SPH3UW/SPH4U Unit 3.2 Forces in Cetripetal Motion Page 1 of 6. Notes Physics Tool Box

Similar documents
Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string

Announcements. Description Linear Angular position x θ displacement x θ rate of change of position v x ω x = = θ average rate of change of position

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Motion in a Plane Uniform Circular Motion

Physics 111. Lecture 14 (Walker: Ch. 6.5) Circular Motion Centripetal Acceleration Centripetal Force February 27, 2009

Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

AP Physics Centripetal Acceleration

Circular Motion. x-y coordinate systems. Other coordinates... PHY circular-motion - J. Hedberg

Objective Notes Summary

PS113 Chapter 5 Dynamics of Uniform Circular Motion

3.3 Centripetal Force

Physics 111 Lecture 5 Circular Motion

DYNAMICS OF UNIFORM CIRCULAR MOTION

Shree Datta Coaching Classes, Contact No Circular Motion

AP Physics 1 - Circular Motion and Gravitation Practice Test (Multiple Choice Section) Answer Section

Physics 101 Lecture 6 Circular Motion

PROJECTILE MOTION. At any given point in the motion, the velocity vector is always a tangent to the path.

Uniform Circular Motion

Chapter 5: Uniform Circular Motion

Force & Motion: Newton s Laws

Solutions Practice Test PHYS 211 Exam 2

Sections and Chapter 10

Chapter 5. Uniform Circular Motion. a c =v 2 /r

Test 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.

ΣF = r r v. Question 213. Checkpoints Chapter 6 CIRCULAR MOTION

r cos, and y r sin with the origin of coordinate system located at

2013 Checkpoints Chapter 6 CIRCULAR MOTION

Chap 5. Circular Motion: Gravitation

Centripetal Force. Lecture 11. Chapter 8. Course website:


Circular Motion. Mr. Velazquez AP/Honors Physics

Motion in a Circle. Content 1. Kinematics of uniform circular motion 2. Centripetal acceleration 3. Centripetal force.

Circular Motion Problem Solving

Name. Date. Period. Engage Examine the pictures on the left. 1. What is going on in these pictures?

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.

Impulse and Momentum

constant t [rad.s -1 ] v / r r [m.s -2 ] (direction: towards centre of circle / perpendicular to circle)

Chapters 5-8. Dynamics: Applying Newton s Laws

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.

Answers to test yourself questions

The study of the motion of a body along a general curve. the unit vector normal to the curve. Clearly, these unit vectors change with time, u ˆ

NEETIIT.COM. Angular Displacement. Page - 1

ω = θ θ o = θ θ = s r v = rω

4. Two and Three Dimensional Motion

V V The circumflex (^) tells us this is a unit vector

Uniform Circular Motion

Discover the answer to this question in this chapter.

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Ch04: Motion in two and three dimensions (2D and 3D)

rt () is constant. We know how to find the length of the radius vector by r( t) r( t) r( t)

Chapter 5 Applications of Newton s Laws

UCSD Phys 4A Intro Mechanics Winter 2016 Ch 5 Solutions

Discover the answer to this question in this chapter.

CIRCULAR MOTION. Particle moving in an arbitrary path. Particle moving in straight line

Physics 2001 Problem Set 5 Solutions

1) Consider a particle moving with constant speed that experiences no net force. What path must this particle be taking?

Physics 231 Lecture 17

Chapter 8. Accelerated Circular Motion

Describing Circular motion

Chapter 19 Webassign Help Problems

Circular Motion. Subtopics. Introduction. Angular displacement. acceleration. Relation between linear velocity and angular velocity

Chapter 5 Force and Motion

PHYSICS 220. Lecture 08. Textbook Sections Lecture 8 Purdue University, Physics 220 1

) 1.5"10 11 m. ( )( 1.99 "10 30 kg)

Introduction to Mechanics Centripetal Force

PHYS 1114, Lecture 21, March 6 Contents:

21 MAGNETIC FORCES AND MAGNETIC FIELDS

Physics Spring 2012 Announcements: Mar 07, 2012

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields

AP * PHYSICS B. Circular Motion, Gravity, & Orbits. Teacher Packet

Chapter 5. Applying Newton s Laws. Newton s Laws. r r. 1 st Law: An object at rest or traveling in uniform. 2 nd Law:

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature)

Circular-Rotational Motion Mock Exam. Instructions: (92 points) Answer the following questions. SHOW ALL OF YOUR WORK.

Physics 1114: Unit 5 Hand-out Homework (Answers)

Quiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible)

Uniform Circular Motion

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines

MAGNETIC FIELD INTRODUCTION

Physics 107 TUTORIAL ASSIGNMENT #8

Example 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example

Understanding the Concepts

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed?

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

Thomas Whitham Sixth Form Mechanics in Mathematics. Rectilinear Motion Dynamics of a particle Projectiles Vectors Circular motion

Chapter 1: Mathematical Concepts and Vectors

Extra notes for circular motion: Circular motion : v keeps changing, maybe both speed and

Between any two masses, there exists a mutual attractive force.

PHYS Summer Professor Caillault Homework Solutions. Chapter 5

HRW 7e Chapter 13 Page 1 of 5

3.2 Centripetal Acceleration

Chapter 5 Force and Motion

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Chap13. Universal Gravitation

Kinematics in 2-D (II)

As observed from the frame of reference of the sidewalk:

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

SECTION 1. Objectives. Solve problems involving centripetal acceleration. Solve problems involving centripetal force.

6.4 Period and Frequency for Uniform Circular Motion

Transcription:

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page 1 o 6 Note Phyic Tool Box Net Foce: acting on an object in uniom cicula motion act towad the cente o the cicle. Magnitude o Net Foce: combine Newton Second Law, F ma, with the equation o m centipetal acceleation aad to poduce F. Fame o Reeence: o an object moing in a cicle i a noninetial ame. Coioli Foce: i a ictitiou oce ued to explain paticle moing in a otating ame o eeence. Ca negotiating cue on a highway poide an example o cicula motion. Recalling that an object taelling at a contant peed in a cicle (o ac) expeience centipetal acceleation towad the cente o the cicle. Accoding the Newton nd Law, centipetal acceleation i the eult o a net oce acting in the diection o the acceleation and pependicula to the intantaneou elocity ecto. m Theeoe F ma and aad combine to gie u F Whee F i the magnitude o the net oce that caue the cicula motion. I you ate gien the peiod, T and equency, then you can ue m 4 m F 4 m T A led with a ma o 0.0 kg et on a hoizontal heet o ictionle ice. It i attached by a 4.00m ope to a pot et in the ice. Once gien a puh, the led eole uniomly in a cicle aound the pot. I the led make 5 complete eolution eey minute, ind the oce F exeted on it by the ope.

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page o 6 Thee i no acceleation in the y-diection, o the net oce in that diection (the um o the nomal and weight0 i zeo. Fo the x-diection, Newton nd law gie along with the gien peiod and ma: 4 m Fx F max T F kg m 1.0 4 0.0 4.00 kg m 1.9 1.9N Note: i you doubled the elocity, then the Foce, F would be 4 time geate. Caution: in doing poblem with uniom cicula motion, you may be tempted to include an exta m outwad oce o magnitude to keep the body out thee o to keep it in equilibium. Thi outwad oce i called Centiugal oce (leeing om cente). Reit thi temptation, becaue thi appoach i imply wong. In an inetial ame o eeence thee i no uch thing a centiugal oce. A ticky tuntable pin 3.5 time in 4.0 econd. I a 45.0g coin it 10cm om the cente o the tuntable, what oce i equied to keep the coin on the tuntable i the coeicient o iction i 0.5? 3.5time Gien: 0.875 Hz, m 0.045 kg, 0.1m, u 0.5, F? 4.0 Now F F F F and F 0 theeoe Fn Fg F net y n g net y mg F Alo F F n mg F m In the x-diection: F F netx ma F m4 mg F m4 F 0.045 4 0.10 0.875 0.045kg 9.8 0.10N mg kg m Hz m 0.5

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page 3 o 6 I a ca i ounding a lat, unbanked cue with adiu 30m. I the coeicient o iction between the tie and the oad i 0.87, what i the maximum peed max at which the die can take the cue without liding? Fx maad m F n mg 0 y The econd equation how that n=mg. the it equation how that the iction oce needed to keep the ca moing in it cicula path inceae with the ca peed. The maximum oce aailable i n mg. max Theeoe m mg m max The maximum peed i about max g m m 44 1 3600 44 m km 158 km 1000m 1h h 0.87 9.8 30m

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page 4 o 6 Fo a ca taelling at a cetain peed, it i poible to bank a cue at jut the ight angle o that no iction at all i needed to maintain the ca tuning adiu. Then a ca can ound the cue een on wet ice with Telon tie. I the adiu o the cue i 50 m and the ca elocity i 88 km/h, what angle hould the bank be? F nin ma x ad F nco mg 0 y Fom the econd equation, mg n co Now ubtitute thi into the it equation: Now a ad mg in co tan ma a g ad ad Theeoe tan g km 1000m 1h 88 1 h km 3600 So tan m 9.8 50m 13.7 The ank i then about 14.

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page 5 o 6 A pilot o ma m in a jet aicat execute a loop-the-loop. In thi manoeue, the aicat moe in a etical cicle o adiu 3.50 km at a contant peed o 55 m/. Detemine the oce exeted by the eat on the pilot (A) at the bottom o the loop and (B) at the top o the loop. Expe you anwe in tem o the weight o the pilot mg. Top G F ma F F ma N mg FN m FN mg m mg 1 g mg 1 0.896mg m 55 3 3.510 m 9.8 m G Bottom F ma F F ma N mg FN m FN m mg mg 1 g mg.90mg m 55 3 3.510 m 9.8 1 m

SPH3UW/SPH4U Unit 3. Foce in Cetipetal Motion Page 6 o 6 Exta Note and Comment