UNIT 1 ONE-DIMENSIONAL MOTION GRAPHING AND MATHEMATICAL MODELING. Objectives

Size: px
Start display at page:

Download "UNIT 1 ONE-DIMENSIONAL MOTION GRAPHING AND MATHEMATICAL MODELING. Objectives"

Transcription

1 UNIT 1 ONE-DIMENSIONAL MOTION GRAPHING AND MATHEMATICAL MODELING Objeces To learn abou hree ways ha a physcs can descrbe moon along a sragh lne words, graphs, and mahemacal modelng. To acqure an nue undersandng o poson, elocy, and acceleraon or one-dmensonal moon. To recognze how graphs can be used o descrbe changes n poson, elocy and acceleraon o an objec mong along a sragh lne. To be able o use mahemacal denons o aerage elocy and aerage acceleraon n one dmenson. To check he aldy o some o he sandard knemacs equaons used o descrbe he moon o objecs undergong consan acceleraon. To be able o use knemacs equaons o descrbe he moon o objecs mong wh consan acceleraon. Equpmen ls: Maskng ape 4 Sopwaches 1 Bowlng Ball Ecel spreadshee 1.1 Below are a seres o snapshos o hree deren bowlng balls a mes 1,, 3, 4, and 5. The mes are equally spaced. Suppose each o he me nerals s 0.5s. 1

2

3 a. Deermne each bowlng ball s speedng up, slowng down, or mong a consan speed. Eplan your reasonng. b. In he rs me neral, compare he dsances coered by each bowlng ball. How does he dsance coered n ha me neral ge you normaon abou he speed o he bowlng ball? Eplan. 1. Oban a bowlng ball. Wh a pece o maskng ape, mark o a sarng pon, and dsances o m, 4m, 6m, and 8m rom he sarng pon. a. Predc wha wll happen, you release he bowlng ball a he sarng pon. Wll moe a consan speed, speed up or slow down? I you record he me reaches he m, 4m, 6m, and 8m marks, wll he me nerals beween adjacen marks ncrease, decrease or reman he same? Eplan. b. Perorm he epermen. Release he bowlng ball a he sarng pon. Use sopwaches, sarng hem a he me he ball s released, and recordng he me he ball crosses he m, 4m, 6m, and 8m marks. Record he posons and mes n an Ecel spreadshee. c. I you were o plo he poson on he ercal as and he me on he horzonal as, wha would he plo look lke? (Ths s a predcon.) d. In Ecel, use Graph o plo he poson on he ercal as and he me on he horzonal as. Eplan why looks he way does. How does compare o your predcon? 3

4 e. Wha would a graph o speed s. me look lke? Dscuss wh an nsrucor. Equpmen ls: Moon deecor LabPro compuer nerace LoggerPro soware.1 An ulrasonc moon deecor s a dece ha can be used o record an objec s moon as a uncon o me. I sends ou a seres o sound pulses (oo hgh requency o hear). These pulses relec rom objecs n he cny and he releced pulses reurn o he sensor. The compuer can record he me akes he releced pulses o reurn o he compuer, and usng he speed o sound, calculae he poson o he objec. When usng a moon sensor: 1. Do no ge closer han 0.5 meers rom he sensor because canno record releced pulses ha come back oo soon aer hey are sen.. The ulrasonc waes spread ou n a cone o abou 15 as hey rael. They wll see he closes objec. Be sure here s a clear pah beween he objec whose moon you wan o rack and he moon sensor. 3. The moon sensor s ery sense and wll deec slgh moons. You can ry o glde smoohly along he loor, bu don be surprsed o see small bumps n poson graphs and een larger bumps laer n elocy and acceleraon graphs. 4. Some objecs lke bulky sweaers are good sound absorbers and may no be seen ery well by a moon sensor. You may wan o hold a book n ron o you you hae loose clohng on. a. Predc and skech poson s. me (me on he horzonal as, poson on he ercal as) graphs or he ollowng suaons: sandng sll sarng near he deecor, walkng a a as seady walkng speed away rom he deecor sandng abou 3m away rom he deecor, walkng a a slow seady walkng speed owards he deecor, soppng brely, walkng a a as seady walkng speed away rom he deecor walkng a a slow seady walkng speed away rom he deecor, hen walkng a a as seady walkng speed urher away rom he deecor walkng away rom he deecor slowly, soppng or a whle, walkng aser away rom he deecor b. A your able you hae Moon Deecor, a LabPro compuer nerace and he manuals ha accompany ha equpmen. Connec he whe (USB) cable o he compuer and he oher end o LabPro compuer nerace (See he Verner LabPro User s Gude or ask 4

5 your nsrucor, you hae quesons.) Connec he power cord o he AC adaper por on he LabPro compuer nerace and plug n. Connec he gray Brsh Telecom end o he cable no DIG/SONIC on he LabPro nerace. Se he moon deecor where you hae an asle n ron o he deecor abou 5m long and 1.5m wde. Clck on hs lnk o he le Poson, go o Seup, choose Daa collecon, under Samplng se epermen o abou 3 sec. (You can change hs. You wll probably wan beween o 6 seconds, dependng on wha you are dong.) and se he samples per second o abou 40. Clck OK. Perorm he moons descrbed n par a. n ron o he moon deecor whle akng daa. c. Dscuss wh your parners he derence n your moon ha produces derenly sloped pars o he graph. Dscuss mong orward and backward and how aecs he graph.. Consder he ollowng graph. a. Descrbe n words how you would moe n ron o he moon deecor n order o creae he graph. b. Walk n ron o he moon deecor and ry o creae he graph..3 Consder he ollowng dagram. (rom Workshop Physcs (Elecronc Verson) by Prslla Laws, e al., John Wley and Sons, NY, 1999) a. Descrbe n words how you would moe n ron o he moon deecor n order o creae he graph. b. Walk n ron o he moon deecor and ry o creae he graph. 5

6 c. How s he graph deren rom he preous graph? How do you hae o walk derenly o creae he graph compared o how you had o walk o creae he preous graph? Dscuss wh an nsrucor. Equpmen ls: None 3.1 Consder he ollowng dagram. a. Dscuss he speed n each segmen o he graph. Descrbe n words how you would deermne a alue or he speed n each segmen o he graph. b. Are you able o deermne he drecon o moon n each segmen n he graph? Could you use a symbol o ndcae he drecon o moon? Eplan. How would you epress boh he speed and he drecon numercally? Dscuss he aboe wh an nsrucor. A quany ha epresses boh speed and drecon s called elocy. The denon o aerage elocy oer a me neral s he dsplacemen durng he me neral dded by he me neral. The dsplacemen s he nal poson mnus he nal poson and he me neral s he nal me mnus he nal me. We can wre hs mahemacally as = or, equalenly, = s he nal poson and s he nal poson. s he nal me and s he nal me. The uns o elocy are meers per second (m/s). Snce dsplacemen s a ecor quany, elocy s also a ecor quany. I has boh a magnude and a drecon. The magnude o he elocy s called he speed. 6

7 When workng n one dmenson, he drecon o he elocy can be descrbed as orward or backward, le or rgh, pose or negae, ec. We wll use he words pose or negae or he symbols + or o descrbe he drecon o he elocy. I s common, when workng n one dmenson, o wre he aboe equaon as a scalar equaon, where he aerage elocy s eher a pose or negae quany dependng on he drecon o moon =. c. Use he equaon or elocy o calculae he aerage elocy or each segmen o he graph. Record your resuls below. Tme Ineral (s) Speed (m/s) Drecon Velocy (m/s) d. Deermne he aerage elocy oer he me neral rom 0-4.5s (boh he magnude and he drecon). Deermne he aerage elocy oer he me neral rom 0-7s (boh he magnude and he drecon). Check your calculaons wh an nsrucor. e. Make a graph o elocy s. me (elocy on he ercal as and me on he horzonal as) or he daa n par c. Equpmen Ls: Moon deecor LabPro Compuer Inerace LoggerPro soware 4.1 a. Predc and skech elocy s. me (me on he horzonal as, elocy on he ercal as) graphs or he ollowng suaons: sandng sll sarng near he deecor, walkng a slow speed away rom he deecor sarng away rom he deecor, walkng a a as speed owards he deecor sandng 3m away rom he deecor, walkng a a slow consan speed owards he deecor, soppng brely, walkng a a as consan speed away rom he deecor 7

8 walkng a a slow consan speed away rom he deecor, hen walkng a a as consan speed urher away rom he deecor b. Clck on hs lnk o he le Poson & elocy. The graph o elocy s. me wll be labeled elocy on he y-as. The moon deecor s acually measurng your elocy. Perorm he moons descrbed n par a. n ron o he moon deecor whle akng daa o es your predcons. 4. Consder he ollowng graph o elocy s. me. a. Descrbe n words how you would moe n ron o he moon deecor n order o creae he graph. b. Walk n ron o he moon deecor and ry o creae he graph. c. Draw he poson s. me graph ha corresponds o he moon o he elocy graph. Check your graph wh an nsrucor. 4.3 Consder he ollowng poson graphs. a. Calculae he slope o each segmen o he graph. b. Compare he slopes calculaed n par a o he aerage elocy n each o he me segmens n par 3.1.c. How do he slopes and he aerage eloces compare? c. Dscuss he saemen: The elocy s he rae o change o poson wh me. Dscuss he saemen: The elocy s he slope o a poson s. me graph. 8

9 4.4 a. Wha would he elocy s. me graph look lke, you were o moe, no a a consan speed, bu geng aser and aser and aser? (Ths s a predcon. Draw he graph.) Wha you were mong slower and slower and slower? b. I you were o moe aser and aser and aser a a consan rae (your elocy s ncreasng a a consan rae), wha would he elocy s. me graph look lke? (Ths s a predcon. Draw he graph.) c. Predc he poson s. me graph or par b. d. Se up he moon deecor and es your predcons o pars a and b. Equpmen Ls: Moon deecor LabPro Compuer Inerace LoggerPro soware Low Frcon Dynamc Track Car Car wh an accessory Rod Sand 5.1 Tl a Dynamcs rack a a small angle o he able, as n he dagram below. a. Place a car a he op o he rack and release. Plo he elocy s. me or he car, usng he moon deecor. Is he elocy ncreasng a a consan rae? Eplan how you know. b. Ge a denon o acceleraon. I does no hae o be ormal. (Descrbe your undersandng o wha means o accelerae.) c. Was he car n par 5.1.a accelerang? Eplan. The denon o aerage acceleraon oer a me neral s he change n elocy durng he me neral dded by he me neral. The change n elocy s he nal elocy mnus he nal elocy and he me neral s he nal me mnus he nal me. We can wre hs mahemacally as 9

10 a = or, equalenly, a = where s he nal elocy and s he nal elocy, s he nal me and s he nal me. The uns o acceleraon are meers per second per second (m/s ). Acceleraon s a ecor quany. I has boh a magnude and a drecon. As or elocy, when workng n one dmenson, he drecon o he acceleraon can be descrbed as orward or backward, le or rgh, pose or negae, ec. We wll use he words pose or negae or he symbols + or o descrbe he drecon o he acceleraon. I s common, when workng n one dmenson, o wre he aboe equaon as a scalar equaon, where he aerage acceleraon s eher a pose or negae quany dependng on he drecon o moon a =. d. Deermne he aerage acceleraon o he car n par a. Check your calculaon wh an nsrucor. 5. a. In each o he our cases below, deermne wheher he car s accelerang a car on a la low rcon dynamcs rack, whch has been gen an nal push (Deermne s accelerang aer he nal push. ) a car on a led rack, released rom he op o he rack beore hs he boom bumper, as n par 5.1.a. a car on a led rack, as n par 5.1.a, ha has been released rom he op o he rack, allowed o h he boom bumper and connue back up he rack (consder he moon aer has h he bumper and s mong up he rack) a car wh a an (oban hs rom an nsrucor) on op o wh he an runnng, on a la low rcon dynamcs rack b. Clck on hs lnk o open he le poson, elocy, and acceleraon and use he moon deecor o plo he acceleraon s. me or each o he cases n par 5..a. Is he daa conssen wh your answers o 5..a? c. Consder he ollowng dagram. 10

11 () Calculae he aerage acceleraon or each segmen. () Calculae he slope o he lne or each segmen. d. Dscuss he saemen: The acceleraon s he rae o change o elocy wh me. Dscuss he saemen: The acceleraon s he slope o a elocy s. me graph. e. Use he moon deecor o plo poson s. me, elocy s. me, and acceleraon s. me or a car on a led (a a small angle) low rcon dynamcs rack or a me long enough or he car o bounce o he bumper hree mes. Dscuss how he acceleraon s he slope o he elocy s. me graph and he elocy s he slope o he poson s. me graph or each segmen. Dscuss he graphs wh an nsrucor. Equpmen Ls: Moon deecor LabPro Compuer Inerace LoggerPro soware Low Frcon Dynamc Track Car Rod Sand Book Soball Bo Coee ler Alumnum Fol Super Ball 6.1 Consder he ollowng graph o acceleraon s. me. 11

12 a. For he me neral s 6s, wha s he aerage acceleraon? Eplan. Would he aerage acceleraon be deren or a deren me neral? Eplan. b. I he acceleraon o an objec remans consan, wha saemen can you make abou he aerage acceleraon? Eplan. c. Descrbe any cases you can hnk o where he acceleraon o a mong objec remans consan. 6. Hang a moon deecor rom he celng wh he sde wh he sensor owards he loor. a. Open he poson, elocy, and acceleraon le and se he epermen lengh or 1s. Use he moon deecor o plo he acceleraon s. me or each o he ollowng cases: () Drop a book rom 0.5m below he deecor o he loor. () Drop a soball rom 0.5m below he deecor o he loor. () Drop a bo rom 0.5m below he deecor o he loor. b. Compare he acceleraons o he hree objecs n par 6..a. For each objec, s he acceleraon appromaely consan whle he objec s allng? Eplan. c. Do all objecs allng owards he earh all wh he same acceleraon? Eplan. d. Use he moon deecor o plo he acceleraon s. me or each o he ollowng cases: () Drop a coee ler rom 0.5m below he deecor o he loor. () Drop a pece o alumnum ol rom 0.5m below he deecor o he loor. () Drop a super ball rom 0.5m below he deecor o he loor. e. For whch o he objecs you hae obsered n pars a and d s here ery lle ar rcon? For whch o he objecs you hae obsered n pars a and d s here a lo o ar rcon? 1

13 Eense epermens hae been done ha ndcae ha all objecs all owards he earh wh a consan acceleraon ar rcon s neglgble (here s ery lle ar rcon). The magnude o ha acceleraon s appromaely 9.8m/s near he surace o he Earh. The symbol g s oen used o represen he magnude o hs acceleraon (g = 9.8m/s ). I you dd no ge good daa or he super ball, look a hs le. Take noe a he acceleraon, on aerage, s 9.8m/s.. For he objecs you obsered n pars a and d or whch here was ery lle ar rcon, how does he acceleraon compare o he alue 9.8m/s? 6.3 Use he moon deecor o plo he acceleraon s. me or a car on a low rcon dynamcs rack led a a small angle. a. Whle he car s on he rack, ecep when hs he bumper, s he acceleraon consan? Eplan. b. When he acceleraon s consan, descrbe he graph o elocy s. me. For he graph n 6.1.a, draw a possble graph o elocy s. me. Dscuss your answer wh an nsrucor. c. I can be shown, ha or a sragh lne graph ha he aerage alue beween wo pons on he lne s he alue o he pon halway beween he wo pons. For eample, or a plo o elocy s. me, he wo pons chosen are 1 and, as shown n he dagram, + below, he aerage alue oer he me neral 1 o s =, as shown. Very he equaon = +, usng he elocy s. me graph you generaed n 6.3.a. Snce he elocy s. me graph s always a sragh lne or he case o consan + acceleraon, he equaon = s always rue or consan acceleraon. Equpmen Ls: 13

14 Moon deecor LabPro Compuer Inerace LoggerPro soware Low Frcon Dynamc Track Car Car wh an accessory Rod Sand Meer Sck 7.1 For objecs mong a consan acceleraon, he hree equaons below can be appled. = a = + = I s also possble o manpulae hese hree equaons o oban our knemacs equaons or use n descrbng objecs mong a consan acceleraon. These equaons are gen below. ( ) ( ) ( ) ( ) ( ) - a a 1 - a - = + = = + = where, he nal me mnus he nal me, s he me neral, (he nal poson mnus he nal poson) s he dsance raeled, and are he nal and nal eloces and ā s he acceleraon. These equaons are somemes wren as 14

15 where = s he me neral. + - = = a a - ( - ) = = + These equaons are ald only or he case o consan acceleraon. a. Se up an epermen wh consan acceleraon ha wll allow you o measure poson, elocy and acceleraon as a uncon o me wh he moon deecor and ery he our knemacs equaons gen aboe. b. Hae someone hold a meer sck, as he person on he rgh n he pcure below. A second person places hs/her hands near he boom o he meer sck wh humb and orenger so ha hey can cach he meer sck when alls. Record he poson o he second person s humb and orenger (wha number on he meer sck hey are algned wh). Hae he person holdng he meer sck release he meer sck (The person should jus release all o a sudden.). The second person should cach as soon as hey percee s released. Record he poson o he person s humb and orenger aer hey hae caugh he meer sck. Deermne he dsance he meer sck ell. Use one o he knemacs equaons o deermne he person s reacon me. Deermne he reacon me or each person n your group. 1 a (rom Fundamenals o College Physcs nd Edon by Peer J. Nolan, Wm. C. Brown Publshers, Chcago, 1995) 15

16 SUMMARY You should be able o descrbe n words he moon o an objec ha would produce a parcular graph o poson, elocy or acceleraon s. me. Gen he moon o an objec, you should be able o draw he poson, elocy, and acceleraon graphs. Gen a parcular graph (eher poson, elocy or acceleraon), you should be able o draw oher graphs: or eample, gen a poson graph, you should be able o draw he elocy and acceleraon graphs. You should undersand he mahemacal denon o aerage elocy, be able o use, and undersand ha elocy s he rae o change o poson and can be ound rom he slope o he poson graph. You should undersand he mahemacal denon o aerage acceleraon, be able o use, and undersand ha acceleraon s he rae o change o elocy and can be ound rom he slope o he elocy graph. You should be able o use he knemacs equaons or he case o consan acceleraon o descrbe he moon o mong objecs and o sole or unknown parameers. 16

Chapters 2 Kinematics. Position, Distance, Displacement

Chapters 2 Kinematics. Position, Distance, Displacement Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen

More information

PHYS 1443 Section 001 Lecture #4

PHYS 1443 Section 001 Lecture #4 PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law

More information

Displacement, Velocity, and Acceleration. (WHERE and WHEN?)

Displacement, Velocity, and Acceleration. (WHERE and WHEN?) Dsplacemen, Velocy, and Acceleraon (WHERE and WHEN?) Mah resources Append A n your book! Symbols and meanng Algebra Geomery (olumes, ec.) Trgonomery Append A Logarhms Remnder You wll do well n hs class

More information

WebAssign HW Due 11:59PM Tuesday Clicker Information

WebAssign HW Due 11:59PM Tuesday Clicker Information WebAssgn HW Due 11:59PM Tuesday Clcker Inormaon Remnder: 90% aemp, 10% correc answer Clcker answers wll be a end o class sldes (onlne). Some days we wll do a lo o quesons, and ew ohers Each day o clcker

More information

CHAPTER 2 Quick Quizzes

CHAPTER 2 Quick Quizzes CHAPTER Quck Quzzes (a) 00 yd (b) 0 (c) 0 (a) False The car may be slowng down, so ha he drecon o s acceleraon s oppose he drecon o s elocy (b) True I he elocy s n he drecon chosen as negae, a pose acceleraon

More information

Motion in Two Dimensions

Motion in Two Dimensions Phys 1 Chaper 4 Moon n Two Dmensons adzyubenko@csub.edu hp://www.csub.edu/~adzyubenko 005, 014 A. Dzyubenko 004 Brooks/Cole 1 Dsplacemen as a Vecor The poson of an objec s descrbed by s poson ecor, r The

More information

First-order piecewise-linear dynamic circuits

First-order piecewise-linear dynamic circuits Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por

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

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

Chapter 3: Vectors and Two-Dimensional Motion

Chapter 3: Vectors and Two-Dimensional Motion Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon

More information

Chapter Lagrangian Interpolation

Chapter Lagrangian Interpolation Chaper 5.4 agrangan Inerpolaon Afer readng hs chaper you should be able o:. dere agrangan mehod of nerpolaon. sole problems usng agrangan mehod of nerpolaon and. use agrangan nerpolans o fnd deraes and

More information

The ray paths and travel times for multiple layers can be computed using ray-tracing, as demonstrated in Lab 3.

The ray paths and travel times for multiple layers can be computed using ray-tracing, as demonstrated in Lab 3. C. Trael me cures for mulple reflecors The ray pahs ad rael mes for mulple layers ca be compued usg ray-racg, as demosraed Lab. MATLAB scrp reflec_layers_.m performs smple ray racg. (m) ref(ms) ref(ms)

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

More information

One-Dimensional Kinematics

One-Dimensional Kinematics One-Dimensional Kinemaics One dimensional kinemaics refers o moion along a sraigh line. Een hough we lie in a 3-dimension world, moion can ofen be absraced o a single dimension. We can also describe moion

More information

Chapter 3 Kinematics in Two Dimensions

Chapter 3 Kinematics in Two Dimensions Chaper 3 KINEMATICS IN TWO DIMENSIONS PREVIEW Two-dimensional moion includes objecs which are moing in wo direcions a he same ime, such as a projecile, which has boh horizonal and erical moion. These wo

More information

s in boxe wers ans Put

s in boxe wers ans Put Pu answers in boxes Main Ideas in Class Toda Inroducion o Falling Appl Old Equaions Graphing Free Fall Sole Free Fall Problems Pracice:.45,.47,.53,.59,.61,.63,.69, Muliple Choice.1 Freel Falling Objecs

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

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

Main Ideas in Class Today

Main Ideas in Class Today Main Ideas in Class Toda Inroducion o Falling Appl Consan a Equaions Graphing Free Fall Sole Free Fall Problems Pracice:.45,.47,.53,.59,.61,.63,.69, Muliple Choice.1 Freel Falling Objecs Refers o objecs

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

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

Energy Storage Devices

Energy Storage Devices Energy Sorage Deces Objece of Lecure Descrbe he consrucon of a capacor and how charge s sored. Inroduce seeral ypes of capacors Dscuss he elecrcal properes of a capacor The relaonshp beween charge, olage,

More information

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations. Soluons o Ordnary Derenal Equaons An ordnary derenal equaon has only one ndependen varable. A sysem o ordnary derenal equaons consss o several derenal equaons each wh he same ndependen varable. An eample

More information

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he

More information

I. OBJECTIVE OF THE EXPERIMENT.

I. OBJECTIVE OF THE EXPERIMENT. I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in

More information

Physics 201 Lecture 2

Physics 201 Lecture 2 Physcs 1 Lecure Lecure Chper.1-. Dene Poson, Dsplcemen & Dsnce Dsngush Tme nd Tme Inerl Dene Velocy (Aerge nd Insnneous), Speed Dene Acceleron Undersnd lgebrclly, hrough ecors, nd grphclly he relonshps

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

Phys 231 General Physics I Lecture 2 1

Phys 231 General Physics I Lecture 2 1 Phys 3 General Physcs I Lecure Fr. 9/0.6-.0 Velocy & Momenum RE.b Mon. 9/3 Tues. 9/4.-.3, (.9,.0) Momenum Prncple & Smple Eamples RE.a EP, HW: Ch Pr.98 Se up compuer or clckers wh se parcpans Dsrbue clckers

More information

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current : . A. IUITS Synopss : GOWTH OF UNT IN IUIT : d. When swch S s closed a =; = d. A me, curren = e 3. The consan / has dmensons of me and s called he nducve me consan ( τ ) of he crcu. 4. = τ; =.63, n one

More information

Chapter 12: Velocity, acceleration, and forces

Chapter 12: Velocity, acceleration, and forces To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable

More information

Page 1 o 13 1. The brighes sar in he nigh sky is α Canis Majoris, also known as Sirius. I lies 8.8 ligh-years away. Express his disance in meers. ( ligh-year is he disance coered by ligh in one year. Ligh

More information

II. Light is a Ray (Geometrical Optics)

II. Light is a Ray (Geometrical Optics) II Lgh s a Ray (Geomercal Opcs) IIB Reflecon and Refracon Hero s Prncple of Leas Dsance Law of Reflecon Hero of Aleandra, who lved n he 2 nd cenury BC, posulaed he followng prncple: Prncple of Leas Dsance:

More information

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!) i+1,q - [(! ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal

More information

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class

More information

Physics 101: Lecture 03 Kinematics Today s lecture will cover Textbook Sections (and some Ch. 4)

Physics 101: Lecture 03 Kinematics Today s lecture will cover Textbook Sections (and some Ch. 4) Physics 101: Lecure 03 Kinemaics Today s lecure will coer Texbook Secions 3.1-3.3 (and some Ch. 4) Physics 101: Lecure 3, Pg 1 A Refresher: Deermine he force exered by he hand o suspend he 45 kg mass as

More information

Best test practice: Take the past test on the class website

Best test practice: Take the past test on the class website Bes es pracice: Take he pas es on he class websie hp://communiy.wvu.edu/~miholcomb/phys11.hml I have posed he key o he WebAssign pracice es. Newon Previous Tes is Online. Forma will be idenical. You migh

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

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

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

Kinematics in two dimensions

Kinematics in two dimensions Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5

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

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

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

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

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

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

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes. umercal negraon of he dffuson equaon (I) Fne dfference mehod. Spaal screaon. Inernal nodes. R L V For hermal conducon le s dscree he spaal doman no small fne spans, =,,: Balance of parcles for an nernal

More information

s = rθ Chapter 10: Rotation 10.1: What is physics?

s = rθ Chapter 10: Rotation 10.1: What is physics? Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous

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

UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION

UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION INTERNATIONAL TRADE T. J. KEHOE UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 27 EXAMINATION Please answer wo of he hree quesons. You can consul class noes, workng papers, and arcles whle you are workng on he

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

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

Vibrations and Waves

Vibrations and Waves Chaper 3 3 Vbraons and Waes PROBEM SOUIONS 3. (a) ang o he rgh as pose, he sprng orce acng on he bloc a he nsan o release s F s 30 N 0.3 7 N or 7 N o he le A hs nsan, he acceleraon s a F s 7 N 0.60 g 8

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

Q2.4 Average velocity equals instantaneous velocity when the speed is constant and motion is in a straight line.

Q2.4 Average velocity equals instantaneous velocity when the speed is constant and motion is in a straight line. CHAPTER MOTION ALONG A STRAIGHT LINE Discussion Quesions Q. The speedomeer measures he magniude of he insananeous eloci, he speed. I does no measure eloci because i does no measure direcion. Q. Graph (d).

More information

Mach Effect Thrusters (Mets) And Over-Unity Energy Production. Professor Emeritus Jim Woodward CalState Fullerton, Dept. of Physics.

Mach Effect Thrusters (Mets) And Over-Unity Energy Production. Professor Emeritus Jim Woodward CalState Fullerton, Dept. of Physics. Mach ec Thrusers (Mes) And Over-Uny nergy Producon Proessor merus Jm Woodward CalSae ulleron, Dep. o Physcs 13 November, 2015 We rounely hear a crcsm o MTs based upon an argumen ha clams: a MT s operaed

More information

Variants of Pegasos. December 11, 2009

Variants of Pegasos. December 11, 2009 Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on

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

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

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL Sco Wsdom, John Hershey 2, Jonahan Le Roux 2, and Shnj Waanabe 2 Deparmen o Elecrcal Engneerng, Unversy o Washngon, Seale, WA, USA

More information

Velocity is a relative quantity

Velocity is a relative quantity Veloci is a relaie quani Disenangling Coordinaes PHY2053, Fall 2013, Lecure 6 Newon s Laws 2 PHY2053, Fall 2013, Lecure 6 Newon s Laws 3 R. Field 9/6/2012 Uniersi of Florida PHY 2053 Page 8 Reference Frames

More information

Topic Astable Circuits. Recall that an astable circuit has two unstable states;

Topic Astable Circuits. Recall that an astable circuit has two unstable states; Topic 2.2. Asable Circuis. Learning Objecives: A he end o his opic you will be able o; Recall ha an asable circui has wo unsable saes; Explain he operaion o a circui based on a Schmi inverer, and esimae

More information

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18 A Firs ourse on Kineics and Reacion Engineering lass 19 on Uni 18 Par I - hemical Reacions Par II - hemical Reacion Kineics Where We re Going Par III - hemical Reacion Engineering A. Ideal Reacors B. Perfecly

More information

[Link to MIT-Lab 6P.1 goes here.] After completing the lab, fill in the following blanks: Numerical. Simulation s Calculations

[Link to MIT-Lab 6P.1 goes here.] After completing the lab, fill in the following blanks: Numerical. Simulation s Calculations Chaper 6: Ordnary Leas Squares Esmaon Procedure he Properes Chaper 6 Oulne Cln s Assgnmen: Assess he Effec of Sudyng on Quz Scores Revew o Regresson Model o Ordnary Leas Squares () Esmaon Procedure o he

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

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

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

Review Equations. Announcements 9/8/09. Table Tennis

Review Equations. Announcements 9/8/09. Table Tennis Announcemens 9/8/09 1. Course homepage ia: phsics.bu.edu Class web pages Phsics 105 (Colon J). (Class-wide email sen) Iclicker problem from las ime scores didn ge recorded. Clicker quizzes from lecures

More information

Notes on the stability of dynamic systems and the use of Eigen Values.

Notes on the stability of dynamic systems and the use of Eigen Values. Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon

More information

x i v x t a dx dt t x

x i v x t a dx dt t x Physics 3A: Basic Physics I Shoup - Miderm Useful Equaions A y A sin A A A y an A y A A = A i + A y j + A z k A * B = A B cos(θ) A B = A B sin(θ) A * B = A B + A y B y + A z B z A B = (A y B z A z B y

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

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm H ( q, p, ) = q p L( q, q, ) H p = q H q = p H = L Equvalen o Lagrangan formalsm Smpler, bu

More information

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese

More information

Equations of motion for constant acceleration

Equations of motion for constant acceleration Lecure 3 Chaper 2 Physics I 01.29.2014 Equaions of moion for consan acceleraion Course websie: hp://faculy.uml.edu/andriy_danylo/teaching/physicsi Lecure Capure: hp://echo360.uml.edu/danylo2013/physics1spring.hml

More information

SPH3U1 Lesson 03 Kinematics

SPH3U1 Lesson 03 Kinematics SPH3U1 Lesson 03 Kinemaics GRAPHICAL ANALYSIS LEARNING GOALS Sudens will Learn how o read values, find slopes and calculae areas on graphs. Learn wha hese values mean on boh posiion-ime and velociy-ime

More information

Two Dimensional Dynamics

Two Dimensional Dynamics Physics 11: Lecure 6 Two Dimensional Dynamics Today s lecure will coer Chaper 4 Exam I Physics 11: Lecure 6, Pg 1 Brie Reiew Thus Far Newon s Laws o moion: SF=ma Kinemaics: x = x + + ½ a Dynamics Today

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm Hqp (,,) = qp Lqq (,,) H p = q H q = p H L = Equvalen o Lagrangan formalsm Smpler, bu wce as

More information

Homework 8: Rigid Body Dynamics Due Friday April 21, 2017

Homework 8: Rigid Body Dynamics Due Friday April 21, 2017 EN40: Dynacs and Vbraons Hoework 8: gd Body Dynacs Due Frday Aprl 1, 017 School of Engneerng Brown Unversy 1. The earh s roaon rae has been esaed o decrease so as o ncrease he lengh of a day a a rae of

More information

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue.

. The geometric multiplicity is dim[ker( λi. number of linearly independent eigenvectors associated with this eigenvalue. Lnear Algebra Lecure # Noes We connue wh he dscusson of egenvalues, egenvecors, and dagonalzably of marces We wan o know, n parcular wha condons wll assure ha a marx can be dagonalzed and wha he obsrucons

More information

Two Dimensional Dynamics

Two Dimensional Dynamics Physics 11: Lecure 6 Two Dimensional Dynamics Today s lecure will coer Chaper 4 Saring Wed Sep 15, W-F oice hours will be in 3 Loomis. Exam I M oice hours will coninue in 36 Loomis Physics 11: Lecure 6,

More information

Example: MOSFET Amplifier Distortion

Example: MOSFET Amplifier Distortion 4/25/2011 Example MSFET Amplfer Dsoron 1/9 Example: MSFET Amplfer Dsoron Recall hs crcu from a prevous handou: ( ) = I ( ) D D d 15.0 V RD = 5K v ( ) = V v ( ) D o v( ) - K = 2 0.25 ma/v V = 2.0 V 40V.

More information

Advanced time-series analysis (University of Lund, Economic History Department)

Advanced time-series analysis (University of Lund, Economic History Department) Advanced me-seres analss (Unvers of Lund, Economc Hsor Dearmen) 3 Jan-3 Februar and 6-3 March Lecure 4 Economerc echnues for saonar seres : Unvarae sochasc models wh Box- Jenns mehodolog, smle forecasng

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

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

Momentum. Momentum. Impulse. Momentum and Collisions

Momentum. Momentum. Impulse. Momentum and Collisions Momentum Momentum and Collsons From Newton s laws: orce must be present to change an object s elocty (speed and/or drecton) Wsh to consder eects o collsons and correspondng change n elocty Gol ball ntally

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

Today s topic: IMPULSE AND MOMENTUM CONSERVATION

Today s topic: IMPULSE AND MOMENTUM CONSERVATION Today s opc: MPULSE ND MOMENTUM CONSERVTON Reew of Las Week s Lecure Elasc Poenal Energy: x: dsplaceen fro equlbru x = : equlbru poson Work-Energy Theore: W o W W W g noncons W non el W noncons K K K (

More information

CHAPTER 10: LINEAR DISCRIMINATION

CHAPTER 10: LINEAR DISCRIMINATION CHAPER : LINEAR DISCRIMINAION Dscrmnan-based Classfcaon 3 In classfcaon h K classes (C,C,, C k ) We defned dscrmnan funcon g j (), j=,,,k hen gven an es eample, e chose (predced) s class label as C f g

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

Energy Storage Devices

Energy Storage Devices Energy Srage Deces Objece f ecure Descrbe The cnsrucn f an nducr Hw energy s sred n an nducr The elecrcal prperes f an nducr Relanshp beween lage, curren, and nducance; pwer; and energy Equalen nducance

More information

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r.

Physics 3A: Basic Physics I Shoup Sample Midterm. Useful Equations. x f. x i v x. a x. x i. v xi v xf. 2a x f x i. y f. a r. Physics 3A: Basic Physics I Shoup Sample Miderm Useful Equaions A y Asin A A x A y an A y A x A = A x i + A y j + A z k A * B = A B cos(θ) A x B = A B sin(θ) A * B = A x B x + A y B y + A z B z A x B =

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

Bag for Sophia by Leonie Bateman and Deirdre Bond-Abel

Bag for Sophia by Leonie Bateman and Deirdre Bond-Abel Bag for Sopha 2012 by Leone Baeman and Derdre Bond-Abel Ths bag was desgned o go wh he beauful feled wool scarf of our book Elegan Quls, Counry Charm. Make boh and you ll have he perfec ensemble o wear

More information

Name: PHYS 110 Dr. McGovern Spring 2018 Exam 1. Multiple Choice: Circle the answer that best evaluates the statement or completes the statement.

Name: PHYS 110 Dr. McGovern Spring 2018 Exam 1. Multiple Choice: Circle the answer that best evaluates the statement or completes the statement. Name: PHYS 110 Dr. McGoern Sprng 018 Exam 1 Multple Choce: Crcle the answer that best ealuates the statement or completes the statement. #1 - I the acceleraton o an object s negate, the object must be

More information

Problem Set 5. Graduate Macro II, Spring 2017 The University of Notre Dame Professor Sims

Problem Set 5. Graduate Macro II, Spring 2017 The University of Notre Dame Professor Sims Problem Se 5 Graduae Macro II, Spring 2017 The Universiy of Nore Dame Professor Sims Insrucions: You may consul wih oher members of he class, bu please make sure o urn in your own work. Where applicable,

More information

12d Model. Civil and Surveying Software. Drainage Analysis Module Detention/Retention Basins. Owen Thornton BE (Mech), 12d Model Programmer

12d Model. Civil and Surveying Software. Drainage Analysis Module Detention/Retention Basins. Owen Thornton BE (Mech), 12d Model Programmer d Model Cvl and Surveyng Soware Dranage Analyss Module Deenon/Reenon Basns Owen Thornon BE (Mech), d Model Programmer owen.hornon@d.com 4 January 007 Revsed: 04 Aprl 007 9 February 008 (8Cp) Ths documen

More information

total distance cov ered time int erval v = average speed (m/s)

total distance cov ered time int erval v = average speed (m/s) Physics Suy Noes Lesson 4 Linear Moion 1 Change an Moion a. A propery common o eeryhing in he unierse is change. b. Change is so imporan ha he funamenal concep of ime woul be meaningless wihou i. c. Since

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics /9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon

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

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