Chapter 8: Dynamics in a plane
|
|
- Jasper Robertson
- 5 years ago
- Views:
Transcription
1 8.1 Dynamics in 2 Dimensions p Chapter 8: Dynamics in a plane 8.2 Velocity and Acceleration in uniform circular motion (a review of sec. 4.6) p Dynamics of Uniform Circular Motion p Circular Orbits p Why does the water stay in the bucket? p Non-uniform Circular Motion p We do not cover 8.5 Fictitious Forces 1
2 Chapter 8: dynamics in a plane 8.1 Dynamics in 2 Dimensions p
3 Newton's FIRST and SECOND laws carried over to 2D motion. This makes it possible to study many different situations. Paticularly important: projectile motion A projectile is an object that moves in two dimensions under the influence of only the gravitational force 3
4 Cliction 8.1 The components of this particle s acceleration are 1. a x > 0, a y > a x = 0, a y > a x < 0, a y > a x > 0, a y < a x < 0, a y < 0. 4
5 8.2 Velocity and Acceleration in Uniform Circular Motion p
6 Velocity of the particle: v is always tangent to the circle Speed: Chapter 8: Dynamics in a plane The speed is constant and has the right unit, m/s a always points in towards the center of the circle and thus is perpendicular to the velocity. This is because the speed is constant Magnitude of acceleration: = a 6
7 Chapter 8: Dynamics in a plane Example: ferris wheel at the Heritage Park Estimates from a visit: radius r = 6m period T = 9 s so ω = 2π/T 0.7 rad/s acceleration: a = ω2 r = 2.9 m/s2 0.3 g In addition, the weight force always pulls you down so that your apparent weight changes. This gives you the funny feeling ^ 7
8 The r-t and r-t-z coordinate systems For circular motion it is more convenient to decompose a vector A into: Radial component A r (positive if pointing inwards) Tangential component A t (positive for counterclockwise) We will sometimes also need a third coordinate axis z perpendicular to the circle: rtz coordinate system 8
9 Components of V and a in the rtz system The three components of the relevant vectors velocity and acceleration are With respect to radial and tangential direction, each of these vectors has only one non-zero component: 9
10 Rank in order, from largest to smallest, the centripetal accelerations (a r ) a to (a r ) e of particles a to e. 1. (a r ) b > (a r ) e > (a r ) a > (a r ) d > (a r ) c 2. (a r ) b = (a r ) e > (a r ) a = (a r ) c > (a r ) d 3. (a r ) b > (a r ) a = (a r ) c = (a r ) e > (a r ) d 4. (a r ) b > (a r ) a = (a r ) a > (a r ) e > (a r ) d 5. (a r ) b > (a r ) e > (a r ) a = (a r ) c > (a r ) d Cliction
11 8.3 Dynamics of Uniform Circular Motion p
12 The relation between speed and magnitude of acceleration is quite often very useful. KNOW IT BY HEART!! Newton's 2 nd law allows to infer the net force from this: Hence, there must always be some force that keeps the object on the circular trajectory 12
13 Example: turning the corner Forces acting on car: Chapter 8: Dynamics in a plane Weight w downwards (w z = -w) Normal force upwards (n z = n) Static friction force f s radially inwards, 0 < (f s ) r < µ s n. The friction force keeps the car in the corner. 13
14 The car continues to corner if it is not too fast, i.e., as long as For an r = 50 m corner radius and µ s = 1 we find 14
15 Cliction 8.3 A block on a string spins in a horizontal circle on a frictionless table. Rank order, from largest to smallest, the tensions T a to T e acting on blocks a to e. 1. T b > T a > T d > T c > T e 2. T d > T b = T e > T c > T a 3. T e > T c = T d > T a = T b 4. T e > T d > T c > T b > T a 5. T d > T b > T e > T c > T a 15
16 End of Week 8 16
17 8.4 Circular Orbits p
18 If the launch speed of the a projectile is sufficiently large, there comes a point where The curve of the trajectory and the curve of the Earth are parallel. In this case the projectile falls but it never gets any closer to the ground! The projectile is said to be in a CIRCULAR ORBIT (c) An object (say a satellite) moving in a circle of radius r around a planet with an acceleration of gravity g will be orbiting at a speed The period T is then T orbit = 2πr Vorbit = 2π r g V = r.g orbit 18
19 8.6 Why does the water stay in the bucket?) p
20 Example: looping in a roller coaster The only forces acting on the car are its weight and the normal force exerted by the track Your apparent weight gives you an intuition about the normal force's magnitude 20
21 The two forces always add up to the acceleration: At the top w points radially inward At the botton its the opposite 21
22 That means: at the bottom your apparent weight (= magnitude of n) is increased, at the top it is decreased, At the top our result for n r becomes negative for small enough velocities. This is unphysical: our assumption that the car stays on a circular orbit is not true anymore 22
23 What really goes on: weight and normal force are added to create the net force that is needed to produce the acceleration a = v 2 / r If v is too small the track had to pull the car rather than to push it, but this is impossible. Instead, the car derails At a minimum critical speed v c, the acceleration is entirely produced by the weight of the car 23
24 The critical speed The critical speed is reached when the normal force at the top is zero (you are not pushed in the chair anymore): v c = ω c r critical angular velocity 24
25 A car is rolling over the top of a hill at speed v. At this instant, Cliction n > w. 2. n = w. 3. n < w. 4. We can t tell about n without knowing v. 25
26 Clicker Question 7.8 A roller coaster car does a loop-the-loop. Which of the free-body diagrams below shows the forces on the car at the top of the loop? Rolling friction can be neglected. A B C D E 26 Slide 7-26
27 Clicker Question 7.8 Answer A roller coaster car does a loop-the-loop. Which of the free-body diagrams below shows the forces on the car at the top of the loop? Rolling friction can be neglected. The track is above the car, so the normal force of the track pushes down. w n A B C D E 27 Slide 7-27
28 8.7 Non-uniform Circular Motion: p
29 NO Tangential acceleration Tangential acceleration is NOT zero The tangential acceleration is what causes the particle to change the speed with which It goes around the circle. 29
30 Equations for non-uniform circular motion in the rtz system Initial angle Initial angular velocity Tangential acceleration For uniform circular motion, simply replace the tangential acceleration by zero, or a t = 0, in the equations. 30
31 Clicker Question 7.3 An ice hockey puck is tied by a string to a stake in the ice. The puck is then swung in a circle. What force or forces does the puck feel? A. A new force: the centripetal force. B. A new force: the centrifugal force. C. One or more of our familiar forces pushing outward. D. One or more of our familiar forces pulling inward. E. I have no clue. 31 Slide 7-31
32 Clicker Question 7.3 Answer An ice hockey puck is tied by a string to a stake in the ice. The puck is then swung in a circle. What force or forces does the puck feel? A. A new force: the centripetal force. B. A new force: the centrifugal force. C. One or more of our familiar forces pushing outward. D. One or more of our familiar forces pulling inward. E. I have no clue. The rules about what is or is not a force haven t changed. 1. Force must be exerted at a point of contact (except for gravity) 2. Force must have an identifiable agent doing the pushing or pulling. 3. The net force must point in the direction of acceleration (Newton s second law) 32 Slide 7-32
33 Clicker Question 7.4 An ice hockey puck is tied by a string to a stake in the ice. The puck is then swung in a circle. What force is producing the centripetal acceleration of the puck? A. Gravity B. Air resistance C. Friction D. Normal force E. Tension in the string Draw a free-body diagram in which you see the puck from ahead or behind, with the z-axis perpendicular to the ice. 33 Slide 7-33
34 Clicker Question 7.4 Answer An ice hockey puck is tied by a string to a stake in the ice. The puck is then swung in a circle. What force is producing the centripetal acceleration of the puck? A. Gravity B. Air resistance C. Friction D. Normal force E. Tension in the string 34 Slide 7-34
35 Clicker Question 7.5 A coin sits on a turntable as the table rotates ccw. The free-body diagrams below show the coin from behind, moving away from you. Which is the correct diagram? z z z z z r r r r r B D A C E 35 Slide 7-35
36 Clicker Question 7.5 Answer A coin sits on a turntable as the table rotates ccw. The free-body diagrams below show the coin from behind, moving away from you. Which is the correct diagram? z Center of circle is to the left. z z z What force is this? z r r r r Static friction! r B D A Net force must point to the center of the circle. C E 36 Slide 7-36
37 Chapter 8 Reading Quiz 37
38 Circular motion is best analyzed in a coordinate system with 1. x- and y-axes. 2. x-, y-, and z-axes. 3. x- and z-axes. 4. r-, t-, and z-axes. 38
39 The quantity with the symbol ω is called 1. the circular weight. 2. the angular velocity. 3. the circular velocity. 4. the centripetal acceleration. 39
40 For uniform circular motion, the net force 1. points toward the center of the circle. 2. points toward the outside of the circle. 3. is tangent to the circle. 4. is zero. 40
41 Selected Problems 41
42 42
43 43
44 44
45 45
46 End of Chapter 8 IMPORTANT: Print a copy of the SUMMARY page (p. 229) and add it here to your lecture notes. It will save you crucial time when trying to recall: Concepts, Symbols, and Strategies 46
47 Chapter 7: motion in a circle 7.5 Fictitious Forces and Apparent Weight p
48 Chapter 7: motion in a circle Why are you pushed to the outside of the corner? The reason, the centrifugal force, is a fictitious force. Such forces are no real forces Fictitious forces appear in noninertial reference frames: If the reference frame is accelerated, uniform straight motion seems to correspond to an accelerated motion. 48
49 Chapter 7: motion in a circle The centrifugal forces simply describes the tendency to continue on a straight line Important: since fictitious forces are related to non-inertial reference frames, they do not appear in a free-body diagram They are related to the apparent weight that we discussed before. Main difference: we now have circular instead of straight motion 49
PHYSICS. Chapter 8 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 8 Lecture RANDALL D. KNIGHT Chapter 8. Dynamics II: Motion in a Plane IN THIS CHAPTER, you will learn to solve problems about motion
More informationChapter 8. Dynamics II: Motion in a Plane
Chapter 8. Dynamics II: Motion in a Plane A roller coaster doing a loop-the-loop is a dramatic example of circular motion. But why doesn t the car fall off the track when it s upside down at the top of
More informationPHYSICS. Chapter 8 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 8 Lecture RANDALL D. KNIGHT Chapter 8. Dynamics II: Motion in a Plane IN THIS CHAPTER, you will learn to solve problems about motion
More informationChapter 8. Dynamics II: Motion in a Plane
Chapter 8. Dynamics II: Motion in a Plane Chapter Goal: To learn how to solve problems about motion in a plane. Slide 8-2 Chapter 8 Preview Slide 8-3 Chapter 8 Preview Slide 8-4 Chapter 8 Preview Slide
More informationCircular Orbits. Slide Pearson Education, Inc.
Circular Orbits The figure shows a perfectly smooth, spherical, airless planet with one tower of height h. A projectile is launched parallel to the ground with speed v 0. If v 0 is very small, as in trajectory
More informationWelcome back to Physics 211. Physics 211 Spring 2014 Lecture ask a physicist
Welcome back to Physics 211 Today s agenda: Forces in Circular Motion Impulse Physics 211 Spring 2014 Lecture 07-1 1 ask a physicist My question is on sonoluminescence, which is supposed to be when a sound
More informationLecture Presentation. Chapter 6 Preview Looking Ahead. Chapter 6 Circular Motion, Orbits, and Gravity
Chapter 6 Preview Looking Ahead Lecture Presentation Chapter 6 Circular Motion, Orbits, and Gravity Text: p. 160 Slide 6-2 Chapter 6 Preview Looking Back: Centripetal Acceleration In Section 3.8, you learned
More informationphysics Chapter 8 Lecture a strategic approach randall d. knight FOR SCIENTISTS AND ENGINEERS CHAPTER8_LECTURE8.1 THIRD EDITION
Chapter 8 Lecture physics FOR SCIENTISTS AND ENGINEERS a strategic approach THIRD EDITION randall d. knight CHAPTER8_LECTURE8.1 2013 Pearson Education, Inc. 1 Chapter 8. Newton s Laws for Circular Motion
More informationAP Physics 1 Lesson 9 Homework Outcomes. Name
AP Physics 1 Lesson 9 Homework Outcomes Name Date 1. Define uniform circular motion. 2. Determine the tangential velocity of an object moving with uniform circular motion. 3. Determine the centripetal
More information1 A car moves around a circular path of a constant radius at a constant speed. Which of the following statements is true?
Slide 1 / 30 1 car moves around a circular path of a constant radius at a constant speed. Which of the following statements is true? The car s velocity is constant The car s acceleration is constant The
More informationCircular Motion Dynamics Concept Questions
Circular Motion Dynamics Concept Questions Problem 1: A puck of mass m is moving in a circle at constant speed on a frictionless table as shown above. The puck is connected by a string to a suspended bob,
More informationContents. Objectives Circular Motion Velocity and Acceleration Examples Accelerating Frames Polar Coordinates Recap. Contents
Physics 121 for Majors Today s Class You will see how motion in a circle is mathematically similar to motion in a straight line. You will learn that there is a centripetal acceleration (and force) and
More informationPhysics 2211 ABC Quiz #3 Solutions Spring 2017
Physics 2211 ABC Quiz #3 Solutions Spring 2017 I. (16 points) A block of mass m b is suspended vertically on a ideal cord that then passes through a frictionless hole and is attached to a sphere of mass
More informationLinear vs. Rotational Motion
Linear vs. Rotational Motion Every term in a linear equation has a similar term in the analogous rotational equation. Displacements: s = r θ v t ω Speeds: v t = ω r Accelerations: a t = α r Every point
More informationAlgebra Based Physics Uniform Circular Motion
1 Algebra Based Physics Uniform Circular Motion 2016 07 20 www.njctl.org 2 Uniform Circular Motion (UCM) Click on the topic to go to that section Period, Frequency and Rotational Velocity Kinematics of
More informationCircular Motion.
1 Circular Motion www.njctl.org 2 Topics of Uniform Circular Motion (UCM) Kinematics of UCM Click on the topic to go to that section Period, Frequency, and Rotational Velocity Dynamics of UCM Vertical
More informationName St. Mary's HS AP Physics Circular Motion HW
Name St. Mary's HS AP Physics Circular Motion HW Base your answers to questions 1 and 2 on the following situation. An object weighing 10 N swings at the end of a rope that is 0.72 m long as a simple pendulum.
More informationExperiment #7 Centripetal Force Pre-lab Questions Hints
Experiment #7 Centripetal Force Pre-lab Questions Hints The following are some hints for this pre-lab, since a few of these questions can be a little difficult. Note that these are not necessarily the
More informationChapter 6. Circular Motion and Other Applications of Newton s Laws
Chapter 6 Circular Motion and Other Applications of Newton s Laws Circular Motion Two analysis models using Newton s Laws of Motion have been developed. The models have been applied to linear motion. Newton
More informationCentripetal force keeps an Rotation and Revolution
Centripetal force keeps an object in circular motion. Which moves faster on a merry-go-round, a horse near the outside rail or one near the inside rail? While a hamster rotates its cage about an axis,
More information7.1 Interacting Systems p Action/reaction pairs p Newton s Third Law p Ropes and Pulleys p.
7.1 Interacting Systems p. 183-185 7.2 Action/reaction pairs p. 185-189 7.3 Newton s Third Law p. 189-194 7.4 Ropes and Pulleys p. 194-198 7.5 Interacting-system Problems p. 198-202 1 7.1 Interacting Systems
More informationIntroductory Physics PHYS101
Introductory Physics PHYS101 Dr Richard H. Cyburt Office Hours Assistant Professor of Physics My office: 402c in the Science Building My phone: (304) 384-6006 My email: rcyburt@concord.edu TRF 9:30-11:00am
More informationChapter 5 Lecture Notes
Formulas: a C = v 2 /r a = a C + a T F = Gm 1 m 2 /r 2 Chapter 5 Lecture Notes Physics 2414 - Strauss Constants: G = 6.67 10-11 N-m 2 /kg 2. Main Ideas: 1. Uniform circular motion 2. Nonuniform circular
More informationChapter 6 Circular Motion, Orbits and Gravity
Chapter 6 Circular Motion, Orbits and Gravity Topics: The kinematics of uniform circular motion The dynamics of uniform circular motion Circular orbits of satellites Newton s law of gravity Sample question:
More informationAngle recap. Angular position: Angular displacement: s. Angular velocity: Angular Acceleration:
Angle recap Angular position: Angular displacement: s Angular velocity: Angular Acceleration: Every point on a rotating rigid object has the same angular, but not the same linear motion! Today s lecture
More informationChapters 5-6. Dynamics: Forces and Newton s Laws of Motion. Applications
Chapters 5-6 Dynamics: orces and Newton s Laws of Motion. Applications That is, describing why objects move orces Newton s 1 st Law Newton s 2 nd Law Newton s 3 rd Law Examples of orces: Weight, Normal,
More informationLecture Presentation Chapter 6 Circular Motion, Orbits, and Gravity
Lecture Presentation Chapter 6 Circular Motion, Orbits, and Gravity Suggested Videos for Chapter 6 Prelecture Videos Forces and Apparent Forces Solving Circular Motion Problems Orbits and Gravity Class
More informationWelcome back to Physics 211
Welcome back to Physics 211 Today s agenda: Circular Motion 04-2 1 Exam 1: Next Tuesday (9/23/14) In Stolkin (here!) at the usual lecture time Material covered: Textbook chapters 1 4.3 s up through 9/16
More informationChapter 8 Lecture Notes
Chapter 8 Lecture Notes Physics 2414 - Strauss Formulas: v = l / t = r θ / t = rω a T = v / t = r ω / t =rα a C = v 2 /r = ω 2 r ω = ω 0 + αt θ = ω 0 t +(1/2)αt 2 θ = (1/2)(ω 0 +ω)t ω 2 = ω 0 2 +2αθ τ
More informationChapter 6. Force and Motion-II (Friction, Drag, Circular Motion)
Chapter 6 Force and Motion-II (Friction, Drag, Circular Motion) 6.2 Frictional Force: Motion of a crate with applied forces There is no attempt at sliding. Thus, no friction and no motion. NO FRICTION
More informationPhysics 12. Unit 5 Circular Motion and Gravitation Part 1
Physics 12 Unit 5 Circular Motion and Gravitation Part 1 1. Nonlinear motions According to the Newton s first law, an object remains its tendency of motion as long as there is no external force acting
More informationUniform Circular Motion. Uniform Circular Motion
Uniform Circular Motion Uniform Circular Motion Uniform Circular Motion An object that moves at uniform speed in a circle of constant radius is said to be in uniform circular motion. Question: Why is uniform
More informationMultiple Choice (A) (B) (C) (D)
Multiple Choice 1. A ball is fastened to a string and is swung in a vertical circle. When the ball is at the highest point of the circle its velocity and acceleration directions are: (A) (B) (C) (D) 2.
More informationLecture 10. Example: Friction and Motion
Lecture 10 Goals: Exploit Newton s 3 rd Law in problems with friction Employ Newton s Laws in 2D problems with circular motion Assignment: HW5, (Chapter 7, due 2/24, Wednesday) For Tuesday: Finish reading
More informationCircular Motion Concept Questions
Circular Motion Concept Questions Question 1 A bead is given a small push at the top of a hoop (position A) and is constrained to slide around a frictionless circular wire (in a vertical plane). Circle
More informationTYPICAL NUMERIC QUESTIONS FOR PHYSICS I REGULAR QUESTIONS TAKEN FROM CUTNELL AND JOHNSON CIRCULAR MOTION CONTENT STANDARD IB
TYPICAL NUMERIC QUESTIONS FOR PHYSICS I REGULAR QUESTIONS TAKEN FROM CUTNELL AND JOHNSON CIRCULAR MOTION CONTENT STANDARD IB 1. A car traveling at 20 m/s rounds a curve so that its centripetal acceleration
More informationExam I Physics 101: Lecture 08 Centripetal Acceleration and Circular Motion Today s lecture will cover Chapter 5 Exam I is Monday, Oct. 7 (2 weeks!
Exam I Physics 101: Lecture 08 Centripetal Acceleration and Circular Motion http://www.youtube.com/watch?v=zyf5wsmxrai Today s lecture will cover Chapter 5 Exam I is Monday, Oct. 7 ( weeks!) Physics 101:
More information66 Chapter 6: FORCE AND MOTION II
Chapter 6: FORCE AND MOTION II 1 A brick slides on a horizontal surface Which of the following will increase the magnitude of the frictional force on it? A Putting a second brick on top B Decreasing the
More informationCircular Motion & Gravitation MC Question Database
(Questions #4,5,6,27,37,38,42 and 58 each have TWO correct answers.) 1) A record player has four coins at different distances from the center of rotation. Coin A is 1 cm away, Coin B is 2 cm away. Coin
More informationPSI AP Physics B Circular Motion
PSI AP Physics B Circular Motion Multiple Choice 1. A ball is fastened to a string and is swung in a vertical circle. When the ball is at the highest point of the circle its velocity and acceleration directions
More informationAP Physics Free Response Practice Dynamics
AP Physics Free Response Practice Dynamics 14) In the system shown above, the block of mass M 1 is on a rough horizontal table. The string that attaches it to the block of mass M 2 passes over a frictionless
More informationWhat path do the longest sparks take after they leave the wand? Today we ll be doing one more new concept before the test on Wednesday.
What path do the longest sparks take after they leave the wand? Today we ll be doing one more new concept before the test on Wednesday. Centripetal Acceleration and Newtonian Gravitation Reminders: 15
More informationAn object moving in a circle with radius at speed is said to be undergoing.
Circular Motion Study Guide North Allegheny High School Mr. Neff An object moving in a circle with radius at speed is said to be undergoing. In this case, the object is because it is constantly changing
More informationUniform Circular Motion
Slide 1 / 112 Uniform Circular Motion 2009 by Goodman & Zavorotniy Slide 2 / 112 Topics of Uniform Circular Motion (UCM) Kinematics of UCM Click on the topic to go to that section Period, Frequency, and
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 111.6 MIDTERM TEST #2 November 15, 2001 Time: 90 minutes NAME: STUDENT NO.: (Last) Please Print (Given) LECTURE SECTION
More informationCircular Motion. Unit 7
Circular Motion Unit 7 Do Now You drive a car that follows a circular path with the radius r = 100 m. Find the distance travelled if you made one complete circle. C 2 R 2(3.14)(100) 6.28(100) 628m Uniform
More informationDynamics Test K/U 28 T/I 16 C 26 A 30
Name: Dynamics Test K/U 28 T/I 16 C 26 A 30 A. True/False Indicate whether the sentence or statement is true or false. 1. The normal force that acts on an object is always equal in magnitude and opposite
More informationASTRONAUT PUSHES SPACECRAFT
ASTRONAUT PUSHES SPACECRAFT F = 40 N m a = 80 kg m s = 15000 kg a s = F/m s = 40N/15000 kg = 0.0027 m/s 2 a a = -F/m a = -40N/80kg = -0.5 m/s 2 If t push = 0.5 s, then v s = a s t push =.0014 m/s, and
More informationB) v `2. C) `2v. D) 2v. E) 4v. A) 2p 25. B) p C) 2p. D) 4p. E) 4p 2 25
1. 3. A ball attached to a string is whirled around a horizontal circle of radius r with a tangential velocity v. If the radius is changed to 2r and the magnitude of the centripetal force is doubled the
More informationDynamics: Forces and Newton s Laws of Motion
Lecture 7 Chapter 5 Dynamics: Forces and Newton s Laws of Motion Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Today we are going to discuss: Chapter 5: Force, Mass: Section 5.1
More informationPractice Test for Midterm Exam
A.P. Physics Practice Test for Midterm Exam Kinematics 1. Which of the following statements are about uniformly accelerated motion? Select two answers. a) If an object s acceleration is constant then it
More informationPHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010
PHYSICS 1, FALL 010 EXAM 1 Solutions WEDNESDAY, SEPTEMBER 9, 010 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively. In
More informationChapter 8: Newton s Laws Applied to Circular Motion
Chapter 8: Newton s Laws Applied to Circular Motion Centrifugal Force is Fictitious? F actual = Centripetal Force F fictitious = Centrifugal Force Center FLEEing Centrifugal Force is Fictitious? Center
More informationBlueberry Muffin Nov. 29/30, 2016 Period: Names:
Blueberry Muffin Nov. 9/30, 016 Period: Names: Congratulations! 1. To solve the problems, use your etextbook, physical textbooks, physics websites, your Sketchbooks.. Show your thinking through calculations,
More informationChapter 5 Review : Circular Motion; Gravitation
Chapter 5 Review : Circular Motion; Gravitation Conceptual Questions 1) Is it possible for an object moving with a constant speed to accelerate? Explain. A) No, if the speed is constant then the acceleration
More informationForces. Dynamics FORCEMAN
1 Forces Dynamics FORCEMAN 2 What causes things to move? Forces What is a force? A push or a pull that one body exerts on another. 3 Balanced No change in motion 4 5 Unbalanced If the forces acting on
More informationPhysics 101: Lecture 08 Centripetal Acceleration and Circular Motion
Physics 101: Lecture 08 Centripetal Acceleration and Circular Motion http://www.youtube.com/watch?v=zyf5wsmxrai Today s lecture will cover Chapter 5 Physics 101: Lecture 8, Pg 1 Circular Motion Act B A
More informationChapter 6. Force and Motion-II
Chapter 6 Force and Motion-II 6.2 Friction Frictional Forces Friction has its basis in surfaces that are not completely smooth: Frictional Forces The static frictional force keeps an object from starting
More informationCircular Motion and Gravitation Notes 1 Centripetal Acceleration and Force
Circular Motion and Gravitation Notes 1 Centripetal Acceleration and Force This unit we will investigate the special case of kinematics and dynamics of objects in uniform circular motion. First let s consider
More informationCircular Motion and Gravitation Notes 1 Centripetal Acceleration and Force
Circular Motion and Gravitation Notes 1 Centripetal Acceleration and Force This unit we will investigate the special case of kinematics and dynamics of objects in uniform circular motion. First let s consider
More informationPhysics. Chapter 8 Rotational Motion
Physics Chapter 8 Rotational Motion Circular Motion Tangential Speed The linear speed of something moving along a circular path. Symbol is the usual v and units are m/s Rotational Speed Number of revolutions
More informationChapter 5 Circular Motion; Gravitation
Chapter 5 Circular Motion; Gravitation Units of Chapter 5 Kinematics of Uniform Circular Motion Dynamics of Uniform Circular Motion Highway Curves, Banked and Unbanked Newton s Law of Universal Gravitation
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Diagram 1 A) B - A. B) A - B. C) A + B. D) A B.
Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) In the diagram shown, the unknown vector is 1) Diagram 1 A) B - A. B) A - B. C) A + B.
More informationLecture 6. Circular Motion. Pre-reading: KJF 6.1 and 6.2. Please take a clicker CIRCULAR MOTION KJF
Lecture 6 Circular Motion Pre-reading: KJF 6.1 and 6.2 Please take a clicker CIRCULAR MOTION KJF 6.1 6.4 Angular position If an object moves in a circle of radius r, then after travelling a distance s
More informationCircular Motion. - The velocity is tangent to the path and perpendicular to the radius of the circle
Circular Motion Level : Physics Teacher : Kim 1. Uniform Circular Motion - According to Newton s 1 st law, an object in motion will move in a straight line at a constant speed unless an unbalance force
More informationProjectile and Circular Motion Review Packet
Conceptual Physics Projectile and Circular Motion Review Packet Mr. Zimmerman Textbook Reference: pp. 33-42, 122-135 Key Terms (fill in definitions) projectile - any object that moves through the air or
More informationChapter 9. Rotational Dynamics
Chapter 9 Rotational Dynamics In pure translational motion, all points on an object travel on parallel paths. The most general motion is a combination of translation and rotation. 1) Torque Produces angular
More informationCIRCULAR MOTION AND GRAVITATION
CIRCULAR MOTION AND GRAVITATION An object moves in a straight line if the net force on it acts in the direction of motion, or is zero. If the net force acts at an angle to the direction of motion at any
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Common Quiz Mistakes / Practice for Final Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A ball is thrown directly upward and experiences
More informationProficient. a. The gravitational field caused by a. The student is able to approximate a numerical value of the
Unit 6. Circular Motion and Gravitation Name: I have not failed. I've just found 10,000 ways that won't work.-- Thomas Edison Big Idea 1: Objects and systems have properties such as mass and charge. Systems
More informationProjectile Motion. directions simultaneously. deal with is called projectile motion. ! An object may move in both the x and y
Projectile Motion! An object may move in both the x and y directions simultaneously! The form of two-dimensional motion we will deal with is called projectile motion Assumptions of Projectile Motion! The
More informationCEE 271: Applied Mechanics II, Dynamics Lecture 9: Ch.13, Sec.4-5
1 / 40 CEE 271: Applied Mechanics II, Dynamics Lecture 9: Ch.13, Sec.4-5 Prof. Albert S. Kim Civil and Environmental Engineering, University of Hawaii at Manoa 2 / 40 EQUATIONS OF MOTION:RECTANGULAR COORDINATES
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) You are standing in a moving bus, facing forward, and you suddenly fall forward as the
More informationMechanics Lecture Notes
Mechanics Lecture Notes Lectures 0 and : Motion in a circle. Introduction The important result in this lecture concerns the force required to keep a particle moving on a circular path: if the radius of
More informationCircular Motion Test Review
Circular Motion Test Review Name: Date: 1) Is it possible for an object moving with a constant speed to accelerate? Explain. A) No, if the speed is constant then the acceleration is equal to zero. B) No,
More informationPS113 Chapter 4 Forces and Newton s laws of motion
PS113 Chapter 4 Forces and Newton s laws of motion 1 The concepts of force and mass A force is described as the push or pull between two objects There are two kinds of forces 1. Contact forces where two
More information4) Vector = and vector = What is vector = +? A) B) C) D) E)
1) Suppose that an object is moving with constant nonzero acceleration. Which of the following is an accurate statement concerning its motion? A) In equal times its speed changes by equal amounts. B) In
More informationExperiencing Acceleration: The backward force you feel when your car accelerates is caused by your body's inertia. Chapter 3.3
Experiencing Acceleration: The backward force you feel when your car accelerates is caused by your body's inertia. Chapter 3.3 Feeling of apparent weight: Caused your body's reaction to the push that the
More informationName (please print): UW ID# score last first
Name (please print): UW ID# score last first Question I. (20 pts) Projectile motion A ball of mass 0.3 kg is thrown at an angle of 30 o above the horizontal. Ignore air resistance. It hits the ground 100
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics. Physics 8.01 Fall Problem Set 2: Applications of Newton s Second Law Solutions
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01 Fall 2012 Problem 1 Problem Set 2: Applications of Newton s Second Law Solutions (a) The static friction force f s can have a magnitude
More informationMotion in a Plane Uniform Circular Motion
Lecture 11 Chapter 8 Physics I Motion in a Plane Uniform Circular Motion Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will learn to solve problems about
More informationCircular Motion and Gravitation. Centripetal Acceleration
Circular Motion and Gravitation Centripetal Acceleration Recall linear acceleration 3. Going around a curve, at constant speed 1. Speeding up vi vi Δv a ac ac vi ac 2. Slowing down v velocity and acceleration
More informationUnit 5 Circular Motion and Gravitation
Unit 5 Circular Motion and Gravitation In the game of tetherball, the struck ball whirls around a pole. In what direction does the net force on the ball point? 1) Tetherball 1) toward the top of the pole
More information1 Page. Uniform Circular Motion Introduction. Earlier we defined acceleration as being the change in velocity with time:
Uniform Circular Motion Introduction Earlier we defined acceleration as being the change in velocity with time: a=δv/t Until now we have only talked about changes in the magnitude of the acceleration:
More informationRotational Motion Examples:
Rotational Motion Examples: 1. A 60. cm diameter wheel rotates through 50. rad. a. What distance will it move? b. How many times will the wheel rotate in this time? 2. A saw blade is spinning at 2000.
More informationQuestion 1. G.M. Paily Phys 211
Question 1 A 0.5 kg hockey puck slides along the surface of the ice with a speed of 10 m s. What force must be acting on the puck to keep it moving at constant velocity? A 0.05 N B 5 N C 20 N D 50 N E
More informationExtension of Circular Motion & Newton s Laws. Chapter 6 Mrs. Warren Kings High School
Extension of Circular Motion & Newton s Laws Chapter 6 Mrs. Warren Kings High chool Review from Chapter 4 Uniform Circular Motion Centripetal Acceleration Uniform Circular Motion, Force F r A force is
More informationContents. Objectives IAI motion w/o force motion with force F=ma third law work and energy circular motion Final Exam mechanics questions Recap IAI
Physics 121 for Majors Section 1 IAI Review 4 Review for IAI and Final Exam Exam Details In the Testing Center Friday - Wednesday Wed. is a late day with a $5 fee Hours: 8 am 9 pm Friday 10 am 3 pm Saturday
More informationBlueberry Muffin Nov. 29/30, 2016 Period: Names:
Blueberry Muffin Nov. 29/30, 2016 Period: Names: Congratulations! 1. To solve the problems, use your etextbook, physical textbooks, physics websites, your Sketchbooks. 2. Show your thinking through calculations,
More informationAP Physics II Summer Packet
Name: AP Physics II Summer Packet Date: Period: Complete this packet over the summer, it is to be turned it within the first week of school. Show all work were needed. Feel free to use additional scratch
More informationGravity. Gravity and Newton. What really happened? The history of Gravity 3/9/15. Sir Isaac Newton theorized the Law of Gravitation in 1687
3/9/15 Gravity and Newton Gravity What really happened? Probably the more correct version of the story is that Newton, upon observing an apple fall from a tree, began to think along the following lines:
More informationDynamics: Forces. Lecture 7. Chapter 5. Course website:
Lecture 7 Chapter 5 Dynamics: Forces Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Today we are going to discuss: Chapter 5: Some leftovers from rotational motion Ch.4 Force,
More informationSection 9.2. Centripetal Acceleration Centripetal Force
Section 9.2 Centripetal Acceleration Centripetal Force Centripetal Acceleration Uniform Circular Motion The motion of an object in a circular path at a constant speed is known as uniform circular motion
More informationAssignment - Periodic Motion. Reading: Giancoli, Chapter 5 Holt, Chapter 7. Objectives/HW:
Assignment - Periodic Motion Reading: Giancoli, Chapter 5 Holt, Chapter 7 Objectives/HW: The student will be able to: 1 Define and calculate period and frequency. 2 Apply the concepts of position, distance,
More informationCircular Motion CENTRIPETAL ACCELERATION. tf-t,
Circular Motion Ill SECTION OBJECTIVES Solve problems involving centripetal acceleration. Solve problems involving centripetal force. Explain how the apparent existence of an outward force in circular
More informationUniform Circular Motion AP
Uniform Circular Motion AP Uniform circular motion is motion in a circle at the same speed Speed is constant, velocity direction changes the speed of an object moving in a circle is given by v circumference
More information5. A car moves with a constant speed in a clockwise direction around a circular path of radius r, as represented in the diagram above.
1. The magnitude of the gravitational force between two objects is 20. Newtons. If the mass of each object were doubled, the magnitude of the gravitational force between the objects would be A) 5.0 N B)
More informationIn this lecture we will discuss three topics: conservation of energy, friction, and uniform circular motion.
1 PHYS:100 LECTURE 9 MECHANICS (8) In this lecture we will discuss three topics: conservation of energy, friction, and uniform circular motion. 9 1. Conservation of Energy. Energy is one of the most fundamental
More informationSAPTARSHI CLASSES PVT. LTD.
SAPTARSHI CLASSES PVT. LTD. NEET/JEE Date : 13/05/2017 TEST ID: 120517 Time : 02:00:00 Hrs. PHYSICS, Chem Marks : 360 Phy : Circular Motion, Gravitation, Che : Halogen Derivatives Of Alkanes Single Correct
More informationLecture 5. Dynamics. Forces: Newton s First and Second
Lecture 5 Dynamics. Forces: Newton s First and Second What is a force? It s a pull or a push: F F Force is a quantitative description of the interaction between two physical bodies that causes them to
More information