KEY. D. 1.3 kg m. Solution: Using conservation of energy on the swing, mg( h) = 1 2 mv2 v = 2mg( h)

Size: px
Start display at page:

Download "KEY. D. 1.3 kg m. Solution: Using conservation of energy on the swing, mg( h) = 1 2 mv2 v = 2mg( h)"

Transcription

1 Phy 5 - Fall 206 Extra credit review eion - Verion A KEY Thi i an extra credit review eion. t will be worth 30 point of extra credit. Dicu and work on the problem with your group. You may ue your text book and your cla note. Name:. What i the magnitude of the momentum of a tenni ball with a diameter of 6.6 cm and a ma of 57 g that i traveling at it terminal velocity near the urface of the earth? The denity of air i.3 kg and, for a phere, c m 3 A. 29 kg m B. 0.4 kg m C kg m D..3 kg m E kg m Solution: Terminal velocity i the velocity at which the force due to gravity i equal to the drag force. So, mg 2 ρcav2 v 2mg. Thu, p mv ρca m 2mg 2m 3 g ρca ρca 2( )g kgm.3.3(0.50)(π ) The correct anwer i D. 2. A rope wing over a lake ha a vertical drop of 2.0 meter between where you (60.0 kg) tart and where the rope hang vertically. f you let go when the rope i vertical and you are.0 meter above the water, how far do you fly through the air before you hit the rock hiding jut below the urface of the water? A..4 m B..0 m C. 2.8 m D. 8.0 m E. 2.3 m Solution: Uing conervation of energy on the wing, mg( h) 2 mv2 v 2mg( h) 2g( h). That the horizontal velocity with which you fly off over the m water. t now become a kinematic problem. Horizontal launch with the velocity jut determined, at a height of h 2.0 m. t 2h 2, giving a horizontal ditance g d v x t 2g( h) 2h 2 2 ( h)h g 2 2 (2.0) m. The correct anwer i C.

2 Phy 5 - Fall 206 Verion A Page 2of 5 3. m going 35.0 m/ on the freeway (horizontal). The tire of the car in front of me pick up a rock and launche it into the air at an angle of 50 o. t reache a height of 2.0 meter before coming back down to.0 meter and triking my windhield, how fat i it going with repect to the windhield? A m B m C m D m E m Solution: vyf 2 vyi 2 + 2a( y) v yi vyf 0 2 2a( y) + 2g(2.0) 2.0 g. Uing thi initial y velocity and the launch angle, we can determine the x-component. v xi 2.0 g. We can alo determine the vertical final velocity, a the ame a an object dropped tan(50 o ) from ret, that ha fallen.0 m, vyf 2 vi 2 +2a( y) v yf 2g. We ve now determined that the final velocity of the rock with repect to the freeway i v F 2.0 g tan(50 o )î + 2gĵ. Due to the relative motion of the car, the velocity with repect to the windhield i v F ( g )î + 2gĵ 40.3î ĵ, giving a magnitude of 40.5 m. tan(50 o ) The correct anwer i C. 4. A 0.0 kg block i propelled up a lope with an angle of 30 o by a pring with a pring contant of 500 N m. f the pring i compreed by m, and µ k 0.20, how far doe the block lide pat the pring equilibrium? A m B m C m D. 3.3 m E. Doen t move. Solution: Let be the ditance the pring i compreed and d be the ditance it lide pat ( equilibrium (the thing we re looking for). All the energy come from the pring U 2 k2), and it goe into friction over the total ditance (µ k mg co θ(d + )) and fighting gravity (mg in θ(d + )). So, 2 k2 µ k mg co θ(d + ) + mg in θ(d + ) d k 2 500( ) 2mg(µ k m. co θ+in θ) 2(0)g(0.20 co 30 o +in 30 3 ) The correct anwer i C.

3 Phy 5 - Fall 206 Verion A Page 3of 5 5. A pace tation i made of a ring of uniformly ditributed ma (8000 kg) with a diameter of 5.00 km. The tation i tarted pinning by 4 thruter located along the ring. Each thruter can apply a contant 900 N force, tangential to the ring, cauing it to pin up. How long do the thruter need to fire o that omeone tanding on a cale on the inide of the ring meaure the ame weight a they did on the earth? A. 74 B. 244 C. 492 D. 348 E. 968 Solution: For the cale to read the ame a it doe on earth, the centripetal acceleration on the ring need to be g. g v2 t (ω)2 ω 2 ω g. Each thruter exert a torque of F in θ F, o Στ 4F. Στ α. r 2 dm 2π 0 ( 2 M 2π dθ) M 2. So, α Στ (900) 4F M 2 4F M. ω αt t ω α (9.806) The correct anwer i D. g 4F M g M M 4F 4F g 6. With the 2 vector, A and B, calculate A B and A B. A 5î 3ĵ + 2ˆk, B 2î + ĵ + 6ˆk A. A B 25, A B 20î 34ĵ ˆk B. A B 25, A B 20î 34ĵ ˆk C. A B, A B 20î 34ĵ ˆk D. A B 25, A B 20î + 34ĵ + ˆk E. A B, A B 20î + 34ĵ + ˆk Solution: A B ax b x + a y b y + a z b z , A B (a y b z b y a z )î (a x b z b x a z )ĵ + (a x b y b x a y )ˆk 20î 34ĵ ˆk The correct anwer i C.

4 Phy 5 - Fall 206 Verion A Page 4of 5 7. A pacehip i traveling at 500 m with repect to earth. There i an exploion which break the hip into 2 piece. The forward ection, which contain 40% of the ma i accelerated to 600 m. What i the peed at which the 2 piece are moving apart? A. 67 m B. 433 m C. 27 m D. 500 m E. 250 m Solution: The velocity of the forward ection increaed v 00 m. Uing conervation of momentum, we know that mv i.40mv f +.60mv 2f. Thi hould work in all inertial reference frame; why not chooe the one moving at 600 m with repect to the earth? That the frame in which we want the anwer anyway. n thi frame, v i 00 m and v f 0. We are looking for v 2f v i.40v f 00.40(0) 67 m. The correct anwer i A. 8. The moment of inertia of a phere around any axi through it center i 2 5 m2. A 5.0 kg phere with a radiu of 50 cm roll 4.00 m without lipping down a ramp with a lope of 35 o. How long doe it take if it i releaed from ret? A B. 3.5 C..4 D E Solution: The height change while rolling down a length ramp with an incline of θ i h in θ, meaning that U mg( h) mg in θ. For rolling motion, K 2 ω2 + 2 mv2 cm, o mg in θ 2 ω2 + 2 mv2 cm. Since it in t lipping, v cm ω ω vcm. mg in θ 2 ( v cm ) mv2 cm meaning that at the end, v cm 2g in θ m v v i+v f which mean that, ince v t 2 i 0, t 2 2 v f 2g in θ 2( 2 +) 5 2(4.00) The correct anwer i C. g in θ g in 35 m We know that 2( m 2 +) g in θ

5 Phy 5 - Fall 206 Verion A Page 5of 5 9. A particle velocity i decribed by the function V ηt 2 for ome contant η and time t. f the particle poition at t.0 i 4.0 m and the particle poition at t i 2.0 m, what i the value of η? A. 2.0 m 3 B m 3 C. 0.3 m 3 D. 3.0 m 3 E m 3 Solution: V ηt 2 mean that x t 2 t V dt t 2 t ηt 2 dt η 3 (t3 ) t 2 t η 3 (t3 2 t 3 ) η 3 ( ) 26η m We alo know that x ( ) m 8.0 m. Thu, 3 26η 8.0 η 0.92 m where the unit came from jut looking at what they would 3 3 need to be o that η 3 (t3 ) end up in unit of meter. The correct anwer i E. 0. A map to Beardle Luke treaure ay to head 200 pace on a bearing 30 o wet of north, then 50 pace wet, followed by 300 pace outh to avoid walking through the forbidden meadow. You decide that the meadow doen t ound o bad and that you hould take the mot direct path. How far hould you go in which direction? A. 380 pace 32 o outh of wet B. 280 pace 63 o outh of wet C. 280 pace 27 o outh of wet D. 535 pace 62 o north of eat E. 380 pace 58 o outh of wet Solution: Firt off... don t cut through the forbidden meadow. That a horrible idea. But if you did, you d want your total diplacement D ( 200 in(30) 50) eat ˆ + (200 co(30) 300) north ˆ 250eat ˆ 27north. ˆ Which ha a magnitude of and a direction of tan (27/250) 27 o, outh of wet. The correct anwer i C.

Physics Exam 3 Formulas

Physics Exam 3 Formulas Phyic 10411 Exam III November 20, 2009 INSTRUCTIONS: Write your NAME on the front of the blue exam booklet. The exam i cloed book, and you may have only pen/pencil and a calculator (no tored equation or

More information

t α z t sin60 0, where you should be able to deduce that the angle between! r and! F 1

t α z t sin60 0, where you should be able to deduce that the angle between! r and! F 1 PART III Problem Problem1 A computer dik tart rotating from ret at contant angular acceleration. If it take 0.750 to complete it econd revolution: a) How long doe it take to complete the firt complete

More information

Uniform Acceleration Problems Chapter 2: Linear Motion

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

More information

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

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

More information

EF 151 Final Exam, Spring, 2009 Page 2 of 10. EF 151 Final Exam, Spring, 2009 Page 1 of 10. Name: Section: sina ( ) ( )( ) 2. a b c = = cosc.

EF 151 Final Exam, Spring, 2009 Page 2 of 10. EF 151 Final Exam, Spring, 2009 Page 1 of 10. Name: Section: sina ( ) ( )( ) 2. a b c = = cosc. EF 5 Final Exam, Spring, 9 Page of EF 5 Final Exam, Spring, 9 Page of Name: Section: Guideline: Aume 3 ignificant figure for all given number unle otherwie tated Show all of your work no work, no credit

More information

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003 FALL TERM EXAM, PHYS 111, INTRODUCTORY PHYSICS I Saturday, 14 December 013, 1PM to 4 PM, AT 1003 NAME: STUDENT ID: INSTRUCTION 1. Thi exam booklet ha 14 page. Make ure none are miing. There i an equation

More information

DYNAMICS OF ROTATIONAL MOTION

DYNAMICS OF ROTATIONAL MOTION DYNAMICS OF ROTATIONAL MOTION 10 10.9. IDENTIFY: Apply I. rad/rev SET UP: 0 0. (400 rev/min) 419 rad/ 60 /min EXECUTE: 0 419 rad/ I I (0 kg m ) 11 N m. t 800 EVALUATE: In I, mut be in rad/. 10.. IDENTIFY:

More information

Linear Motion, Speed & Velocity

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

More information

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

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

More information

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

Physics 218: Exam 1. Class of 2:20pm. February 14th, You have the full class period to complete the exam.

Physics 218: Exam 1. Class of 2:20pm. February 14th, You have the full class period to complete the exam. Phyic 218: Exam 1 Cla of 2:20pm February 14th, 2012. Rule of the exam: 1. You have the full cla period to complete the exam. 2. Formulae are provided on the lat page. You may NOT ue any other formula heet.

More information

Halliday/Resnick/Walker 7e Chapter 6

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

More information

Holt Physics Problem 3E

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

More information

( kg) (410 m/s) 0 m/s J. W mv mv m v v. 4 mv

( kg) (410 m/s) 0 m/s J. W mv mv m v v. 4 mv PHYS : Solution to Chapter 6 Home ork. RASONING a. The work done by the gravitational orce i given by quation 6. a = (F co θ). The gravitational orce point downward, oppoite to the upward vertical diplacement

More information

Midterm Review - Part 1

Midterm Review - Part 1 Honor Phyic Fall, 2016 Midterm Review - Part 1 Name: Mr. Leonard Intruction: Complete the following workheet. SHOW ALL OF YOUR WORK. 1. Determine whether each tatement i True or Fale. If the tatement i

More information

Name: Answer Key Date: Regents Physics. Energy

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

More information

two equations that govern the motion of the fluid through some medium, like a pipe. These two equations are the

two equations that govern the motion of the fluid through some medium, like a pipe. These two equations are the Fluid and Fluid Mechanic Fluid in motion Dynamic Equation of Continuity After having worked on fluid at ret we turn to a moving fluid To decribe a moving fluid we develop two equation that govern the motion

More information

Physics 2212 G Quiz #2 Solutions Spring 2018

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

More information

PHYSICS 211 MIDTERM II 12 May 2004

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

More information

Constant Force: Projectile Motion

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

More information

Bernoulli s equation may be developed as a special form of the momentum or energy equation.

Bernoulli s equation may be developed as a special form of the momentum or energy equation. BERNOULLI S EQUATION Bernoulli equation may be developed a a pecial form of the momentum or energy equation. Here, we will develop it a pecial cae of momentum equation. Conider a teady incompreible flow

More information

HSC PHYSICS ONLINE KINEMATICS EXPERIMENT

HSC PHYSICS ONLINE KINEMATICS EXPERIMENT HSC PHYSICS ONLINE KINEMATICS EXPERIMENT RECTILINEAR MOTION WITH UNIFORM ACCELERATION Ball rolling down a ramp Aim To perform an experiment and do a detailed analyi of the numerical reult for the rectilinear

More information

Physics 6A. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6A. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic 6A Angular Momentum For Campu earning Angular Momentum Thi i the rotational equivalent of linear momentum. t quantifie the momentum of a rotating object, or ytem of object. f we imply tranlate the

More information

Physics 2. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 2. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic Angular Momentum For Campu earning Angular Momentum Thi i the rotational equivalent of linear momentum. t quantifie the momentum of a rotating object, or ytem of object. To get the angular momentum,

More information

Elastic Collisions Definition Examples Work and Energy Definition of work Examples. Physics 201: Lecture 10, Pg 1

Elastic Collisions Definition Examples Work and Energy Definition of work Examples. Physics 201: Lecture 10, Pg 1 Phyic 131: Lecture Today Agenda Elatic Colliion Definition i i Example Work and Energy Definition of work Example Phyic 201: Lecture 10, Pg 1 Elatic Colliion During an inelatic colliion of two object,

More information

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym NAME: STUDENT ID: INSTRUCTION 1. This exam booklet has 13 pages. Make sure none are missing 2.

More information

Prof. Dr. Ibraheem Nasser Examples_6 October 13, Review (Chapter 6)

Prof. Dr. Ibraheem Nasser Examples_6 October 13, Review (Chapter 6) Prof. Dr. Ibraheem Naer Example_6 October 13, 017 Review (Chapter 6) cceleration of a loc againt Friction (1) cceleration of a bloc on horizontal urface When body i moving under application of force P,

More information

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

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

More information

Conservation of Energy

Conservation of Energy Conervative Force Conervation of Energ force i conervative if the work done b the force from r to r, but depend on initial and final poition onl Conervative Non-conervative Section #4.5 #4.6 Conervation

More information

PROBLEMS ON WORK AND ENERGY PRINCIPLE

PROBLEMS ON WORK AND ENERGY PRINCIPLE PROLEMS ON WORK ND ENERGY PRINCIPLE PROLEMS. he.8 kg collar lide with negligible friction on the fixed rod in the vertical plane. If the collar tart from ret at under the action of the contant 8-N horizontal

More information

We define angular displacement, θ, and angular velocity, ω. What's a radian?

We define angular displacement, θ, and angular velocity, ω. What's a radian? We define angular displacement, θ, and angular velocity, ω Units: θ = rad ω = rad/s What's a radian? Radian is the ratio between the length of an arc and its radius note: counterclockwise is + clockwise

More information

Displacement vs. Distance Suppose that an object starts at rest and that the object is subject to the acceleration function t

Displacement vs. Distance Suppose that an object starts at rest and that the object is subject to the acceleration function t MTH 54 Mr. Simond cla Diplacement v. Ditance Suppoe that an object tart at ret and that the object i ubject to the acceleration function t a() t = 4, t te over the time interval [,1 ]. Find both the diplacement

More information

PHYSICS 221 SPRING EXAM 1: February 20, 2014; 8:15pm 10:15pm

PHYSICS 221 SPRING EXAM 1: February 20, 2014; 8:15pm 10:15pm PHYSICS 221 SPRING 2014 EXAM 1: February 20, 2014; 8:15pm 10:15pm Name (printed): Recitation Instructor: Section # INSTRUCTIONS: This exam contains 25 multiple-choice questions plus 2 extra credit questions,

More information

AP Physics Charge Wrap up

AP Physics Charge Wrap up AP Phyic Charge Wrap up Quite a few complicated euation for you to play with in thi unit. Here them babie i: F 1 4 0 1 r Thi i good old Coulomb law. You ue it to calculate the force exerted 1 by two charge

More information

particle p = m v F ext = d P = M d v cm dt

particle p = m v F ext = d P = M d v cm dt Lecture 11: Momentum and Collisions; Introduction to Rotation 1 REVIEW: (Chapter 8) LINEAR MOMENTUM and COLLISIONS The first new physical quantity introduced in Chapter 8 is Linear Momentum Linear Momentum

More information

Unit 2 Linear Motion

Unit 2 Linear Motion Unit Linear Motion Linear Motion Key Term - How to calculate Speed & Ditance 1) Motion Term: a. Symbol for time = (t) b. Diplacement (X) How far omething travel in a given direction. c. Rate How much omething

More information

PHYSICSBOWL March 29 April 14, 2017

PHYSICSBOWL March 29 April 14, 2017 PHYSICSBOWL 2017 March 29 April 14, 2017 40 QUESTIONS 45 MINUTES The ponor of the 2017 PhyicBowl, including the American Aociation of Phyic Teacher, are providing ome of the prize to recognize outtanding

More information

PHY 171 Practice Test 3 Solutions Fall 2013

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

More information

Practice Midterm #1 Solutions. Physics 6A

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

More information

Frictional Forces. Friction has its basis in surfaces that are not completely smooth: 1/29

Frictional Forces. Friction has its basis in surfaces that are not completely smooth: 1/29 Frictional Force Friction ha it bai in urface that are not completely mooth: 1/29 Microcopic Friction Surface Roughne Adheion Magnified ection of a polihed teel urface howing urface irregularitie about

More information

UCM/CNF Worksheet 3: Universal Gravitation Adapted from AMTA 2013 Modeling Instruction Materials (U7 CNF Model WS4, V3.1)

UCM/CNF Worksheet 3: Universal Gravitation Adapted from AMTA 2013 Modeling Instruction Materials (U7 CNF Model WS4, V3.1) UCM/CNF Workheet 3: Univeral Gravitation Adapted from AMA 2013 Modeling Intruction Material (U7 CNF Model WS4, V3.1) CELESIAL EFEENCE ABLE Body Ma (kg) adiu (km) Ditance from Surface Gravitational Sun

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

Discover the answer to this question in this chapter.

Discover the answer to this question in this chapter. Erwan, whoe ma i 65 kg, goe Bungee jumping. He ha been in free-fall for 0 m when the bungee rope begin to tretch. hat will the maximum tretching of the rope be if the rope act like a pring with a 100 N/m

More information

ME 141. Engineering Mechanics

ME 141. Engineering Mechanics ME 141 Engineering Mechanic Lecture 14: Plane motion of rigid bodie: Force and acceleration Ahmad Shahedi Shakil Lecturer, Dept. of Mechanical Engg, BUET E-mail: hakil@me.buet.ac.bd, hakil6791@gmail.com

More information

Physics Sp Exam #3 Name:

Physics Sp Exam #3 Name: Phyic 160-0 Sp. 017 Exa #3 Nae: 1) In electrodynaic, a agnetic field produce a force on a oving charged particle that i alway perpendicular to the direction the particle i oving. How doe thi force affect

More information

PHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010

PHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010 PHYSICS 1, FALL 010 EXAM 1 Solutions WEDNESDAY, SEPTEMBER 9, 010 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively. In

More information

Physics 6A. Practice Final (Fall 2009) solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6A. Practice Final (Fall 2009) solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic 6A Practice inal (all 009) olution or Capu Learning Aitance Service at UCSB . A locootive engine of a M i attached to 5 train car, each of a M. The engine produce a contant force that ove the train

More information

ELECTROMAGNETIC WAVES AND PHOTONS

ELECTROMAGNETIC WAVES AND PHOTONS CHAPTER ELECTROMAGNETIC WAVES AND PHOTONS Problem.1 Find the magnitude and direction of the induced electric field of Example.1 at r = 5.00 cm if the magnetic field change at a contant rate from 0.500

More information

Momentum. Momentum and Energy. Momentum and Impulse. Momentum. Impulse. Impulse Increasing Momentum

Momentum. Momentum and Energy. Momentum and Impulse. Momentum. Impulse. Impulse Increasing Momentum Momentum and Energy Chapter 3, page 59-80 Review quetion: 1,3,4,7, 8, 11, 1, 14-17, 0, 1 Momentum Momentum i inertia in motion Ma x velocity Ha both magnitude and direction Large ma or high peed can give

More information

Chapters 10 & 11: Rotational Dynamics Thursday March 8 th

Chapters 10 & 11: Rotational Dynamics Thursday March 8 th Chapters 10 & 11: Rotational Dynamics Thursday March 8 th Review of rotational kinematics equations Review and more on rotational inertia Rolling motion as rotation and translation Rotational kinetic energy

More information

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

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

More information

Chapter 9 Review. Block: Date:

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

More information

Translational vs Rotational. m x. Connection Δ = = = = = = Δ = = = = = = Δ =Δ = = = = = 2 / 1/2. Work

Translational vs Rotational. m x. Connection Δ = = = = = = Δ = = = = = = Δ =Δ = = = = = 2 / 1/2. Work Translational vs Rotational / / 1/ Δ m x v dx dt a dv dt F ma p mv KE mv Work Fd / / 1/ θ ω θ α ω τ α ω ω τθ Δ I d dt d dt I L I KE I Work / θ ω α τ Δ Δ c t s r v r a v r a r Fr L pr Connection Translational

More information

Circular Motion, Pt 2: Angular Dynamics. Mr. Velazquez AP/Honors Physics

Circular Motion, Pt 2: Angular Dynamics. Mr. Velazquez AP/Honors Physics Circular Motion, Pt 2: Angular Dynamics Mr. Velazquez AP/Honors Physics Formulas: Angular Kinematics (θ must be in radians): s = rθ Arc Length 360 = 2π rads = 1 rev ω = θ t = v t r Angular Velocity α av

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

Unit I Review Worksheet Key

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

More information

Chapter 6: Work and Kinetic Energy

Chapter 6: Work and Kinetic Energy Chapter 6: Work and Kinetic Energy Suppose you want to find the final velocity of an object being acted on by a variable force. Newton s 2 nd law gives the differential equation (for 1D motion) dv dt =

More information

y(t) = y 0 t! 1 2 gt 2. With y(t final ) = 0, we can solve this for v 0 : v 0 A ĵ. With A! ĵ =!2 and A! = (2) 2 + (!

y(t) = y 0 t! 1 2 gt 2. With y(t final ) = 0, we can solve this for v 0 : v 0 A ĵ. With A! ĵ =!2 and A! = (2) 2 + (! 1. The angle between the vector! A = 3î! 2 ĵ! 5 ˆk and the positive y axis, in degrees, is closest to: A) 19 B) 71 C) 90 D) 109 E) 161 The dot product between the vector! A = 3î! 2 ĵ! 5 ˆk and the unit

More information

4) Vector = and vector = What is vector = +? A) B) C) D) E)

4) Vector = and vector = What is vector = +? A) B) C) D) E) 1) Suppose that an object is moving with constant nonzero acceleration. Which of the following is an accurate statement concerning its motion? A) In equal times its speed changes by equal amounts. B) In

More information

HSC PHYSICS ONLINE B F BA. repulsion between two negatively charged objects. attraction between a negative charge and a positive charge

HSC PHYSICS ONLINE B F BA. repulsion between two negatively charged objects. attraction between a negative charge and a positive charge HSC PHYSICS ONLINE DYNAMICS TYPES O ORCES Electrostatic force (force mediated by a field - long range: action at a distance) the attractive or repulsion between two stationary charged objects. AB A B BA

More information

Physics 6A. Practice Midterm #2 solutions

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

More information

Two-Dimensional Rotational Kinematics

Two-Dimensional Rotational Kinematics Two-Dimensional Rotational Kinematics Rigid Bodies A rigid body is an extended object in which the distance between any two points in the object is constant in time. Springs or human bodies are non-rigid

More information

Problem 1 Problem 2 Problem 3 Problem 4 Total

Problem 1 Problem 2 Problem 3 Problem 4 Total Name Section THE PENNSYLVANIA STATE UNIVERSITY Department of Engineering Science and Mechanics Engineering Mechanics 12 Final Exam May 5, 2003 8:00 9:50 am (110 minutes) Problem 1 Problem 2 Problem 3 Problem

More information

Chapters 5-6. Dynamics: Forces and Newton s Laws of Motion. Applications

Chapters 5-6. Dynamics: Forces and Newton s Laws of Motion. Applications Chapters 5-6 Dynamics: orces and Newton s Laws of Motion. Applications That is, describing why objects move orces Newton s 1 st Law Newton s 2 nd Law Newton s 3 rd Law Examples of orces: Weight, Normal,

More information

SKAA 1213 Engineering Mechanics

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

More information

PLANAR KINETICS OF A RIGID BODY FORCE AND ACCELERATION

PLANAR KINETICS OF A RIGID BODY FORCE AND ACCELERATION PLANAR KINETICS OF A RIGID BODY FORCE AND ACCELERATION I. Moment of Inertia: Since a body has a definite size and shape, an applied nonconcurrent force system may cause the body to both translate and rotate.

More information

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

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

More information

Review questions. Before the collision, 70 kg ball is stationary. Afterward, the 30 kg ball is stationary and 70 kg ball is moving to the right.

Review questions. Before the collision, 70 kg ball is stationary. Afterward, the 30 kg ball is stationary and 70 kg ball is moving to the right. Review questions Before the collision, 70 kg ball is stationary. Afterward, the 30 kg ball is stationary and 70 kg ball is moving to the right. 30 kg 70 kg v (a) Is this collision elastic? (b) Find the

More information

= o + t = ot + ½ t 2 = o + 2

= o + t = ot + ½ t 2 = o + 2 Chapters 8-9 Rotational Kinematics and Dynamics Rotational motion Rotational motion refers to the motion of an object or system that spins about an axis. The axis of rotation is the line about which the

More information

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

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

More information

= 40 N. Q = 60 O m s,k

= 40 N. Q = 60 O m s,k Sample Exam #2 Technical Physics Multiple Choice ( 6 Points Each ): F app = 40 N 20 kg Q = 60 O = 0 1. A 20 kg box is pulled along a frictionless floor with an applied force of 40 N. The applied force

More information

Notes on Torque. We ve seen that if we define torque as rfsinθ, and the N 2. i i

Notes on Torque. We ve seen that if we define torque as rfsinθ, and the N 2. i i Notes on Torque We ve seen that if we define torque as rfsinθ, and the moment of inertia as N, we end up with an equation mr i= 1 that looks just like Newton s Second Law There is a crucial difference,

More information

CHAPTER VII FRICTION

CHAPTER VII FRICTION CHAPTER VII FRICTION 1- The block brake conit of a pin-connected lever and friction block at B. The coefficient of tatic friction between the wheel and the lever i and a torque of i applied to the wheel.

More information

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

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

More information

Table of Contents. Pg. # Momentum & Impulse (Bozemanscience Videos) 1 1/11/16

Table of Contents. Pg. # Momentum & Impulse (Bozemanscience Videos) 1 1/11/16 Table of Contents g. # 1 1/11/16 Momentum & Impulse (Bozemanscience Videos) 2 1/13/16 Conservation of Momentum 3 1/19/16 Elastic and Inelastic Collisions 4 1/19/16 Lab 1 Momentum 5 1/26/16 Rotational Dynamics

More information

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

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

More information

CEE 320 Midterm Examination (1 hour)

CEE 320 Midterm Examination (1 hour) Examination (1 hour) Pleae write your name on thi cover. Pleae write you lat name on all other exam page Thi examination i open-book, open-note. There are 5 quetion worth a total of 100 point. Each quetion

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

Afternoon Section. Physics 1210 Exam 2 November 8, ! v = d! r dt. a avg. = v2. ) T 2! w = m g! f s. = v at v 2 1.

Afternoon Section. Physics 1210 Exam 2 November 8, ! v = d! r dt. a avg. = v2. ) T 2! w = m g! f s. = v at v 2 1. Name Physics 1210 Exam 2 November 8, 2012 Afternoon Section Please write directly on the exam and attach other sheets of work if necessary. Calculators are allowed. No notes or books may be used. Multiple-choice

More information

Conservation of Energy

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

More information

PRACTICE TEST for Midterm Exam

PRACTICE TEST for Midterm Exam South Pasadena AP Physics PRACTICE TEST for Midterm Exam FORMULAS Name Period Date / / d = vt d = v o t + ½ at 2 d = v o + v 2 t v = v o + at v 2 = v 2 o + 2ad v = v x 2 + v y 2 = tan 1 v y v v x = v cos

More information

s much time does it take for the dog to run a distance of 10.0m

s much time does it take for the dog to run a distance of 10.0m ATTENTION: All Diviion I tudent, START HERE. All Diviion II tudent kip the firt 0 quetion, begin on #.. Of the following, which quantity i a vector? Energy (B) Ma Average peed (D) Temperature (E) Linear

More information

Webreview Torque and Rotation Practice Test

Webreview Torque and Rotation Practice Test Please do not write on test. ID A Webreview - 8.2 Torque and Rotation Practice Test Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A 0.30-m-radius automobile

More information

PHY2053 General Physics I

PHY2053 General Physics I PHY2053 General Physics I Section 584771 Prof. Douglas H. Laurence Final Exam May 3, 2018 Name: 1 Instructions: This final exam is a take home exam. It will be posted online sometime around noon of the

More information

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003 FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003 NAME: STUDENT ID: INSTRUCTION 1. This exam booklet has 14 pages. Make sure none are missing 2. There is

More information

Physics 11 Fall 2012 Practice Problems 6

Physics 11 Fall 2012 Practice Problems 6 Physics 11 Fall 2012 Practice Problems 6 1. Two points are on a disk that is turning about a fixed axis perpendicular to the disk and through its center at increasing angular velocity. One point is on

More information

(k = force constant of the spring)

(k = force constant of the spring) Lecture 10: Potential Energy, Momentum and Collisions 1 Chapter 7: Conservation of Mechanical Energy in Spring Problems The principle of conservation of Mechanical Energy can also be applied to systems

More information

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009 PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively.

More information

Phys 1401: General Physics I

Phys 1401: General Physics I 1. (0 Points) What course is this? a. PHYS 1401 b. PHYS 1402 c. PHYS 2425 d. PHYS 2426 2. (0 Points) Which exam is this? a. Exam 1 b. Exam 2 c. Final Exam 3. (0 Points) What version of the exam is this?

More information

Work. Kinetic and Potential Energy. Work. Transference of Energy Work = Force x distance. Supplemental Text Material Pages

Work. Kinetic and Potential Energy. Work. Transference of Energy Work = Force x distance. Supplemental Text Material Pages Kinetic and Potential Energy Supplemental Text Material Page 36-333 Tranference of Energy = Force x ditance Lifting load againt the force of the weight of the object Twice the ditance reult in twice the

More information

Phys101 Third Major-161 Zero Version Coordinator: Dr. Ayman S. El-Said Monday, December 19, 2016 Page: 1

Phys101 Third Major-161 Zero Version Coordinator: Dr. Ayman S. El-Said Monday, December 19, 2016 Page: 1 Coordinator: Dr. Ayman S. El-Said Monday, December 19, 2016 Page: 1 Q1. A water molecule (H 2 O) consists of an oxygen (O) atom of mass 16m and two hydrogen (H) atoms, each of mass m, bound to it (see

More information

Uniform Circular Motion

Uniform Circular Motion Uniform Circular Motion Motion in a circle at constant angular speed. ω: angular velocity (rad/s) Rotation Angle The rotation angle is the ratio of arc length to radius of curvature. For a given angle,

More information

MHS. Applied Math. Sample Questions. Exam to go from grade 11 to grade 12

MHS. Applied Math. Sample Questions. Exam to go from grade 11 to grade 12 MHS Applied Math Exam to go from grade 11 to grade 1 Sample Questions 1. OP + PA + AR = 1. OPAR. AR 3. OR. Given two vectors u and v in the box below, how can we correctly find their sum, u + v, using

More information

Chapter 10: Dynamics of Rotational Motion

Chapter 10: Dynamics of Rotational Motion Chapter 10: Dynamics of Rotational Motion What causes an angular acceleration? The effectiveness of a force at causing a rotation is called torque. QuickCheck 12.5 The four forces shown have the same strength.

More information

303b Reducing the impact (Accelerometer & Light gate)

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

More information

Physics Final Exam Formulas

Physics Final Exam Formulas INSTRUCTIONS: Write your NAME on the front of the blue exam booklet. The exam is closed book, and you may have only pens/pencils and a calculator (no stored equations or programs and no graphing). Show

More information

General Physics (PHY 2130)

General Physics (PHY 2130) General Physics (PHY 130) Lecture 0 Rotational dynamics equilibrium nd Newton s Law for rotational motion rolling Exam II review http://www.physics.wayne.edu/~apetrov/phy130/ Lightning Review Last lecture:

More information

Version A (01) Question. Points

Version A (01) Question. Points Question Version A (01) Version B (02) 1 a a 3 2 a a 3 3 b a 3 4 a a 3 5 b b 3 6 b b 3 7 b b 3 8 a b 3 9 a a 3 10 b b 3 11 b b 8 12 e e 8 13 a a 4 14 c c 8 15 c c 8 16 a a 4 17 d d 8 18 d d 8 19 a a 4

More information

Angular Displacement. θ i. 1rev = 360 = 2π rads. = "angular displacement" Δθ = θ f. π = circumference. diameter

Angular Displacement. θ i. 1rev = 360 = 2π rads. = angular displacement Δθ = θ f. π = circumference. diameter Rotational Motion Angular Displacement π = circumference diameter π = circumference 2 radius circumference = 2πr Arc length s = rθ, (where θ in radians) θ 1rev = 360 = 2π rads Δθ = θ f θ i = "angular displacement"

More information

Impulse. calculate the impulse given to an object calculate the change in momentum as the result of an impulse

Impulse. calculate the impulse given to an object calculate the change in momentum as the result of an impulse Add Important Impule Page: 386 Note/Cue Here NGSS Standard: N/A Impule MA Curriculum Framework (2006): 2.5 AP Phyic 1 Learning Objective: 3.D.2.1, 3.D.2.2, 3.D.2.3, 3.D.2.4, 4.B.2.1, 4.B.2.2 Knowledge/Undertanding

More information