PHYSICS 211 MIDTERM I 22 October 2003

Similar documents
PHYSICS 211 MIDTERM I 21 April 2004

Physics 110. Spring Exam #1. April 16, Name

PRACTICE EXAM 2 SOLUTIONS

First, we will find the components of the force of gravity: Perpendicular Forces (using away from the ramp as positive) ma F

PHYS Summer Professor Caillault Homework Solutions. Chapter 2

Problems (Show your work!)

AP Physics 1. Slide 1 / 71. Slide 2 / 71. Slide 3 / 71. Circular Motion. Topics of Uniform Circular Motion (UCM)

Physics Honors. Final Exam Review Free Response Problems

PHYS 601 HW 5 Solution. We wish to find a Fourier expansion of e sin ψ so that the solution can be written in the form

Dynamics: Newton s Laws of Motion

A wire. 100 kg. Fig. 1.1

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Plane Motion of Rigid Bodies: Forces and Accelerations. Seventh Edition CHAPTER

Distance And Velocity

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

MATH 115 FINAL EXAM. April 25, 2005

In-Class Problems 2 and 3: Projectile Motion Solutions. In-Class Problem 2: Throwing a Stone Down a Hill

Practice Final. Name: Problem 1. Show all of your work, label your answers clearly, and do not use a calculator.

Mathematics of Motion II Projectiles

13.4 Work done by Constant Forces

Physics 207 Lecture 7

16 Newton s Laws #3: Components, Friction, Ramps, Pulleys, and Strings

JURONG JUNIOR COLLEGE

Forces from Strings Under Tension A string under tension medites force: the mgnitude of the force from section of string is the tension T nd the direc

Phys101 Lecture 4,5 Dynamics: Newton s Laws of Motion

( ) where f ( x ) is a. AB Calculus Exam Review Sheet. A. Precalculus Type problems. Find the zeros of f ( x).

Student Session Topic: Particle Motion

3. Vectors. Vectors: quantities which indicate both magnitude and direction. Examples: displacemement, velocity, acceleration

200 points 5 Problems on 4 Pages and 20 Multiple Choice/Short Answer Questions on 5 pages 1 hour, 48 minutes

_3-----"/- ~StudI_G u_id_e_-..,...-~~_~

4-4 E-field Calculations using Coulomb s Law

( ) Same as above but m = f x = f x - symmetric to y-axis. find where f ( x) Relative: Find where f ( x) x a + lim exists ( lim f exists.

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

Year 12 Mathematics Extension 2 HSC Trial Examination 2014

Study Guide Final Exam. Part A: Kinetic Theory, First Law of Thermodynamics, Heat Engines

7.1 Integral as Net Change Calculus. What is the total distance traveled? What is the total displacement?

A little harder example. A block sits at rest on a flat surface. The block is held down by its weight. What is the interaction pair for the weight?

MASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS WEEK 11 WRITTEN EXAMINATION 2 SOLUTIONS SECTION 1 MULTIPLE CHOICE QUESTIONS

Physics 212. Faraday s Law

pivot F 2 F 3 F 1 AP Physics 1 Practice Exam #3 (2/11/16)

Section 5.1 #7, 10, 16, 21, 25; Section 5.2 #8, 9, 15, 20, 27, 30; Section 5.3 #4, 6, 9, 13, 16, 28, 31; Section 5.4 #7, 18, 21, 23, 25, 29, 40

20.2. The Transform and its Inverse. Introduction. Prerequisites. Learning Outcomes

1. Find the derivative of the following functions. a) f(x) = 2 + 3x b) f(x) = (5 2x) 8 c) f(x) = e2x

HIGHER SCHOOL CERTIFICATE EXAMINATION MATHEMATICS 4 UNIT (ADDITIONAL) Time allowed Three hours (Plus 5 minutes reading time)

[ ( ) ( )] Section 6.1 Area of Regions between two Curves. Goals: 1. To find the area between two curves

Version 001 HW#6 - Electromagnetic Induction arts (00224) 1 3 T

Motion. Acceleration. Part 2: Constant Acceleration. October Lab Phyiscs. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Sample Problems for the Final of Math 121, Fall, 2005

SOLUTIONS TO CONCEPTS CHAPTER 6

7.1 Integral as Net Change and 7.2 Areas in the Plane Calculus

Section 4.8. D v(t j 1 ) t. (4.8.1) j=1

FULL MECHANICS SOLUTION

SAINT IGNATIUS COLLEGE

Physics 105 Exam 2 10/31/2008 Name A

ME 141. Lecture 10: Kinetics of particles: Newton s 2 nd Law

4-6 ROTATIONAL MOTION

Mathematics Extension 2

2. The Laplace Transform

Physics 2135 Exam 3 April 21, 2015

ES.182A Topic 32 Notes Jeremy Orloff

A formula sheet and table of physical constants is attached to this paper.

Lecture 8. Newton s Laws. Applications of the Newton s Laws Problem-Solving Tactics. Physics 105; Fall Inertial Frames: T = mg

DO NOT OPEN THIS EXAM BOOKLET UNTIL INSTRUCTED TO DO SO.

SOLUTIONS TO CONCEPTS CHAPTER

Ch AP Problems

Physics 121 Sample Common Exam 1 NOTE: ANSWERS ARE ON PAGE 8. Instructions:

Numerical Problems With Solutions(STD:-XI)

Prep Session Topic: Particle Motion

Mathematics Extension 1

DESCRIBING MOTION: KINEMATICS IN ONE DIMENSION

A B C. Solution: a The cart moves down the incline with acceleration a

BME 207 Introduction to Biomechanics Spring 2018

Chapter 5 Exercise 5A

Section 14.3 Arc Length and Curvature

Types of forces. Types of Forces

SECTION B Circular Motion

approaches as n becomes larger and larger. Since e > 1, the graph of the natural exponential function is as below

A. Limits - L Hopital s Rule ( ) How to find it: Try and find limits by traditional methods (plugging in). If you get 0 0 or!!, apply C.! 1 6 C.

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 16 CHAPTER 16

Review Exercises for Chapter 4

Lecture 5. Today: Motion in many dimensions: Circular motion. Uniform Circular Motion

APPLIED THERMODYNAMICS TUTORIAL 6 AIR-VAPOUR MIXTURES

MATH 144: Business Calculus Final Review

SPECIALIST MATHEMATICS

ROB EBY Blinn College Mathematics Department

Dynamics Applying Newton s Laws Accelerated Frames

PHYSICS 211 MIDTERM II 12 May 2004

PhysicsAndMathsTutor.com

Math 8 Winter 2015 Applications of Integration

Assistant Professor: Zhou Yufeng. N , ,

5 Accumulated Change: The Definite Integral

Math 113 Exam 1-Review

( ) where f ( x ) is a. AB Calculus Exam Review Sheet. A. Precalculus Type problems. Find the zeros of f ( x).

MEP Practice Book ES19

- 5 - TEST 2. This test is on the final sections of this session's syllabus and. should be attempted by all students.

+ r Position Velocity

Model Solutions to Assignment 4

Section 6: Area, Volume, and Average Value

Correct answer: 0 m/s 2. Explanation: 8 N

Version 001 Review 1: Mechanics tubman (IBII ) During each of the three intervals correct

A. Limits - L Hopital s Rule. x c. x c. f x. g x. x c 0 6 = 1 6. D. -1 E. nonexistent. ln ( x 1 ) 1 x 2 1. ( x 2 1) 2. 2x x 1.

Transcription:

PHYSICS MIDTERM I October 3 Exm i cloed book, cloed note. Ue onl our formul heet. Write ll work nd nwer in exm booklet. The bck of pge will not be grded unle ou o requet on the front of the pge. Show ll our work nd explin our reoning (except on #). Prtil credit will be given (not on #). No credit will be given if no work i hown (not on #). If ou hve quetion, rie our hnd or come to the front.. ( point) For ech of thee multiple choice quetion, indicte the correct repone (A, B, C, or D (where needed)) on the pge for problem in our exm booklet. i) Two block re puhed cro frictionle floor b horizontl force F pplied to block. I the mgnitude of F (the force on block due to block ), greter thn, le thn, or the me the mgnitude of F? A) Greter thn. B) Le thn. C) The me. ii) To drive from point A to point B, there re four poible route, hown t right. If the time to drive ech route i the me, long which route i the verge peed gretet? A) B) C) 3 A D) 3 F m m B iii) The m m i ttched b rope to pot t the upper end of the rmp. Wht hppen to the mgnitude of the norml force on the block (due to the rmp) the ngle θ of the rmp i increed? A) It incree. B) It decree. C) It doe not chnge. m θ iv) The figure t right how three ditinct poibilitie for the velocit nd ccelertion of prticle t prticulr intnt. For which poibilit (A, B, or C) i the peed of the prticle not chnging t thi prticulr intnt? v v v A B C v) Two bll re thrown imultneoul in the ir nd follow the prbolic trjectorie hown t right. Which bll h the lrget mgnitude of the verticl component of velocit when it hit the ground? A) B) C) The bll hve the me verticl component of velocit.

. ( point) The grph below how the velocit of our cr ou trvel from home (trting t t = ) to the tore (rriving t t = ): velocit (m/) 6 8 6-6 8 time (econd) ) Drw grph of the ccelertion of our cr during the journe. b) How fr did ou trvel from our houe to the tore? c) Wht w our verge velocit during the time intervl -> econd? d) Wht w our verge ccelertion during the time intervl -> econd? 3. ( point) A bll i thrown from the ground into the ir. When the bll i t height of.8 m, the velocit i oberved to be v r = 9. mˆi + m ˆj ( î horizontl nd ĵ upwrd). Aume g = m/. ) To wht mximum height bove the ground will the bll rie? b) How fr doe the bll lnd from where it w thrown (uming flt ground)? c) How long doe the bll remin in the ir?. ( point) A 5 kg bowling bll i dropped from tower into deep vt of melted chocolte. When the bll hit the chocolte it h peed of 8 m/. The bll come to ret in the chocolte fter trveling ditnce of 8 m. Aume g = m/. () Wht i the ccelertion of the bll in the chocolte, uming it remin contnt? (b) Wht i the force exerted b the chocolte on the bll it i moving in the chocolte? (c) How long doe it tke for the bll to come to ret fter entering the chocolte? 5. ( point) Conider pulle tem in the initil tte hown t right. The green dog i up. The ellow dog i down. The green dog h m (m ) three time the m (m ) of the ellow dog. Ignore the m of the bucket, the rope, nd the pulle. Ignore friction. Grvit (g) point down. () Drw free-bod digrm for ech dog. (b) Find the ccelertion of the dog, in term of g. (c) Find the tenion in the rope. (d) Compre (i.e., >, <, or =) the tenion in the rope to the weight of the green dog? I thi wht ou would expect? Wh? m m

PHYSICS MIDTERM I SOLUTIONS October 3. i) B The force F h to ccelerte both me, while the force F onl h to ccelerte m m. Since the block both ccelerte together, the mgnitude of F i le thn the mgnitude of F. ii) D Route h the longet pth from A to B. Since verge peed i totl ditnce trveled divided b time tken, route will hve the lrget peed. iii) B The norml force blnce the component of grvit tht i perpendiculr to the inclined plne. A the ngle θ incree, thi component of grvit will decree, cuing the norml force to decree. iv) A In ce (A), the ccelertion i perpendiculr to the velocit, which i the itution for uniform circulr motion. The velocit chnge direction, but the peed i contnt. v) A For n bll thrown up in the ir, the verticl component of velocit upon return i oppoite the originl verticl component of velocit. Since bll goe to higher height, it mut hve hd lrger initil verticl component of velocit, o it hit the ground with lrger verticl component of velocit.

PHYSICS MIDTERM I SOLUTIONS October 3. ) The velocit i onl chnging during three intervl of the motion. During ech of thee, the ccelertion cn be found with = v/ t, which men find the lope. The plot i hown below. ccelertion (m//) 6 - - -6-8 - 6 8 time (econd) b) Since the poition i the integrl of the velocit, the totl ditnce trveled cn be found b finding the re under the velocit curve. Note tht ech rectngle in the figure h n re of m. There re 6 rectngle under the curve, o the totl ditnce trveled i x = 6 x m = m. c) The verge velocit i the diplcement divided b the time: v x m = = t v =. m/ d) The verge ccelertion i the chnge in velocit divided b the time, but the initil nd finl velocitie re both zero, o there i no chnge in velocit nd hence no verge ccelertion. = m/

PHYSICS MIDTERM I SOLUTIONS October 3 3. Put the origin t the poition where the bll w thrown (t t = ). Let t be the time when the velocit i oberved, t be the time when the mximum height i reched, nd t 3 be the time when the bll return to the ground. h =.8 m H 3 O R ) Ue the height = h nd the velocit v r = 9. m/ ˆ i + m/ ˆj to find the initil velocit, which will help olve the ret of the problem: v = v + ( ) v = v + ( g)( h ) v = v + gh v = v + gh = ( m/ ) + ( m/ )(. 8m) = m/ At the top of the pth, v =, o we cn olve for the mximum height H: v = v + ( ) = v + ( g)( H ) H v ( m/ ) = = g ( m/ ) H = m b) We know tht for uch prbolic pth, t 3 = t (i.e., time up = time down). Since the horizontl velocit i unchnged during the flight, we cn olve for the rnge R: R= vxt3 = vxt v v = v gt t = ince v = g vxv 9 (. m/ )( m/ ) R = = g m/ R= 36m c) The time of flight cn be found uing the time eqution found bove: t t v m t / = = = g m/ = 3 3 3

PHYSICS MIDTERM I SOLUTIONS October 3. Let the -dimenionl coordinte tem hve it origin t the urfce of the chocolte o tht =, v = -8 m/. The bll come to ret t = -d = -8 m, o we know tht v =. -8m ) To find the ccelertion ue: v = v + ( ) = v + ( d ) v ( 8m 6m = = / ) / = d 8 ( m) 6m = m/ b) Firt drw free bod digrm for the bll. Then write down the eqution of motion. F mg= m F = m+ mg= m( + g) F = 5kg( m/ + m/ ) F = 7N F mg c) The time for the bll to come to ret i found from: v = v + t = v + t v 8m t = = ( / ) m/ t =

PHYSICS MIDTERM I SOLUTIONS October 3 5. ) Cll the tenion in the rope T, which i the me for ech dog. Since the green dog i hevier, we expect it to go down, nd o we ume it ccelertion to be down hown, which men tht the ellow dog will go up with the me ccelertion, lo hown. Green dog Yellow dog T T m m m g m g b) The eqution of motion for the two dog re mg T= m T mg = m Adding the two eqution together, nd uing m = 3 m, we cn find : mg mg = ( m+ m) m m m m g 3m m m m g m = = = m g + 3 + g = c) We cn find the tenion from either of the eqution of motion: g T = m( g ) = m( g ) mg T = mg or T = 3 d) From bove we ee tht mg T = T < m g So the tenion i le thn the weight of the green dog. Thi i wht we expected, ince we id originll tht we expected the green dog to fll down. Thi mut men tht the force down, m g, i greter thn the force up, T, giving net force down. 5