PhysicsAndMathsTutor.com
|
|
- Solomon George
- 6 years ago
- Views:
Transcription
1 . A raindrop falls vertically under gravity through a cloud. In a odel of the otion the raindrop is assued to be spherical at all ties and the cloud is assued to consist of stationary water particles. At tie t = 0, the raindrop is at rest and has radius a. As the raindrop falls, water particles fro the cloud condense onto it and the radius of the raindrop is assued to increase at a constant rate. A tie t the speed of the raindrop is v. (a) Show that v + ( t + a) = g. (8) Find the speed of the raindrop when its radius is a. (7) (Total 5 arks). A spaceship is oving in a straight line in deep space and needs to increase its speed. This is done by ejecting fuel backwards fro the spaceship at a constant speed c relative to the spaceship. When the speed of the spaceship is v, its ass is. (a) Show that, while the spaceship is ejecting fuel, = c. (5) The initial ass of the spaceship is 0 and at tie t the ass of the spaceship is given by = 0 ( kt), where k is a positive constant. Find the acceleration of the spaceship at tie t. (4) (Total 9 arks) Edexcel Internal Review
2 . At tie t = 0 a rocket is launched fro rest vertically upwards. The rocket propels itself upwards by expelling burnt fuel vertically downwards with constant speed U s relative to the rocket. The initial ass of the rocket is M 0 kg. At tie t seconds, where t <, its ass is M 0( t) kg, and it is oving upwards with speed v s. (a) Show that U = 9.8 ( t) (7) Hence show that U > 9.6 () (c) Find, in ters of U, the speed of the rocket one second after its launch. (5) (Total 4 arks) 4. A otor boat of ass M is oving in a straight line, with its engine switched off, across a stretch of still water. The boat is oving with speed U when, at tie t = 0, it develops a leak. The water coes in at a constant rate so that at tie t, the ass of water in the boat is t. At tie t the speed of the boat is v and it experiences a total resistance to otion of agnitude v. (a) Show that. ( M + t) + v = 0. (6) Show that the tie taken for the speed of the boat to reduce to M U is. (6) The boat sinks when the ass of water inside the boat is M. Edexcel Internal Review
3 (c) Show that the boat does not sink before the speed of the boat is U. () (Total 4 arks) 5. A space-ship is oving in a straight line in deep space and needs to reduce its speed fro U to V. This is done by ejecting fuel fro the front of the space-ship at a constant speed k relative to the space-ship. When the speed of the space-ship is v its ass is. (a) Show that, while the space-ship is ejecting fuel, =. k (6) The initial ass of the space-ship is M. Find, in ters of U, V, k and M, the aount of fuel which needs to be used to reduce the speed of the space-ship fro U to V. (6) (Total arks) 6. At tie t = 0, a sall body is projected vertically upwards. While ascending it picks up sall drops of oisture fro the atosphere. The drops of oisture are at rest before they are picked up. At tie t, the cobined body P has ass and speed v. (a) Show that, while P is oving upwards, + v = g. d t (5) The initial ass of P is M, and = Me kt, where k is a positive constant. kt kt Show that, while P is oving upwards, ( ve ) ge d =. () Given that the initial projection speed of P is g k, (c) find, in ters of M, the ass of P when it reaches its highest point. (7) (Total 5 arks) Edexcel Internal Review
4 7. A rocket-driven car oves along a straight horizontal road. The car has total initial ass M. It propels itself forwards by ejecting ass backwards at a constant rate per unit tie at a constant speed U relative to the car. The car starts fro rest at tie t = 0. At tie t the speed of the car is v. The total resistance to otion is odelled as having agnitude kv, where k is a constant. Given that t < M, show that (a) = U kv, M t (7) v = U k k t. M (6) (Total arks) 8. A rocket is launched vertically upwards under gravity fro rest at tie t = 0. The rocket propels itself upward by ejecting burnt fuel vertically downwards at a constant speed u relative to the rocket. The initial ass of the rocket, including fuel, is M. At tie t, before all the fuel has been used up, the ass of the rocket, including fuel, is M( kt) and the speed of the rocket is v. (a) Show that ku = g. kt (7) Hence find the speed of the rocket when t =. k () (Total 0 arks) Edexcel Internal Review 4
5 9. A rocket-driven car propels itself forwards in a straight line on a horizontal track by ejecting burnt fuel backwards at a constant rate kg s and at a constant speed U s relative to the car. At tie t seconds, the speed of the car is v s and the total resistance to the otion of the car has agnitude kv N, where k is a positive constant. When t = 0 the total ass of the car, including fuel, is M kg. Assuing that at tie t seconds soe fuel reains in the car, (a) show that = U kv, M t (7) find the speed of the car at tie t seconds, given that it starts fro rest when t = 0 and that = k = 0. (6) (Total arks) 0. A spaceship is oving in deep space with no external forces acting on it. Initially it has total ass M and is oving with speed V. The spaceship reduces its speed to V by ejecting fuel fro its front end with a speed of c relative to itself and in the sae direction as its own otion. Find the ass of fuel ejected. (Total arks) Edexcel Internal Review 5
6 . (a) dr = r = t + a B ( + δ)( v + δv) v = gδt A v + = g D A = 4πr (ρ) A B d d 4 r g v v g π ρ 4πr ρ r D v + d t t+ a = g * A 8 t+a ln( t+a) ln( t+a) R= e = e = e = ( t+ a) A v( t+ a) = g ( t+ a) D v(t + a) = g(t + a)4 A 4 4 = 0, = 0 = D 4 t v C ga t+ a= a D 4 ga 0ag v= 4 g( a) 4 = A 7 7a 7 [5]. (a) v = (+δ)(v +δv) ( δ)(c v) A v = v + δv + vδ+ cδ vδ δv = cδ d v c D A 5 = 0k B = c = 0k c0k = kt D 0 ( kt) ( ) ck = A 4 [9] Edexcel Internal Review 6
7 . (a) g δt = ( + δ)(v + δv) + δ(u v) v g δt = v + δv + vδ + U δ vδ v A d v g = + U A = M 0 ( t) = M 0 B M 0 g( t) = M 0 ( t) M 0U U g( t ) = ( t) U 9.8 = * ( t) A 7 U > 0 when t = > 0 U > 9.6* A (c) U v = 9.8 ( t) = U ln( t) 9.8t + C A t = 0, v = 0: 0 = U ln + C C = U ln so, v = U ln 9. 8t ( t) t = : v = U ln 9.8 A 5 [4] 4. (a) ( + δ)(v + δv) v = vδt A + v = v = ; = M + t B; B ( M + t) + v = 0* DA 6 Edexcel Internal Review 7
8 = t) u [ ln v] [ ] T u = ln( M + t) 0 DA (M + T ) ln = ln M D M T = ( ) * DA 6 v ( M + (c) Sinks at T S = M M Reaches speed U at T = ( ) Since ) <, T < T S I.e. Reaches speed U before it sinks Acso ( [4] 5. (a) v ( + )( v+ v) + ( )(K + v+ v) A v = ~ v + δv + vδ Kδ vδ Kδ δv In the liit, as t 0, = K A 6 Edexcel Internal Review 8
9 V M = U K ln ln M = (V U) A K = ln (V U) M K = V U K M e A Aount of fuel = M = M e V U K A 6 [] 6. O δ v + δv v + δ (a) ( + δ)(v + δv) v = gδt A,, 0 / / v + δv + vδ + / δ / / δv/ / / v = gδt + v = g A 5 = Me kt = kme kt B Hence Me kt + kv. kme kt = Me kt g d ( ve kt kt ) = ge A Edexcel Internal Review 9
10 (c) ve kt = g e kt g kt = e (+c) k g g t = o, v = c = k k e kt = A = 0 A Hence = Me kt = M A 7 [5] 7. (a) v v + v v U kv + t t + t + ve Ipulse oentu: kvδt = ( + δ)(v + δv) + ( δ)(v µ) v A kvδt = v + δv + δv δµ + δµ v δ v δ kv = + µ δt δt liit as δt 0: kv = µ d t d t d = = M t B kv = (M ) µ µ kv = (*) A 7 M t Edexcel Internal Review 0
11 t v µ kv A t µ [ln( M t)] 0 = [ln( µ kv)] 0 k A k (ln(m t) lnm) = ln(µ kv) lnµ k M t µ kv = M µ µ t k v = ( ) k (*) M A 6 = 0 M t 0 [] 8. (a) v t + v + v v u ( + δ) (v + δ) + ( δ) (v u) v = gδt A ( ee) v + δv + vδ vδ + uδ v = gδt + u d t d t = g A = M( kt) = km B M( kt) + u( km) = M( kt)g d v ku = kt g (*) A 7 v = k ku kt g 0 u ln ( kt) gt 0 A = [ ] k = u ln ( ) g k A [0] Edexcel Internal Review
12 9. (a) ( + δ)(v + δv) + ( δ )(v U) v = kvδ A A + U = kv A = M t B d v (M t) = U kv U kv = M t (*) (no incorrect working seen) A cso 7 0 Separating variables: = U v M 0t or equivalent Integrating: ln (U v) = ln (M 0 t ) (+ c) A 0 0 Using liits correctly: [ ] v = [ ] t applied or t = 0, v = 0 to find c U [c = ln ] M U M Coplete ethod to find v [ ln = ln ] U v M 0t 0Ut v = M A 6 [] 0. v (Tie δt) v+ δv v + c + δ δ ( + δ)(v + δv) + ( δ)(v + c) v = 0 A,, 0 c = 0 reducing equation V V d v = c M separating variables Edexcel Internal Review
13 v V V = v = c ln c ln M M integration applying liits A = V c Me eliinating ln and = Fuel used = M = M( V - c e ) A [] Edexcel Internal Review
14 . Many candidates knew exactly what to do here and there were a good nuber of fully correct solutions. Part (a) required a standard technique which ost candidates followed successfully to the given answer. It was pleasing to see the steps required were clearly set out. A few were unable to ake a correct start and then attepted to fudge the given answer. Many copletely correct solutions to part were seen. Most were able to find the correct Integrating Factor, solve the differential equation correctly, reeber the constant and use initial conditions to find v correctly. Soe candidates attepted to put in the initial conditions at the start before attepting to solve their differential equation, a costly error, as this lost the all of the arks in this part of the question.. The ajority of candidates recognise that they ust start variable ass questions by considering the change in oentu over a sall tie interval (in this question the change in oentu was zero!). They ust put the total ass at the beginning of the interval as and that of the rocket at the end of the interval as + δ (in the case of rocket questions, δ is negative). Candidates who siply try to eorise the solution to one version of this question and then try to adapt it are alost invariably unsuccessful. Although a significant nuber struggled with the first part, there was ore success with part. The easiest ethod was to use the chain rule to split up /, but soe candidates successfully integrated the result fro part (a) by separating the variables and then differentiating the result with respect to t.. In order to gain all of the arks in part (a), it was necessary to consider the change in oentu in a tie δt. Soe candidates obviously consider this to be a standard piece of bookwork, whereas others are clearly trying to work it out in the exa, in soe cases considering M 0 to be the ass at a general tie t. Candidates trying to use the given answer to correct their signs should beware of altering the wrong ones! Edexcel Internal Review 4
15 In part, any candidates gave the very siple explanation involving the acceleration at tie t = 0 being positive. Others considered the general expression for acceleration and struggled to produce the given inequality. Most candidates were successful with part (c). 4. Candidates who were successful in part (a) could either consider the change of oentu in a tie δt or else use Newton s Second Law and consider the rate of change of oentu i.e. d( v). Soe candidates tried to do this part fro eory, often apparently considering the alternative proble of a rocket ejecting fuel. Other difficulties included taking as t or else putting U in the general equation for v and t. Part was usually successfully done, ostly by separating the variables. Many candidates argued part (c) correctly, but others copared appropriate values of t or or v but did not then state any conclusion. 5. Candidates who attepted part (a) of this question fro first principles were often successful, with the possible exception of their signs. Those who tried to fit it to a solution that they had et before had probles, often caused by the inclusion of an ipulse ter which should not have been there. Many candidates gained four arks for the second part of the question, starting fro the printed answer but issing out the subtraction of the final ass fro M. Soe however worked with the answer that they had obtained for part (a). Others got confused over which speed went with which tie and often introduced a speed of zero. 6. This was found to be reasonable straightforward as a question on variable ass. The derivation of the given differential equation was generally good with nearly all correctly considering a sall tie interval appropriately. Parts and (c) were also generally well done. In ost cases, the question proved to be a good source of arks. 7. In part (a), any candidates proved the result correctly, deriving the result fro first principles as required. Those who did not either oitted ters or confused signs, writing δ instead of (-δ) and / = (but then writing = M t since that was in the given answer) In part, since the differential equation was given, candidates were able to progress and the standard of integration was pleasing, with any correct solutions seen. 8. This was for the ost part done extreely well. It was very pleasing to see the derivation of the equation of otion done fro first principles accurately (with the δ ter having the correct sign). Also the solution of the differential equation in part was also generally done fully accurately. Edexcel Internal Review 5
16 9. The derivation of the differential equation was often very good, with the ajority of candidates working, often successfully, fro first principles. In part which was well answered by any of the candidates who had a correct strategy, a significant nuber of candidates ade it uch harder for theselves by not substituting for and k iediately. Soe candidates, too, used an integrating factor approach to solve the differential equation; in this case leaving and k ade it quite a challenge but it was good to see soe succeed. 0. No Report available for this question. Edexcel Internal Review 6
26 Impulse and Momentum
6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction
More informationVARIABLE MASS PROBLEMS
VARIABLE MASS PROBLEMS Question 1 (**) A rocket is moving vertically upwards relative to the surface of the earth. The motion takes place close to the surface of the earth and it is assumed that g is the
More information3. In the figure below, the coefficient of friction between the center mass and the surface is
Physics 04A Exa October 9, 05 Short-answer probles: Do any seven probles in your exa book. Start each proble on a new page and and clearly indicate the proble nuber for each. If you attept ore than seven
More information8.012 Physics I: Classical Mechanics Fall 2008
MIT OpenCourseWare http://ocw.it.edu 8.012 Physics I: Classical Mechanics Fall 2008 For inforation about citing these aterials or our Ters of Use, isit: http://ocw.it.edu/ters. MASSACHUSETTS INSTITUTE
More informationTAP 222-4: Momentum questions
TAP -4: Moentu questions These questions change in difficulty and ask you to relate ipulse to change of oentu. 1. Thrust SSC is a supersonic car powered by jet engines giving a total thrust of 180 kn.
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 017 Saskatchewan High School Physics Scholarship Copetition Wednesday May 10, 017 Tie allowed: 90 inutes This copetition is based
More information2009 Academic Challenge
009 Acadeic Challenge PHYSICS TEST - REGIONAL This Test Consists of 5 Questions Physics Test Production Tea Len Stor, Eastern Illinois University Author/Tea Leader Doug Brandt, Eastern Illinois University
More informationCHAPTER 7 TEST REVIEW -- MARKSCHEME
AP PHYSICS Nae: Period: Date: Points: 53 Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS 50 Multiple Choice 45 Single Response 5 Multi-Response Free Response 3 Short Free Response 2 Long Free Response
More informationBALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass
BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the
More informationChapter 10 Atmospheric Forces & Winds
Chapter 10 Atospheric Forces & Winds Chapter overview: Atospheric Pressure o Horizontal pressure variations o Station vs sea level pressure Winds and weather aps Newton s 2 nd Law Horizontal Forces o Pressure
More informationProblem T1. Main sequence stars (11 points)
Proble T1. Main sequence stars 11 points Part. Lifetie of Sun points i..7 pts Since the Sun behaves as a perfectly black body it s total radiation power can be expressed fro the Stefan- Boltzann law as
More informationName Class Date. two objects depends on the masses of the objects.
CHAPTER 12 2 Gravity SECTION Forces KEY IDEAS As you read this section keep these questions in ind: What is free fall? How are weight and ass related? How does gravity affect the otion of objects? What
More informationFlipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions
2015 FRQ #1 Free Response Question #1 - AP Physics 1-2015 Exa Solutions (a) First off, we know both blocks have a force of gravity acting downward on the. et s label the F & F. We also know there is a
More informationYear 12 Physics Holiday Work
Year 1 Physics Holiday Work 1. Coplete questions 1-8 in the Fields assessent booklet and questions 1-3 In the Further Mechanics assessent booklet (repeated below in case you have lost the booklet).. Revise
More informationQuadratic Equations. Save My Exams! The Home of Revision For more awesome GCSE and A level resources, visit us at
Quadratic Equations Mark Schee 1 Level A LEVEL Ea Board Edecel GCE Subject Matheatics Module Core 1 Topic Algebra and Functions Sub-Topic Quadratic Equations Booklet Mark Schee 1 Tie Allowed: Score: Percentage:
More informationTactics Box 2.1 Interpreting Position-versus-Time Graphs
1D kineatic Retake Assignent Due: 4:32p on Friday, October 31, 2014 You will receive no credit for ites you coplete after the assignent is due. Grading Policy Tactics Box 2.1 Interpreting Position-versus-Tie
More informationPhysics 231 Lecture 13
Physics 3 Lecture 3 Mi Main points it o td today s lecture: Elastic collisions in one diension: ( ) v = v0 + v0 + + ( ) v = v0 + v0 + + Multiple ipulses and rocket propulsion. F Δ t = Δ v Δ v propellant
More informationLesson 24: Newton's Second Law (Motion)
Lesson 24: Newton's Second Law (Motion) To really appreciate Newton s Laws, it soeties helps to see how they build on each other. The First Law describes what will happen if there is no net force. The
More informationMassachusetts Institute of Technology Quantum Mechanics I (8.04) Spring 2005 Solutions to Problem Set 4
Massachusetts Institute of Technology Quantu Mechanics I (8.04) Spring 2005 Solutions to Proble Set 4 By Kit Matan 1. X-ray production. (5 points) Calculate the short-wavelength liit for X-rays produced
More informationNewton's Laws. Lecture 2 Key Concepts. Newtonian mechanics and relation to Kepler's laws The Virial Theorem Tidal forces Collision physics
Lecture 2 Key Concepts Newtonian echanics and relation to Kepler's laws The Virial Theore Tidal forces Collision physics Newton's Laws 1) An object at rest will reain at rest and an object in otion will
More informationPhysically Based Modeling CS Notes Spring 1997 Particle Collision and Contact
Physically Based Modeling CS 15-863 Notes Spring 1997 Particle Collision and Contact 1 Collisions with Springs Suppose we wanted to ipleent a particle siulator with a floor : a solid horizontal plane which
More informationPHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS.
!! www.clutchprep.co INTRO TO FRICTION Friction happens when two surfaces are in contact f = μ =. KINETIC FRICTION (v 0 *): STATIC FRICTION (v 0 *): - Happens when ANY object slides/skids/slips. * = Point
More informationCHAPTER 7: Linear Momentum
CHAPTER 7: Linear Moentu Solution Guide to WebAssign Probles 7.1 [1] p v ( 0.08 kg) ( 8.4 s) 0.4 kg s 7. [] Fro Newton s second law, p Ft. For a constant ass object, p v. Equate the two expression for
More informationWork, Energy and Momentum
Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered
More informationPhysics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10
There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference
More informationXI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we
More informationIn the session you will be divided into groups and perform four separate experiments:
Mechanics Lab (Civil Engineers) Nae (please print): Tutor (please print): Lab group: Date of lab: Experients In the session you will be divided into groups and perfor four separate experients: (1) air-track
More informationCHAPTER 1 MOTION & MOMENTUM
CHAPTER 1 MOTION & MOMENTUM SECTION 1 WHAT IS MOTION? All atter is constantly in MOTION Motion involves a CHANGE in position. An object changes position relative to a REFERENCE POINT. DISTANCE is the total
More informationma x = -bv x + F rod.
Notes on Dynaical Systes Dynaics is the study of change. The priary ingredients of a dynaical syste are its state and its rule of change (also soeties called the dynaic). Dynaical systes can be continuous
More informationUNIT HOMEWORK MOMENTUM ANSWER KEY
UNIT HOMEWORK MOMENTUM ANSWER KEY MOMENTUM FORMULA & STUFF FROM THE PAST: p = v, TKE = ½v 2, d = v t 1. An ostrich with a ass of 146 kg is running to the right with a velocity of 17 /s. a. Calculate the
More informationPhysics Chapter 6. Momentum and Its Conservation
Physics Chapter 6 Moentu and Its Conservation Linear Moentu The velocity and ass of an object deterine what is needed to change its otion. Linear Moentu (ρ) is the product of ass and velocity ρ =v Unit
More informationPhysicsAndMathsTutor.com
M Collisions - Direct impact. A small ball A of mass m is moving with speed u in a straight line on a smooth horizontal table. The ball collides directly with another small ball B of mass m moving with
More informationNote-A-Rific: Mechanical
Note-A-Rific: Mechanical Kinetic You ve probably heard of inetic energy in previous courses using the following definition and forula Any object that is oving has inetic energy. E ½ v 2 E inetic energy
More informationName Period. What force did your partner s exert on yours? Write your answer in the blank below:
Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:
More informationPractice Final Exam PY 205 Monday 2004 May 3
Practice Final Exa PY 05 Monday 004 May 3 Nae There are THREE forula pages. Read all probles carefully before attepting to solve the. Your work ust be legible, and the organization ust be clear. Correct
More informationPhysicsAndMathsTutor.com
. A small ball A of mass m is moving with speed u in a straight line on a smooth horizontal table. The ball collides directly with another small ball B of mass m moving with speed u towards A along the
More informationOcean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers
Ocean 40 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers 1. Hydrostatic Balance a) Set all of the levels on one of the coluns to the lowest possible density.
More informationDepartment of Physics Preliminary Exam January 3 6, 2006
Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.
More informationChapter 5, Conceptual Questions
Chapter 5, Conceptual Questions 5.1. Two forces are present, tension T in the cable and gravitational force 5.. F G as seen in the figure. Four forces act on the block: the push of the spring F, sp gravitational
More informationPhysics 218 Exam 3 Fall 2010, Sections
Physics 28 Exa 3 Fall 200, Sections 52-524 Do not fill out the inforation below until instructed to do so! Nae Signature Student ID E-ail Section # : SOUTIONS ules of the exa:. You have the full class
More informationConservation of Momentum
Conseration of Moentu We left off last with the idea that when one object () exerts an ipulse onto another (), exerts an equal and opposite ipulse onto. This happens in the case of a classic collision,
More informationSRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES
SRI LANKAN PHYSICS OLYMPIAD - 5 MULTIPLE CHOICE TEST QUESTIONS ONE HOUR AND 5 MINUTES INSTRUCTIONS This test contains ultiple choice questions. Your answer to each question ust be arked on the answer sheet
More informationToday s s topics are: Collisions and Momentum Conservation. Momentum Conservation
Today s s topics are: Collisions and P (&E) Conservation Ipulsive Force Energy Conservation How can we treat such an ipulsive force? Energy Conservation Ipulsive Force and Ipulse [Exaple] an ipulsive force
More informationSome Perspective. Forces and Newton s Laws
Soe Perspective The language of Kineatics provides us with an efficient ethod for describing the otion of aterial objects, and we ll continue to ake refineents to it as we introduce additional types of
More informationRelativity and Astrophysics Lecture 25 Terry Herter. Momenergy Momentum-energy 4-vector Magnitude & components Invariance Low velocity limit
Mo Mo Relativity and Astrophysics Lecture 5 Terry Herter Outline Mo Moentu- 4-vector Magnitude & coponents Invariance Low velocity liit Concept Suary Reading Spacetie Physics: Chapter 7 Hoework: (due Wed.
More informationCHAPTER 15: Vibratory Motion
CHAPTER 15: Vibratory Motion courtesy of Richard White courtesy of Richard White 2.) 1.) Two glaring observations can be ade fro the graphic on the previous slide: 1.) The PROJECTION of a point on a circle
More informationPhysicsAndMathsTutor.com
1. A particle P of mass 0.5 kg is moving under the action of a single force F newtons. At time t seconds, F = (6t 5) i + (t 2 2t) j. The velocity of P at time t seconds is v m s 1. When t = 0, v = i 4j.
More informationPhysics Circular Motion: Energy and Momentum Conservation. Science and Mathematics Education Research Group
F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Departent of Curriculu and Pedagogy Physics Circular Motion: Energy and Moentu Conservation Science and Matheatics Education Research Group Supported
More informationCalculations Manual 5-1
Calculations Manual 5-1 Although you ay be anxious to begin building your rocket, soe iportant decisions need to be ade about launch conditions that can help ensure a ore accurate launch. Reeber: the goal
More informationTake-Home Midterm Exam #2, Part A
Physics 151 Due: Friday, March 20, 2009 Take-Hoe Midter Exa #2, Part A Roster No.: Score: NO exa tie liit. Calculator required. All books and notes are allowed, and you ay obtain help fro others. Coplete
More information2.003 Engineering Dynamics Problem Set 2 Solutions
.003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study
More information(a) Why cannot the Carnot cycle be applied in the real world? Because it would have to run infinitely slowly, which is not useful.
PHSX 446 FINAL EXAM Spring 25 First, soe basic knowledge questions You need not show work here; just give the answer More than one answer ight apply Don t waste tie transcribing answers; just write on
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More information15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams
Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces
More informationNB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016
NB1140: Physics 1A - Classical echanics and Therodynaics Proble set 2 - Forces and energy Week 2: 21-25 Noveber 2016 Proble 1. Why force is transitted uniforly through a assless string, a assless spring,
More informationMomentum. February 15, Table of Contents. Momentum Defined. Momentum Defined. p =mv. SI Unit for Momentum. Momentum is a Vector Quantity.
Table of Contents Click on the topic to go to that section Moentu Ipulse-Moentu Equation The Moentu of a Syste of Objects Conservation of Moentu Types of Collisions Collisions in Two Diensions Moentu Return
More informationy scalar component x scalar component A. 770 m 250 m file://c:\users\joe\desktop\physics 2A\PLC Assignments - F10\2a_PLC7\index.
Page 1 of 6 1. A certain string just breaks when it is under 400 N of tension. A boy uses this string to whirl a 10-kg stone in a horizontal circle of radius 10. The boy continuously increases the speed
More informationm potential kinetic forms of energy.
Spring, Chapter : A. near the surface of the earth. The forces of gravity and an ideal spring are conservative forces. With only the forces of an ideal spring and gravity acting on a ass, energy F F will
More informationFor a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).
Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D
More informationAstro 7B Midterm 1 Practice Worksheet
Astro 7B Midter 1 Practice Worksheet For all the questions below, ake sure you can derive all the relevant questions that s not on the forula sheet by heart (i.e. without referring to your lecture notes).
More informationQuestion 1. [14 Marks]
6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is
More informationI. Understand get a conceptual grasp of the problem
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Departent o Physics Physics 81T Fall Ter 4 Class Proble 1: Solution Proble 1 A car is driving at a constant but unknown velocity,, on a straightaway A otorcycle is
More informationProjectile Motion with Air Resistance (Numerical Modeling, Euler s Method)
Projectile Motion with Air Resistance (Nuerical Modeling, Euler s Method) Theory Euler s ethod is a siple way to approxiate the solution of ordinary differential equations (ode s) nuerically. Specifically,
More informationEnergy and Momentum: The Ballistic Pendulum
Physics Departent Handout -10 Energy and Moentu: The Ballistic Pendulu The ballistic pendulu, first described in the id-eighteenth century, applies principles of echanics to the proble of easuring the
More informationQ5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!
Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In
More informationNational 5 Summary Notes
North Berwick High School Departent of Physics National 5 Suary Notes Unit 3 Energy National 5 Physics: Electricity and Energy 1 Throughout the Course, appropriate attention should be given to units, prefixes
More informationChapter 9 Centre of Mass and Linear Momentum
Chater 9 Centre o Mass and Linear Moentu Centre o ass o a syste o articles / objects Linear oentu Linear oentu o a syste o articles Newton s nd law or a syste o articles Conseration o oentu Elastic and
More informationm A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations
P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.
More informationENGI 3424 Engineering Mathematics Problem Set 1 Solutions (Sections 1.1 and 1.2)
ENGI 344 Engineering Matheatics Proble Set 1 Solutions (Sections 1.1 and 1.) 1. Find the general solution of the ordinary differential equation y 0 This ODE is not linear (due to the product y ). However,
More information2. Which of the following best describes the relationship between force and potential energy?
Work/Energy with Calculus 1. An object oves according to the function x = t 5/ where x is the distance traveled and t is the tie. Its kinetic energy is proportional to (A) t (B) t 5/ (C) t 3 (D) t 3/ (E)
More informationPHY 171. Lecture 14. (February 16, 2012)
PHY 171 Lecture 14 (February 16, 212) In the last lecture, we looked at a quantitative connection between acroscopic and icroscopic quantities by deriving an expression for pressure based on the assuptions
More informationChapter 11 Simple Harmonic Motion
Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion
More informationPhysics 120 Final Examination
Physics 120 Final Exaination 12 August, 1998 Nae Tie: 3 hours Signature Calculator and one forula sheet allowed Student nuber Show coplete solutions to questions 3 to 8. This exaination has 8 questions.
More informationThe ballistic pendulum
(ta initials) first nae (print) last nae (print) brock id (ab17cd) (lab date) Experient 4 The ballistic pendulu In this Experient you will learn how to deterine the speed of a projectile as well as the
More informationPHYS 102 Previous Exam Problems
PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal
More informationUSEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta
1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve
More informationLecture 6. Announcements. Conservation Laws: The Most Powerful Laws of Physics. Conservation Laws Why they are so powerful
Conseration Laws: The Most Powerful Laws of Physics Potential Energy gh Moentu p = + +. Energy E = PE + KE +. Kinetic Energy / Announceents Mon., Sept. : Second Law of Therodynaics Gie out Hoework 4 Wed.,
More informationAnnouncement. Grader s name: Qian Qi. Office number: Phys Office hours: Thursday 4:00-5:00pm in Room 134
Lecture 3 1 Announceent Grader s nae: Qian Qi Office nuber: Phys. 134 -ail: qiang@purdue.edu Office hours: Thursday 4:00-5:00p in Roo 134 2 Millikan s oil Drop xperient Consider an air gap capacitor which
More informationPY /005 Practice Test 1, 2004 Feb. 10
PY 205-004/005 Practice Test 1, 2004 Feb. 10 Print nae Lab section I have neither given nor received unauthorized aid on this test. Sign ature: When you turn in the test (including forula page) you ust
More informationMomentum, p = m v. Collisions and Work(L8) Crash! Momentum and Collisions. Conservation of Momentum. elastic collisions
Collisions and Work(L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details
More informationMidterm 1 Sample Solution
Midter 1 Saple Solution NOTE: Throughout the exa a siple graph is an undirected, unweighted graph with no ultiple edges (i.e., no exact repeats of the sae edge) and no self-loops (i.e., no edges fro a
More informationHonors Lab 4.5 Freefall, Apparent Weight, and Friction
Nae School Date Honors Lab 4.5 Freefall, Apparent Weight, and Friction Purpose To investigate the vector nature of forces To practice the use free-body diagras (FBDs) To learn to apply Newton s Second
More informationPhysics 120. Exam #2. May 23, 2014
Physics 10 Exa # May 3, 014 Nae Please read and follow these instructions carefully: ead all probles carefully before attepting to solve the. Your work ust be legible, and the organization clear. You ust
More informationPhysics 41 HW Set 1 Chapter 15 Serway 7 th Edition
Physics HW Set Chapter 5 Serway 7 th Edition Conceptual Questions:, 3, 5,, 6, 9 Q53 You can take φ = π, or equally well, φ = π At t= 0, the particle is at its turning point on the negative side of equilibriu,
More informationPhysicsAndMathsTutor.com
1. A ball is projected vertically upwards with a speed of 14.7 ms 1 from a point which is 49 m above horizontal ground. Modelling the ball as a particle moving freely under gravity, find (a) the greatest
More informationCelal S. Konor Release 1.1 (identical to 1.0) 3/21/08. 1-Hybrid isentropic-sigma vertical coordinate and governing equations in the free atmosphere
Celal S. Konor Release. (identical to.0) 3/2/08 -Hybrid isentropic-siga vertical coordinate governing equations in the free atosphere This section describes the equations in the free atosphere of the odel.
More informationSupervised assessment: Modelling and problem-solving task
Matheatics C 2008 Saple assessent instruent and indicative student response Supervised assessent: Modelling and proble-solving tas This saple is intended to infor the design of assessent instruents in
More informationMomentum, p. Crash! Collisions (L8) Momentum is conserved. Football provides many collision examples to think about!
Collisions (L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details of the
More informationP235 Midterm Examination Prof. Cline
P235 Mier Exaination Prof. Cline THIS IS A CLOSED BOOK EXAMINATION. Do all parts of all four questions. Show all steps to get full credit. 7:00-10.00p, 30 October 2009 1:(20pts) Consider a rocket fired
More informationForce and dynamics with a spring, analytic approach
Force and dynaics with a spring, analytic approach It ay strie you as strange that the first force we will discuss will be that of a spring. It is not one of the four Universal forces and we don t use
More information1 Brownian motion and the Langevin equation
Figure 1: The robust appearance of Robert Brown (1773 1858) 1 Brownian otion and the Langevin equation In 1827, while exaining pollen grains and the spores of osses suspended in water under a icroscope,
More informationPh 20.3 Numerical Solution of Ordinary Differential Equations
Ph 20.3 Nuerical Solution of Ordinary Differential Equations Due: Week 5 -v20170314- This Assignent So far, your assignents have tried to failiarize you with the hardware and software in the Physics Coputing
More informationOSCILLATIONS AND WAVES
OSCILLATIONS AND WAVES OSCILLATION IS AN EXAMPLE OF PERIODIC MOTION No stories this tie, we are going to get straight to the topic. We say that an event is Periodic in nature when it repeats itself in
More informationModule #1: Units and Vectors Revisited. Introduction. Units Revisited EXAMPLE 1.1. A sample of iron has a mass of mg. How many kg is that?
Module #1: Units and Vectors Revisited Introduction There are probably no concepts ore iportant in physics than the two listed in the title of this odule. In your first-year physics course, I a sure that
More information8.1 Force Laws Hooke s Law
8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which
More informationEN40: Dynamics and Vibrations. Midterm Examination Tuesday March
EN4: Dynaics and Vibrations Midter Exaination Tuesday March 8 16 School of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on this exaination. You ay bring
More informationExperiment 2: Hooke s Law
COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance
More informationLecture #8-3 Oscillations, Simple Harmonic Motion
Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.
More informationDonald Fussell. October 28, Computer Science Department The University of Texas at Austin. Point Masses and Force Fields.
s Vector Moving s and Coputer Science Departent The University of Texas at Austin October 28, 2014 s Vector Moving s Siple classical dynaics - point asses oved by forces Point asses can odel particles
More informationChapter VI: Motion in the 2-D Plane
Chapter VI: Motion in the -D Plane Now that we have developed and refined our vector calculus concepts, we can ove on to specific application of otion in the plane. In this regard, we will deal with: projectile
More information