyclit their velocitie are the ae. Thi provide u with two algebraic equation. When the chae car catche the cyclit their poition are the ae, thu Furtherore, when their poition coincide, by deign, their velocitie are the ae, thu

2 ALBERT SCHUELLER Together, we have two equation in the two unknown and. () ()! " Uing the equation (), we eliinate fro the equation () and olve for. We find two olution, and $#. The firt olution i conitent with the fact that their poition coincided at the refrehent tation. The econd tie, econd, i when the upport car catche the cyclit. The velocity of the cyclit a a function of tie i given by %, where i a contant. Deterining will give the velocity of the cyclit. We know that at &# equation () hold. We can deterine by ubtituting '# #)( into equation ().#)( Doing o we find /. Thu the cyclit i traveling at a rate of /.. DIFFERENT VELOCITIES We will now conider what happen if i allowed to vary. We will derive a forula for in ter of for the tie when the poition of the cyclit and the car coincide. By etting the two poition function equal to each other and olving for, we can deterine the length of tie it take for the puruing car to catch the cyclit. Fro thi calculation we ee that * +, - /. - /. i one olution, which i conitent with the fact that their poition are the ae when the cyclit pae the refrehent tation. We ee that there are potentially two ore tie where the car and the cyclit have the ae poition. To deterine thee tie, we ut apply the quadratic forula, :9; 9 -

3 where 9, and ; THE BICYCLE RACE. Doing o we have ) In order for the olution to be real valued, we ut have +<. Auing >=, we ee that the expreion for i alway poitive and yield two #)( ditinct tie. Fro thi we ay conclude that if he ride fater than #( /, the upport car will not catch her. If he ride lower than /, the upport car will eet her twice. #)(. GRAPHICAL ILLUSTRATION In thi ection we provide graph to illutrate what happen in the firt cae where the car and the cyclit eet and have the ae velocity and in the econd cae where the velocity ay change. Figure, how#)( the poition function of the cyclit and the car on the ae axe with / the optial peed. We ee that after the two function interect. only once at?# FIGURE. A@ Figure ( how the ae graph with the cyclit velocity lightly fater at B /. In thi cae we ee that the two plot fail to interect after. Figure ( how the ae graph with the cyclit velocity lightly lower at /. In thi cae we ee that the two plot interect twice after.

4 ALBERT SCHUELLER FIGURE. AC FIGURE. AD In the ituation depicted in Figure, it would be difficult for the upport car to give refrehent ince there would till be oe ditance between the car the cyclit. In the ituation depicted in Figure, it would be difficult for the car to give refrehent becaue the velocitie of the cyclit and the car would be too different.. CUBIC POLYNOMIALS We will now how that if a cubic polynoial, E root at 9, then EF 9 G relationhip between the cyclit and the auto. Let 9, ha a repeated real. We will then ue thi reult to interpret the be a double root. If

5 I i the reaining root of E E HJI K9 I where i the coefficient on the E HJI "L9 Hence, EM 9 H. THE BICYCLE RACE, then we ay write KL ter. Thu, "L9 KL Thi reult i relevant to the firt ituation in which the car and the cyclit are traveling at the ae peed when they eet. The cubic polynoial in quetion i E N O and repreent the difference in the poition #)( of the cyclit and the car. Uing the factor() call in aple with / we have E H P #) We ee that Q# i a double root of E. Notice further that ER give the difference in the velocitie #Sof the cyclit and the auto. The above double root reult tate that E which i conitent with the fact that at the tie that they eet the cyclit and the auto are traveling at the ae peed. In the later exaple where i allowed to vary, we find that E ha not double root and the delicate condition of atching poition and peed i detroyed.

Conservation of Energy

Conservation of Energy Add Iportant Conervation of Energy Page: 340 Note/Cue Here NGSS Standard: HS-PS3- Conervation of Energy MA Curriculu Fraework (006):.,.,.3 AP Phyic Learning Objective: 3.E.., 3.E.., 3.E..3, 3.E..4, 4.C..,

More information

Uniform Acceleration Problems Chapter 2: Linear Motion

Uniform Acceleration Problems Chapter 2: Linear Motion Name Date Period Uniform Acceleration Problem Chapter 2: Linear Motion INSTRUCTIONS: For thi homework, you will be drawing a coordinate axi (in math lingo: an x-y board ) to olve kinematic (motion) problem.

More information

Practice Problems Solutions. 1. Frame the Problem - Sketch and label a diagram of the motion. Use the equation for acceleration.

Practice Problems Solutions. 1. Frame the Problem - Sketch and label a diagram of the motion. Use the equation for acceleration. Chapter 3 Motion in a Plane Practice Proble Solution Student Textbook page 80 1. Frae the Proble - Sketch and label a diagra of the otion. 40 v(/) 30 0 10 0 4 t () - The equation of otion apply to the

More information

V = 4 3 πr3. d dt V = d ( 4 dv dt. = 4 3 π d dt r3 dv π 3r2 dv. dt = 4πr 2 dr

V = 4 3 πr3. d dt V = d ( 4 dv dt. = 4 3 π d dt r3 dv π 3r2 dv. dt = 4πr 2 dr 0.1 Related Rate In many phyical ituation we have a relationhip between multiple quantitie, and we know the rate at which one of the quantitie i changing. Oftentime we can ue thi relationhip a a convenient

More information

Practice Midterm #1 Solutions. Physics 6A

Practice Midterm #1 Solutions. Physics 6A Practice Midter # Solution Phyic 6A . You drie your car at a peed of 4 k/ for hour, then low down to k/ for the next k. How far did you drie, and what wa your aerage peed? We can draw a iple diagra with

More information

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4.

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4. Chapter 5 Newton Law Practice Proble Solution Student Textbook page 163 1. Frae the Proble - Draw a free body diagra of the proble. - The downward force of gravity i balanced by the upward noral force.

More information

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr Flipping Phyic Lecture Note: Introduction to Acceleration with Priu Brake Slaing Exaple Proble a Δv a Δv v f v i & a t f t i Acceleration: & flip the guy and ultiply! Acceleration, jut like Diplaceent

More information

Linear Motion, Speed & Velocity

Linear Motion, Speed & Velocity Add Important Linear Motion, Speed & Velocity Page: 136 Linear Motion, Speed & Velocity NGSS Standard: N/A MA Curriculum Framework (006): 1.1, 1. AP Phyic 1 Learning Objective: 3.A.1.1, 3.A.1.3 Knowledge/Undertanding

More information

Introduction to Laplace Transform Techniques in Circuit Analysis

Introduction to Laplace Transform Techniques in Circuit Analysis Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found

More information

Halliday/Resnick/Walker 7e Chapter 6

Halliday/Resnick/Walker 7e Chapter 6 HRW 7e Chapter 6 Page of Halliday/Renick/Walker 7e Chapter 6 3. We do not conider the poibility that the bureau might tip, and treat thi a a purely horizontal motion problem (with the peron puh F in the

More information

DIFFERENTIAL EQUATIONS

DIFFERENTIAL EQUATIONS Matheatic Reviion Guide Introduction to Differential Equation Page of Author: Mark Kudlowki MK HOME TUITION Matheatic Reviion Guide Level: A-Level Year DIFFERENTIAL EQUATIONS Verion : Date: 3-4-3 Matheatic

More information

15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object.

15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object. Chapter 4 orce and ewton Law of Motion Goal for Chapter 4 to undertand what i force to tudy and apply ewton irt Law to tudy and apply the concept of a and acceleration a coponent of ewton Second Law to

More information

Solving Radical Equations

Solving Radical Equations 10. Solving Radical Equation Eential Quetion How can you olve an equation that contain quare root? Analyzing a Free-Falling Object MODELING WITH MATHEMATICS To be proficient in math, you need to routinely

More information

1.1 Speed and Velocity in One and Two Dimensions

1.1 Speed and Velocity in One and Two Dimensions 1.1 Speed and Velocity in One and Two Dienion The tudy of otion i called kineatic. Phyic Tool box Scalar quantity ha agnitude but no direction,. Vector ha both agnitude and direction,. Aerage peed i total

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281 72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition

More information

PHYSICS 211 MIDTERM II 12 May 2004

PHYSICS 211 MIDTERM II 12 May 2004 PHYSIS IDTER II ay 004 Exa i cloed boo, cloed note. Ue only your forula heet. Write all wor and anwer in exa boolet. The bac of page will not be graded unle you o requet on the front of the page. Show

More information

Physics 6A. Practice Midterm #2 solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6A. Practice Midterm #2 solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic 6A Practice Midter # olution or apu Learning Aitance Service at USB . A locootive engine of a M i attached to 5 train car, each of a M. The engine produce a contant force that ove the train forward

More information

POSTER PRESENTATION OF A PAPER BY: Alex Shved, Mark Logillo, Spencer Studley AAPT MEETING, JANUARY, 2002, PHILADELPHIA

POSTER PRESENTATION OF A PAPER BY: Alex Shved, Mark Logillo, Spencer Studley AAPT MEETING, JANUARY, 2002, PHILADELPHIA POSTER PRESETATIO OF A PAPER BY: Ale Shved, Mar Logillo, Spencer Studley AAPT MEETIG, JAUARY, 00, PHILADELPHIA Daped Haronic Ocillation Uing Air a Drag Force Spencer Studley Ale Shveyd Mar Loguillo Santa

More information

Answer keys. EAS 1600 Lab 1 (Clicker) Math and Science Tune-up. Note: Students can receive partial credit for the graphs/dimensional analysis.

Answer keys. EAS 1600 Lab 1 (Clicker) Math and Science Tune-up. Note: Students can receive partial credit for the graphs/dimensional analysis. Anwer key EAS 1600 Lab 1 (Clicker) Math and Science Tune-up Note: Student can receive partial credit for the graph/dienional analyi. For quetion 1-7, atch the correct forula (fro the lit A-I below) to

More information

Physics 6A. Practice Midterm #2 solutions

Physics 6A. Practice Midterm #2 solutions Phyic 6A Practice Midter # olution 1. A locootive engine of a M i attached to 5 train car, each of a M. The engine produce a contant force that ove the train forward at acceleration a. If 3 of the car

More information

Second Law of Motion. Force mass. Increasing mass. (Neglect air resistance in this example)

Second Law of Motion. Force mass. Increasing mass. (Neglect air resistance in this example) Newton Law of Motion Moentu and Energy Chapter -3 Second Law of Motion The acceleration of an object i directly proportional to the net force acting on the object, i in the direction of the net force,

More information

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer Suppleental Material for Tranport Proce and Separation Proce Principle hapter 7 Principle of Unteady - State and onvective Ma Tranfer Thi chapter cover different ituation where a tranfer i taking place,

More information

Name: Answer Key Date: Regents Physics. Energy

Name: Answer Key Date: Regents Physics. Energy Nae: Anwer Key Date: Regent Phyic Tet # 9 Review Energy 1. Ue GUESS ethod and indicate all vector direction.. Ter to know: work, power, energy, conervation of energy, work-energy theore, elatic potential

More information

Math 273 Solutions to Review Problems for Exam 1

Math 273 Solutions to Review Problems for Exam 1 Math 7 Solution to Review Problem for Exam True or Fale? Circle ONE anwer for each Hint: For effective tudy, explain why if true and give a counterexample if fale (a) T or F : If a b and b c, then a c

More information

Related Rates section 3.9

Related Rates section 3.9 Related Rate ection 3.9 Iportant Note: In olving the related rate proble, the rate of change of a quantity i given and the rate of change of another quantity i aked for. You need to find a relationhip

More information

AP CHEM WKST KEY: Atomic Structure Unit Review p. 1

AP CHEM WKST KEY: Atomic Structure Unit Review p. 1 AP CHEM WKST KEY: Atoic Structure Unit Review p. 1 1) a) ΔE = 2.178 x 10 18 J 1 2 nf 1 n 2i = 2.178 x 10 18 1 1 J 2 2 6 2 = 4.840 x 10 19 J b) E = λ hc λ = E hc = (6.626 x 10 34 J )(2.9979 x 10 4.840 x

More information

Solution to Theoretical Question 1. A Swing with a Falling Weight. (A1) (b) Relative to O, Q moves on a circle of radius R with angular velocity θ, so

Solution to Theoretical Question 1. A Swing with a Falling Weight. (A1) (b) Relative to O, Q moves on a circle of radius R with angular velocity θ, so Solution to Theoretical uetion art Swing with a Falling Weight (a Since the length of the tring Hence we have i contant, it rate of change ut be zero 0 ( (b elative to, ove on a circle of radiu with angular

More information

Chapter 9 Review. Block: Date:

Chapter 9 Review. Block: Date: Science 10 Chapter 9 Review Name: KEY Block: Date: 1. A change in velocity occur when the peed o an object change, or it direction o motion change, or both. Thee change in velocity can either be poitive

More information

Position. If the particle is at point (x, y, z) on the curved path s shown in Fig a,then its location is defined by the position vector

Position. If the particle is at point (x, y, z) on the curved path s shown in Fig a,then its location is defined by the position vector 34 C HAPTER 1 KINEMATICS OF A PARTICLE 1 1.5 Curvilinear Motion: Rectangular Component Occaionall the motion of a particle can bet be decribed along a path that can be epreed in term of it,, coordinate.

More information

represented in the table? How are they shown on the graph?

represented in the table? How are they shown on the graph? Application. The El Pao Middle School girl baketball team i going from El Pao to San Antonio for the Tea tate championhip game. The trip will be 0 mile. Their bu travel at an average peed of 0 mile per

More information

4 Conservation of Momentum

4 Conservation of Momentum hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding

More information

Scale Efficiency in DEA and DEA-R with Weight Restrictions

Scale Efficiency in DEA and DEA-R with Weight Restrictions Available online at http://ijdea.rbiau.ac.ir Int. J. Data Envelopent Analyi (ISSN 2345-458X) Vol.2, No.2, Year 2014 Article ID IJDEA-00226, 5 page Reearch Article International Journal of Data Envelopent

More information

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin technical proof TP A.30 The effect of cue tip offet, cue weight, and cue peed on cue all peed and pin technical proof upporting: The Illutrated Principle of Pool and Billiard http://illiard.colotate.edu

More information

PHYS 110B - HW #6 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #6 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased PHYS B - HW #6 Spring 4, Solution by David Pace Any referenced equation are from Griffith Problem tatement are paraphraed. Problem. from Griffith Show that the following, A µo ɛ o A V + A ρ ɛ o Eq..4 A

More information

3.3. The Derivative as a Rate of Change. Instantaneous Rates of Change. DEFINITION Instantaneous Rate of Change

3.3. The Derivative as a Rate of Change. Instantaneous Rates of Change. DEFINITION Instantaneous Rate of Change 3.3 The Derivative a a Rate of Change 171 3.3 The Derivative a a Rate of Change In Section 2.1, we initiated the tudy of average and intantaneou rate of change. In thi ection, we continue our invetigation

More information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov Transformation in Classical Mechanics Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How

More information

a = f s,max /m = s g. 4. We first analyze the forces on the pig of mass m. The incline angle is.

a = f s,max /m = s g. 4. We first analyze the forces on the pig of mass m. The incline angle is. Chapter 6 1. The greatet deceleration (of magnitude a) i provided by the maximum friction force (Eq. 6-1, with = mg in thi cae). Uing ewton econd law, we find a = f,max /m = g. Eq. -16 then give the hortet

More information

Problem Set 8 Solutions

Problem Set 8 Solutions Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem

More information

Fair Game Review. Chapter 7 A B C D E Name Date. Complete the number sentence with <, >, or =

Fair Game Review. Chapter 7 A B C D E Name Date. Complete the number sentence with <, >, or = Name Date Chapter 7 Fair Game Review Complete the number entence with , or =. 1. 3.4 3.45 2. 6.01 6.1 3. 3.50 3.5 4. 0.84 0.91 Find three decimal that make the number entence true. 5. 5.2 6. 2.65 >

More information

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes ecture Phy 798S Spring 6 Steven Anlage The heart and oul of uperconductivity i the Meiner Effect. Thi feature uniquely ditinguihe uperconductivity fro any other tate of atter. Here we dicu oe iple phenoenological

More information

Question 1 Equivalent Circuits

Question 1 Equivalent Circuits MAE 40 inear ircuit Fall 2007 Final Intruction ) Thi exam i open book You may ue whatever written material you chooe, including your cla note and textbook You may ue a hand calculator with no communication

More information

Frames of Reference and Relative Velocity

Frames of Reference and Relative Velocity 1.5 frame of reference coordinate ytem relative to which motion i oberved Frame of Reference and Relative Velocity Air how provide element of both excitement and danger. When high-peed airplane fly in

More information

NCAAPMT Calculus Challenge Challenge #3 Due: October 26, 2011

NCAAPMT Calculus Challenge Challenge #3 Due: October 26, 2011 NCAAPMT Calculu Challenge 011 01 Challenge #3 Due: October 6, 011 A Model of Traffic Flow Everyone ha at ome time been on a multi-lane highway and encountered road contruction that required the traffic

More information

Chapter 4. The Laplace Transform Method

Chapter 4. The Laplace Transform Method Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination

More information

Application of Newton s Laws. F fr

Application of Newton s Laws. F fr Application of ewton Law. A hocey puc on a frozen pond i given an initial peed of 0.0/. It lide 5 before coing to ret. Deterine the coefficient of inetic friction ( μ between the puc and ice. The total

More information

Chemistry I Unit 3 Review Guide: Energy and Electrons

Chemistry I Unit 3 Review Guide: Energy and Electrons Cheitry I Unit 3 Review Guide: Energy and Electron Practice Quetion and Proble 1. Energy i the capacity to do work. With reference to thi definition, decribe how you would deontrate that each of the following

More information

Represent each of the following combinations of units in the correct SI form using an appropriate prefix: (a) m/ms (b) μkm (c) ks/mg (d) km μn

Represent each of the following combinations of units in the correct SI form using an appropriate prefix: (a) m/ms (b) μkm (c) ks/mg (d) km μn 2007 R. C. Hibbeler. Publihed by Pearon Education, Inc., Upper Saddle River, J. All right reerved. Thi aterial i protected under all copyright law a they currently exit. o portion of thi aterial ay be

More information

3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard

3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard 3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honor Phyic Impule-Momentum Theorem Spring, 2017 Intruction: Complete the following workheet. Show all of you work. Name: Anwer Key Mr. Leonard 1. A 0.500 kg ball i dropped

More information

PHY 171 Practice Test 3 Solutions Fall 2013

PHY 171 Practice Test 3 Solutions Fall 2013 PHY 171 Practice et 3 Solution Fall 013 Q1: [4] In a rare eparatene, And a peculiar quietne, hing One and hing wo Lie at ret, relative to the ground And their wacky hairdo. If hing One freeze in Oxford,

More information

Chapter 7. Root Locus Analysis

Chapter 7. Root Locus Analysis Chapter 7 Root Locu Analyi jw + KGH ( ) GH ( ) - K 0 z O 4 p 2 p 3 p Root Locu Analyi The root of the cloed-loop characteritic equation define the ytem characteritic repone. Their location in the complex

More information

Unit I Review Worksheet Key

Unit I Review Worksheet Key Unit I Review Workheet Key 1. Which of the following tatement about vector and calar are TRUE? Anwer: CD a. Fale - Thi would never be the cae. Vector imply are direction-conciou, path-independent quantitie

More information

Optics. Measuring the velocity of light Geometrical Optics. What you need:

Optics. Measuring the velocity of light Geometrical Optics. What you need: Geoetrical Optic Optic Meauring the velocity of light -01 What you can learn about Refractive index Wavelength Frequency Phae Modulation Electric field contant Magnetic field contant Principle: The intenity

More information

Constant Force: Projectile Motion

Constant Force: Projectile Motion Contant Force: Projectile Motion Abtract In thi lab, you will launch an object with a pecific initial velocity (magnitude and direction) and determine the angle at which the range i a maximum. Other tak,

More information

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004 METR4200 Advanced Control Lecture 4 Chapter Nie Controller Deign via Frequency Repone G. Hovland 2004 Deign Goal Tranient repone via imple gain adjutment Cacade compenator to improve teady-tate error Cacade

More information

Physics 2212 G Quiz #2 Solutions Spring 2018

Physics 2212 G Quiz #2 Solutions Spring 2018 Phyic 2212 G Quiz #2 Solution Spring 2018 I. (16 point) A hollow inulating phere ha uniform volume charge denity ρ, inner radiu R, and outer radiu 3R. Find the magnitude of the electric field at a ditance

More information

24P 2, where W (measuring tape weight per meter) = 0.32 N m

24P 2, where W (measuring tape weight per meter) = 0.32 N m Ue of a 1W Laer to Verify the Speed of Light David M Verillion PHYS 375 North Carolina Agricultural and Technical State Univerity February 3, 2018 Abtract The lab wa et up to verify the accepted value

More information

time? How will changes in vertical drop of the course affect race time? How will changes in the distance between turns affect race time?

time? How will changes in vertical drop of the course affect race time? How will changes in the distance between turns affect race time? Unit 1 Leon 1 Invetigation 1 Think About Thi Situation Name: Conider variou port that involve downhill racing. Think about the factor that decreae or increae the time it take to travel from top to bottom.

More information

5.5. Collisions in Two Dimensions: Glancing Collisions. Components of momentum. Mini Investigation

5.5. Collisions in Two Dimensions: Glancing Collisions. Components of momentum. Mini Investigation Colliion in Two Dienion: Glancing Colliion So ar, you have read aout colliion in one dienion. In thi ection, you will exaine colliion in two dienion. In Figure, the player i lining up the hot o that the

More information

e st t u(t 2) dt = lim t dt = T 2 2 e st = T e st lim + e st

e st t u(t 2) dt = lim t dt = T 2 2 e st = T e st lim + e st Math 46, Profeor David Levermore Anwer to Quetion for Dicuion Friday, 7 October 7 Firt Set of Quetion ( Ue the definition of the Laplace tranform to compute Lf]( for the function f(t = u(t t, where u i

More information

Moment of Inertia of an Equilateral Triangle with Pivot at one Vertex

Moment of Inertia of an Equilateral Triangle with Pivot at one Vertex oment of nertia of an Equilateral Triangle with Pivot at one Vertex There are two wa (at leat) to derive the expreion f an equilateral triangle that i rotated about one vertex, and ll how ou both here.

More information

Nonlinear Single-Particle Dynamics in High Energy Accelerators

Nonlinear Single-Particle Dynamics in High Energy Accelerators Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction

More information

Physics 20 Lesson 28 Simple Harmonic Motion Dynamics & Energy

Physics 20 Lesson 28 Simple Harmonic Motion Dynamics & Energy Phyic 0 Leon 8 Siple Haronic Motion Dynaic & Energy Now that we hae learned about work and the Law of Coneration of Energy, we are able to look at how thee can be applied to the ae phenoena. In general,

More information

303b Reducing the impact (Accelerometer & Light gate)

303b Reducing the impact (Accelerometer & Light gate) Senor: Logger: Accelerometer High g, Light gate Any EASYSENSE capable of fat logging Science in Sport Logging time: 1 econd 303b Reducing the impact (Accelerometer & Light gate) Read In many porting activitie

More information

The Extended Balanced Truncation Algorithm

The Extended Balanced Truncation Algorithm International Journal of Coputing and Optiization Vol. 3, 2016, no. 1, 71-82 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.12988/ijco.2016.635 The Extended Balanced Truncation Algorith Cong Huu Nguyen

More information

1-D SEDIMENT NUMERICAL MODEL AND ITS APPLICATION. Weimin Wu 1 and Guolu Yang 2

1-D SEDIMENT NUMERICAL MODEL AND ITS APPLICATION. Weimin Wu 1 and Guolu Yang 2 U-CHINA WORKHOP ON ADVANCED COMPUTATIONAL MODELLING IN HYDROCIENCE & ENGINEERING epteber 9-, Oxford, Miiippi, UA -D EDIMENT NUMERICAL MODEL AND IT APPLICATION Weiin Wu and Guolu Yang ABTRACT A one dienional

More information

4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2

4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2 4.5 Evaporation and Diffuion 4.5.4 Evaporation and Diffuion through Quiecent Air (page 86) z bul otion of air and j z diffuion of air (a) diffuion of containant (j) y a,, y j, or P a,, P j, z 1 volatile

More information

AP Physics Momentum AP Wrapup

AP Physics Momentum AP Wrapup AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol

More information

SKAA 1213 Engineering Mechanics

SKAA 1213 Engineering Mechanics SKAA 113 Engineering Mechanic TOPIC 8 KINEMATIC OF PARTICLES Lecturer: Roli Anang Dr. Mohd Yunu Ihak Dr. Tan Cher Siang Outline Introduction Rectilinear Motion Curilinear Motion Problem Introduction General

More information

MAE 101A. Homework 3 Solutions 2/5/2018

MAE 101A. Homework 3 Solutions 2/5/2018 MAE 101A Homework 3 Solution /5/018 Munon 3.6: What preure gradient along the treamline, /d, i required to accelerate water upward in a vertical pipe at a rate of 30 ft/? What i the anwer if the flow i

More information

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002 Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in

More information

State Space: Observer Design Lecture 11

State Space: Observer Design Lecture 11 State Space: Oberver Deign Lecture Advanced Control Sytem Dr Eyad Radwan Dr Eyad Radwan/ACS/ State Space-L Controller deign relie upon acce to the tate variable for feedback through adjutable gain. Thi

More information

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

Control Systems Analysis and Design by the Root-Locus Method

Control Systems Analysis and Design by the Root-Locus Method 6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If

More information

The Hassenpflug Matrix Tensor Notation

The Hassenpflug Matrix Tensor Notation The Haenpflug Matrix Tenor Notation D.N.J. El Dept of Mech Mechatron Eng Univ of Stellenboch, South Africa e-mail: dnjel@un.ac.za 2009/09/01 Abtract Thi i a ample document to illutrate the typeetting of

More information

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment Journal of Multidiciplinary Engineering Science and Technology (JMEST) ISSN: 59- Vol. Iue, January - 5 Advanced D-Partitioning Analyi and it Comparion with the haritonov Theorem Aement amen M. Yanev Profeor,

More information

Holt Physics Problem 3E

Holt Physics Problem 3E NAME DATE CLASS Holt Phyic Problem 3E PROJECTILES LAUNCHED AT AN ANGLE PROBLEM SOLUTION 1. DEFINE. PLAN A flying fih leap out of the water with a peed of 15.3. Normally thee fih ue winglike fin to glide

More information

Final Comprehensive Exam Physical Mechanics Friday December 15, Total 100 Points Time to complete the test: 120 minutes

Final Comprehensive Exam Physical Mechanics Friday December 15, Total 100 Points Time to complete the test: 120 minutes Final Comprehenive Exam Phyical Mechanic Friday December 15, 000 Total 100 Point Time to complete the tet: 10 minute Pleae Read the Quetion Carefully and Be Sure to Anwer All Part! In cae that you have

More information

Velocity or 60 km/h. a labelled vector arrow, v 1

Velocity or 60 km/h. a labelled vector arrow, v 1 11.7 Velocity en you are outide and notice a brik wind blowing, or you are riding in a car at 60 km/, you are imply conidering te peed of motion a calar quantity. ometime, owever, direction i alo important

More information

Math Skills. Scientific Notation. Uncertainty in Measurements. Appendix A5 SKILLS HANDBOOK

Math Skills. Scientific Notation. Uncertainty in Measurements. Appendix A5 SKILLS HANDBOOK ppendix 5 Scientific Notation It i difficult to work with very large or very mall number when they are written in common decimal notation. Uually it i poible to accommodate uch number by changing the SI

More information

Electrical Boundary Conditions. Electric Field Boundary Conditions: Magnetic Field Boundary Conditions: K=J s

Electrical Boundary Conditions. Electric Field Boundary Conditions: Magnetic Field Boundary Conditions: K=J s Electrical Boundar Condition Electric Field Boundar Condition: a n i a unit vector noral to the interface fro region to region 3 4 Magnetic Field Boundar Condition: K=J K=J 5 6 Dielectric- dielectric boundar

More information

Lecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell

Lecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell Lecture 15 - Current Puzzle... Suppoe an infinite grounded conducting plane lie at z = 0. charge q i located at a height h above the conducting plane. Show in three different way that the potential below

More information

Highway Capacity Manual 2010

Highway Capacity Manual 2010 RR = minimum number of lane change that mut be made by one ramp-toramp ehicle to execute the deired maneuer uccefully. MIN for two-ided weaing egment i gien by Equation 12-3: MIN RR For two-ided weaing

More information

Overflow from last lecture: Ewald construction and Brillouin zones Structure factor

Overflow from last lecture: Ewald construction and Brillouin zones Structure factor Lecture 5: Overflow from lat lecture: Ewald contruction and Brillouin zone Structure factor Review Conider direct lattice defined by vector R = u 1 a 1 + u 2 a 2 + u 3 a 3 where u 1, u 2, u 3 are integer

More information

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax: Control Sytem Engineering ( Chapter 7. Steady-State Error Prof. Kwang-Chun Ho kwangho@hanung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Introduction In thi leon, you will learn the following : How to find the

More information

Chapter 13. Root Locus Introduction

Chapter 13. Root Locus Introduction Chapter 13 Root Locu 13.1 Introduction In the previou chapter we had a glimpe of controller deign iue through ome imple example. Obviouly when we have higher order ytem, uch imple deign technique will

More information

Clustering Methods without Given Number of Clusters

Clustering Methods without Given Number of Clusters Clutering Method without Given Number of Cluter Peng Xu, Fei Liu Introduction A we now, mean method i a very effective algorithm of clutering. It mot powerful feature i the calability and implicity. However,

More information

ROUTH HURWITZ ANALYSIS

ROUTH HURWITZ ANALYSIS ROUTH HURWITZ ANALYSIS The Routh Hurwitz analyi tell you how many root are located in the a) let-hand plane, ) right-hand plane, and c) on the jω-axi. The technique i illutrated here with an example. The

More information

ME 375 FINAL EXAM SOLUTIONS Friday December 17, 2004

ME 375 FINAL EXAM SOLUTIONS Friday December 17, 2004 ME 375 FINAL EXAM SOLUTIONS Friday December 7, 004 Diviion Adam 0:30 / Yao :30 (circle one) Name Intruction () Thi i a cloed book eamination, but you are allowed three 8.5 crib heet. () You have two hour

More information

Homework #7 Solution. Solutions: ΔP L Δω. Fig. 1

Homework #7 Solution. Solutions: ΔP L Δω. Fig. 1 Homework #7 Solution Aignment:. through.6 Bergen & Vittal. M Solution: Modified Equation.6 becaue gen. peed not fed back * M (.0rad / MW ec)(00mw) rad /ec peed ( ) (60) 9.55r. p. m. 3600 ( 9.55) 3590.45r.

More information

( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s.

( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s. THE VIBRATION ABSORBER Preable - A NEED arie: Lui San Andre (c) 8 MEEN 363-617 Conider the periodic forced repone of a yte (Kp-Mp) defined by : 1 1 5 lbf in : 1 3 lb (t) It natural frequency i: : ec F(t)

More information

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document. SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU CİHAN BAHRAN I will collect my olution to ome of the exercie in thi book in thi document. Section 2.1 1. Let A = k[[t ]] be the ring of

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

More information

4-4 E-field Calculations using Coulomb s Law

4-4 E-field Calculations using Coulomb s Law 1/21/24 ection 4_4 -field calculation uing Coulomb Law blank.doc 1/1 4-4 -field Calculation uing Coulomb Law Reading Aignment: pp. 9-98 1. xample: The Uniform, Infinite Line Charge 2. xample: The Uniform

More information

Codes Correcting Two Deletions

Codes Correcting Two Deletions 1 Code Correcting Two Deletion Ryan Gabry and Frederic Sala Spawar Sytem Center Univerity of California, Lo Angele ryan.gabry@navy.mil fredala@ucla.edu Abtract In thi work, we invetigate the problem of

More information

Chapter 7: The Laplace Transform Part 1

Chapter 7: The Laplace Transform Part 1 Chapter 7: The Laplace Tranform Part 1 王奕翔 Department of Electrical Engineering National Taiwan Univerity ihwang@ntu.edu.tw November 26, 213 1 / 34 王奕翔 DE Lecture 1 Solving an initial value problem aociated

More information

NOTE: The items d) and e) of Question 4 gave you bonus marks.

NOTE: The items d) and e) of Question 4 gave you bonus marks. MAE 40 Linear ircuit Summer 2007 Final Solution NOTE: The item d) and e) of Quetion 4 gave you bonu mark. Quetion [Equivalent irciut] [4 mark] Find the equivalent impedance between terminal A and B in

More information

List coloring hypergraphs

List coloring hypergraphs Lit coloring hypergraph Penny Haxell Jacque Vertraete Department of Combinatoric and Optimization Univerity of Waterloo Waterloo, Ontario, Canada pehaxell@uwaterloo.ca Department of Mathematic Univerity

More information

THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER

THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER Proceeding of IMAC XXXI Conference & Expoition on Structural Dynamic February -4 Garden Grove CA USA THE EXPERIMENTAL PERFORMANCE OF A NONLINEAR DYNAMIC VIBRATION ABSORBER Yung-Sheng Hu Neil S Ferguon

More information

CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS

CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS Copyright 22 IFAC 5th Triennial World Congre, Barcelona, Spain CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS Tritan Pérez Graham C. Goodwin Maria M. Serón Department of Electrical

More information

1. Basic introduction to electromagnetic field. wave properties and particulate properties.

1. Basic introduction to electromagnetic field. wave properties and particulate properties. Lecture Baic Radiometric Quantitie. The Beer-Bouguer-Lambert law. Concept of extinction cattering plu aborption and emiion. Schwarzchild equation. Objective:. Baic introduction to electromagnetic field:

More information