Chapter 7 Impulse and Momentum

Size: px
Start display at page:

Download "Chapter 7 Impulse and Momentum"

Transcription

1 Chapter 7 Ipulse and Mentu Gals r Chapter 7 T study pulse and entu. T understand cnseratn entu. T study entu changes durng cllsns. T understand center ass and hw rces act n the c... T apply entu t rcket prpulsn. When the bat strkes the ball, the agntude the rce exerted n the ball rses t a axu alue and then returns t zer DEINITION O IMPULSE The pulse a rce s the prduct the aerage rce and the te nteral durng whch the rce acts: J t The cllsn te between a bat and a ball s ery shrt, ten less than a llsecnd, but the rce can be qute large. The te nteral durng whch the rce acts s t, and the agntude the aerage rce s. Ipulse s a ectr quantty and has the sae drectn as the aerage rce. SI unt: newtn secnds (N s) Mentu transer (cllsn) tescales Cllsns typcally nle nteractns that happen quckly. rce and Ipulse sae area Durng ths bre te, the rces nled can be qute large t t t bg, sall t t J t ntal nal The balls are n cntact r a ery shrt te. V t t t t t sall, bg

2 DEINITION O LINEAR MOMENTUM p The lnear entu an bject s the prduct the bject s ass tes ts elcty: SI unt: klgra eter/secnd (kg /s) Lnear Mentu Mentu a partcle s dened as the prduct ts ass and elcty p Mentu cpnents p x = x and p y = y Apples t tw-densnal tn as well Mentu (agntude) s related t knetc energy K p Relatn between Ipulse and Mentu (Newtn nd) a a t t t IMPULSE-MOMENTUM THEOREM When a net rce acts n an bject, the pulse ths rce s equal t the change n the entu the bject pulse t J p t nal entu ntal entu Ipulse s a ectr quantty; SI Unt: N s r kg / s pulse = change n entu! Ipulse and aerage rce We can use the ntn pulse t dene aerage rce, whch s a useul cncept. Dene aerage rce such that (een s nt cnstant), pulse s gen by a Exaple: A Well Ht Ball A baseball ( = 0.4 kg) has an ntal elcty = - 38 /s as t appraches a bat. The bat apples an aerage rce that s uch larger than the weght the ball, and the ball departs r the bat wth a nal elcty = 58 /s. (a) Deterne the pulse appled t the ball by the bat. (b) Assung that the te cntact s t = s, nd the aerage rce exerted n the ball by the bat. J a (t t ) a t r: a p t

3 Exaple : A Ranstr Ran ces dwn wth a elcty -5 /s and hts the r a car. The ass ran per secnd that strkes the r the car s kg/s. Assung that ran ces t rest upn strkng the car, nd the aerage rce exerted by the ran n the r. t t Neglectng the weght the randrps, the net rce n a randrp s sply the rce n the randrp due t the r. t kg s5 s 0.90 N (rce n the randrp) n-the-r = (Newtn s thrd law) Cnceptual Exaple: Halstnes ersus Randrps Instead ran, suppse hal s allng. Unlke ran, hal usually bunces the r the car. I hal ell nstead ran, wuld the rce be saller than, equal t, r greater than that calculated preusly? J t t r a randrp, the change n elcty s r (dwnward) t zer. r a halstne, the change s r (dwnward) t (upward). Thus halstnes hae a larger t Ipulse appled t aut cllsns The st prtant actr s the cllsn te r the te t takes the persn t ce t a rest Ths wll reduce the chance dyng n a car crash Ways t ncrease the te Seat belts Ar bags a p ( ) t t The ar bag ncreases the te the cllsn and absrbs se the energy r the bdy Cnseratn Lnear Mentu WORK-ENERGY THEOREM CONSERVATION O ENERGY Apply the pulse-entu there t the dar cllsn IMPULSE-MOMENTUM between tw bjects.. THEOREM??? Internal rces rces that bjects wthn the syste exert n each ther. External rces rces exerted n bjects by agents external t the syste. e.g. Weght=W Cnseratn Lnear Mentu t OBJECT W t OBJECT W t Cnseratn Lnear Mentu W t + W t W W t The nternal rces cancel ut. P Cnsder syste: bth bjects nled P

4 Prncple Cnseratn Lnear Mentu W W t P P su aerageexternalrcest I the su the external rces s zer, then P P P P 0 P P CONSERVATION O LINEAR MOMENTUM The ttal lnear entu an slated syste s cnstant (cnsered). An slated syste s ne r whch the su the aerage external rces actng n the syste s zer. Dentn Ttal Mentu r a Syste Partcles r a syste partcles the ttal entu P s the ectr su the nddual partcle enta: P p A p B p... cpnents ttal entu P (p A C p B p P p x P p y...) A,x A,y P The entu each bject wll change The ttal entu the syste reans cnstant there are n external rces C A A net B B C C pb,x... p... t B.y N N p... Exaple: Asseblng a reght Tran A reght tran s beng assebled n a swtchng yard. Car has a ass = kg and es at a elcty 0 = /s. Car, wth a ass = kg and a elcty 0 = +.3 /s, ertakes car and cuples t t. Neglectng rctn, nd the cn elcty the cars ater they bece cupled. Exaple: Recl a rle A arksan hlds a 3.00 kg rle lsely, allwng t t recl reely when red, and res a bullet ass 5.00 g hrzntally wth a speed B = 300 /s. What s the recl speed the rle? = PT P R P B Bere PT 0 Ater P R P B 0 0 B B R R B R B / s R Cncept Test: Expldng Prjectle A del rcket traels as a prjectle n a parablc path ater ts rst stage burns ut. At the tp ts trajectry, where ts elcty pnts hrzntally t the rght, a sall explsn separates t nt tw sectns wth equal asses. One sectn alls straght dwn, wth n hrzntal tn. What s the drectn the ther part just ater the explsn? A. Up and t the let B. Straght up C. Up and t the rght bere Exaple: Mentu Cnseratn A bx wth ass = 6.0 kg sldes wth speed = 4.0 /s acrss a rctnless lr n the pste drectn an x axs. It suddenly expldes nt tw peces. One pece, wth ass =.0 kg, es n the pste x-drectn wth speed = 8.0 /s. What s the elcty the secnd pece, wth ass = 4.0 kg? ater

5 Exaple: Cnseratn Lnear Mentu - Ice Skaters Startng r rest, tw skaters push aganst each ther n ce where rctn s neglgble. One s a 54-kg wan and ne s a 88-kg an. The wan es away wth a speed +.5 /s. nd the recl elcty the an. P P 54kg.5 s.5 88kg s 0 Cncept Test: Cnseratn Mentu A by stands at ne end a latng rat that s statnary relate t the shre. He then walks t the ppste end, twards the shre. Des the rat e (assue n rctn)?. N, t wll nt e at all. Yes, t wll e away r the shre 3. Yes, t wll e twards the shre Nte: Snce entu s cnsered n the by-rat syste and nether was ng at rst, the rat ust e n the drectn ppste t the by s. In Cllssns Ttal Mentu s Cnsered In cllsns, we assue that external rces ether su t zer, r are sall enugh t be gnred. Hence, entu s cnsered n all cllsns. A cllsn ay be the result physcal cntact between tw bjects Cntact ay als arse r the electrstatc nteractns the electrns n the surace ats the bdes Matheatcally (r tw bjects): Mentu s cnsered r the syste bjects The syste ncludes all the bjects nteractng wth each ther Assues nly nternal rces are actng durng the cllsn Can be generalzed t any nuber bjects Types Cllsns Mentu s cnsered n any cllsn Elastc cllsns bth entu and knetc energy are cnsered Inelastc cllsns Knetc energy s nt cnsered Se the knetc energy s cnerted nt ther types energy such as heat, sund, wrk t peranently der an bject Perectly nelastc cllsns ccur when the bjects stck tgether Nt all the KE s necessarly lst Mst cllsns all between elastc and perectly nelastc cllsns Elastc Cllsns Elastc eans that knetc energy s cnsered as well as entu. Ths ges us re cnstrants We can sle re cplcated prbles!! Bllards (-D cllsn) The clldng bjects hae separate tns ater the cllsn as well as bere. rst: spler -D prble Intal nal Inelastc and Elastc Cllsns A cpletely nelastc cllsn An elastc cllsn

6 Applyng the Prncple Cnseratn Mentu. Decde whch bjects are ncluded n the syste.. Relate t the syste, denty the nternal and external rces. 3. Very that the syste s slated. 4. Set the nal entu the syste equal t ts ntal entu. Reeber that entu s a ectr. Prble Slng r One-Densnal Cllsns Set up a crdnate axs and dene the elctes wth respect t ths axs It s cnenent t ake yur axs cncde wth ne the ntal elctes In yur sketch, draw all the elcty ectrs wth labels ncludng all the gen nratn Draw bere and ater sketches Label each bject nclude the drectn elcty keep track subscrpts Prble Slng r One-Densnal Cllsns Sketch r perectly nelastc clllsn The bjects stck tgether Include all the elcty drectns The ater cllsn cbnes the asses Wrte the expressns r the entu each bject bere and ater the cllsn Reeber t nclude the apprprate sgns Wrte an expressn r the ttal entu bere and ater the cllsn --- entu the syste s cnsered I the cllsn s nelastc, sle the entu equatn r the unknwn --- Reeber, KE s nt cnsered I the cllsn s elastc, yu can use the KE equatn t sle r tw unknwns Perectly Inelastc Cllsns Suppse, r exaple, =0. Cnseratn entu beces ( ) 0 ( ) E.g., 000 kg, (000kg)(50 s) 0 (500kg) 4 50 kg s 0 s kg 500 kg :, Perectly Inelastc Cllsns What aunt KE lst durng cllsn? KE bere (000 kg)(50 s) KEater ( ) (500 kg)(0 s) KE lst J lst n heat and sund 6.50 J J Exaple: A Ballstc Pendulu The ass the blck wd s.50-kg and the ass the bullet s kg. The blck swngs t a axu heght abe the ntal pstn. nd the ntal speed the bullet. Apply cnseratn entu t the cllsn:

7 Applyng cnseratn energy t the swngng tn: gh gh gh g h s Elastc Cllsns Bth entu and knetc energy are cnsered Typcally hae tw unknwns Sle the equatns sultaneusly s s kg.50 kg kg Incng and utgng elctes are ery ass dependant ass ntally at rest Tw-densnal Cllsns r a general cllsn tw bjects n threedensnal space, the cnseratn entu prncple Elastc Cllsn () () ples that the ttal entu the syste n each drectn s cnsered Use subscrpts r dentyng the bject, ntal and nal, and cpnents and x y x y x y x y A Cllsn n Tw Densns Use entu cnseratn t deterne the agntude and drectn the nal elcty ball ater the cllsn. x x x x y y y y

8 Center Mass The center ass s a pnt that represents the aerage lcatn r the ttal ass a syste. x c x x Center Mass Crdnates The crdnates the center ass are x y CM CM x y Tw asses n x-axs x x = M s the ttal ass CM the syste x Velcty Center Mass x c c x x x t In an slated syste, the ttal lnear entu des nt change, therere the elcty the center ass des nt change. p c c M x t c p p x t Exaple: Center Mass Mtn c = cnst. In slated syste BEORE c 0 Mtn the Center Mass The syste wll e as an external rce were appled t a sngle partcle ass M lcated at the center ass c ATER 88 kg.5 s 54 kg.5 s 88 kg 54 kg

WYSE Academic Challenge 2004 Sectional Physics Solution Set

WYSE Academic Challenge 2004 Sectional Physics Solution Set WYSE Acadec Challenge 004 Sectnal Physcs Slutn Set. Answer: e. The axu pssble statc rctn r ths stuatn wuld be: ax µ sn µ sg (0.600)(40.0N) 4.0N. Snce yur pushng rce s less than the axu pssble rctnal rce,

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

PHY2053 Summer 2012 Exam 2 Solutions N F o f k

PHY2053 Summer 2012 Exam 2 Solutions N F o f k HY0 Suer 0 Ea Slutns. he ree-bdy dagra r the blck s N F 7 k F g Usng Newtn s secnd law r the -cnents F a F F cs7 k 0 k F F cs7 (0 N ( Ncs7 N he wrk dne by knetc rctn k r csθ ( N(6 cs80 0 N. Mechancal energy

More information

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision?

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision? Experent 9 Conseraton o Lnear Moentu - Collsons In ths experent you wll be ntroduced to the denton o lnear oentu. You wll learn the derence between an elastc and an nelastc collson. You wll explore how

More information

Center of Mass and Momentum. See animation An Object Tossed Along a Parabolic Path.

Center of Mass and Momentum. See animation An Object Tossed Along a Parabolic Path. Readng: Chapter 9 The Center ass Center ass and mentum See anmatn An Object Tssed Alng a Parablc Path The center mass a bdy r a system bdes s the pnt that mves as thugh all the mass were cncentrated there

More information

Physics 105: Mechanics Lecture 13

Physics 105: Mechanics Lecture 13 Physcs 05: Mechancs Lecture 3 Wenda Cao NJIT Physcs Department Momentum and Momentum Conseraton Momentum Impulse Conseraton o Momentum Collsons Lnear Momentum A new undamental quantty, lke orce, energy

More information

Momentum and Collisions. Rosendo Physics 12-B

Momentum and Collisions. Rosendo Physics 12-B Moentu and Collsons Rosendo Physcs -B Conseraton o Energy Moentu Ipulse Conseraton o Moentu -D Collsons -D Collsons The Center o Mass Lnear Moentu and Collsons February 7, 08 Conseraton o Energy D E =

More information

Physic 231 Lecture 14

Physic 231 Lecture 14 Physc 3 Lecture 4 Man ponts o last lecture: Ipulses: orces that last only a short te Moentu p Ipulse-Moentu theore F t p ( ) Ipulse-Moentu theore ptot, p, p, p, p, ptot, Moentu and external orces F p ext

More information

p p +... = p j + p Conservation Laws in Physics q Physical states, process, and state quantities: Physics 201, Lecture 14 Today s Topics

p p +... = p j + p Conservation Laws in Physics q Physical states, process, and state quantities: Physics 201, Lecture 14 Today s Topics Physcs 0, Lecture 4 Conseraton Laws n Physcs q Physcal states, process, and state quanttes: Today s Topcs Partcle Syste n state Process Partcle Syste n state q Lnear Moentu And Collsons (Chapter 9.-9.4)

More information

Physics 101 Lecture 9 Linear Momentum and Collisions

Physics 101 Lecture 9 Linear Momentum and Collisions Physcs 0 Lecture 9 Lnear Momentum and Collsons Dr. Al ÖVGÜN EMU Physcs Department www.aogun.com Lnear Momentum and Collsons q q q q q q q Conseraton o Energy Momentum Impulse Conseraton o Momentum -D Collsons

More information

Lecture 09 Systems of Particles and Conservation of Linear Momentum

Lecture 09 Systems of Particles and Conservation of Linear Momentum Lecture 09 Systes o Partcles and Conseraton o Lnear oentu 9. Lnear oentu and Its Conseraton 9. Isolated Syste lnear oentu: P F dp dt d( dt d dt a solated syste F ext 0 dp dp F, F dt dt dp dp d F F 0, 0

More information

EMU Physics Department.

EMU Physics Department. Physcs 0 Lecture 9 Lnear Momentum and Collsons Assst. Pro. Dr. Al ÖVGÜN EMU Physcs Department www.aogun.com Lnear Momentum q Conseraton o Energy q Momentum q Impulse q Conseraton o Momentum q -D Collsons

More information

Energy & Work

Energy & Work rk Dne by a Cntant Frce 6.-6.4 Energy & rk F N m jule () J rk Dne by a Cntant Frce Example Pullng a Sutcae-n-heel Fnd the wrk dne the rce 45.0-N, the angle 50.0 degree, and the dplacement 75.0 m. 3 ( F

More information

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy Chapter 8 Moentu Ipulse and Collsons Analyss o oton: key deas Newton s laws o oton Conseraton o Energy Newton s Laws st Law: An object at rest or traelng n unor oton wll rean at rest or traelng n unor

More information

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy? Perod & Frequency Perod (T): Tme to complete one ull rotaton Frequency (): Number o rotatons completed per second. = 1/T, T = 1/ v = πr/t Work and Energy Work: W = F!d (pcks out parallel components) F

More information

Chapter 6 Work and Energy

Chapter 6 Work and Energy as p5309 L3 Chapter 6 rk and Energy Gals r Chapter 6 Study wrk as dened n physcs Relate wrk t knetc energy Cnsder wrk dne by a arable rce Study ptental energy Understand energy cnseratn Include tme and

More information

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions.

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions. Lesson 0: Collsons, Rotatonal netc Energy, Torque, Center o Graty (Sectons 7.8 Last te we used ewton s second law to deelop the pulse-oentu theore. In words, the theore states that the change n lnear oentu

More information

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum Physcs or Scentsts and Engneers Chapter 9 Impulse and Momentum Sprng, 008 Ho Jung Pak Lnear Momentum Lnear momentum o an object o mass m movng wth a velocty v s dened to be p mv Momentum and lnear momentum

More information

2015 Regional Physics Exam Solution Set

2015 Regional Physics Exam Solution Set 05 Reginal hysics Exa Slutin Set. Crrect answer: D Nte: [quantity] dentes: units f quantity WYSE Acadeic Challenge 05 Reginal hysics Exa SOLUTION SET r F r a lengthass length / tie ass length / tie. Crrect

More information

CHAPTER If two balls swing in initial momentum is 2 mv and balls 4 and 5 will swing out.

CHAPTER If two balls swing in initial momentum is 2 mv and balls 4 and 5 will swing out. HPTER 4 4. Slutn: Mentu s cnsered. Therefre 5 th ball es ut wth sae elcty as st ball n pact. 4. If tw balls swng n ntal entu s and balls 4 and 5 wll swng ut. 4.3 Slutn: L n L L n 4.4 Slutn: M b M. kg kg

More information

element k Using FEM to Solve Truss Problems

element k Using FEM to Solve Truss Problems sng EM t Slve Truss Prblems A truss s an engneerng structure cmpsed straght members, a certan materal, that are tpcall pn-ned at ther ends. Such members are als called tw-rce members snce the can nl transmt

More information

Physics 207, Lecture 13, Oct. 15. Energy

Physics 207, Lecture 13, Oct. 15. Energy Physcs 07 Lecture 3 Physcs 07, Lecture 3, Oct. 5 Goals: Chapter 0 Understand the relatonshp between moton and energy Dene Potental Energy n a Hooke s Law sprng Deelop and explot conseraton o energy prncple

More information

5/24/2007 Collisions ( F.Robilliard) 1

5/24/2007 Collisions ( F.Robilliard) 1 5/4/007 Collsons ( F.Robllard) 1 Interactons: In our earler studes o orce and work, we saw, that both these quanttes arse n the context o an nteracton between two bodes. We wll now look ore closely at

More information

Linear Momentum. Center of Mass.

Linear Momentum. Center of Mass. Lecture 16 Chapter 9 Physcs I 11.06.2013 Lnear oentu. Center of ass. Course webste: http://faculty.ul.edu/ndry_danylov/teachng/physcsi Lecture Capture: http://echo360.ul.edu/danylov2013/physcs1fall.htl

More information

Chapter 3 and Chapter 4

Chapter 3 and Chapter 4 Chapter 3 and Chapter 4 Chapter 3 Energy 3. Introducton:Work Work W s energy transerred to or rom an object by means o a orce actng on the object. Energy transerred to the object s postve work, and energy

More information

Chapter 8. Momentum, Impulse and Collisions (continued) 10/22/2014 Physics 218

Chapter 8. Momentum, Impulse and Collisions (continued) 10/22/2014 Physics 218 Chater 8 Moentu, Iulse and Collsons (contnued 0//04 Physcs 8 Learnng Goals The eanng of the oentu of a artcle(syste and how the ulse of the net force actng on a artcle causes the oentu to change. The condtons

More information

Physics 207: Lecture 20. Today s Agenda Homework for Monday

Physics 207: Lecture 20. Today s Agenda Homework for Monday Physcs 207: Lecture 20 Today s Agenda Homework for Monday Recap: Systems of Partcles Center of mass Velocty and acceleraton of the center of mass Dynamcs of the center of mass Lnear Momentum Example problems

More information

Collisions! Short, Sharp Shocks

Collisions! Short, Sharp Shocks d b n, b d,, -4 Introducng Collsons Quz 9 L9 Mult-artcle Systes 6-8 Scatterng 9- Collson Colcatons L Collsons 5, Derent Reerence Fraes ranslatonal ngular Moentu Quz RE a RE b RE c EP9 RE a; HW: Pr s 3*,,

More information

CHAPTER 6 WORK AND ENERGY

CHAPTER 6 WORK AND ENERGY CHAPTER 6 WORK AND ENERGY CONCEPTUAL QUESTIONS 16. REASONING AND SOLUTION A trapeze artist, starting rm rest, swings dwnward n the bar, lets g at the bttm the swing, and alls reely t the net. An assistant,

More information

Spring 2002 Lecture #17

Spring 2002 Lecture #17 1443-51 Sprng 22 Lecture #17 r. Jaehn Yu 1. Cndtns fr Equlbrum 2. Center f Gravty 3. Elastc Prpertes f Slds Yung s dulus Shear dulus ulk dulus Tday s Hmewrk Assgnment s the Hmewrk #8!!! 2 nd term eam n

More information

Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum

Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum Recall that there was ore to oton than just spee A ore coplete escrpton of oton s the concept of lnear oentu: p v (8.) Beng a prouct of a scalar () an a vector (v), oentu s a vector: p v p y v y p z v

More information

PHYS 1443 Section 002 Lecture #20

PHYS 1443 Section 002 Lecture #20 PHYS 1443 Secton 002 Lecture #20 Dr. Jae Condtons for Equlbru & Mechancal Equlbru How to Solve Equlbru Probles? A ew Exaples of Mechancal Equlbru Elastc Propertes of Solds Densty and Specfc Gravty lud

More information

Linear Momentum and Collisions

Linear Momentum and Collisions Lnear Momentum and Collsons Chater 9 Lnear Momentum [kg m/s] x y mv x mv y Newton s nd Law n terms o momentum: Imulse I - [kg m/s] I t t Fdt I = area under curve bounded by t axs Imulse-Momentum Theorem

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

ANALOG ELECTRONICS 1 DR NORLAILI MOHD NOH

ANALOG ELECTRONICS 1 DR NORLAILI MOHD NOH 24 ANALOG LTRONIS TUTORIAL DR NORLAILI MOHD NOH . 0 8kΩ Gen, Y β β 00 T F 26, 00 0.7 (a)deterne the dc ltages at the 3 X ternals f the JT (,, ). 0kΩ Z (b) Deterne g,r π and r? (c) Deterne the ltage gan

More information

PHYSICS 151 Notes for Online Lecture #23

PHYSICS 151 Notes for Online Lecture #23 PHYSICS 5 Ntes fr Online Lecture #3 Peridicity Peridic eans that sething repeats itself. r exaple, eery twenty-fur hurs, the Earth aes a cplete rtatin. Heartbeats are an exaple f peridic behair. If yu

More information

Linear Momentum. Equation 1

Linear Momentum. Equation 1 Lnear Momentum OBJECTIVE Obsere collsons between two carts, testng or the conseraton o momentum. Measure energy changes durng derent types o collsons. Classy collsons as elastc, nelastc, or completely

More information

Chapter 7. Impulse and Momentum

Chapter 7. Impulse and Momentum Chapter 7 Ipulse and Moentu 7. The Ipulse-Moentu Theore There are any situations when the force on an object is not constant. 7. The Ipulse-Moentu Theore DEFINITION OF IMPULSE The ipulse of a force is

More information

ME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function

ME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function Mdellng Physcal Systems The Transer Functn Derental Equatns U Plant Y In the plant shwn, the nput u aects the respnse the utput y. In general, the dynamcs ths respnse can be descrbed by a derental equatn

More information

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics Lecture 16 Chapter 11 Physcs I Energy Dsspaton Lnear Momentum Course webste: http://aculty.uml.edu/andry_danylov/teachng/physcsi Department o Physcs and Appled Physcs IN IN THIS CHAPTER, you wll learn

More information

Chapter 7. Impulse and Momentum

Chapter 7. Impulse and Momentum Chapter 7 Ipulse and Moentu 7. The Ipulse-Moentu Theore 7. The Ipulse-Moentu Theore There are any situations when the force on an object is not constant. 7. The Ipulse-Moentu Theore DEFINITION OF IMPULSE

More information

Physics 123. Exam #1. October 11, 2006

Physics 123. Exam #1. October 11, 2006 hyscs Exa # October, 006 roble /0 roble /0 roble /0 roble 4 /0 roble 5 /0 roble 6 /0 roble 7 /0 roble 8 /0 roble 9 /0 roble 0 /0 Total /00 Free-Response robles: lease show all work n order to receve partal

More information

Chapter 9 Linear Momentum and Collisions

Chapter 9 Linear Momentum and Collisions Chapter 9 Lnear Momentum and Collsons m = 3. kg r = ( ˆ ˆ j ) P9., r r (a) p m ( ˆ ˆj ) 3. 4. m s = = 9.. kg m s Thus, p x = 9. kg m s and p y =. kg m s (b) p px p y p y θ = tan = tan (.33) = 37 px = +

More information

CHAPTER 10 ROTATIONAL MOTION

CHAPTER 10 ROTATIONAL MOTION CHAPTER 0 ROTATONAL MOTON 0. ANGULAR VELOCTY Consder argd body rotates about a fxed axs through pont O n x-y plane as shown. Any partcle at pont P n ths rgd body rotates n a crcle of radus r about O. The

More information

(T > w) F R = T - w. Going up. T - w = ma

(T > w) F R = T - w. Going up. T - w = ma ANSES Suspended Acceleratng-Objects A resultant orce causes a syste to accelerate. he drecton o the acceleraton s n the drecton o the resultant orce. As llustrated belo, hen suspended objects accelerate,

More information

Solution to HW14 Fall-2002

Solution to HW14 Fall-2002 Slutin t HW14 Fall-2002 CJ5 10.CQ.003. REASONING AND SOLUTION Figures 10.11 and 10.14 shw the velcity and the acceleratin, respectively, the shadw a ball that underges unirm circular mtin. The shadw underges

More information

EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017

EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017 OBJECTIVES 1. Ft Pressure EXAM #1 PHYSICAL SCIENCE 103 FALLF, 2017 Determine the surface area f an bject. Given the weight and surface area, calculate the pressure. 2. Measuring Vlume & Mass Prvided a

More information

Physics 207 Lecture 13. Lecture 13

Physics 207 Lecture 13. Lecture 13 Physcs 07 Lecture 3 Goals: Lecture 3 Chapter 0 Understand the relatonshp between moton and energy Defne Potental Energy n a Hooke s Law sprng Develop and explot conservaton of energy prncple n problem

More information

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F) EN40: Dynacs and Vbratons Hoework 4: Work, Energy and Lnear Moentu Due Frday March 6 th School of Engneerng Brown Unversty 1. The Rydberg potental s a sple odel of atoc nteractons. It specfes the potental

More information

ONE-DIMENSIONAL COLLISIONS

ONE-DIMENSIONAL COLLISIONS Purpose Theory ONE-DIMENSIONAL COLLISIONS a. To very the law o conservaton o lnear momentum n one-dmensonal collsons. b. To study conservaton o energy and lnear momentum n both elastc and nelastc onedmensonal

More information

Lecture 2: Single-particle Motion

Lecture 2: Single-particle Motion Lecture : Single-particle Mtin Befre we start, let s l at Newtn s 3 rd Law Iagine a situatin where frces are nt transitted instantly between tw bdies, but rather prpagate at se velcity c This is true fr

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

f = µ mg = kg 9.8m/s = 15.7N. Since this is more than the applied

f = µ mg = kg 9.8m/s = 15.7N. Since this is more than the applied Phsics 141H lutins r Hmewrk et #5 Chapter 5: Multiple chice: 8) (a) he maimum rce eerted b static rictin is µ N. ince the blck is resting n a level surace, N = mg. the maimum rictinal rce is ( ) ( ) (

More information

Chapter 07: Kinetic Energy and Work

Chapter 07: Kinetic Energy and Work Chapter 07: Knetc Energy and Work Conservaton o Energy s one o Nature s undamental laws that s not volated. Energy can take on derent orms n a gven system. Ths chapter we wll dscuss work and knetc energy.

More information

Page 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda

Page 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda SPH4U Agenda Fro Newton Two New Concepts Ipulse & oentu Ipulse Collisions: you gotta consere oentu! elastic or inelastic (energy consering or not) Inelastic collisions in one diension and in two diensions

More information

v c motion is neither created nor destroyed, but transferred via interactions. Fri. Wed (.18,.19) Introducing Potential Energy RE 6.

v c motion is neither created nor destroyed, but transferred via interactions. Fri. Wed (.18,.19) Introducing Potential Energy RE 6. r. 6.5-.7 (.) Rest Mass,ork by Changng orces Columba Rep 3pm, here RE 6.b (last day to drop) ed. 6.8-.9(.8,.9) Introducng Potental Energy RE 6.c Tues. H6: Ch 6 Pr s 58,59, 99(a-c), 05(a-c) moton s nether

More information

Physics 321 Solutions for Final Exam

Physics 321 Solutions for Final Exam Page f 8 Physics 3 Slutins fr inal Exa ) A sall blb f clay with ass is drpped fr a height h abve a thin rd f length L and ass M which can pivt frictinlessly abut its center. The initial situatin is shwn

More information

Physics 2A Chapter 9 HW Solutions

Physics 2A Chapter 9 HW Solutions Phscs A Chapter 9 HW Solutons Chapter 9 Conceptual Queston:, 4, 8, 13 Problems: 3, 8, 1, 15, 3, 40, 51, 6 Q9.. Reason: We can nd the change n momentum o the objects b computng the mpulse on them and usng

More information

Conservation of Energy

Conservation of Energy Cnservatn f Energy Equpment DataStud, ruler 2 meters lng, 6 n ruler, heavy duty bench clamp at crner f lab bench, 90 cm rd clamped vertcally t bench clamp, 2 duble clamps, 40 cm rd clamped hrzntally t

More information

Physics for Scientists and Engineers. Chapter 10 Energy

Physics for Scientists and Engineers. Chapter 10 Energy Physcs or Scentsts and Engneers Chapter 0 Energy Sprng, 008 Ho Jung Pak Introducton to Energy Energy s one o the ost portant concepts n scence although t s not easly dened Eery physcal process that occurs

More information

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

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

More information

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with

Approach: (Equilibrium) TD analysis, i.e., conservation eqns., state equations Issues: how to deal with Schl f Aerspace Chemcal D: Mtvatn Prevus D Analyss cnsdered systems where cmpstn f flud was frzen fxed chemcal cmpstn Chemcally eactng Flw but there are numerus stuatns n prpulsn systems where chemcal

More information

Chapter 2. Pythagorean Theorem. Right Hand Rule. Position. Distance Formula

Chapter 2. Pythagorean Theorem. Right Hand Rule. Position. Distance Formula Chapter Moton n One Dmenson Cartesan Coordnate System The most common coordnate system or representng postons n space s one based on three perpendcular spatal axes generally desgnated x, y, and z. Any

More information

Physics 2A Chapter 3 HW Solutions

Physics 2A Chapter 3 HW Solutions Phscs A Chapter 3 HW Solutons Chapter 3 Conceptual Queston: 4, 6, 8, Problems: 5,, 8, 7, 3, 44, 46, 69, 70, 73 Q3.4. Reason: (a) C = A+ B onl A and B are n the same drecton. Sze does not matter. (b) C

More information

Grade 12 Physics Exam Review

Grade 12 Physics Exam Review Grade 12 Physcs Exam Revew 1. A 40 kg wagn s pulled wth an appled frce f 50 N [E 37 degrees abve the hrzntal. The wagn mves 8 m [E] hrzntally whle 5 N f frctn act. Fnd the wrk dne n the wagn by the...

More information

Physic 231 Lecture 33

Physic 231 Lecture 33 Physc 231 Lecture 33 Man pnts f tday s lecture: eat and heat capacty: Q cm Phase transtns and latent heat: Q Lm ( ) eat flw Q k 2 1 t L Examples f heat cnductvty, R values fr nsulatrs Cnvectn R L / k Radatn

More information

Conservation of Energy

Conservation of Energy Conservaton o nergy The total energy o a system can change only by amounts o energy that are transerred nto or out o the system W mec th nt Ths s one o the great conservaton laws n nature! Other conservaton

More information

2015 Sectional Physics Exam Solution Set

2015 Sectional Physics Exam Solution Set . Crrec answer: D Ne: [quan] denes: uns quan WYSE cadec Challenge 05 Secnal Phscs Ea SOLUTION SET / / / / rce lengh lengh rce enu ass lengh e a) / ass ass b) energ c) wrk lengh e pwer energ e d) (crrec

More information

The two main types of FETs are the junction field effect transistor (JFET) and the metal oxide field effect transistor (MOSFET).

The two main types of FETs are the junction field effect transistor (JFET) and the metal oxide field effect transistor (MOSFET). Mcrelectrncs Chapter three: Feld Effect Transstr sall snal analyss Intrductn: Feld-effect transstr aplfers prde an excellent ltae an wth the added feature f hh nput pedance. They are als lw-pwercnsuptn

More information

Conservation Laws (Collisions) Phys101 Lab - 04

Conservation Laws (Collisions) Phys101 Lab - 04 Conservaton Laws (Collsons) Phys101 Lab - 04 1.Objectves The objectves o ths experment are to expermentally test the valdty o the laws o conservaton o momentum and knetc energy n elastc collsons. 2. Theory

More information

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11)

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11) We..7 -.9, (.) Moton Wth & Wthout Torque E. ab r. otaton ab Evals.0 Quantzaton, Quz, ect Evals E.e Mon. evew or nal (-) HW: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. nal Exam (Ch. -) Usng ngular Momentum The

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

Modeling motion with VPython Every program that models the motion of physical objects has two main parts:

Modeling motion with VPython Every program that models the motion of physical objects has two main parts: 1 Modelng moton wth VPython Eery program that models the moton o physcal objects has two man parts: 1. Beore the loop: The rst part o the program tells the computer to: a. Create numercal alues or constants

More information

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax .9.1: AC power analyss Reson: Deceber 13, 010 15 E Man Sute D Pullan, WA 99163 (509 334 6306 Voce and Fax Oerew n chapter.9.0, we ntroduced soe basc quanttes relate to delery of power usng snusodal sgnals.

More information

SPH3U1 Lesson 06 Kinematics

SPH3U1 Lesson 06 Kinematics PROJECTILE MOTION LEARNING GOALS Students will: Describe the mtin f an bject thrwn at arbitrary angles thrugh the air. Describe the hrizntal and vertical mtins f a prjectile. Slve prjectile mtin prblems.

More information

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

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

More information

( ) WYSE ACADEMIC CHALLENGE Regional Physics Exam 2009 Solution Set. 1. Correct answer: D. m t s. 2. Correct answer: A. 3.

( ) WYSE ACADEMIC CHALLENGE Regional Physics Exam 2009 Solution Set. 1. Correct answer: D. m t s. 2. Correct answer: A. 3. YSE CDEMIC CHLLENGE Regnl hyscs E 009 Slutn Set. Crrect nswer: D d hrzntl v hrzntl 3 345 t s t 0.3565s t d d d ll ll ll gt 9.80 s 0.63 ( 0.3565s). Crrect nswer: (-70. 0 ) ( 3 /s) t ( 4. 0 /s ) ( 4. 0 /s

More information

10/2/2003 PHY Lecture 9 1

10/2/2003 PHY Lecture 9 1 Announceents. Exa wll be returned at the end of class. Please rework the exa, to help soldfy your knowledge of ths ateral. (Up to 0 extra cre ponts granted for reworked exa turn n old exa, correctons on

More information

Chapter 5: Force and Motion I-a

Chapter 5: Force and Motion I-a Chapter 5: rce and Mtin I-a rce is the interactin between bjects is a vectr causes acceleratin Net frce: vectr sum f all the frces n an bject. v v N v v v v v ttal net = i = + + 3 + 4 i= Envirnment respnse

More information

Physics 1200 Mechanics, Kinematics, Fluids, Waves

Physics 1200 Mechanics, Kinematics, Fluids, Waves Physics 100 Mechanics, Kinematics, Fluids, Waes Lecturer: Tm Humanic Cntact inf: Office: Physics Research Building, Rm. 144 Email: humanic@mps.hi-state.edu Phne: 614 47 8950 Office hurs: Tuesday 3:00 pm,

More information

WYSE Academic Challenge 2014 Sectional Physics Exam SOLUTION SET. [ F][ d] [ t] [ E]

WYSE Academic Challenge 2014 Sectional Physics Exam SOLUTION SET. [ F][ d] [ t] [ E] WYSE Aaem Challenge 0 Setnal hss Exam SOLUTION SET. Crret answer: E Unts Trque / unts pwer: [ r ][ ] [ E] [ t] [ r ][ ][ t] [ E] [ r ][ ][ t] [ ][ ] [ r ][ t] [ ] m s m s. Crret answer: D The net external

More information

Recitation: Energy, Phys Energies. 1.2 Three stones. 1. Energy. 1. An acorn falling from an oak tree onto the sidewalk.

Recitation: Energy, Phys Energies. 1.2 Three stones. 1. Energy. 1. An acorn falling from an oak tree onto the sidewalk. Rectaton: Energy, Phys 207. Energy. Energes. An acorn fallng from an oak tree onto the sdewalk. The acorn ntal has gravtatonal potental energy. As t falls, t converts ths energy to knetc. When t hts the

More information

Chapter 3, Solution 1C.

Chapter 3, Solution 1C. COSMOS: Cmplete Onlne Slutns Manual Organzatn System Chapter 3, Slutn C. (a If the lateral surfaces f the rd are nsulated, the heat transfer surface area f the cylndrcal rd s the bttm r the tp surface

More information

Is current gain generally significant in FET amplifiers? Why or why not? Substitute each capacitor with a

Is current gain generally significant in FET amplifiers? Why or why not? Substitute each capacitor with a FET Sall Snal Mdband Mdel Ntatn: C arables and quanttes are enerally desnated wth an uppercase subscrpt. AC arables and quanttes are enerally desnated wth a lwercase subscrpt. Phasr ntatn wll be used when

More information

Physics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87

Physics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87 Physcs 4C Solutons to Chater 9 HW Chater 9: Concetual Questons: 6, 8, 0 Problems:,, 4,,, 48,, 6, 6, 78, 87 Queston 9-6 (a) 0 (b) 0 (c) negate (d) oste Queston 9-8 (a) 0 (b) 0 (c) negate (d) oste Queston

More information

Week 8: Chapter 9. Linear Momentum. Newton Law and Momentum. Linear Momentum, cont. Conservation of Linear Momentum. Conservation of Momentum, 2

Week 8: Chapter 9. Linear Momentum. Newton Law and Momentum. Linear Momentum, cont. Conservation of Linear Momentum. Conservation of Momentum, 2 Lnear omentum Week 8: Chapter 9 Lnear omentum and Collsons The lnear momentum of a partcle, or an object that can be modeled as a partcle, of mass m movng wth a velocty v s defned to be the product of

More information

Chapter 8: Potential Energy and The Conservation of Total Energy

Chapter 8: Potential Energy and The Conservation of Total Energy Chapter 8: Potental Energy and The Conservaton o Total Energy Work and knetc energy are energes o moton. K K K mv r v v F dr Potental energy s an energy that depends on locaton. -Dmenson F x d U( x) dx

More information

Phys 344 Ch 5 Lect 5 Feb 28 th,

Phys 344 Ch 5 Lect 5 Feb 28 th, hys 44 Ch 5 Lect 5 Feb 8 th, 009 1 Wed. /4 Fr. /6 Mn. /9 Wed. /11 Fr. / 1 5.5 Dlute lutn 5.6 Checal Equlbru Revew Exa (C 10.7 6.0, 6.1 ltzann tatstcs nus: hys. r. hess resentatns @ 4p HW17: 7,76,8 HW18:8,84,86,88,89,91

More information

Page 1. Clicker Question 9: Physics 131: Lecture 15. Today s Agenda. Clicker Question 9: Energy. Energy is Conserved.

Page 1. Clicker Question 9: Physics 131: Lecture 15. Today s Agenda. Clicker Question 9: Energy. Energy is Conserved. Physcs 3: Lecture 5 Today s Agenda Intro to Conseraton o Energy Intro to some derent knds o energy Knetc Potental Denton o Mechancal Energy Conseraton o Mechancal Energy Conserate orces Examples Pendulum

More information

Chapter 9 Centre of Mass and Linear Momentum

Chapter 9 Centre of Mass and Linear Momentum Chater 9 Centre o Mass and Linear Moentu Centre o ass o a syste o articles / objects Linear oentu Linear oentu o a syste o articles Newton s nd law or a syste o articles Conseration o oentu Elastic and

More information

Study Guide: PS. 10 Motion, Forces, Work & Simple Machines DESCRIBING MOTION SPEED

Study Guide: PS. 10 Motion, Forces, Work & Simple Machines DESCRIBING MOTION SPEED DESCRIBING MOTION Distance: hw far smething has mved; SI unit meters (m) Reference pint: nn-mving bject used as a cmparisn pint t detect an bject s mtin. Displacement: the distance between the starting

More information

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas Sectn : Detaled Slutns f Wrd Prblems Unt : Slvng Wrd Prblems by Mdelng wth Frmulas Example : The factry nvce fr a mnvan shws that the dealer pad $,5 fr the vehcle. If the stcker prce f the van s $5,, hw

More information

2-D Momentum Conservation

2-D Momentum Conservation -D Mmentum Cnseratin Saleback Cllege Physics Department Purpse: T cnirm that linear mmentum is cnsere in tw-imensinal cllisins. T shw that kinetic energy is nearly cnsere in tw-imensinal near-elastic cllisins.

More information

Momentum, p = m v. Collisions and Work(L8) Crash! Momentum and Collisions. Conservation of Momentum. elastic collisions

Momentum, p = m v. Collisions and Work(L8) Crash! Momentum and Collisions. Conservation of Momentum. elastic collisions Collisions and Work(L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details

More information

TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 2211, Exam 2 Section 1 Version 1 October 18, 2013 Total Weight: 100 points

TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 2211, Exam 2 Section 1 Version 1 October 18, 2013 Total Weight: 100 points TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES PHYS, Exam Secton Verson October 8, 03 Total Weght: 00 ponts. Check your examnaton or completeness pror to startng. There are a total o nne

More information

AP Physics Kinematic Wrap Up

AP Physics Kinematic Wrap Up AP Physics Kinematic Wrap Up S what d yu need t knw abut this mtin in tw-dimensin stuff t get a gd scre n the ld AP Physics Test? First ff, here are the equatins that yu ll have t wrk with: v v at x x

More information

Exercises for Frequency Response. ECE 102, Winter 2011, F. Najmabadi

Exercises for Frequency Response. ECE 102, Winter 2011, F. Najmabadi Eercses r Frequency espnse EE 0, Wnter 0, F. Najabad Eercse : A Mdy the crcut belw t nclude a dnant ple at 00 Mz ( 00 Ω, k, k, / 00 Ω, λ 0, and nre nternal capactances the MOS. pute the dnant ple n the

More information

NAME Borough of Manhattan Community College Course Physics 110 Sec 721 Instructor: Dr. Hulan E. Jack Jr. Date December 19, 2006

NAME Borough of Manhattan Community College Course Physics 110 Sec 721 Instructor: Dr. Hulan E. Jack Jr. Date December 19, 2006 Brug f Manattan unity llege urse Pysics 110 Sec 721 nstructr: Dr. Hulan E. Jack Jr. Date Deceber 19, 2006 inal Exa NSTRUTONS - D 7 prbles : D Prble 1, 2 fr Prble 2,3 and 4, 2 fr Prbles 5,6 and 7, 2 fr

More information

EXAM #1 PHYSICAL SCIENCE 103 Spring, 2016

EXAM #1 PHYSICAL SCIENCE 103 Spring, 2016 OBJECTIVES 1. Ft Pressure EXAM #1 PHYSICAL SCIENCE 103 Spring, 2016 Determine the surface area f an bject. Given the weight and surface area, calculate the pressure. 2. Measuring Vlume & Mass Prvided a

More information

ESCI 341 Atmospheric Thermodynamics Lesson 6 Thermodynamic Processes

ESCI 341 Atmospheric Thermodynamics Lesson 6 Thermodynamic Processes ESCI 341 Atmosherc Thermodynamcs Lesson 6 Thermodynamc Processes Reerences: An Introducton to Atmosherc Thermodynamcs, Tsons Introducton to Theoretcal Meteorology, Hess Physcal Chemstry (4 th edton), Lene

More information