15210 RECORDING TIMER - AC STUDENT NAME:

Size: px
Start display at page:

Download "15210 RECORDING TIMER - AC STUDENT NAME:"

Transcription

1 CONTENTS RECORDING TIMER - AC STUDENT NAME: REQUIRED ACCESSORIES o C-Clamps o Ruler or Meer Sick o Mass (200 g or larger) OPTIONAL ACCESSORIES o Ticker Tape Dispenser (#15225) o Consan Speed Vehicle ( #10-103) PURPOSE To produce a posiion versus ime record of moving objecs using a mechanical sriker and paper ape CONCEPT Timing evens is an essenial skill for many scienific invesigaions as well as oher pracical applicaions While many evens can be imed accuraely by using a sopwach, he recording imer provides capabiliies ha a sopwach canno achieve: The recording imer works in fixed ime inervals (1/60 or 1/50 second) The recording imer creaes a physical record of moion on a icker ape Analysis of recorded daa does no depend on hasily recorded values; daa from a icker ape can be measured and analyzed afer he compleion of an invesigaion In order o record imed evens successfully, pracice using he recording imer SAFETY This device runs on 110V, 60 Hz elecriciy from sandard household oules Observe normal safey precauions for any elecrical appliance To avoid elecrical shock, do no use near waer Do no use his device if i is damaged in any way Use appropriae eye proecion, as his device has rapidly vibraing pars ha can propel debris a high speeds Also, say clear of any areas where falling objecs may be used When invesigaing he acceleraion due o graviy, sand clear of he area direcly under he recording imer where weighs are being dropped Also, pick up weighs afer hey have been dropped, so ha hey do no presen a ripping hazard INTRODUCTION Recording he moion of a swifly moving objec cannon balls, falling rocks or flying birds, for example made some observaions very challenging for early scieniss During he 1600s Galileo observed and described he moion of falling objecs These observaions are essenial o undersanding physics, bu his accomplishmens were limied by he echnology of his day Galileo used simple pendulum-driven imers, his own pulse, and waer clocks o keep ime during his experimens The inabiliy o observe shor ime inervals also limied he observaions of Isaac Newon This difficuly, and problems of analyzing moion, led Newon o develop calculus of infiniesimals, a branch of mahemaics which focuses on infiniesimal inervals o calculae raes of change, as well as oher significan quaniies Wihou exremely accurae iming equipmen, modern advances such as communicaion saellies, air ravel, and global posiioning would be impossible Timing can now be accomplished using digial devices ha are accurae o millionhs of a second Phoogaes and oher auomaic riggers can sar and sop iming faser han a human can rip a sop wach SCIENCE FIRST Gene Lasserre Blvd, Yulee, FL wwwsciencefirscom info@sciencefirscom

2 This recording imer records inervals of 1/60 of a second (1/50 of a second in counries which use 50 Hz AC elecriciy) and provides a record of posiions on a paper ape For many lab projecs, he recording imer provides an easy-o-undersand record of moion wih far more deail han simple observaions can provide ASSEMBLY & SUGGESTIONS FOR USE Clamp he imer o a able op, ring sand, or oher sable suppor Place a carbon disc, carbon side down, over he pos in he base of he imer Slip he recording ape hrough he wo guides and under he sriker Make sure ha he paper ape ress under he carbon disc The ape should move freely hrough he recording imer The end of he paper ape can be aached o a variey of objecs o record he posiion of ha objec as a funcion of ime Velociy and acceleraion can be calculaed from his recorded daa Make sure he ape is drawn sraigh hrough he imer Avoid siuaions where he ape will be pulled o he side; his may cause he ape o cach or bind When he paper ape is properly loaded and a recording is abou o be made, urn he recording imer on by using he slide swich on he back of he uni, hen release he objec ha is o be imed The imer needs no calibraion, as i runs on 110V AC power The sriker will make a mark on he recording ape 60 imes each second (In counries ha use 50 Hz AC elecriciy, his imer will make a mark on he recording ape 50 imes a second In counries ha use AC elecriciy a a volage oher han 110V, a volage converer will be necessary #15210A is a recording imer which runs on 220V AC elecriciy) The clariy of he dos on he recording ape can be conrolled by adjusing he heigh of he sriker The cleares dos are obained when he sriker jus ouches he paper ape when in operaion To make his adjusmen, place he plasic feeler gauge beween he poin of he sriker and he base of he imer Loosen he wing-nus on he sriker and move hem up or down unil he sriker jus ouches he gauge Tighen he wing-nus afer calibraing he heigh of he sriker The posiion of he dos on he paper ape (from side o side) can be conrolled by loosening he wing-nus and sliding he sriker along he slo in he sriker arm When he desired locaion is reached, ighen he wing-nus This adjusmen will allow differen porions of he carbon disk o be used Afer iming an experimen, he recording ape provides a direc measure of posiion as a funcion of ime for a paricular objec Below is an example of a recording ape aken from an objec wih consan acceleraion In order o deermine he successive posiions of he objec, pick a saring poin on he recording ape o use as a reference (This is usually a poin near he beginning of he run Ofen, his reference poin is he firs poin ha can be clearly disinguished from he smudge ha he imer makes when i sars, bu he saring poin can be any arbirary posiion) Measure he disance from his reference poin o each poin marked on he ape by he recording imer If you are measuring many daa poins, you may wish o measure secions of 5, 10, or 20 inervals beween dos (I is ofen helpful o circle he poins on he ape ha are acually used for measuremen) Afer you have measured he disance from he reference poin o each seleced poin on he ape, record your posiion values (x 1, x 2, ec) in a daa able, such as he able shown on he nex page The ime for he saring poin is 0 = 0 The ime for each successive recorded poin is he number of spaces (n) beween ha poin and he saring poin divided by he frequency of your AC elecriciy (since he recording imer srikes he icker ape a he same frequency as your AC elecriciy) The velociy of he objec can be deermined by measuring he displacemen beween wo adjacen poins and dividing his displacemen by he ime inerval beween he wo poins (use he same ime inerval for all calculaions) Record hese values in he able in a column o he righ of he posiions The acceleraion of he objec can be deermined by calculaing he change in velociy beween wo adjacen able values and dividing his by he ime inerval beween he wo poins Record his new value in a column o he righ of he velociies Wih his able you now have a record of he posiion, velociy, and acceleraion of he objec as a funcion of ime Noice ha each calculaed quaniy has one less enry han he column before i SCIENCE FIRST Gene Lasserre Blvd, Yulee, FL wwwsciencefirscom info@sciencefirscom

3 TABLE FOR DATA COLLECTION For recording and analyzing daa from Recording Timer apes (See noes on nex page) Time Posiion Velociy ( = +1 - ) NO VALUE Acceleraion 0 =0 x 0 = NO VALUE v 1 =(x 1 -x 0 )/ 1 =n/60 x 1 = a 1 =(v 2 -v 1 )/ v 2 =(x 2 -x 1 )/ 2 =2n/60 x 2 = a 2 =(v 3 -v 2 )/ v 3 =(x 3 -x 2 )/ 3 =3n/60 x 3 = a 3 =(v 4 -v 3 )/ v 4 =(x 4 -x 3 )/ 4 =4n/60 x 4 = a 4 =(v 5 -v 4 )/ v 5 =(x 5 -x 4 )/ 5 =5n/60 x 5 = a 5 =(v 6 -v 5 )/ v 6 =(x 6 -x 5 )/ 6 =6n/60 x 6 = a 6 =(v 7 -v 6 )/ v 7 =(x 7 -x 6 )/ 7 =7n/60 x 7 = a 7 =(v 8 -v 7 )/ v 8 =(x 8 -x 7 )/ 8 =8n/60 x 8 = a 8 =(v 9 -v 8 )/ v 9 =(x 9 -x 8 )/ 9 =9n/60 x 9 = SCIENCE FIRST Gene Lasserre Blvd, Yulee, FL wwwsciencefirscom info@sciencefirscom

4 SUGGESTIONS FOR USE: DATA TABLE For he recording imer, he inerval beween srikes is 1/60 of a second, so ime is he number of spaces divided by 60 (Using 1/50 of a second in counries which use 50 Hz AC elecriciy, change each 60 in he Time column o a 50 ) In he Time column, n is a muliplier for he number of inervals beween srikes ha you choose o coun For example, if you coun displacemen on your icker ape as a span of five inervals beween srikes, hen n = 5 for your paricular daa se The saring poin for measuring displacemen (x 0 = 0) is a any do which can be clearly disinguished from he smudge of dos made by saring he imer, or any arbirary saring posiion on he ape ha is useful for your experimen In he Posiion column, record he disance of he do on he icker ape measured from he saring poin (a x 0 = 0) Speed is a change in displacemen divided by a change in ime (v = Δx/Δ) You mus have a leas wo posiion erms o calculae a velociy If you find i useful, you can noe he changes in displacemen, Δx, in he exra space under each Posiion value recorded as x 0, x 1, x 2, x 3, ec Noe ha speeds (velociies) ha are recorded are he average speeds calculaed for he ime inervals beween each lised ime We have no way o calculae speed before he firs change in displacemen, so NO VALUE is shown prior o v 1 Acceleraion is a change in velociy divided by a change in ime (a = Δv/Δ) You mus have a leas wo velociy erms o calculae an acceleraion If you find i useful, you can noe he changes in velociy, Δv, in he exra space under each Velociy value recorded as v 1, v 2, v 3, ec Acceleraions ha are recorded are average acceleraions calculaed for approximaely each of he lised imes We have no way o calculae acceleraion before he firs change in velociy, so NO VALUE is shown prior o a 1 PROCEDURE A (MEASURING CONSTANT VELOCITY) Preparaion and Procedure (1) Clamp a recording imer o a able or bench Feed a paper ape hrough he recording imer, and aach his paper ape o a Consan Speed Vehicle (CSV), or a similar device ha moves wih consan velociy Eliminae any possibiliy of obsrucing he paper ape (see Assembly and Operaion secion of his handou) Turn on he recording imer and sar he CSV Sop he vehicle when i approaches he end of he bench Afer sopping he CSV, rerieve and analyze your ape Q1 Does he paper ape indicae uniform speed for he vehicle? Explain To deermine he speed of he vehicle, find a segmen of seven dos ha show clearly uniform speed Measure he oal lengh of hese spaces Then, divide his measuremen by he ime inerval Q2 Wha ime inerval does his lengh represen? Q3 Wha is he speed of he vehicle? Preparaion and Procedure (2) The CSV can operae a wo differen speeds, depending on he number of baeries powering he vehicle If using he CSV, change he number of baeries used o power he Vehicle If you are no using he CSV, find a way o change he operaing speed of he apparaus you used in he previous segmen Se up he recording imer, paper ape, and vehicle as you did in he previous segmen Once you are ready o record daa, sar he recording imer and he CSV Sop he vehicle when necessary Afer sopping he CSV, rerieve and analyze your ape Q4 Does he paper ape show uniform speed for he vehicle? Wha is ha speed? Q5 How can you accoun for he difference in speed? SCIENCE FIRST Gene Lasserre Blvd, Yulee, FL wwwsciencefirscom info@sciencefirscom

5 PROCEDURE B (MEASURING ACCELERATION DUE TO GRAVITY) Suggesed Grade Level: Grades 5-12 Conen Area Focus: Velociy and Acceleraion (Linear Kinemaics) Preparaion and Procedure Clamp a recording imer o a suppor, and hang he recording imer over he edge of a bench or able When conducing his experimen, he paper ape mus fall verically hrough he guides Feed a piece of icker ape one meer long hrough he imer Aach a large mass (250 grams or more) o he icker ape, and hold he icker ape so ha he mass hangs jus below he recording imer Be sure ha he ape will fall hrough he imer wih lile fricion Sar he imer, and drop he mass Sop he imer once he objec reaches he floor and he ape has fallen hrough Examine he ape If any dos appear o be missing, repea his procedure If your daa appears o have no missing poins, measure he posiions of each of he dos, and calculae he velociy and acceleraion of he falling objec Q1 Does he objec appear o fall wih consan speed or wih acceleraion? How can you ell? Q2 If he objec acceleraed as i fell o he ground, wha is he value of ha acceleraion? If he objec fell wih consan speed, wha is ha speed? SCIENCE FIRST Gene Lasserre Blvd, Yulee, FL wwwsciencefirscom info@sciencefirscom

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

1. Kinematics I: Position and Velocity

1. Kinematics I: Position and Velocity 1. Kinemaics I: Posiion and Velociy Inroducion The purpose of his eperimen is o undersand and describe moion. We describe he moion of an objec by specifying is posiion, velociy, and acceleraion. In his

More information

Displacement ( x) x x x

Displacement ( x) x x x Kinemaics Kinemaics is he branch of mechanics ha describes he moion of objecs wihou necessarily discussing wha causes he moion. 1-Dimensional Kinemaics (or 1- Dimensional moion) refers o moion in a sraigh

More information

Lab #2: Kinematics in 1-Dimension

Lab #2: Kinematics in 1-Dimension Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion

More information

Constant Acceleration

Constant Acceleration Objecive Consan Acceleraion To deermine he acceleraion of objecs moving along a sraigh line wih consan acceleraion. Inroducion The posiion y of a paricle moving along a sraigh line wih a consan acceleraion

More information

d = ½(v o + v f) t distance = ½ (initial velocity + final velocity) time

d = ½(v o + v f) t distance = ½ (initial velocity + final velocity) time BULLSEYE Lab Name: ANSWER KEY Dae: Pre-AP Physics Lab Projecile Moion Weigh = 1 DIRECTIONS: Follow he insrucions below, build he ramp, ake your measuremens, and use your measuremens o make he calculaions

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

Physics 20 Lesson 5 Graphical Analysis Acceleration

Physics 20 Lesson 5 Graphical Analysis Acceleration Physics 2 Lesson 5 Graphical Analysis Acceleraion I. Insananeous Velociy From our previous work wih consan speed and consan velociy, we know ha he slope of a posiion-ime graph is equal o he velociy of

More information

Practicing Problem Solving and Graphing

Practicing Problem Solving and Graphing Pracicing Problem Solving and Graphing Tes 1: Jan 30, 7pm, Ming Hsieh G20 The Bes Ways To Pracice for Tes Bes If need more, ry suggesed problems from each new opic: Suden Response Examples A pas opic ha

More information

Section A: Forces and Motion

Section A: Forces and Motion I is very useful o be able o make predicions abou he way moving objecs behave. In his chaper you will learn abou some equaions of moion ha can be used o calculae he speed and acceleraion of objecs, and

More information

Position, Velocity, and Acceleration

Position, Velocity, and Acceleration rev 06/2017 Posiion, Velociy, and Acceleraion Equipmen Qy Equipmen Par Number 1 Dynamic Track ME-9493 1 Car ME-9454 1 Fan Accessory ME-9491 1 Moion Sensor II CI-6742A 1 Track Barrier Purpose The purpose

More information

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0.

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0. PHYSICS 20 UNIT 1 SCIENCE MATH WORKSHEET NAME: A. Sandard Noaion Very large and very small numbers are easily wrien using scienific (or sandard) noaion, raher han decimal (or posiional) noaion. Sandard

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance Ch: Moion along a sraigh line Moion Posiion and Displacemen Average Velociy and Average Speed Insananeous Velociy and Speed Acceleraion Consan Acceleraion: A Special Case Anoher Look a Consan Acceleraion

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections

PHYSICS 220 Lecture 02 Motion, Forces, and Newton s Laws Textbook Sections PHYSICS 220 Lecure 02 Moion, Forces, and Newon s Laws Texbook Secions 2.2-2.4 Lecure 2 Purdue Universiy, Physics 220 1 Overview Las Lecure Unis Scienific Noaion Significan Figures Moion Displacemen: Δx

More information

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration

Solution: b All the terms must have the dimension of acceleration. We see that, indeed, each term has the units of acceleration PHYS 54 Tes Pracice Soluions Spring 8 Q: [4] Knowing ha in he ne epression a is acceleraion, v is speed, is posiion and is ime, from a dimensional v poin of view, he equaion a is a) incorrec b) correc

More information

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs. Physics 180A Fall 2008 Tes 1-120 poins Name Provide he bes answer o he following quesions and problems. Wach your sig figs. 1) The number of meaningful digis in a number is called he number of. When numbers

More information

2. What is the displacement of the bug between t = 0.00 s and t = 20.0 s? A) cm B) 39.9 cm C) cm D) 16.1 cm E) +16.

2. What is the displacement of the bug between t = 0.00 s and t = 20.0 s? A) cm B) 39.9 cm C) cm D) 16.1 cm E) +16. 1. For which one of he following siuaions will he pah lengh equal he magniude of he displacemen? A) A jogger is running around a circular pah. B) A ball is rolling down an inclined plane. C) A rain ravels

More information

1. VELOCITY AND ACCELERATION

1. VELOCITY AND ACCELERATION 1. VELOCITY AND ACCELERATION 1.1 Kinemaics Equaions s = u + 1 a and s = v 1 a s = 1 (u + v) v = u + as 1. Displacemen-Time Graph Gradien = speed 1.3 Velociy-Time Graph Gradien = acceleraion Area under

More information

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2 Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne

More information

PHYSICS 149: Lecture 9

PHYSICS 149: Lecture 9 PHYSICS 149: Lecure 9 Chaper 3 3.2 Velociy and Acceleraion 3.3 Newon s Second Law of Moion 3.4 Applying Newon s Second Law 3.5 Relaive Velociy Lecure 9 Purdue Universiy, Physics 149 1 Velociy (m/s) The

More information

Suggested Practice Problems (set #2) for the Physics Placement Test

Suggested Practice Problems (set #2) for the Physics Placement Test Deparmen of Physics College of Ars and Sciences American Universiy of Sharjah (AUS) Fall 014 Suggesed Pracice Problems (se #) for he Physics Placemen Tes This documen conains 5 suggesed problems ha are

More information

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should Cambridge Universiy Press 978--36-60033-7 Cambridge Inernaional AS and A Level Mahemaics: Mechanics Coursebook Excerp More Informaion Chaper The moion of projeciles In his chaper he model of free moion

More information

MEI Mechanics 1 General motion. Section 1: Using calculus

MEI Mechanics 1 General motion. Section 1: Using calculus Soluions o Exercise MEI Mechanics General moion Secion : Using calculus. s 4 v a 6 4 4 When =, v 4 a 6 4 6. (i) When = 0, s = -, so he iniial displacemen = - m. s v 4 When = 0, v = so he iniial velociy

More information

Today: Graphing. Note: I hope this joke will be funnier (or at least make you roll your eyes and say ugh ) after class. v (miles per hour ) Time

Today: Graphing. Note: I hope this joke will be funnier (or at least make you roll your eyes and say ugh ) after class. v (miles per hour ) Time +v Today: Graphing v (miles per hour ) 9 8 7 6 5 4 - - Time Noe: I hope his joke will be funnier (or a leas make you roll your eyes and say ugh ) afer class. Do yourself a favor! Prof Sarah s fail-safe

More information

LAB 5 - PROJECTILE MOTION

LAB 5 - PROJECTILE MOTION Lab 5 Projecile Moion 71 Name Dae Parners OVEVIEW LAB 5 - POJECTILE MOTION We learn in our sudy of kinemaics ha wo-dimensional moion is a sraighforward exension of one-dimensional moion. Projecile moion

More information

Welcome Back to Physics 215!

Welcome Back to Physics 215! Welcome Back o Physics 215! (General Physics I) Thurs. Jan 19 h, 2017 Lecure01-2 1 Las ime: Syllabus Unis and dimensional analysis Today: Displacemen, velociy, acceleraion graphs Nex ime: More acceleraion

More information

Lab 10: RC, RL, and RLC Circuits

Lab 10: RC, RL, and RLC Circuits Lab 10: RC, RL, and RLC Circuis In his experimen, we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors. We will sudy he way volages and currens change in

More information

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS For more deails see las page or conac @aimaiims.in Physics Mock Tes Paper AIIMS/NEET 07 Physics 06 Saurday Augus 0 Uni es : Moion in

More information

Physics Notes - Ch. 2 Motion in One Dimension

Physics Notes - Ch. 2 Motion in One Dimension Physics Noes - Ch. Moion in One Dimension I. The naure o physical quaniies: scalars and ecors A. Scalar quaniy ha describes only magniude (how much), NOT including direcion; e. mass, emperaure, ime, olume,

More information

4.5 Constant Acceleration

4.5 Constant Acceleration 4.5 Consan Acceleraion v() v() = v 0 + a a() a a() = a v 0 Area = a (a) (b) Figure 4.8 Consan acceleraion: (a) velociy, (b) acceleraion When he x -componen of he velociy is a linear funcion (Figure 4.8(a)),

More information

0 time. 2 Which graph represents the motion of a car that is travelling along a straight road with a uniformly increasing speed?

0 time. 2 Which graph represents the motion of a car that is travelling along a straight road with a uniformly increasing speed? 1 1 The graph relaes o he moion of a falling body. y Which is a correc descripion of he graph? y is disance and air resisance is negligible y is disance and air resisance is no negligible y is speed and

More information

Physics for Scientists and Engineers I

Physics for Scientists and Engineers I Physics for Scieniss and Engineers I PHY 48, Secion 4 Dr. Beariz Roldán Cuenya Universiy of Cenral Florida, Physics Deparmen, Orlando, FL Chaper - Inroducion I. General II. Inernaional Sysem of Unis III.

More information

University Physics with Modern Physics 14th Edition Young TEST BANK

University Physics with Modern Physics 14th Edition Young TEST BANK Universi Phsics wih Modern Phsics 14h Ediion Young SOLUTIONS MANUAL Full clear download (no formaing errors) a: hps://esbankreal.com/download/universi-phsics-modern-phsics- 14h-ediion-oung-soluions-manual-/

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

More information

SPH3U: Projectiles. Recorder: Manager: Speaker:

SPH3U: Projectiles. Recorder: Manager: Speaker: SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0

More information

RC, RL and RLC circuits

RC, RL and RLC circuits Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.

More information

Physics 5A Review 1. Eric Reichwein Department of Physics University of California, Santa Cruz. October 31, 2012

Physics 5A Review 1. Eric Reichwein Department of Physics University of California, Santa Cruz. October 31, 2012 Physics 5A Review 1 Eric Reichwein Deparmen of Physics Universiy of California, Sana Cruz Ocober 31, 2012 Conens 1 Error, Sig Figs, and Dimensional Analysis 1 2 Vecor Review 2 2.1 Adding/Subracing Vecors.............................

More information

LABORATORY I: DESCRIPTION OF MOTION IN ONE DIMENSION

LABORATORY I: DESCRIPTION OF MOTION IN ONE DIMENSION LABORATORY I: DESCRIPTION OF MOTION IN ONE DIMENSION In his laboraory you will measure and analyze one-dimensional moion; ha is, moion along a sraigh line. Wih digial videos, you will measure he posiions

More information

a 10.0 (m/s 2 ) 5.0 Name: Date: 1. The graph below describes the motion of a fly that starts out going right V(m/s)

a 10.0 (m/s 2 ) 5.0 Name: Date: 1. The graph below describes the motion of a fly that starts out going right V(m/s) Name: Dae: Kinemaics Review (Honors. Physics) Complee he following on a separae shee of paper o be urned in on he day of he es. ALL WORK MUST BE SHOWN TO RECEIVE CREDIT. 1. The graph below describes he

More information

Acceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry

Acceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry Acceleraion Team: Par I. Uniformly Acceleraed Moion: Kinemaics & Geomery Acceleraion is he rae of change of velociy wih respec o ime: a dv/d. In his experimen, you will sudy a very imporan class of moion

More information

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3 A.P. Physics B Uni 1 Tes Reiew Physics Basics, Moemen, and Vecors Chapers 1-3 * In sudying for your es, make sure o sudy his reiew shee along wih your quizzes and homework assignmens. Muliple Choice Reiew:

More information

Acceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry

Acceleration. Part I. Uniformly Accelerated Motion: Kinematics & Geometry Acceleraion Team: Par I. Uniformly Acceleraed Moion: Kinemaics & Geomery Acceleraion is he rae of change of velociy wih respec o ime: a dv/d. In his experimen, you will sudy a very imporan class of moion

More information

INSTANTANEOUS VELOCITY

INSTANTANEOUS VELOCITY INSTANTANEOUS VELOCITY I claim ha ha if acceleraion is consan, hen he elociy is a linear funcion of ime and he posiion a quadraic funcion of ime. We wan o inesigae hose claims, and a he same ime, work

More information

LAB 6: SIMPLE HARMONIC MOTION

LAB 6: SIMPLE HARMONIC MOTION 1 Name Dae Day/Time of Lab Parner(s) Lab TA Objecives LAB 6: SIMPLE HARMONIC MOTION To undersand oscillaion in relaion o equilibrium of conservaive forces To manipulae he independen variables of oscillaion:

More information

Testing What You Know Now

Testing What You Know Now Tesing Wha You Know Now To bes each you, I need o know wha you know now Today we ake a well-esablished quiz ha is designed o ell me his To encourage you o ake he survey seriously, i will coun as a clicker

More information

Q.1 Define work and its unit?

Q.1 Define work and its unit? CHP # 6 ORK AND ENERGY Q.1 Define work and is uni? A. ORK I can be define as when we applied a force on a body and he body covers a disance in he direcion of force, hen we say ha work is done. I is a scalar

More information

Brock University Physics 1P21/1P91 Fall 2013 Dr. D Agostino. Solutions for Tutorial 3: Chapter 2, Motion in One Dimension

Brock University Physics 1P21/1P91 Fall 2013 Dr. D Agostino. Solutions for Tutorial 3: Chapter 2, Motion in One Dimension Brock Uniersiy Physics 1P21/1P91 Fall 2013 Dr. D Agosino Soluions for Tuorial 3: Chaper 2, Moion in One Dimension The goals of his uorial are: undersand posiion-ime graphs, elociy-ime graphs, and heir

More information

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a Kinemaics Paper 1 1. The graph below shows he ariaion wih ime of he acceleraion a of an objec from = o = T. a T The shaded area under he graph represens change in A. displacemen. B. elociy. C. momenum.

More information

Motion along a Straight Line

Motion along a Straight Line chaper 2 Moion along a Sraigh Line verage speed and average velociy (Secion 2.2) 1. Velociy versus speed Cone in he ebook: fer Eample 2. Insananeous velociy and insananeous acceleraion (Secions 2.3, 2.4)

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

Conceptual Physics Review (Chapters 2 & 3)

Conceptual Physics Review (Chapters 2 & 3) Concepual Physics Review (Chapers 2 & 3) Soluions Sample Calculaions 1. My friend and I decide o race down a sraigh srech of road. We boh ge in our cars and sar from res. I hold he seering wheel seady,

More information

NEWTON S SECOND LAW OF MOTION

NEWTON S SECOND LAW OF MOTION Course and Secion Dae Names NEWTON S SECOND LAW OF MOTION The acceleraion of an objec is defined as he rae of change of elociy. If he elociy changes by an amoun in a ime, hen he aerage acceleraion during

More information

- Graphing: Position Velocity. Acceleration

- Graphing: Position Velocity. Acceleration Tes Wednesday, Jan 31 in 101 Clark Hall a 7PM Main Ideas in Class Today - Graphing: Posiion Velociy v avg = x f f x i i a avg = v f f v i i Acceleraion Pracice ess & key online. Tes over maerial up o secion

More information

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

LabQuest 24. Capacitors

LabQuest 24. Capacitors Capaciors LabQues 24 The charge q on a capacior s plae is proporional o he poenial difference V across he capacior. We express his wih q V = C where C is a proporionaliy consan known as he capaciance.

More information

2001 November 15 Exam III Physics 191

2001 November 15 Exam III Physics 191 1 November 15 Eam III Physics 191 Physical Consans: Earh s free-fall acceleraion = g = 9.8 m/s 2 Circle he leer of he single bes answer. quesion is worh 1 poin Each 3. Four differen objecs wih masses:

More information

9702/1/O/N/02. are set up a vertical distance h apart. M 1 M 2. , it is found that the ball takes time t 1. to reach M 2 ) 2

9702/1/O/N/02. are set up a vertical distance h apart. M 1 M 2. , it is found that the ball takes time t 1. to reach M 2 ) 2 PhysicsndMahsTuor.com 7 car is ravelling wih uniform acceleraion along a sraigh road. The road has marker poss every 1 m. When he car passes one pos, i has a speed of 1 m s 1 and, when i passes he nex

More information

AP Physics 1 - Summer Assignment

AP Physics 1 - Summer Assignment AP Physics 1 - Summer Assignmen This assignmen is due on he firs day of school. You mus show all your work in all seps. Do no wai unil he las minue o sar his assignmen. This maerial will help you wih he

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

2.5. The equation of the spring

2.5. The equation of the spring 2.5. The equaion of he spring I moun a spring wih a weigh on i. I ie he op of he spring o a sick projecing ou he op end of a cupboard door, and fasen a ruler down he edge of he door, so ha as he spring

More information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

Electromagnetic Induction: The creation of an electric current by a changing magnetic field.

Electromagnetic Induction: The creation of an electric current by a changing magnetic field. Inducion 1. Inducion 1. Observaions 2. Flux 1. Inducion Elecromagneic Inducion: The creaion of an elecric curren by a changing magneic field. M. Faraday was he firs o really invesigae his phenomenon o

More information

Phys1112: DC and RC circuits

Phys1112: DC and RC circuits Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.

More information

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me

Of all of the intellectual hurdles which the human mind has confronted and has overcome in the last fifteen hundred years, the one which seems to me Of all of he inellecual hurdles which he human mind has confroned and has overcome in he las fifeen hundred years, he one which seems o me o have been he mos amazing in characer and he mos supendous in

More information

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

AP Calculus BC Chapter 10 Part 1 AP Exam Problems AP Calculus BC Chaper Par AP Eam Problems All problems are NO CALCULATOR unless oherwise indicaed Parameric Curves and Derivaives In he y plane, he graph of he parameric equaions = 5 + and y= for, is a

More information

LAB 4: PROJECTILE MOTION

LAB 4: PROJECTILE MOTION 55 Name Dae Parners LAB 4: POJECTILE MOTION A famous illusraion from Newon s Principia showing he relaionship beween projecile moion and orbial moion OVEVIEW We learned in our sudy of kinemaics ha wo-dimensional

More information

Physics 101 Fall 2006: Exam #1- PROBLEM #1

Physics 101 Fall 2006: Exam #1- PROBLEM #1 Physics 101 Fall 2006: Exam #1- PROBLEM #1 1. Problem 1. (+20 ps) (a) (+10 ps) i. +5 ps graph for x of he rain vs. ime. The graph needs o be parabolic and concave upward. ii. +3 ps graph for x of he person

More information

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole Phys 221 Fall 2014 Chaper 2 Moion in One Dimension 2014, 2005 A. Dzyubenko 2004 Brooks/Cole 1 Kinemaics Kinemaics, a par of classical mechanics: Describes moion in erms of space and ime Ignores he agen

More information

Chapter 1 Rotational dynamics 1.1 Angular acceleration

Chapter 1 Rotational dynamics 1.1 Angular acceleration Chaper Roaional dynamics. Angular acceleraion Learning objecives: Wha do we mean by angular acceleraion? How can we calculae he angular acceleraion of a roaing objec when i speeds up or slows down? How

More information

Unit 1 - Descriptive Models for Linear Motion

Unit 1 - Descriptive Models for Linear Motion Uni 1 - Descripive Models for Linear Moion A workbook and noebook for sudens aking Physics wih Mr. Lonon. Version 3. 212 1 Aciviy 1 - Umm, which way did he go? Designing an invesigaion for our buggy. You

More information

(c) Several sets of data points can be used to calculate the velocity. One example is: distance speed = time 4.0 m = 1.0 s speed = 4.

(c) Several sets of data points can be used to calculate the velocity. One example is: distance speed = time 4.0 m = 1.0 s speed = 4. Inquiry an Communicaion 8. (a) ensiy eermine by Group A is he mos reasonable. (b) When roune off o wo significan igis, Group B has he same alue as Group A. Howeer, saing an experimenal measuremen o six

More information

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B)

AP CALCULUS AB 2003 SCORING GUIDELINES (Form B) SCORING GUIDELINES (Form B) Quesion A blood vessel is 6 millimeers (mm) long Disance wih circular cross secions of varying diameer. x (mm) 6 8 4 6 Diameer The able above gives he measuremens of he B(x)

More information

Speed and Velocity. Overview. Velocity & Speed. Speed & Velocity. Instantaneous Velocity. Instantaneous and Average

Speed and Velocity. Overview. Velocity & Speed. Speed & Velocity. Instantaneous Velocity. Instantaneous and Average Overview Kinemaics: Descripion of Moion Posiion and displacemen velociy»insananeous acceleraion»insananeous Speed Velociy Speed and Velociy Speed & Velociy Velociy & Speed A physics eacher walks 4 meers

More information

Kinematics in One Dimension

Kinematics in One Dimension Kinemaics in One Dimension PHY 7 - d-kinemaics - J. Hedberg - 7. Inroducion. Differen Types of Moion We'll look a:. Dimensionaliy in physics 3. One dimensional kinemaics 4. Paricle model. Displacemen Vecor.

More information

x(m) t(sec ) Homework #2. Ph 231 Introductory Physics, Sp-03 Page 1 of 4

x(m) t(sec ) Homework #2. Ph 231 Introductory Physics, Sp-03 Page 1 of 4 Homework #2. Ph 231 Inroducory Physics, Sp-03 Page 1 of 4 2-1A. A person walks 2 miles Eas (E) in 40 minues and hen back 1 mile Wes (W) in 20 minues. Wha are her average speed and average velociy (in ha

More information

AP Physics 1 - Summer Assignment

AP Physics 1 - Summer Assignment AP Physics 1 - Summer Assignmen This assignmen is due on he firs day of school. You mus show all your work in all seps. Do no wai unil he las minue o sar his assignmen. This maerial will help you wih he

More information

3.6 Derivatives as Rates of Change

3.6 Derivatives as Rates of Change 3.6 Derivaives as Raes of Change Problem 1 John is walking along a sraigh pah. His posiion a he ime >0 is given by s = f(). He sars a =0from his house (f(0) = 0) and he graph of f is given below. (a) Describe

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

CHAPTER 1. Motion. CHAPTER s Objectives

CHAPTER 1. Motion. CHAPTER s Objectives 1 CHAPTER 1 Moion CHAPTER s Objecives Moion was he firs naural even ha riggered human ineres o sudy naural phenomena long before recording ime. To he ancien people, everyhing in he universe seems o move

More information

1.6. Slopes of Tangents and Instantaneous Rate of Change

1.6. Slopes of Tangents and Instantaneous Rate of Change 1.6 Slopes of Tangens and Insananeous Rae of Change When you hi or kick a ball, he heigh, h, in meres, of he ball can be modelled by he equaion h() 4.9 2 v c. In his equaion, is he ime, in seconds; c represens

More information

Summary:Linear Motion

Summary:Linear Motion Summary:Linear Moion D Saionary objec V Consan velociy D Disance increase uniformly wih ime D = v. a Consan acceleraion V D V = a. D = ½ a 2 Velociy increases uniformly wih ime Disance increases rapidly

More information

Effects of Coordinate Curvature on Integration

Effects of Coordinate Curvature on Integration Effecs of Coordinae Curvaure on Inegraion Chrisopher A. Lafore clafore@gmail.com Absrac In his paper, he inegraion of a funcion over a curved manifold is examined in he case where he curvaure of he manifold

More information

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

Chapter 15 Oscillatory Motion I

Chapter 15 Oscillatory Motion I Chaper 15 Oscillaory Moion I Level : AP Physics Insrucor : Kim Inroducion A very special kind of moion occurs when he force acing on a body is proporional o he displacemen of he body from some equilibrium

More information

UNC resolution Uncertainty Learning Objectives: measurement interval ( You will turn in two worksheets and

UNC resolution Uncertainty Learning Objectives: measurement interval ( You will turn in two worksheets and UNC Uncerainy revised Augus 30, 017 Learning Objecives: During his lab, you will learn how o 1. esimae he uncerainy in a direcly measured quaniy.. esimae he uncerainy in a quaniy ha is calculaed from quaniies

More information

Kinematics. See if you can define distance. We think you ll run into the same problem.

Kinematics. See if you can define distance. We think you ll run into the same problem. Kinemaics Inroducion Moion is fundamenal o our lives and o our hinking. Moving from place o place in a given amoun of ime helps define boh who we are and how we see he world. Seeing oher people, objecs

More information

Key points. Energy Storage. Kinetic Energy -E K orke 1/23/2018. Energy Storage and Transfer Model (ETM)

Key points. Energy Storage. Kinetic Energy -E K orke 1/23/2018. Energy Storage and Transfer Model (ETM) Key poins Energy Sorage and Transfer Model (ETM) Uni 7 Energy-a conserved, subsance-like quaniy wih he capabiliy o produce change in physical sysems I does no come in differen forms i s jus energy. I s

More information

Physics for Scientists and Engineers. Chapter 2 Kinematics in One Dimension

Physics for Scientists and Engineers. Chapter 2 Kinematics in One Dimension Physics for Scieniss and Engineers Chaper Kinemaics in One Dimension Spring, 8 Ho Jung Paik Kinemaics Describes moion while ignoring he agens (forces) ha caused he moion For now, will consider moion in

More information

A man pushes a 500 kg block along the x axis by a constant force. Find the power required to maintain a speed of 5.00 m/s.

A man pushes a 500 kg block along the x axis by a constant force. Find the power required to maintain a speed of 5.00 m/s. Coordinaor: Dr. F. hiari Wednesday, July 16, 2014 Page: 1 Q1. The uniform solid block in Figure 1 has mass 0.172 kg and edge lenghs a = 3.5 cm, b = 8.4 cm, and c = 1.4 cm. Calculae is roaional ineria abou

More information

Topic 1: Linear motion and forces

Topic 1: Linear motion and forces TOPIC 1 Topic 1: Linear moion and forces 1.1 Moion under consan acceleraion Science undersanding 1. Linear moion wih consan elociy is described in erms of relaionships beween measureable scalar and ecor

More information

72 Calculus and Structures

72 Calculus and Structures 72 Calculus and Srucures CHAPTER 5 DISTANCE AND ACCUMULATED CHANGE Calculus and Srucures 73 Copyrigh Chaper 5 DISTANCE AND ACCUMULATED CHANGE 5. DISTANCE a. Consan velociy Le s ake anoher look a Mary s

More information

Today: Falling. v, a

Today: Falling. v, a Today: Falling. v, a Did you ge my es email? If no, make sure i s no in your junk box, and add sbs0016@mix.wvu.edu o your address book! Also please email me o le me know. I will be emailing ou pracice

More information

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series Final Review A Puzzle... Consider wo massless springs wih spring consans k 1 and k and he same equilibrium lengh. 1. If hese springs ac on a mass m in parallel, hey would be equivalen o a single spring

More information

The average rate of change between two points on a function is d t

The average rate of change between two points on a function is d t SM Dae: Secion: Objecive: The average rae of change beween wo poins on a funcion is d. For example, if he funcion ( ) represens he disance in miles ha a car has raveled afer hours, hen finding he slope

More information

Farr High School NATIONAL 5 PHYSICS. Unit 3 Dynamics and Space. Exam Questions

Farr High School NATIONAL 5 PHYSICS. Unit 3 Dynamics and Space. Exam Questions Farr High School NATIONAL 5 PHYSICS Uni Dynamics and Space Exam Quesions VELOCITY AND DISPLACEMENT D B D 4 E 5 B 6 E 7 E 8 C VELOCITY TIME GRAPHS (a) I is acceleraing Speeding up (NOT going down he flume

More information

Principle of Least Action

Principle of Least Action The Based on par of Chaper 19, Volume II of The Feynman Lecures on Physics Addison-Wesley, 1964: pages 19-1 hru 19-3 & 19-8 hru 19-9. Edwin F. Taylor July. The Acion Sofware The se of exercises on Acion

More information