12/01/10. STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc.

Size: px
Start display at page:

Download "12/01/10. STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc."

Transcription

1 GENERAL PHYSICS PH -3A (Dr. S. Mirv) Tet 4 (/03/07) Key /0/0 STUDENT NAME: STUDENT id #: ALL QUESTIONS ARE WORTH 0 POINTS. WORK OUT FIVE PROBLEMS. NOTE: Clearly write ut lutin and anwer (circle the anwer) by ectin r each part (a., b., c., etc.) Iprtant Frula:. Mtin alng a traight line with a cntant acceleratin v aver. peed [dit. taken]/[tie trav.]s/t; v aver.vel. Δ/Δt; v in d/δt; a aver. Δv aver. vel. /Δt; a dv/δt; v v + at; /(v +v)t; v t + / at ; v v + a (i 0 at t 0). Free all tin (with pitive directin ) g 9.80 / ; y v aver. t v aver. (v+v )/; v v - gt; y v t - / g t ; v v gy (i y 0 at t 0) 3. Mtin in a plane v v cθ; v y v inθ; v t+ / a t ; y v y t + / a y t ; v v + at; v y v y + at; 4. Prjectile tin (with pitive directin ) v v v cθ; v t; a ( v inθ cθ)/g (v inθ)/g r y in y in ; v y v y - gt v inθ - gt; y v y t - / gt ; 5. Unir circular Mtin av /r, Tπr/v 6. Relative tin v P A v P B + v B A a a PA PB 7. Cpnent ethd vectr additin

2 A A + A ; A A + A and A y A y + A y ; A A + A y ; θ tan - A y /A ; The calar prduct A a b a b c φ a b ( a ˆ ˆ ˆ) ( ˆ ˆ ˆ i + a y j + a zk b i + b y j + b zk ) a b a b + a yb y + a zb z The vectr prduct a b ( a iˆ + a ˆj + a kˆ) ( b iˆ + b ˆj + b kˆ) y z y z iˆ ˆj kˆ a y a z a ˆ ˆ a a z ˆ a y a b b a a a y a z i j + k b y b z b b b z b y b b b y z ( a b b a ) iˆ + ( a b b a ) ˆj + ( a b b a ) kˆ y z y z z z y y. Secnd Newtn Law af net ;. Kinetic rictin k μ k N; 3. Static rictin μ N; 4. Univeral Law Gravitatin: FGM/r ; G N /kg ; 5. Drag ceicient D C ρ A v 6. Terinal peed v t g C ρ A 7. Centripetal rce: F c v /r 8. Speed the atellite in a circular rbit: v GM E /r 9. The wrk dne by a cntant rce acting n an bject: W F d cφ F d 0. Kinetic energy: K v. Ttal echanical energy: EK+U. The wrk-energy there: WK -K ; W nc ΔK+ΔUE -E 3. The principle cnervatin echanical energy: when W nc 0, E E 4. Wrk dne by the gravitatinal rce: W g d cφ g

3 . Wrk dne in Liting and Lwering the bject: Δ K K K W + W ; i K K ; W W i a g i a g. Spring Frce: F k (H k' law ) 3. Wrk dne by a pring rce: W k k ; i 0 and ; W k i i 4. Wrk dne by a variable rce: W F ( ) d W d W 5. Pwer: P avg ; P ; P F v cφ F v Δ t d t 6. Ptential energy: Δ U W ; Δ U F ( ) d 7. Gravitatinal Ptential Energy: Δ U g ( y y ) g Δ y ; i y 0 a n d U 0 ; U ( y ) g y i i i i i 8. Elatic ptential Energy: U ( ) k 9. Ptential energy curve: du ( ) F ( ) ; K ( ) E e c U ( ) d 0. Wrk dne n a yte by an eternal rce: F ric ti n i n t in v lv e d W h e n k in e tic ric ti n rc e a c t w ith in th e y te Δ E d th k W Δ E Δ K + Δ U e c W Δ E + Δ E e c th. Cnervatin energy: W Δ E Δ E + Δ E + Δ E e c th r ilated yte (W 0) Δ E + Δ E + Δ E 0 in t e c th in t Δ E. Pwer: P avg ; P Δ t de d t ; 3. Center a: r r n c i i M i 4. Newtn Secnd Law r a yte particle: F net M a c 3

4 . Linear Mentu and Newtn Secnd law r a yte particle: P M v and F c net dp dt t. Clliin and ipule: J F ( t ) d t; J F Δ t; t i avg when a trea bdie with a and n n Δ peed v, cllide with a bdy whe pitin i ied F avg Δ p Δ v Δ v Δ t Δ t Δ t Ipule-Linear Mentu There: p p i J 3. Law Cnervatin Linear entu: P P r cled, ilated yte 4. Inelatic clliin in ne dienin: p + p p + p i i i 5. Mtin the Center Ma: The center a a cled, ilated yte tw clliding bdie i nt aected by a clliin. 6. Elatic Clliin in One Dienin: v v ; v v i i Clliin in Tw Dienin: p + p p + p ; p + p p + p i i iy iy y y 8. Variable-a yte: Rv rel v v v M a (irt rcket equatin) i r e l M i ln (ecnd rcket equatin) M S 9. Angular Pitin: θ (radian eaure) r 0. Angular Diplaceent: Δ θ θ θ (p itiv e r c u n terclc k w ie r tatin ) Δ θ d θ. Angular velcity and peed: ω avg ; ω (p itive r c u n tercl ck w ie rtati n ) Δ t d t Δ ω. Angular acceleratin: α avg ; α Δ t d ω d t 4

5 ω ω + α t θ θ ( ω + ω ) t. angular acceleratin: θ θ ω t + α t ω ω + α ( θ θ ) θ θ ω t ω t. Linear and angular variable related: I r d v π r π θ r ; v ω r ; a t α r ; a r ω r ; T r v ω 3. Rtatinal Kinetic Energy and Rtatinal Inertia: K I ω ; I iri r bdy a a yte dicrete particle; r a bdy w ith cntinuuly ditributed a. 4. The parallel ae there: I I c + M h 5. Trque: τ rf r F rf in t φ 6. Newtn ecnd law in angular r: τ net I 7. Wrk and Rtatinal Kinetic Energy: α W θ θ i τ dθ ; W τ ( θ θ ) r τ cnt; i dw P Δ K K K I ω I ω W dt ; i i w rk energy there r rtating bdie v c ω R K I cω + v 8. Rlling bdie: a c α R g in θ a c + I / M R c c r r llin g th ly d w n th e ra p 9. Trque a a vectr: τ r F ; τ r F inφ r F r F 5

6 l r p ( r v ) ;. Angular Mentu a particle: l r v in φ r p r v r p r v dl. Newtn Secnd law in Angular Fr: τ net dt 3. Angular entu a yte particle: L τ net n l i i 4. Angular Mentu a Rigid Bdy: L I ω 5. Cnervatin Angular Mentu: L i L (i la te d y te ) F net 0; τ net 0 6. Static equilibriu: i all the rce lie in y plane F 0; F 0; τ 0 7. Elatic Mduli: tre dulu train F Δ L 8. Tenin and Cprein: E, E i the Y ung' dulu A L F Δ L 9. Shearing: G, G i the hear dulu A L Δ V 0. Hydraulic Stre: p B, B i th e b u lk d u lu V et dl dt net, net, y net, z. Siple harnic tin: t + v t + a t + c( ω φ ); ω in( ω φ ); ω c( ω φ ) k. The Linear Ocillatr: ω, T π k 3. Pendulu: T T π I k, trin pendulu π L g, i ple pendulu T I π, phyical pendulu g h 6

7 . Daped Harnic Mtin: bt k b ( t ) e c ( ω ' t + φ ), ω ', E ( t ) k e 4 bt. Sinuidal wave: y (, t ) y in( k π ω ω λ ω t ), k,, v λ λ π T k T 3. Wave peed n tretched tring: v τ μ 4. Average pwer tranitted by a inuidal wave n a tretched tring: P avg μ v ω y 5. Intererence wave: y '(, t ) [ y c φ ] in ( k ω t + φ ) 6. Standing wave: y '(, t ) [ y in k ] c ω t v v 7. Renance: n, r n,,3,... λ L B 8. Sund wave: v, ρ Δ L φ π ( π ) r 0,,,3..., cntructive intererence λ 9. Intererence: Δ L φ π ( + ) π r 0,,,3..., detructive intererence λ 0. Sund Intenity: P P I, I ρ v ω, I A 4 π r. Sund level in decibel: β I ( 0 db ) l g, I 0 W / I. Standing wave pattern in pipe: v n v λ L, n,,3,..., r pipe pened r bth end v n v λ 4 L, n,3,5,..., r pipe cled at ne end and pened at the ther 3. Beat: beat 7

8 vr. The Dppler eect: ' ( ± ) v und;(v 33/); ' v E v v ± vr ' general Dppler Eect v v E, v R the peed the receiver; v the peed the + r receiver appraching tatinary eitter, - r receiver ving away r the tatinary eitter;, v E the peed the eitter, v the peed the und, - r eitter appraching tatinary receiver, + r eitter ving away r the tatinary receiver; 8

9 9

10 . A iple pendulu length.0 i ued by a tudent t deterine the acceleratin gravity. The pendulu wing back and rth thrugh 0 cplete wing in.. What value g i btained? L Fr a iple pendulu T π g 0 wing in. ean that T (. /0). 4π 4π. L g 9.6 / T. 0

11 3. A tranvere traveling inuidal wave n a tring ha a requency 00Hz, a wavelength 0.040, and an aplitude.0. What i a) the aiu velcity in / any pint n the tring? b) the peed the wave? The ablute value the aiu velcity any particle n a tring i v ωy π y π(00 Hz) (0.00 ).3 / pa v λ (0.04 ) (00 Hz) 4 / wave

12 4. I the length a pian wire ( given denity) i increaed by 5%, what appriate change in tenin i neceary t keep it undaental requency unchanged? TL T.05L v L L (.05 L) T T.05 (.05) T (.05) T T T T(.05 ) 5% increae T T

13 5. 3

14 6. Fr AC> BC AC r AC<; BC AC 0.55 () BC + AC () ()-() AC.7485 AC 0.9 4

15 7. 5

16 8. A urce eit und with a requency 000Hz. It i ving at 0/ tward a tatinary relecting wall. I the peed und i 340 /, what i the beat requency heard by an berver pitined at ret directly behind the urce? v ± vr ' general Dppler Eect v v E ' '' Statinary receiver hear beat requency beat, v Hz v v ' where i a requency E heard by a tatinary receiver r appraching eitter. v Hz v + v '' where i a requency heard by a tatinary receiver r the urce relected r the wall and ving away r the receiver. beat Hz E 6

GENERAL PHYSICS PH 221-1D (Dr. S. Mirov) Test 4 (Sample) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

GENERAL PHYSICS PH 221-1D (Dr. S. Mirov) Test 4 (Sample) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GENERAL PHYSICS PH -D (Dr. S. Mirv) Test 4 (Sple) STUDENT NAME: Ke STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

GENERAL PHYSICS PH 221-1D (Dr. S. Mirov) Test 4 (04/29/13) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

GENERAL PHYSICS PH 221-1D (Dr. S. Mirov) Test 4 (04/29/13) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GENERAL PHYSICS PH -D (Dr. S. Mirov) Test 4 (04/9/3) STUDENT NAME: key STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

Sample Test 3. STUDENT NAME: STUDENT id #:

Sample Test 3. STUDENT NAME: STUDENT id #: GENERAL PHYSICS PH -3A (Dr. S. Mirv) Test 3 (/7/07) ke Sample Test 3 STUDENT NAME: STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1

Phys101 Final Code: 1 Term: 132 Wednesday, May 21, 2014 Page: 1 Phys101 Final Cde: 1 Term: 1 Wednesday, May 1, 014 Page: 1 Q1. A car accelerates at.0 m/s alng a straight rad. It passes tw marks that are 0 m apart at times t = 4.0 s and t = 5.0 s. Find the car s velcity

More information

Flipping Physics Lecture Notes: AP Physics 1 Review of Kinematics

Flipping Physics Lecture Notes: AP Physics 1 Review of Kinematics Flipping Phyic Lecture Nte: AP Phyic 1 Review f Kinematic AP i a regitered trademark f the Cllege Bard, which wa nt invlved in the prductin f, and de nt endre, thi prduct. Intrductry Cncept: Vectr: Magnitude

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

Sample Test 2. GENERAL PHYSICS PH 221-3A (Dr. S. Mirov) Test 2 (10/10/07) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

Sample Test 2. GENERAL PHYSICS PH 221-3A (Dr. S. Mirov) Test 2 (10/10/07) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS. GENERAL PHYSICS PH -3A (Dr. S. Mirov) Test (0/0/07) Sample Test STUDENT NAME: _Key STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

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

Kinetics of Particles. Chapter 3

Kinetics of Particles. Chapter 3 Kinetics f Particles Chapter 3 1 Kinetics f Particles It is the study f the relatins existing between the frces acting n bdy, the mass f the bdy, and the mtin f the bdy. It is the study f the relatin between

More information

Please pick up your Exam1 Answer Sheets at front

Please pick up your Exam1 Answer Sheets at front Pleae pick up yur Exam1 Anwer Sheet at frnt PHY205 Lecture 17 Ch. 8.4, 8.6 (kip 8.5) Rtatinal Equilibrium, Rtatinal rmulatin f ewtn Law Linear v Rtatinal Variable Linear Variable Tranfrmatin Table Rtatinal

More information

Phys101 Second Major-061 Zero Version Coordinator: AbdelMonem Saturday, December 09, 2006 Page: 1

Phys101 Second Major-061 Zero Version Coordinator: AbdelMonem Saturday, December 09, 2006 Page: 1 Crdinatr: AbdelMnem Saturday, December 09, 006 Page: Q. A 6 kg crate falls frm rest frm a height f.0 m nt a spring scale with a spring cnstant f.74 0 3 N/m. Find the maximum distance the spring is cmpressed.

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

Q x = cos 1 30 = 53.1 South

Q x = cos 1 30 = 53.1 South Crdinatr: Dr. G. Khattak Thursday, August 0, 01 Page 1 Q1. A particle mves in ne dimensin such that its psitin x(t) as a functin f time t is given by x(t) =.0 + 7 t t, where t is in secnds and x(t) is

More information

Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1

Phy 213: General Physics III 6/14/2007 Chapter 28 Worksheet 1 Ph 13: General Phsics III 6/14/007 Chapter 8 Wrksheet 1 Magnetic Fields & Frce 1. A pint charge, q= 510 C and m=110-3 m kg, travels with a velcit f: v = 30 ˆ s i then enters a magnetic field: = 110 T ˆj.

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

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

STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc.

STUDENT NAME: STUDENT id #: NOTE: Clearly write out solutions and answers (circle the answers) by section for each part (a., b., c., etc. GENERAL PHYSICS PH 1-3A (Dr. S. Mirov) Test 1 (09/17/07) Key STUDENT NAME: STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

The bending of a wave around an obstacle or the edges of an opening is called diffraction.

The bending of a wave around an obstacle or the edges of an opening is called diffraction. 17.3 Diractin The bending a wae arund an btacle r the edge an pening i called diractin. http://www.yutube.cm/watch?ksig_eaifrw 1 17.3 Diractin 2 dimenin: ingle lit irt minimum inθ λ D Linear Meaurement:

More information

Chapter 9 Vector Differential Calculus, Grad, Div, Curl

Chapter 9 Vector Differential Calculus, Grad, Div, Curl Chapter 9 Vectr Differential Calculus, Grad, Div, Curl 9.1 Vectrs in 2-Space and 3-Space 9.2 Inner Prduct (Dt Prduct) 9.3 Vectr Prduct (Crss Prduct, Outer Prduct) 9.4 Vectr and Scalar Functins and Fields

More information

Phys101 First Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Wednesday, September 25, 2013 Page: 1

Phys101 First Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Wednesday, September 25, 2013 Page: 1 Phys11 First Majr-11 Zer Versin Crdinatr: Dr. A. A. Naqvi Wednesday, September 5, 1 Page: 1 Q1. Cnsider tw unifrm slid spheres A and B made f the same material and having radii r A and r B, respectively.

More information

PHYSICS LAB Experiment 10 Fall 2004 ROTATIONAL DYNAMICS VARIABLE I, FIXED

PHYSICS LAB Experiment 10 Fall 2004 ROTATIONAL DYNAMICS VARIABLE I, FIXED ROTATIONAL DYNAMICS VARIABLE I, FIXED In this experiment we will test Newtn s Secnd Law r rtatinal mtin and examine hw the mment inertia depends n the prperties a rtating bject. THE THEORY There is a crrespndence

More information

Name Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes.

Name Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes. Name Student ID II. [25 pt] Thi quetin cnit f tw unrelated part. Part 1. In the circuit belw, bulb 1-5 are identical, and the batterie are identical and ideal. Bxe,, and cntain unknwn arrangement f linear

More information

PHYSICS 151 Notes for Online Lecture 4.1

PHYSICS 151 Notes for Online Lecture 4.1 PHYSICS 5 Nte r Online ecture 4. Peridicity Peridic ean that ethin repeat itel. r exaple, eery twenty-ur hur, the ae a cplete rtatin. Heartbeat are an exaple peridic behair. I yu l at heartbeat n an electrcardira,

More information

Conceptual Dynamics SDC. An Interactive Text and Workbook. Kirstie Plantenberg Richard Hill. Better Textbooks. Lower Prices.

Conceptual Dynamics SDC. An Interactive Text and Workbook. Kirstie Plantenberg Richard Hill. Better Textbooks. Lower Prices. Cnceptual Dynamics An Interactive Text and Wrkbk Kirstie Plantenberg Richard Hill SDC P U B L I C AT I O N S Better Textbks. Lwer Prices. www.sdcpublicatins.cm Pwered by TCPDF (www.tcpdf.rg) Visit the

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

Honors Physics Final Review Summary

Honors Physics Final Review Summary Hnrs Physics Final Review Summary Wrk Dne By A Cnstant Frce: Wrk describes a frce s tendency t change the speed f an bject. Wrk is dne nly when an bject mves in respnse t a frce, and a cmpnent f the frce

More information

Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Professor and Chair Mechanical Engineering Department Christian Brothers University 650 East Parkway South Memphis, TN

Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Professor and Chair Mechanical Engineering Department Christian Brothers University 650 East Parkway South Memphis, TN Yeu-Sheng Paul Shiue, Ph.D 薛宇盛 Prfessr and Chair Mechanical Engineering Department Christian Brthers University 650 East Parkway Suth Memphis, TN 38104 Office: (901) 321-3424 Rm: N-110 Fax : (901) 321-3402

More information

Harmonic Motion (HM) Oscillation with Laminar Damping

Harmonic Motion (HM) Oscillation with Laminar Damping Harnic Mtin (HM) Oscillatin with Lainar Daping If yu dn t knw the units f a quantity yu prbably dn t understand its physical significance. Siple HM r r Hke' s Law: F k x definitins: f T / T / Bf x A sin

More information

Study Guide Physics Pre-Comp 2013

Study Guide Physics Pre-Comp 2013 I. Scientific Measurement Metric Units S.I. English Length Meter (m) Feet (ft.) Mass Kilgram (kg) Pund (lb.) Weight Newtn (N) Ounce (z.) r pund (lb.) Time Secnds (s) Secnds (s) Vlume Liter (L) Galln (gal)

More information

PHY 140Y FOUNDATIONS OF PHYSICS Problem Set #2

PHY 140Y FOUNDATIONS OF PHYSICS Problem Set #2 PHY 140Y FOUNDATIONS OF PHYSICS 2001-2002 Prble Set #2 HANDED OUT: DUE: Friday, Octber 5, 2001 (in cla) 5:00 PM, Thurday, Octber 18, 2001 in the apprpriate bx, labeled by tutrial grup, in the baeent at

More information

WYSE Academic Challenge Sectional Physics 2007 Solution Set

WYSE Academic Challenge Sectional Physics 2007 Solution Set WYSE caemic Challenge Sectinal Physics 7 Slutin Set. Crrect answer: E. Energy has imensins f frce times istance. Since respnse e. has imensins f frce ivie by istance, it clearly es nt represent energy.

More information

Work, Energy, and Power

Work, Energy, and Power rk, Energy, and Pwer Physics 1 There are many different TYPES f Energy. Energy is expressed in JOULES (J 419J 4.19 1 calrie Energy can be expressed mre specifically by using the term ORK( rk The Scalar

More information

Disclaimer: This lab write-up is not

Disclaimer: This lab write-up is not Diclaier: Thi lab write-up i nt t be cpied, in whle r in part, unle a prper reference i ade a t the urce. (It i trngly recended that yu ue thi dcuent nly t generate idea, r a a reference t explain cplex

More information

Projectile Motion. What is projectile? Projectile -Any object which projected by some means and continues to move due to its own inertia (mass).

Projectile Motion. What is projectile? Projectile -Any object which projected by some means and continues to move due to its own inertia (mass). Prjectile Mtin AP Phyic B What i prjectile? Prjectile -Any bject which prjected by me mean and cntinue t me due t it wn inertia (ma). 1 Prjectile me in TWO dimenin Since a prjectile me in - dimenin, it

More information

= m. Suppose the speed of a wave on a string is given by v = Κ τμ

= m. Suppose the speed of a wave on a string is given by v = Κ τμ Phys101 First Majr-11 Zer Versin Sunday, Octber 07, 01 Page: 1 Q1. Find the mass f a slid cylinder f cpper with a radius f 5.00 cm and a height f 10.0 inches if the density f cpper is 8.90 g/cm 3 (1 inch

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

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2.

Q1. A) 48 m/s B) 17 m/s C) 22 m/s D) 66 m/s E) 53 m/s. Ans: = 84.0 Q2. Phys10 Final-133 Zer Versin Crdinatr: A.A.Naqvi Wednesday, August 13, 014 Page: 1 Q1. A string, f length 0.75 m and fixed at bth ends, is vibrating in its fundamental mde. The maximum transverse speed

More information

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed

More information

ENGI 4430 Parametric Vector Functions Page 2-01

ENGI 4430 Parametric Vector Functions Page 2-01 ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr

More information

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1

Phys102 Final-061 Zero Version Coordinator: Nasser Wednesday, January 24, 2007 Page: 1 Crdinatr: Nasser Wednesday, January 4, 007 Page: 1 Q1. Tw transmitters, S 1 and S shwn in the figure, emit identical sund waves f wavelength λ. The transmitters are separated by a distance λ /. Cnsider

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

Rigid Body Dynamics (continued)

Rigid Body Dynamics (continued) Last time: Rigid dy Dynamics (cntinued) Discussin f pint mass, rigid bdy as useful abstractins f reality Many-particle apprach t rigid bdy mdeling: Newtn s Secnd Law, Euler s Law Cntinuus bdy apprach t

More information

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle? Physics 0 Public Exam Questins Unit 1: Circular Mtin NAME: August 009---------------------------------------------------------------------------------------------------------------------- 1. Which describes

More information

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle?

14. Which shows the direction of the centripetal force acting on a mass spun in a vertical circle? Physics 3204 Public Exam Questins Unit 1: Circular Mtin NAME: August 2009---------------------------------------------------------------------------------------------------------------------- 12. Which

More information

Conservation of Momentum

Conservation of Momentum Cnervatin f Mmentum PES 1150 Prelab Quetin Name: Lab Statin: 003 ** Diclaimer: Thi re-lab i nt t be cied, in whle r in art, unle a rer reference i made a t the urce. (It i trngly recmmended that yu ue

More information

SIMPLE NUMERICAL METHOD FOR KINETICAL INVESTIGATION OF PLANAR MECHANICAL SYSTEMS WITH TWO DEGREES OF FREEDOM

SIMPLE NUMERICAL METHOD FOR KINETICAL INVESTIGATION OF PLANAR MECHANICAL SYSTEMS WITH TWO DEGREES OF FREEDOM Interdisciplinar Descriptin f Cple Sstes 4(), 6-69, 06 SIMPLE NUMERICAL METHOD FOR KINETICAL INVESTIGATION OF PLANAR MECHANICAL SYSTEMS WITH TWO DEGREES OF FREEDOM István Bíró* Facult f Engineering Universit

More information

PHY 211: General Physics I 1 CH 10 Worksheet: Rotation

PHY 211: General Physics I 1 CH 10 Worksheet: Rotation PHY : General Phyic CH 0 Workheet: Rotation Rotational Variable ) Write out the expreion for the average angular (ω avg ), in ter of the angular diplaceent (θ) and elaped tie ( t). ) Write out the expreion

More information

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string?

Q1. A string of length L is fixed at both ends. Which one of the following is NOT a possible wavelength for standing waves on this string? Term: 111 Thursday, January 05, 2012 Page: 1 Q1. A string f length L is fixed at bth ends. Which ne f the fllwing is NOT a pssible wavelength fr standing waves n this string? Q2. λ n = 2L n = A) 4L B)

More information

Phys102 First Major-122 Zero Version Coordinator: Sunaidi Wednesday, March 06, 2013 Page: 1

Phys102 First Major-122 Zero Version Coordinator: Sunaidi Wednesday, March 06, 2013 Page: 1 Crdinatr: Sunaidi Wednesday, March 06, 2013 Page: 1 Q1. An 8.00 m lng wire with a mass f 10.0 g is under a tensin f 25.0 N. A transverse wave fr which the wavelength is 0.100 m, and the amplitude is 3.70

More information

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System

Flipping Physics Lecture Notes: Simple Harmonic Motion Introduction via a Horizontal Mass-Spring System Flipping Physics Lecture Ntes: Simple Harmnic Mtin Intrductin via a Hrizntal Mass-Spring System A Hrizntal Mass-Spring System is where a mass is attached t a spring, riented hrizntally, and then placed

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

CHAPTER 8b Static Equilibrium Units

CHAPTER 8b Static Equilibrium Units CHAPTER 8b Static Equilibrium Units The Cnditins fr Equilibrium Slving Statics Prblems Stability and Balance Elasticity; Stress and Strain The Cnditins fr Equilibrium An bject with frces acting n it, but

More information

Sample Test 3. STUDENT NAME: STUDENT id #:

Sample Test 3. STUDENT NAME: STUDENT id #: GENERAL PHYSICS PH -3A (Dr. S. Mirv) Test 3 (/7/07) ke Smple Test 3 STUDENT NAME: STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------

More information

SAFE HANDS & IIT-ian's PACE EDT-04 (JEE) Solutions

SAFE HANDS & IIT-ian's PACE EDT-04 (JEE) Solutions ED- (JEE) Slutins Answer : Optin () ass f the remved part will be / I Answer : Optin () r L m (u csθ) (H) Answer : Optin () P 5 rad/s ms - because f translatin ωr ms - because f rtatin Cnsider a thin shell

More information

Flipping Physics Lecture Notes: You Can t Run from Momentum

Flipping Physics Lecture Notes: You Can t Run from Momentum Flipping Phyic Lecture Nte: Yu Can t Run frm Mmentum Symbl fr mmentum i a lwercae p. p i fr the Latin wrd petere which mean t make fr, t travel t, t eek, r t purue. It pretty clear thi wrd i where the

More information

Q1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges.

Q1. In figure 1, Q = 60 µc, q = 20 µc, a = 3.0 m, and b = 4.0 m. Calculate the total electric force on q due to the other 2 charges. Phys10 Secnd Majr-08 Zer Versin Crdinatr: Dr. I. M. Nasser Saturday, May 3, 009 Page: 1 Q1. In figure 1, Q = 60 µc, q = 0 µc, a = 3.0 m, and b = 4.0 m. Calculate the ttal electric frce n q due t the ther

More information

Torque and Angular Momentum

Torque and Angular Momentum CHAPTER 10 (TRQUE, 2 ND LAW FR RTATIN) CHAPTER 11 (TRQUE, ANGULAR MMENTUM) Torque and Angular Momentum 1. Torque a. Definition b. Work, Power, W-K Theorem 2. Angular Momentum a. Newton s 2 nd Law in angular

More information

NGSS High School Physics Domain Model

NGSS High School Physics Domain Model NGSS High Schl Physics Dmain Mdel Mtin and Stability: Frces and Interactins HS-PS2-1: Students will be able t analyze data t supprt the claim that Newtn s secnd law f mtin describes the mathematical relatinship

More information

Inertial Mass of Charged Elementary Particles

Inertial Mass of Charged Elementary Particles David L. Bergan 1 Inertial Mass Inertial Mass f Charged Eleentary Particles David L. Bergan Cn Sense Science P.O. Bx 1013 Kennesaw, GA 30144-8013 Inertial ass and its prperty f entu are derived fr electrdynaic

More information

1 Course Notes in Introductory Physics Jeffrey Seguritan

1 Course Notes in Introductory Physics Jeffrey Seguritan Intrductin & Kinematics I Intrductin Quickie Cncepts Units SI is standard system f units used t measure physical quantities. Base units that we use: meter (m) is standard unit f length kilgram (kg) is

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

Seat: PHYS 1500 (Fall 2006) Exam #2, V1. After : p y = m 1 v 1y + m 2 v 2y = 20 kg m/s + 2 kg v 2y. v 2x = 1 m/s v 2y = 9 m/s (V 1)

Seat: PHYS 1500 (Fall 2006) Exam #2, V1. After : p y = m 1 v 1y + m 2 v 2y = 20 kg m/s + 2 kg v 2y. v 2x = 1 m/s v 2y = 9 m/s (V 1) Seat: PHYS 1500 (Fall 006) Exa #, V1 Nae: 5 pt 1. Two object are oving horizontally with no external force on the. The 1 kg object ove to the right with a peed of 1 /. The kg object ove to the left with

More information

sin θ = = y = r sin θ & cos θ = = x = r cos θ

sin θ = = y = r sin θ & cos θ = = x = r cos θ Flipping Phyic Lecture Nte: Intrductin t Circular Mtin and Arc Length Circular Mtin imply take what yu have learned befre and applie it t bject which are mving alng a circular path. Let begin with a drawing

More information

. (7.1.1) This centripetal acceleration is provided by centripetal force. It is directed towards the center of the circle and has a magnitude

. (7.1.1) This centripetal acceleration is provided by centripetal force. It is directed towards the center of the circle and has a magnitude Lecture #7-1 Dynamics f Rtatin, Trque, Static Equilirium We have already studied kinematics f rtatinal mtin We discussed unifrm as well as nnunifrm rtatin Hwever, when we mved n dynamics f rtatin, 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

FIELDS AND RADIATION FROM A MOVING ELECTRIC CHARGE

FIELDS AND RADIATION FROM A MOVING ELECTRIC CHARGE FIELDS AND RADIATION FROM A MOING ELECTRIC CHARGE Musa D. Abdullahi, U.M.Y. University P.M.B. 18, Katsina, Katsina State, Nigeria E-ail: usadab@utlk.c, Tel: +348034080399 Abstract The paper assued that

More information

Physics 20 Lesson 28 Simple Harmonic Motion Dynamics & Energy

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

More information

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations

Plan o o. I(t) Divide problem into sub-problems Modify schematic and coordinate system (if needed) Write general equations STAPLE Physics 201 Name Final Exam May 14, 2013 This is a clsed bk examinatin but during the exam yu may refer t a 5 x7 nte card with wrds f wisdm yu have written n it. There is extra scratch paper available.

More information

Lecture 11 DAMPED AND DRIVEN HARMONIC OSCILLATIONS. Composition of harmonic oscillations (1) Harmonic motion diff. equation is: -linear -uniform

Lecture 11 DAMPED AND DRIVEN HARMONIC OSCILLATIONS. Composition of harmonic oscillations (1) Harmonic motion diff. equation is: -linear -uniform Lecture DMPED ND DRIVEN HRMONIC OSCILLTIONS Ntes: Lecture - Cpsitin f harnic scillatins () Learn re: Linear differential equatin Harnic tin diff. equatin is: -linear -unifr d + http://en.wikipedia.rg/wiki/linear_differential_eq

More information

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N Q1. A transverse sinusidal wave travelling n a string is given by: y (x,t) = 0.20 sin (2.5 x 80 t) (SI units). The length f the string is 2.0 m and its mass is 1.5 g. What is the magnitude f the tensin

More information

Chapter 3. Electric Flux Density, Gauss s Law and Divergence

Chapter 3. Electric Flux Density, Gauss s Law and Divergence Chapter 3. Electric Flu Denity, Gau aw and Diergence Hayt; 9/7/009; 3-1 3.1 Electric Flu Denity Faraday Eperiment Cncentric phere filled with dielectric material. + i gien t the inner phere. - i induced

More information

Kinematics (special case) Dynamics gravity, tension, elastic, normal, friction. Energy: kinetic, potential gravity, spring + work (friction)

Kinematics (special case) Dynamics gravity, tension, elastic, normal, friction. Energy: kinetic, potential gravity, spring + work (friction) Kinematics (special case) a = constant 1D motion 2D projectile Uniform circular Dynamics gravity, tension, elastic, normal, friction Motion with a = constant Newton s Laws F = m a F 12 = F 21 Time & Position

More information

Aircraft Performance - Drag

Aircraft Performance - Drag Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce

More information

MODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b

MODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b . REVIEW OF SOME BASIC ALGEBRA MODULE () Slving Equatins Yu shuld be able t slve fr x: a + b = c a d + e x + c and get x = e(ba +) b(c a) d(ba +) c Cmmn mistakes and strategies:. a b + c a b + a c, but

More information

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1

Phys102 Second Major-102 Zero Version Coordinator: Al-Shukri Thursday, May 05, 2011 Page: 1 Crdinatr: Al-Shukri Thursday, May 05, 2011 Page: 1 1. Particles A and B are electrically neutral and are separated by 5.0 μm. If 5.0 x 10 6 electrns are transferred frm particle A t particle B, the magnitude

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

= s = 3.33 s s. 0.3 π 4.6 m = rev = π 4.4 m. (3.69 m/s)2 = = s = π 4.8 m. (5.53 m/s)2 = 5.

= s = 3.33 s s. 0.3 π 4.6 m = rev = π 4.4 m. (3.69 m/s)2 = = s = π 4.8 m. (5.53 m/s)2 = 5. Seat: PHYS 500 (Fall 0) Exa #, V 5 pt. Fro book Mult Choice 8.6 A tudent lie on a very light, rigid board with a cale under each end. Her feet are directly over one cale and her body i poitioned a hown.

More information

PHYS 314 HOMEWORK #3

PHYS 314 HOMEWORK #3 PHYS 34 HOMEWORK #3 Due : 8 Feb. 07. A unifrm chain f mass M, lenth L and density λ (measured in k/m) hans s that its bttm link is just tuchin a scale. The chain is drpped frm rest nt the scale. What des

More information

Introduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem

Introduction: A Generalized approach for computing the trajectories associated with the Newtonian N Body Problem A Generalized apprach fr cmputing the trajectries assciated with the Newtnian N Bdy Prblem AbuBar Mehmd, Syed Umer Abbas Shah and Ghulam Shabbir Faculty f Engineering Sciences, GIK Institute f Engineering

More information

Professional Development. Implementing the NGSS: High School Physics

Professional Development. Implementing the NGSS: High School Physics Prfessinal Develpment Implementing the NGSS: High Schl Physics This is a dem. The 30-min vide webinar is available in the full PD. Get it here. Tday s Learning Objectives NGSS key cncepts why this is different

More information

( ) + θ θ. ω rotation rate. θ g geographic latitude - - θ geocentric latitude - - Reference Earth Model - WGS84 (Copyright 2002, David T.

( ) + θ θ. ω rotation rate. θ g geographic latitude - - θ geocentric latitude - - Reference Earth Model - WGS84 (Copyright 2002, David T. 1 Reference Earth Mdel - WGS84 (Cpyright, David T. Sandwell) ω spherid c θ θ g a parameter descriptin frmula value/unit GM e (WGS84) 3.9864418 x 1 14 m 3 s M e mass f earth - 5.98 x 1 4 kg G gravitatinal

More information

PHYS 219 Spring semester Lecture 02: Coulomb s Law how point charges interact. Ron Reifenberger Birck Nanotechnology Center Purdue University

PHYS 219 Spring semester Lecture 02: Coulomb s Law how point charges interact. Ron Reifenberger Birck Nanotechnology Center Purdue University PHYS 19 Spring semester 016 Lecture 0: Culmb s Law hw pint charges interact Rn Reifenberger Birck Nantechnlg Center Purdue Universit Lecture 0 1 Earl Develpments in Electrstatics Tw f the ur rces in Nature:

More information

Springs in parallel. Two springs in parallel. Springs in series. Springs in series. Resonance. Forced vibrations and resonance. 2 C. 2 1/2 m.

Springs in parallel. Two springs in parallel. Springs in series. Springs in series. Resonance. Forced vibrations and resonance. 2 C. 2 1/2 m. Springs in parallel w springs in parallel Suppse yu had tw identical springs each with frce cnstant frm which an bject f mass m was suspended. he scillatin perid fr ne spring is. What wuld the scillatin

More information

Fall 2013 Physics 172 Recitation 3 Momentum and Springs

Fall 2013 Physics 172 Recitation 3 Momentum and Springs Fall 03 Physics 7 Recitatin 3 Mmentum and Springs Purpse: The purpse f this recitatin is t give yu experience wrking with mmentum and the mmentum update frmula. Readings: Chapter.3-.5 Learning Objectives:.3.

More information

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data

Examiner: Dr. Mohamed Elsharnoby Time: 180 min. Attempt all the following questions Solve the following five questions, and assume any missing data Benha University Cllege f Engineering at Banha Department f Mechanical Eng. First Year Mechanical Subject : Fluid Mechanics M111 Date:4/5/016 Questins Fr Final Crrective Examinatin Examiner: Dr. Mhamed

More information

Quiz 3 July 31, 2007 Chapters 16, 17, 18, 19, 20 Phys 631 Instructor R. A. Lindgren 9:00 am 12:00 am

Quiz 3 July 31, 2007 Chapters 16, 17, 18, 19, 20 Phys 631 Instructor R. A. Lindgren 9:00 am 12:00 am Quiz 3 July 31, 2007 Chapters 16, 17, 18, 19, 20 Phys 631 Instructor R. A. Lindgren 9:00 am 12:00 am No Books or Notes allowed Calculator without access to formulas allowed. The quiz has two parts. The

More information

Figure 1a. A planar mechanism.

Figure 1a. A planar mechanism. ME 5 - Machine Design I Fall Semester 0 Name f Student Lab Sectin Number EXAM. OPEN BOOK AND CLOSED NOTES. Mnday, September rd, 0 Write n ne side nly f the paper prvided fr yur slutins. Where necessary,

More information

Physics 111. Exam #2. February 23, 2018

Physics 111. Exam #2. February 23, 2018 Phyic Exam # February 3, 08 ame Pleae read and fllw thee intructin carefully: Read all prblem carefully befre attempting t lve them. Yur wrk mut be legible, and the rganizatin clear. Yu mut hw all wrk,

More information

Chapter II Newtonian Mechanics Single Particle

Chapter II Newtonian Mechanics Single Particle Chapter II Newtnian Mechanics Sinle Particle Recended prbles: -, -5, -6, -8, -9, -, -, -, -6, -, -, -, -5, -6, -7, -9, -30, -3, -3, -37, -38, -39, -, -, -3, -, -7, -5, -5, -53, -5.. . Newtn s Laws The

More information

205MPa and a modulus of elasticity E 207 GPa. The critical load 75kN. Gravity is vertically downward and the weight of link 3 is W3

205MPa and a modulus of elasticity E 207 GPa. The critical load 75kN. Gravity is vertically downward and the weight of link 3 is W3 ME 5 - Machine Design I Fall Semester 06 Name f Student: Lab Sectin Number: Final Exam. Open bk clsed ntes. Friday, December 6th, 06 ur name lab sectin number must be included in the spaces prvided at

More information

Solution to phys101-t112-final Exam

Solution to phys101-t112-final Exam Solution to phys101-t112-final Exam Q1. An 800-N man stands halfway up a 5.0-m long ladder of negligible weight. The base of the ladder is.0m from the wall as shown in Figure 1. Assuming that the wall-ladder

More information

Exam 1 Solutions. Prof. Darin Acosta Prof. Selman Hershfield February 6, 2007

Exam 1 Solutions. Prof. Darin Acosta Prof. Selman Hershfield February 6, 2007 PHY049 Spring 008 Prf. Darin Acta Prf. Selman Herhfiel Februar 6, 007 Nte: Mt prblem have mre than ne verin with ifferent anwer. Be careful that u check ur eam againt ur verin f the prblem. 1. Tw charge,

More information

CLASS XI SET A PHYSICS

CLASS XI SET A PHYSICS PHYSIS. If the acceleratin f wedge in the shwn arrangement is a twards left then at this instant acceleratin f the blck wuld be, (assume all surfaces t be frictinless) a () ( cs )a () a () cs a If the

More information

Chapter 2 Analysis of Power System Stability by Classical Methods

Chapter 2 Analysis of Power System Stability by Classical Methods Chapter Analyi f wer Syte Stability by Claical Methd.1 Claical Mdel A dicued in the previu Chapter, the firt tep in analyzing pwer tability i t repreent the pwer yte cpnent atheatically. The iplet yet

More information

Chapter 10. Simple Harmonic Motion and Elasticity. Example 1 A Tire Pressure Gauge

Chapter 10. Simple Harmonic Motion and Elasticity. Example 1 A Tire Pressure Gauge 0. he Ideal Spring and Simple Harmnic Mtin Chapter 0 Simple Harmnic Mtin and Elasticity F Applied x k x spring cnstant Units: N/m 0. he Ideal Spring and Simple Harmnic Mtin 0. he Ideal Spring and Simple

More information

Faculty of Engineering and Department of Physics Engineering Physics 131 Midterm Examination February 27, 2006; 7:00 pm 8:30 pm

Faculty of Engineering and Department of Physics Engineering Physics 131 Midterm Examination February 27, 2006; 7:00 pm 8:30 pm Faculty f Engineering and Department f Physics Engineering Physics 131 Midterm Examinatin February 27, 2006; 7:00 pm 8:30 pm N ntes r textbks allwed. Frmula sheet is n the last page (may be remved). Calculatrs

More information

1. Show that if the angular momentum of a boby is determined with respect to an arbitrary point A, then. r r r. H r A can be expressed by H r r r r

1. Show that if the angular momentum of a boby is determined with respect to an arbitrary point A, then. r r r. H r A can be expressed by H r r r r 1. Shw that if the angula entu f a bb is deteined with espect t an abita pint, then H can be epessed b H = ρ / v + H. This equies substituting ρ = ρ + ρ / int H = ρ d v + ρ ( ω ρ ) d and epanding, nte

More information

CHAPTER 6 -- ENERGY. Approach #2: Using the component of mg along the line of d:

CHAPTER 6 -- ENERGY. Approach #2: Using the component of mg along the line of d: Slutins--Ch. 6 (Energy) CHAPTER 6 -- ENERGY 6.) The f.b.d. shwn t the right has been prvided t identify all the frces acting n the bdy as it mves up the incline. a.) T determine the wrk dne by gravity

More information

Lecture 5: Equilibrium and Oscillations

Lecture 5: Equilibrium and Oscillations Lecture 5: Equilibrium and Oscillatins Energy and Mtin Last time, we fund that fr a system with energy cnserved, v = ± E U m ( ) ( ) One result we see immediately is that there is n slutin fr velcity if

More information

Chapter 9 Compressible Flow 667

Chapter 9 Compressible Flow 667 Chapter 9 Cmpreible Flw 667 9.57 Air flw frm a tank thrugh a nzzle int the tandard atmphere, a in Fig. P9.57. A nrmal hck tand in the exit f the nzzle, a hwn. Etimate (a) the tank preure; and (b) the ma

More information