3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard
|
|
- Lionel Ross
- 5 years ago
- Views:
Transcription
1 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 kg ball i dropped from ret at a point 1.20 m above the floor. The ball rebound traight upward to a height of m. a) What wa the magnitude and direction of the impule that the floor exert on the ball, when the ball hit the ground? Hint: Ue energy or kinematic to find the velocity of the ball before and after hitting the floor. Then ue the Impule-Momentum Theorem.) The known and unknown variable are: v 0 = 0 m m = 0.5 kg h h 0 = 1.2 m f = 0.7 m J =? Since there i no mention of in the problem, we need to ue the impule-momentum theorem to olve thi problem. However, in order to ue thi theorem, we will need to determine the velocity of the ball jut before and jut after it hit the ground. Since the ball doe not return to it initial height, we can ay that ome of the ball energy i lot when it hit the floor. However, energy i conerved before the ball hit the floor. Moreover, energy i alo conerved after the ball bounce off the floor. Uing conervation of energy, we can eaily calculate the velocity of the ball before, v 0, and after, v f, it hit the floor. E 0 = E f mgh 0 = 1 2 mv2 0 v0 2 = 2gh 0 v 0 = 2gh 0 E 0 = E f 1 2 mv2 f = mgh f vf 2 = 2gh f v f = 2gh f = 4.85 m = 3.7 m Note that v 0 i negative becaue the ball i initially moving downward. Plugging thee reult into the impule-momentum theorem, we get: J = p = p f p 0 = mv f v 0 ) = 0.5 kg) 3.7 m 4.85 m )) = 4.28 kg m b) If the ball i in contact with the floor for ) econd, what average force did the floor exert on the ball? Recall that force i given by the equation: F = p/. Plugging our value into thi give: F = p = 4.28 kg m ) = 855 N
2 Honor Phyic/Impule-Momentum Tet Review Page 2 of 7 Name: Anwer Key 2. A firehoe pray 160 kg of water ever econd, at a peed of 25 m. What force would you need to apply to the end of the firehoe to hold it in place? When a firehoe eject water, it generate a thrut force. Recall that we can derive the formula from F = p. Becaue the hoe change the momentum of the water it eject by p = m v, and the hoe m v doe thi for a ma m during a time, the momentum i changing at a rate given of: or ) m v, where m/ i the rate that water i ejected from the hoe in thi cae 160 kg/). So, ) m F = v. Plugging value into thi formula give: ) m F = v = 160 kg ) 25 m ) = 4000 N
3 Honor Phyic/Impule-Momentum Tet Review Page 3 of 7 Name: Anwer Key 3. A 0.50 kg ball i traveling to the right with a velocity of m. The ball collide elatically with a econd ball, which ha a ma of 1.5 kg and i alo traveling to the right with a peed of 4.0 m. Calculate the final velocitie of both ball, auming a head-on colliion. The known and unknown variable are: m 1 = 0.50 kg m 2 = 1.5 kg v 1 = 10.0 m v 2 = 4.0 m v 1 =? v 2 =? During elatic colliion, both object move with different final velocitie. A a reult there are two unknown v 1 and v 2). We alo have two equation conervation of momentum and conervation of energy). Recall that we can rewrite conervation of energy and conervation of momentum a: v 1 v 2 = v 2 v 1 m 1 v 1 + m 2 v 2 = m 1 v 1 + m 2 v 2 Plugging our known value into thee two equation give: 6 = v 2 v 1 1) 11 = 0.5v v 2 2) Where the unit have been dropped for convenience and readability. When faced with two equation and two unknown, we firt pick one equation and olve for one of the unknown. In thi cae, I ll ue equation 1) to olve for v 1. Plugging thi into equation 2) allow u to olve for v 2. 6 = v 2 v 1 v 1 = v 2 6 3) 11 = 0.5v 2 6) + 1.5v 2 11 = 0.5v v 2 14 = 2v 2 v 2 = 7 m Finally, we can olve for v 1 by plugging thi reult into equation 3): v 1 = 7 6 = 1 m So, v 1 = 1 m and v 2 = 7 m.
4 Honor Phyic/Impule-Momentum Tet Review Page 4 of 7 Name: Anwer Key 4. A father ha a ma of 87 kg and i kating along the ice. He ee hi 22 kg on tanding on the ice. The father kate by hi on, and pick him up a he pae by. After grabbing hi on, the father kate away with a peed of 2.4 m. Ignoring friction, how fat wa the father moving before he grabbed hi on? The known and unknown variable are: m F = 87 kg v f = 2.4 m m = 22 kg v F,0 =? Thi problem involve a perfectly inelatic colliion. An inelatic colliion occur whenever the two object tick together after a colliion. In inelatic colliion, momentum i conerved but energy i not. Applying conervation of linear momentum, we get: m F v F,0 = m F + m b )v ) f mf + m b v F,0 = v f = 3 m m F 5. A 10 g bullet i fired horizontally at a 5 kg wooden target which it on top of a 1 m tall platform. The bullet travel at a peed of 200 m. The bullet hit the target and get embedded inide it. A a reult, the target flie off of the platform, and fall to the ground. How far, horizontally, doe the target travel before hitting the ground? m b = 0.01 kg y = 1 m m t = 5 kg x =? Firt, we need to calculate the peed that the target i moving immediately after the bullet get embedded in it. A alway, the momentum immediately before the colliion i equal to the momentum immediately after the colliion. Uing thi, we can calculate the velocity of the target after the bullet hit it: m b + m t ) v f = m b v 0 v f = mb = 0.4 m m b + m t After the bullet collide with the target, the target i in free-fall. To find the ditance the target travel before hitting the ground, we need to calculate the amount of time it will take the target to fall 1 m. Uing the kinematic equation y = 1 2 a y) 2 + v 0,y, we ee that: ) v 0
5 Honor Phyic/Impule-Momentum Tet Review Page 5 of 7 Name: Anwer Key y = 1 2 a y) v 0,y ) 2 = 2 y = a y 2 y a y 2 1 m) = 9.8 m 2 = Since there i no acceleration in the horizontal direction, the horizontal ditance the target travel i given by x = v x. Therefore, x = v x = 0.4 m ) ) = m 6. An automobile ha a ma of 2100 kg and velocity of +17 m. The car collide with a tationary car whoe ma i 1900 kg. The car lock bumper and kid off together with the wheel locked. a) What i the velocity of the two car immediately after the colliion? The known and unknown variable are: m 1 = 2100 kg v 1 = 17 m m 2 = 1900 kg v f =? J =? v 2 = 0 m x =? µ k = 0.68 Since the car tick together, the colliion i perfectly inelatic. Thi mean that momentum i conerved and energy i not. Applying conervation of linear momentum to olve for v f, give: m 1 + m 2 )v f = m 1 v 1 m1 v f = m 1 + m 2 = ) v kg kg = 8.93 m ) 17 m b) What wa the impule acting on the kidding car from the moment after the colliion until the car come to ret?
6 Honor Phyic/Impule-Momentum Tet Review Page 6 of 7 Name: Anwer Key After the colliion, friction caue the car to come to ret. The impule caued by friction i eaily calculated uing the Impule-Momentum Theorem. J = p = p f p 0 = 0 m 1 + m 2 )v f = ) kg m 7. A 50.0 kg kater i traveling due Eat at a contant peed of 3.00 m. A 70.0 kg kater i moving due South at 7.00 m. The two kater collide, and hold on to each other after the colliion. a) What i the final peed of the two kater? The known and unknown variable are: m 1 = 50 kg v 1 = 3 m Eat m 2 = 70 kg v 2 = 7 m South θ =? v f =? Since the two kater cling together after colliding, the colliion i perfectly inelatic. Thi mean that momentum i conerved, and energy i not. Since the two kater are not moving along a onedimenional line, we mut apply conervation of momentum along the x and y-direction. Applying conervation of momentum along the x-direction Eat-Wet) give: m 1 + m 2 )v f,x = m 1 v 1,x + m 2 v 0 ) 2,x m1 v f,x = v 1 m 1 + m 2 = 1.25 m Similarly, applying conervation of linear momentum along the y-direction give: m 1 + m 2 )v f,y = m 1 v 0 1,y + m 2 v ) 2,x m2 v f,x = v 2 m 1 + m 2 = 4.08 m Combining thee reult, we ee that: v f,x = 1.25 m and v f,y = 4.08 m. Calculating the magnitude, we get:
7 Honor Phyic/Impule-Momentum Tet Review Page 7 of 7 Name: Anwer Key v f = vx 2 + vy 2 = 1.25 m ) m )2 = 4.27 m b) In that direction are they moving after the colliion? Uing trigonometry, we can determine the direction of the kater motion after the colliion: tanθ) = v y v x ) θ = tan 1 vy v x = 73 South of Eat
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 informationElastic 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 informationUniform 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 informationLinear Momentum. calculate the momentum of an object solve problems involving the conservation of momentum. Labs, Activities & Demonstrations:
Add Important Linear Momentum Page: 369 Note/Cue Here NGSS Standard: HS-PS2-2 Linear Momentum MA Curriculum Framework (2006): 2.5 AP Phyic 1 Learning Objective: 3.D.1.1, 3.D.2.1, 3.D.2.2, 3.D.2.3, 3.D.2.4,
More information( 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 informationKEY. D. 1.3 kg m. Solution: Using conservation of energy on the swing, mg( h) = 1 2 mv2 v = 2mg( h)
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
More informationAssessment Schedule 2017 Scholarship Physics (93103)
Scholarhip Phyic (93103) 201 page 1 of 5 Aement Schedule 201 Scholarhip Phyic (93103) Evidence Statement Q Evidence 1-4 mark 5-6 mark -8 mark ONE (a)(i) Due to the motion of the ource, there are compreion
More informationImpulse. 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 informationEF 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 informationa = 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 information5.4 Conservation of Momentum in Two Dimensions
Phyic Tool bo 5.4 Coneration of Moentu in Two Dienion Law of coneration of Moentu The total oentu before a colliion i equal to the total oentu after a colliion. Thi i written a Tinitial Tfinal If the net
More informationMomentum. 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 informationPhysics 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 informationSecond 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 informationName: 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 informationAP 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 information1. A 500-kilogram car is driving at 15 meters/second. What's its kinetic energy? How much does the car weigh?
9. Solution Work & Energy Homework - KINETIC ENERGY. A 500-kilogram car i driing at 5 meter/econd. What' it kinetic energy? How much doe the car weigh? m= 500 kg 5 m/ Write Equation: Kinetic Energy = ½
More information5.5. Collisions in Two Dimensions: Glancing Collisions. Components of momentum. Mini Investigation
Colliion in Two Dienion: Glancing Colliion So ar, you have read aout colliion in one dienion. In thi ection, you will exaine colliion in two dienion. In Figure, the player i lining up the hot o that the
More informationMomentum. Momentum. Impulse. Impulse Momentum Theorem. Deriving Impulse. v a t. Momentum and Impulse. Impulse. v t
Moentu and Iule Moentu Moentu i what Newton called the quantity of otion of an object. lo called Ma in otion The unit for oentu are: = oentu = a = elocity kg Moentu Moentu i affected by a and elocity eeding
More informationFinal Comprehensive Exam Physical Mechanics Friday December 15, Total 100 Points Time to complete the test: 120 minutes
Final Comprehenive Exam Phyical Mechanic Friday December 15, 000 Total 100 Point Time to complete the tet: 10 minute Pleae Read the Quetion Carefully and Be Sure to Anwer All Part! In cae that you have
More informationPractice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4.
Chapter 5 Newton Law Practice Proble Solution Student Textbook page 163 1. Frae the Proble - Draw a free body diagra of the proble. - The downward force of gravity i balanced by the upward noral force.
More informationProf. 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 informationPhysics 30 Lesson 1 Momentum and Conservation of Momentum in One Dimension
Phyic 30 Leon 1 Moentu and Conervation of Moentu in One Dienion I. Phyic rincile Student often ak e if Phyic 30 i harder than Phyic 0. Thi, of coure, deend on the atitude, attitude and work ethic of the
More informationConservation 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 informationFrames of Reference and Relative Velocity
1.5 frame of reference coordinate ytem relative to which motion i oberved Frame of Reference and Relative Velocity Air how provide element of both excitement and danger. When high-peed airplane fly in
More informationDYNAMICS 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 informationHalliday/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 information15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object.
Chapter 4 orce and ewton Law of Motion Goal for Chapter 4 to undertand what i force to tudy and apply ewton irt Law to tudy and apply the concept of a and acceleration a coponent of ewton Second Law to
More informationPhysics 30 Lesson 3 Impulse and Change in Momentum
Phyic 30 Leon 3 Ipule and Change in Moentu I. Ipule and change in oentu According to Newton nd Law of Motion (Phyic Principle 1 on the Data Sheet), to change the otion (i.e. oentu) of an object an unbalanced
More informationUCM/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 informationPhysics 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 informationLinear 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 informationPractice 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 informationConstant 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 informationChapter 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 informationPhysics 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 informationFrictional 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 informationt 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 informations 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 information23. A force in the negative direction of an x-axis is applied for 27ms to a 0.40kg ball initially moving at 14m/s in the positive direction of the
23. A force in the negative direction of an x-axis is applied for 27ms to a 0.40kg ball initially moving at 14m/s in the positive direction of the axis. The force varies in magnitude, and the impulse has
More informationAP Physics Momentum AP Wrapup
AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol
More information303b 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 informationPhysics 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 informationtwo 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 informationChapter Work, Energy and Power. Q1. The co-efficient of restitution e for a perfectly elastic collision is [1988] (a) 1 (b) 0 (c) (d) 1 Ans: (a)
Chapter Work, Energy and Power Q1. The co-efficient of restitution e for a perfectly elastic collision is [1988] (a) 1 (b) 0 (c) (d) 1 Q2. A bullet of mass 10g leaves a rifle at an initial velocity of
More informationConservation of Momentum
Conservation of Momentum Newton: Quantity of Motion Forces applied for a period of time change an object s quantity of motion. F = ma F = m Δ v t F t = mδv = mv f mv i p mv Ft = Δp F = dp dt Conservation?
More informationPhysics 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 informationCenter of Mass & Linear Momentum
PHYS 101 Previous Exam Problems CHAPTER 9 Center of Mass & Linear Momentum Center of mass Momentum of a particle Momentum of a system Impulse Conservation of momentum Elastic collisions Inelastic collisions
More informationFALL 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 informationChapter 4. Forces and Newton s Laws of Motion. continued
Chapter 4 Forces and Newton s Laws of Motion continued Clicker Question 4.3 A mass at rest on a ramp. How does the friction between the mass and the table know how much force will EXACTLY balance the gravity
More informationSeat: 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 informationBernoulli 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 informationLecture 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 informationPhysics 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 informationUnit 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 informationMomentum Conceptual Questions. 1. Which variable has more impact on an object s motion? Its mass or its velocity?
AP Physics I Momentum Conceptual Questions 1. Which variable has more impact on an object s motion? Its mass or its velocity? 2. Is momentum a vector or a scalar? Explain. 3. How does changing the duration
More informationME 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 informationMomentum Practice Problems
Momentum Practice Problems PSI AP Physics C Name Multiple Choice 1. A steel ball and a piece of clay have equal mass. They are dropped from the same height on a horizontal steel platform. The ball bounces
More informationIMPACT (Section 15.4)
IMPACT (Section 15.4) Today s Objectives: Students will be able to: a) Understand and analyze the mechanics of impact. b) Analyze the motion of bodies undergoing a collision, in both central and oblique
More information= 16.7 m. Using constant acceleration kinematics then yields a = v v E The expression for the resistance of a resistor is given as R = ρl 4 )
016 PhyicBowl Solution # An # An # An # An # An 1 C 11 C 1 B 31 E 41 D A 1 B E 3 D 4 B 3 D 13 A 3 C 33 B 43 C 4 D 14 E 4 B 34 C 44 E 5 B 15 B 5 A 35 A 45 D 6 D 16 C 6 C 36 B 46 A 7 E 17 A 7 D 37 E 47 C
More informationMath 273 Solutions to Review Problems for Exam 1
Math 7 Solution to Review Problem for Exam True or Fale? Circle ONE anwer for each Hint: For effective tudy, explain why if true and give a counterexample if fale (a) T or F : If a b and b c, then a c
More information6.1 Momentum and Impulse A. What is momentum? Newton defined momentum as the quantity of motion
AP Physics Mechanics Chapter 6 Momentum and Collisions Text chapter 6 - Reading pp. 141-161 - textbook HW -- #1,3,4,6,9,15,16,20,21,23,26,27,25,34,63,70,71 1 6.1 Momentum and Impulse A. What is momentum?
More informationDescription: Conceptual: A bullet embeds in a stationary, frictionless block: type of collision? what is conserved? v_final?
Chapter 8 [ Edit ] Overview Summary View Diagnostics View Print View with Answers Chapter 8 Due: 11:59pm on Tuesday, March 20, 2018 To understand how points are awarded, read the Grading Policy for this
More informationThe Electric Potential Energy
Lecture 6 Chapter 28 Phyic II The Electric Potential Energy Coure webite: http://aculty.uml.edu/andriy_danylov/teaching/phyicii New Idea So ar, we ued vector quantitie: 1. Electric Force (F) Depreed! 2.
More informationPHYSICSBOWL 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 information2015 PhysicsBowl Solutions Ans Ans Ans Ans Ans B 2. C METHOD #1: METHOD #2: 3. A 4.
05 PhyicBowl Solution # An # An # An # An # An B B B 3 D 4 A C D A 3 D 4 C 3 A 3 C 3 A 33 C 43 B 4 B 4 D 4 C 34 A 44 E 5 E 5 E 5 E 35 E 45 B 6 D 6 A 6 A 36 B 46 E 7 A 7 D 7 D 37 A 47 C 8 E 8 C 8 B 38 D
More informationMechanics Physics 151
Mechanic Phyic 5 Lecture 6 Special Relativity (Chapter 7) What We Did Lat Time Defined covariant form of phyical quantitie Collectively called tenor Scalar, 4-vector, -form, rank- tenor, Found how to Lorentz
More informationME 375 EXAM #1 Tuesday February 21, 2006
ME 375 EXAM #1 Tueday February 1, 006 Diviion Adam 11:30 / Savran :30 (circle one) Name Intruction (1) Thi i a cloed book examination, but you are allowed one 8.5x11 crib heet. () You have one hour to
More informationHolt 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 informationSAPTARSHI JEE/NEET-2014
SAPTARSHI JEE/NEET-4 : Phyic Mark Time: Hour Note: For each wrong anwer, /4 th mark will be eucte. ) Two particle are releae from the ame height at an interval of. How long after the firt particle being
More informationAP Physics 1 Momentum and Impulse Practice Test Name
AP Physics 1 Momentum and Impulse Practice Test Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A rubber ball and a lump of clay have equal
More informationMAE 101A. Homework 3 Solutions 2/5/2018
MAE 101A Homework 3 Solution /5/018 Munon 3.6: What preure gradient along the treamline, /d, i required to accelerate water upward in a vertical pipe at a rate of 30 ft/? What i the anwer if the flow i
More informationAP Physics C. Momentum. Free Response Problems
AP Physics C Momentum Free Response Problems 1. A bullet of mass m moves at a velocity v 0 and collides with a stationary block of mass M and length L. The bullet emerges from the block with a velocity
More informationDisplacement 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 informationCHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS
CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS 103 Phy 1 9.1 Lnear Momentum The prncple o energy conervaton can be ued to olve problem that are harder to olve jut ung Newton law. It ued to decrbe moton
More informationSample Physics Placement Exam
Sample Physics 130-1 Placement Exam A. Multiple Choice Questions: 1. A cable is used to take construction equipment from the ground to the top of a tall building. During the trip up, when (if ever) is
More informationRELEVANT REVIEW ASSIGNMENTS:
RELEVANT REVIEW ASSIGNMENTS: RELEVANT REVIEW ANSWER KEYS: MOMENTUM QUIZ REVIEW KEY Intruction: Show your work completely in your journal when anwering the following quetion. 1. If a 3.0 kg object
More information(A) 0 (B) mv (C) 2mv (D) 2mv sin θ (E) 2mv cos θ
Physics 1 Lesson 8 Forces and Momentum Homework Outcomes 1. Define linear momentum. 2. Determine the total linear momentum of a system. 3. Apply the Law of Conservation of Momentum to solve problems. 4.
More informationPhysics 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 informationPhysics I (Navitas) FINAL EXAM Fall 2015
95.141 Physics I (Navitas) FINAL EXAM Fall 2015 Name, Last Name First Name Student Identification Number: Write your name at the top of each page in the space provided. Answer all questions, beginning
More informationPHYSICS 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 informationPhysics 5A Final Review Solutions
Physics A Final Review Solutions Eric Reichwein Department of Physics University of California, Santa Cruz November 6, 0. A stone is dropped into the water from a tower 44.m above the ground. Another stone
More informationGeneral Physics I Momentum
General Physics I Momentum Linear Momentum: Definition: For a single particle, the momentum p is defined as: p = mv (p is a vector since v is a vector). So p x = mv x etc. Units of linear momentum are
More informationPhysics 1A, Summer 2011, Summer Session 1 Quiz 3, Version A 1
Physics 1A, Summer 2011, Summer Session 1 Quiz 3, Version A 1 Closed book and closed notes. No work needs to be shown. 1. Three rocks are thrown with identical speeds from the top of the same building.
More informationV = 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 informationYour Name: PHYSICS 101 MIDTERM. Please circle your section 1 9 am Galbiati 2 10 am Kwon 3 11 am McDonald 4 12:30 pm McDonald 5 12:30 pm Kwon
1 Your Name: PHYSICS 101 MIDTERM October 26, 2006 2 hours Please circle your section 1 9 am Galbiati 2 10 am Kwon 3 11 am McDonald 4 12:30 pm McDonald 5 12:30 pm Kwon Problem Score 1 /13 2 /20 3 /20 4
More informationMechanics II. Which of the following relations among the forces W, k, N, and F must be true?
Mechanics II 1. By applying a force F on a block, a person pulls a block along a rough surface at constant velocity v (see Figure below; directions, but not necessarily magnitudes, are indicated). Which
More information1 kg. 10,000 kg. 1 Page. Momentum is a vector so it has a magnitude and a velocity. Its magnitude is the product of its mass and velocity, p = mv.
Momentum The momentum of a single object is simply equal to the product of its mass and its velocity. The symbol for momentum is p. Since mass is a scalar and velocity is a vector, momentum is also a vector.
More informationDiscover 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 informationNotes on Phase Space Fall 2007, Physics 233B, Hitoshi Murayama
Note on Phae Space Fall 007, Phyic 33B, Hitohi Murayama Two-Body Phae Space The two-body phae i the bai of computing higher body phae pace. We compute it in the ret frame of the two-body ytem, P p + p
More informationα f k θ y N m mg Figure 1 Solution 1: (a) From Newton s 2 nd law: From (1), (2), and (3) Free-body diagram (b) 0 tan 0 then
Question [ Work ]: A constant force, F, is applied to a block of mass m on an inclined plane as shown in Figure. The block is moved with a constant velocity by a distance s. The coefficient of kinetic
More informationChapter 9. Linear Momentum and Collisions
Chapter 9 Linear Momentum and Collisions Momentum Analysis Models Force and acceleration are related by Newton s second law. When force and acceleration vary by time, the situation can be very complicated.
More informationSt. Joseph s Anglo-Chinese School
Time allowed:.5 hours Take g = 0 ms - if necessary. St. Joseph s Anglo-Chinese School 008 009 First Term Examination Form 6 ASL Physics Section A (40%) Answer ALL questions in this section. Write your
More informationPractice Problems Solutions. 1. Frame the Problem - Sketch and label a diagram of the motion. Use the equation for acceleration.
Chapter 3 Motion in a Plane Practice Proble Solution Student Textbook page 80 1. Frae the Proble - Sketch and label a diagra of the otion. 40 v(/) 30 0 10 0 4 t () - The equation of otion apply to the
More information4 Conservation of Momentum
hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding
More informationPhysics 231 Lecture 14
Physics 231 Lecture 14 Impulses: forces that last a short time Momentum: p = mv Impulse-Momentum theorem: FΔt = Δp = mδv = m( v f v i ) Momentum conservation: p tot,f p 1,f + p 2,f = p 1,i + p 2,i p tot,i
More informations 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 informationv v y = v sinθ Component Vectors:
Component Vectors: Recall that in order to simplify vector calculations we change a complex vector into two simple horizontal (x) and vertical (y) vectors v v y = v sinθ v x = v cosθ 1 Component Vectors:
More informationTHE BICYCLE RACE ALBERT SCHUELLER
THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The
More informationPhysics 41 Homework Set 3 Chapter 17 Serway 7 th Edition
Pyic 41 Homework Set 3 Capter 17 Serway 7 t Edition Q: 1, 4, 5, 6, 9, 1, 14, 15 Quetion *Q17.1 Anwer. Te typically iger denity would by itelf make te peed of ound lower in a olid compared to a ga. Q17.4
More information