PHY 121 Finals Review FSE Tutoring Centers Spring 2016

Size: px
Start display at page:

Download "PHY 121 Finals Review FSE Tutoring Centers Spring 2016"

Transcription

1 11-Ap Apil,016 Vecto Addition PHY 11 Final Reiew FSE Tutoing Cente Sping 016 Vecto Addition: Place the ecto tip to tail. A ecto ma be moed an wa ou pleae poided that ou do not change it length no otate it. The eultant point fom the tail of the fit ecto to the tip of the econd (A+). To add ecto togethe the mut fit be eoled into component. The () component of a ecto i found b pojecting the ecto onto the () ai. Eample: Vecto A ha a length of 5.00 mete and point along the -ai. Vecto ha a length of 3.00 mete and point 10 fom the +-ai. Compute A+ (=C). A A C A 10 A 3 4 1

2 11-Ap-16 Eample continued opp in hp adj co hp in opp tan co adj A in60 in min60.60m co60 co mco m And A = 5.00 m and A = 0.00 m 5 Eample continued C A 5.00m -1.50m 3.50m The component of C: C A 0.00m.60m.60m The length of C i: C C C C C C =.60 m 3.50 m.60 m C = 3.50 m 4.36 m C.60 m The diection of C i: tan C 3.50 m 1 tan Fom the +-ai 6 Eample: At the intant a taffic light tun geen, an automobile tat with a contant acceleation of. m/. At the ame intant a tuc, taeling with a contant peed of 9.5 m/, oetae and pae the automobile. Eample continued (b) How fat will the ca be taeling at that intant? (a) How much time will elape befoe the automobile oetae the tuc? What i the data ou ae gien? U(tuc)=9.5; u(ca)=0; a(ca)=.; The ditance coeed b both ae the ame; Hence in the ame peiod of time (c) Whee do the meet? 7 8

3 11-Ap-16 Eample: A penn i dopped fom the obeation dec of the Empie State uilding 369 m aboe the gound. With what elocit doe it tie the gound? Ignoe ai eitance. Eample: You thow a ball into the ai with peed 15.0 m/, how high doe the ball ie? 0 Gien: 0 = 0 m/; a = 9.8 m/ ; 0 = 0 m; and f= 369 m Gien: 0 = m/; a = 9.8 m/ a a Unnown: f 369 m 9 10 Eample: An aow i hot into the ai with = 60 (fom the hoizontal) and 0 = 0.0 m/. The aow i eleaed fom a height of 1.80 m aboe the gound. (b) What ae the and component of the diplacement of the aow duing the 3.0 ec inteal? (a) What ae and of the aow when t=3 ec? 0 The component of the initial elocit ae: 60 At t = 3 ec: f f 0 0 co 10.0 m/ in 17.3 m/ gt 1.1m/ m/ 0 f t t t

4 11-Ap-16 Eample continued The initial poition of the aow i 0ˆ 1.8 mˆ The final poition of the aow i 0 Eample: How fa doe the aow in the peiou eample land fom whee it i eleaed? 1 The aow land when = 0 0 0t gt 0 t 30.0 m f f 0 0t gt 9.60m The diplacement i 30m 7.8 m ˆ ˆ Detemine the oot with quadatic fomula The ditance taeled i: t 0.10eco 3.64ec 0t 36.4 m Eample: How high doe the aow go? d The aow ie until 0 d The ma height i eached when with d d dt d d dt d 0 0 gt dt 0 t 1.77ec g Relatie motion Eample: You ae taeling in a ca (A) at 60 mile/hou eat on a long taight oad. The ca () net to ou i taeling at 65 mile/hou eat. What i the peed of ca elatie to ca A? The -coodinate of the aow i 1 t 1.77 t gt 17.1 m

5 11-Ap-16 Eample continued: t=0 t>0 + A AG A G A Eample: You ae taeling in a ca (A) at 60 mile/hou eat on a long taight oad. The ca () net to ou i taeling at 65 mile/hou wet. What i the peed of ca elatie to ca A? Fom the pictue: G AG A A G AG Diide b t: A G AG A 65mile/h eat 60mile/h eat 5 mile/houeat Eample continued: t>0 t=0 + t>0 Eample: The cuent in a ie ha a tead peed of 0.5 m/. A tudent wim upteam a ditance of 1 m and then wim bac to the tating point. If the tudent can wim 1. m/ in till wate, how long doe the ound tip in the ie tae? How long would the ame tip tae in till wate? A AG A Fom the pictue: Diide b t: G A A A G G AG AG In till wate: d t 000m m/ O 835 econd pe leg 65mile/h wet 60mile/h eat 15mile/h wet

6 11-Ap-16 Eample continued Upteam 0.7 m/ up d t 1000m m/ Eample: A jet moing initiall with = 300 mph due eat ente a egion whee the wind i blowing at 100 mph at 30 noth of eat. What i the new elocit of the jet? (noth) wind jet Downteam d t 1.7 m/ up 1000m m/ Place the ecto tip-to-tail: (eat) new jet wind The total time i 00 econd! 1 Eample continued new jet wind 300mph ˆ 100mphco30 ˆ 100mphin30 ˆ 387ˆ 50ˆ mph The magnitude and diection of the elocit ae Fee od Diagam Ue idealized model to account fo all foce acting on each ma (bod) inoled in the tem being analzed. new 390mph tan 0.19 The plane tael 390 mph 7.4 noth of eat 3 4 6

7 11-Ap-16 Eample: Find the tenion in each cod of the tem hown in the figue. Eample: A bo lide aco a ough uface. If the coefficient of inetic fiction i 0.3, what i the acceleation of the bo? FD fo bo: F ;b N b w Appl Newton nd Law: F N f b F f F N ;b w ma b ;b ma w Eample continued (1) () f ma N w 0 b ;b N w mg b Eample: In the peiou eample, a bo liding aco a ough uface wa found to hae an acceleation of -.94 m/. If the initial peed of the bo i 10.0 m/, how long doe it tae fo the bo to come to et? Know: a =.94 m/, 0=10.0 m/, = 0.0 m/ Want: t. Fom (1): Soling fo a: f ;b N mg ma a g b m/.94m/ 0 t a a t m/ 3.40ec. 94m/ 7 8 7

8 11-Ap-16 Eample: A 1.00 g ma i at et an on amp that mae an angle of 0 with epect to the hoizontal. Fo thi ituation = What i the magnitude of the tatic fiction foce? FD fo bo f ;b N b Eample continued (1) () F f F N b ;b mg in 0 mg co 0 The magnitude of the tatic fiction foce can be found fom (1) w f mg in 3.35N ; b Appl Newton nd law F N b f ;b w 0 What i the magnitude of the maimum tatic fiction foce? f ; b Nb mg co 3.68N 9 30 Eample continued If the angle of the amp i changed to 40, what i the acceleation of the ma? Tae = Eample: A 3.00 g ma et on a fictionle tabletop. Thi ma i connected to a 5.00 g ma b a light ting a hown. Aume the pulle i male. The FD i unchanged, ecept f ;b i now the inetic fiction foce of the amp on the bo. a. Daw fee bod diagam fo the two mae and the pulle. Appl Newton nd law F N f b ;b w ma (1) () F f F N b ;b mg in ma mg co

9 11-Ap-16 Eample continued b. Appl Newton Second law to the two mae. Dnamic of Cicula Motion t t t a co ˆ in ˆ in ˆ co ˆ co ˆ in ˆ Rotational motion can be elated to tanlational motion b coneting between Cateian and pola coodinate tem The tangential elocit and adial acceleation of a bod (contant peed cae). Eample: The Hubble Space Telecope obit the Eath at an altitude of about 600 m with an obit peiod of about 100 minute, what i Hubble obital peed? (Aume a cicula obit.) a total ditance a 7300m/ total time t T a a a = R e + h = m T =

10 11-Ap-16 Eample continued (b) What i HST angula peed? Eample: What i the magnitude of the adial acceleation of HST? π a t T 3 ad/ec a 7.63m/ 0. 78g Peioul: Conide an object in unifom cicula motion (peed=contant). t t t a co ˆ in ˆ in ˆ co ˆ The magnitude of the (tangential) elocit i co ˆ in ˆ Eample: The oto i an amuement pa ide whee people tand againt the inide of a clinde. Once the clinde i pinning fat enough the floo dop out. (a) What foce eep the people fom falling out the bottom of the clinde? Daw an FD fo a peon with thei bac to the wall: N wp f ;wp The magnitude of the (adial) acceleation i a 39 w ep It i the foce of tatic fiction

11 11-Ap-16 Eample continued (b) If = 0.40 and the clinde ha =.5 m. what i the minimum angula peed of the clinde o that the people don t fall out? Eample: A coin i placed on a ecod that i otating at 33.3 pm. If = 0.1, how fa fom the cente of the ecod can the coin be placed without haing it lip off? Appl Newton nd law: Fom (): f ;wp N wp w ep m F Nwp f;wp wep ma 1 F N ma m wp F f wep 0 ;wp mg g Fom (1) mg 9.8 m/ 3.13ad/ m 41 Daw an FD fo the coin: N c f ;c w ec Appl Newton nd law: F N f c ;c w ma 1 F f ma m ;c adial F N wec 0 c ec 4 Eample continued Fom 1 : f m ;c f N mg m ;c c Fom () Eample: What i the minimum peed fo the ca o that it maintain contact with the loop when it i in the pictued poition? Soling fo : g What i? FD fo the ca at the top of the loop: e ad 1min ad/ min 1e 60ec g m/ 3.50ad/ 0.08m 43 N w ec Appl Newton nd law: F N w ma F N w ma ec ec N wec m 44 11

12 11-Ap-16 Eample continued N mg m The appaent weight at the top of loop i N m g N m g N = 0 when 0 g Thi i the minimum peed needed to mae it aound the loop. 45 Eample continued Conide the ca at the bottom of the loop, how doe the appaent weight compae to the tue weight? FD fo the ca at the bottom of the loop: N w ec Appl Newton nd law: F N w ma F N wec ma m N mg m N m g Hee, ec N mg 46 Eample continued Eample continued Fom () the nomal foce i Nb mg co c. What i the acceleation of the tem? Uing (1): f ;b mg in ma mg N mg in ma b co mg in ma d. What i the tenion in the ope? a g in co 3.67 m/

13 11-Ap-16 Wo and Eneg Eample: The etinction of the dinoau and the majoit of pecie on Eath in the Cetaceou Peiod (65 M ago) i thought to hae been caued b an ateoid tiing the Eath nea the Yucatan Peninula. The eulting ejecta caued widepead global climate change. If the ma of the ateoid wa g (diamete in the ange of 4-9 mile) and had a peed of 30.0 m/ec, what wa the ateoid inetic eneg? 1 1 K m J g3010 m/ 49 Thi i equialent to ~10 9 Megaton of TNT. 50 Eample: What i the net wo done on a bo of ma m that i being puhed along a ough uface a hown? Eample continued The foce and diplacement (in unit ecto notation) ae F An FD fo the bo at left: N b f ;b w F pb N w f b ;b ˆ ˆ mg F in ˆ ˆ mg ˆ ˆ mg F in F F co ˆ F in ˆ pb N w f b ;b ˆ The wo done b the puhing foce i: 51 W pb F pb F co 5 13

14 11-Ap-16 The wo done b the Nomal foce i: W N Nb 0 The nomal foce i pependicula to the diplacement. The net wo done on the bo i: The wo done b gait i: W g w 0 The foce of gait i pependicula to the diplacement. Wnet Wpf WN Wg Wf F co 0 0 mg F in F co mg F in The wo done b inetic fiction i: W f f ;b mg F in Eample: A ball i toed taight up. What i the wo done b the foce of gait on the ball a it ie? Eample: An ideal ping ha = 0.0 N/m. What i the amount of wo done (b an etenal agent) to teh the ping 0.40 m fom it elaed length? FD fo iing ball: w W g w w co180 mg W F d m 0 1 Fd 0.40 m N/m0.40m 1.6 J W < 0 and the KE of the ball deceae

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

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION Phyic 1 1 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal plane. At the point indicated, the ting beak. Looking down

More information

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

Chapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION 103 PHYS 1 1 L:\103 Phy LECTURES SLIDES\103Phy_Slide_T1Y3839\CH6Flah 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal

More information

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

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 Announcement In the lectue link Look o tet 1 beakdown liting the topic o the quetion. Look o m umma o topic o the eam. We ll ue it on the eiew net Tueda. Look o a lit o baic phic act eleant o thi eam.

More information

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

Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion. 5. Cicula otion By Liew Sau oh Content 5.1 Angula diplaceent and angula elocity 5. Centipetal acceleation 5.3 Centipetal foce Objectie a) expe angula diplaceent in adian b) define angula elocity and peiod

More information

AP Physics Centripetal Acceleration

AP Physics Centripetal Acceleration AP Phyic Centipetal Acceleation All of ou motion tudie thu fa hae dealt with taight-line tuff. We haen t dealt with thing changing diection duing thei tael. Thi type of motion i called angula motion. A

More information

UCSD Phys 4A Intro Mechanics Winter 2016 Ch 5 Solutions

UCSD Phys 4A Intro Mechanics Winter 2016 Ch 5 Solutions UCSD Phs 4 Into Mechanics Winte 016 Ch 5 Solutions 0. Since the uppe bloc has a highe coefficient of iction, that bloc will dag behind the lowe bloc. Thus thee will be tension in the cod, and the blocs

More information

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

Test 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction. Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae

More information

DYNAMICS OF UNIFORM CIRCULAR MOTION

DYNAMICS OF UNIFORM CIRCULAR MOTION Chapte 5 Dynamics of Unifom Cicula Motion Chapte 5 DYNAMICS OF UNIFOM CICULA MOTION PEVIEW An object which is moing in a cicula path with a constant speed is said to be in unifom cicula motion. Fo an object

More information

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

Circular Motion. x-y coordinate systems. Other coordinates... PHY circular-motion - J. Hedberg Cicula Motion PHY 207 - cicula-motion - J. Hedbeg - 2017 x-y coodinate systems Fo many situations, an x-y coodinate system is a geat idea. Hee is a map on Manhattan. The steets ae laid out in a ectangula

More information

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

Ch04: Motion in two and three dimensions (2D and 3D) Ch4: Motion in two and thee dimensions (D and 3D) Displacement, elocity and acceleation ectos Pojectile motion Cicula motion Relatie motion 4.: Position and displacement Position of an object in D o 3D

More information

Circular Motion Problem Solving

Circular Motion Problem Solving iula Motion Poblem Soling Aeleation o a hange in eloity i aued by a net foe: Newton nd Law An objet aeleate when eithe the magnitude o the dietion of the eloity hange We aw in the lat unit that an objet

More information

Force & Motion: Newton s Laws

Force & Motion: Newton s Laws oce & otion: Newton Law ( t Law) If no net foce act on a body then the body velocity cannot change. Zeo net foce implie zeo acceleation. The ma of an object detemine how difficult it i to change the object

More information

Motion in a Plane Uniform Circular Motion

Motion in a Plane Uniform Circular Motion Lectue 11 Chapte 8 Physics I Motion in a Plane Unifom Cicula Motion Couse website: http://faculty.uml.edu/andiy_danylo/teaching/physicsi PHYS.1410 Lectue 11 Danylo Depatment of Physics and Applied Physics

More information

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

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

TP A.4 Post-impact cue ball trajectory for any cut angle, speed, and spin

TP A.4 Post-impact cue ball trajectory for any cut angle, speed, and spin technical poof TP A.4 Pot-impact cue ball tajectoy fo any cut anle, peed, and pin uppotin: The Illutated Pinciple of Pool and Billiad http://billiad.colotate.edu by Daid G. Alciatoe, PhD, PE ("D. Dae")

More information

Solutions Practice Test PHYS 211 Exam 2

Solutions Practice Test PHYS 211 Exam 2 Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following

More information

Impulse and Momentum

Impulse and Momentum Impule and Momentum 1. A ca poee 20,000 unit of momentum. What would be the ca' new momentum if... A. it elocity wee doubled. B. it elocity wee tipled. C. it ma wee doubled (by adding moe paenge and a

More information

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.

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. Unit 6 actice Test 1. Which one of the following gaphs best epesents the aiation of the kinetic enegy, KE, and of the gaitational potential enegy, GE, of an obiting satellite with its distance fom the

More information

Physics 101 Lecture 6 Circular Motion

Physics 101 Lecture 6 Circular Motion Physics 101 Lectue 6 Cicula Motion Assist. Pof. D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Equilibium, Example 1 q What is the smallest value of the foce F such that the.0-kg block will not slide

More information

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

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once. Honos Physics Fall, 2016 Cicula Motion & Toque Test Review Name: M. Leonad Instuctions: Complete the following woksheet. SHOW ALL OF YOUR WORK ON A SEPARATE SHEET OF PAPER. 1. Detemine whethe each statement

More information

Physics 201 Homework 4

Physics 201 Homework 4 Physics 201 Homewok 4 Jan 30, 2013 1. Thee is a cleve kitchen gadget fo dying lettuce leaves afte you wash them. 19 m/s 2 It consists of a cylindical containe mounted so that it can be otated about its

More information

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.

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. Unit 6 actice Test 1. Which one of the following gaphs best epesents the aiation of the kinetic enegy, KE, and of the gaitational potential enegy, GE, of an obiting satellite with its distance fom the

More information

Physics 111 Lecture 5 Circular Motion

Physics 111 Lecture 5 Circular Motion Physics 111 Lectue 5 Cicula Motion D. Ali ÖVGÜN EMU Physics Depatment www.aovgun.com Multiple Objects q A block of mass m1 on a ough, hoizontal suface is connected to a ball of mass m by a lightweight

More information

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

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

More information

PS113 Chapter 5 Dynamics of Uniform Circular Motion

PS113 Chapter 5 Dynamics of Uniform Circular Motion PS113 Chapte 5 Dynamics of Unifom Cicula Motion 1 Unifom cicula motion Unifom cicula motion is the motion of an object taveling at a constant (unifom) speed on a cicula path. The peiod T is the time equied

More information

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

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session. - 5 - TEST 1R This is the epeat vesion of TEST 1, which was held duing Session. This epeat test should be attempted by those students who missed Test 1, o who wish to impove thei mak in Test 1. IF YOU

More information

Chapter 5 Applications of Newton s Laws

Chapter 5 Applications of Newton s Laws Chapte 5 Application of Newton Law Conceptual Poblem Detemine the Concept Becaue the object ae peeding up (acceleating), thee mut be a net foce acting on them. The foce acting on an object ae the nomal

More information

Sections and Chapter 10

Sections and Chapter 10 Cicula and Rotational Motion Sections 5.-5.5 and Chapte 10 Basic Definitions Unifom Cicula Motion Unifom cicula motion efes to the motion of a paticle in a cicula path at constant speed. The instantaneous

More information

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

PROJECTILE MOTION. At any given point in the motion, the velocity vector is always a tangent to the path. PROJECTILE MOTION A pojectile is any object that has been thown though the ai. A foce must necessaily set the object in motion initially but, while it is moing though the ai, no foce othe than gaity acts

More information

Physics 201 Lecture 18

Physics 201 Lecture 18 Phsics 0 ectue 8 ectue 8 Goals: Define and anale toque ntoduce the coss poduct Relate otational dnamics to toque Discuss wok and wok eneg theoem with espect to otational motion Specif olling motion (cente

More information

Section 25 Describing Rotational Motion

Section 25 Describing Rotational Motion Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two

More information

3.3 Centripetal Force

3.3 Centripetal Force 3.3 Centipetal Foce Think of a time when ou wee a passenge in a ca going aound a shap cue at high speed (Figue 1). If the ca wee going fast enough, ou might feel the side of the ca doo pushing on ou side.

More information

Describing Circular motion

Describing Circular motion Unifom Cicula Motion Descibing Cicula motion In ode to undestand cicula motion, we fist need to discuss how to subtact vectos. The easiest way to explain subtacting vectos is to descibe it as adding a

More information

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

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 10, 2012 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding

More information

Honors Classical Physics I

Honors Classical Physics I Hono Claical Phyic I PHY141 Lectue 9 Newton Law of Gavity Pleae et you Clicke Channel to 1 9/15/014 Lectue 9 1 Newton Law of Gavity Gavitational attaction i the foce that act between object that have a

More information

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

Name. Date. Period. Engage Examine the pictures on the left. 1. What is going on in these pictures? AP Physics 1 Lesson 9.a Unifom Cicula Motion Outcomes 1. Define unifom cicula motion. 2. Detemine the tangential velocity of an object moving with unifom cicula motion. 3. Detemine the centipetal acceleation

More information

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block? Geneal Physics I Exam 2 - Chs. 4,5,6 - Foces, Cicula Motion, Enegy Oct. 13, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults with

More information

( ) rad ( 2.0 s) = 168 rad

( ) rad ( 2.0 s) = 168 rad .) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω

More information

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

Physics 111. Lecture 14 (Walker: Ch. 6.5) Circular Motion Centripetal Acceleration Centripetal Force February 27, 2009 Physics 111 Lectue 14 (Walke: Ch. 6.5) Cicula Motion Centipetal Acceleation Centipetal Foce Febuay 7, 009 Midtem Exam 1 on Wed. Mach 4 (Chaptes 1-6) Lectue 14 1/8 Connected Objects If thee is a pulley,

More information

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS

Radian Measure CHAPTER 5 MODELLING PERIODIC FUNCTIONS 5.4 Radian Measue So fa, ou hae measued angles in degees, with 60 being one eolution aound a cicle. Thee is anothe wa to measue angles called adian measue. With adian measue, the ac length of a cicle is

More information

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

Centripetal Force. Lecture 11. Chapter 8. Course website: Lectue 11 Chapte 8 Centipetal Foce Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi PHYS.1410 Lectue 11 Danylov Depatment of Physics and Applied Physics Today we ae going to discuss:

More information

Chapter 19 Webassign Help Problems

Chapter 19 Webassign Help Problems Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply

More information

ω = θ θ o = θ θ = s r v = rω

ω = θ θ o = θ θ = s r v = rω Unifom Cicula Motion Unifom cicula motion is the motion of an object taveling at a constant(unifom) speed in a cicula path. Fist we must define the angula displacement and angula velocity The angula displacement

More information

Chapters 5-8. Dynamics: Applying Newton s Laws

Chapters 5-8. Dynamics: Applying Newton s Laws Chaptes 5-8 Dynamics: Applying Newton s Laws Systems of Inteacting Objects The Fee Body Diagam Technique Examples: Masses Inteacting ia Nomal Foces Masses Inteacting ia Tensions in Ropes. Ideal Pulleys

More information

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

Physics 4A Chapter 8: Dynamics II Motion in a Plane Physics 4A Chapte 8: Dynamics II Motion in a Plane Conceptual Questions and Example Poblems fom Chapte 8 Conceptual Question 8.5 The figue below shows two balls of equal mass moving in vetical cicles.

More information

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE Fundamental Jounal of Mathematical Physics Vol. 3 Issue 1 13 Pages 33-44 Published online at http://www.fdint.com/ ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES

More information

Rotational Kinetic Energy

Rotational Kinetic Energy Add Impotant Rotational Kinetic Enegy Page: 353 NGSS Standad: N/A Rotational Kinetic Enegy MA Cuiculum Famewok (006):.1,.,.3 AP Phyic 1 Leaning Objective: N/A, but olling poblem have appeaed on peviou

More information

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( ) : PHYS 55 (Pat, Topic ) Eample Solutions p. Review of Foce Eample ( ) ( ) What is the dot poduct fo F =,,3 and G = 4,5,6? F G = F G + F G + F G = 4 +... = 3 z z Phs55 -: Foce Fields Review of Foce Eample

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In chaptes 2 and 4 we have studied kinematics i.e. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to

More information

Understanding the Concepts

Understanding the Concepts Chistian Bache Phsics Depatment Bn Maw College Undestanding the Concepts PHYSICS 101-10 Homewok Assignment #5 - Solutions 5.7. A cclist making a tun must make use of a centipetal foce, one that is pependicula

More information

HRW 7e Chapter 13 Page 1 of 5

HRW 7e Chapter 13 Page 1 of 5 HW 7e Chapte Pae o 5 Halliday/enick/Walke 7e Chapte Gaitation The manitude o the oce o one paticle on the othe i ien by F = Gm m /, whee m and m ae the mae, i thei epaation, and G i the unieal aitational

More information

Phys 201A. Homework 6 Solutions. F A and F r. B. According to Newton s second law, ( ) ( )2. j = ( 6.0 m / s 2 )ˆ i ( 10.4m / s 2 )ˆ j.

Phys 201A. Homework 6 Solutions. F A and F r. B. According to Newton s second law, ( ) ( )2. j = ( 6.0 m / s 2 )ˆ i ( 10.4m / s 2 )ˆ j. 7. We denote the two foces F A + F B = ma,sof B = ma F A. (a) In unit vecto notation F A = ( 20.0 N)ˆ i and Theefoe, Phys 201A Homewok 6 Solutions F A and F B. Accoding to Newton s second law, a = [ (

More information

Answers to test yourself questions

Answers to test yourself questions Answes to test youself questions opic. Cicula motion π π a he angula speed is just ω 5. 7 ad s. he linea speed is ω 5. 7 3. 5 7. 7 m s.. 4 b he fequency is f. 8 s.. 4 3 a f. 45 ( 3. 5). m s. 3 a he aeage

More information

PHYSICS 151 Notes for Online Lecture 2.6

PHYSICS 151 Notes for Online Lecture 2.6 PHYSICS 151 Note fo Online Lectue.6 Toque: The whole eaon that we want to woy about cente of ma i that we ae limited to lookin at point mae unle we know how to deal with otation. Let eviit the metetick.

More information

From Newton to Einstein. Mid-Term Test, 12a.m. Thur. 13 th Nov Duration: 50 minutes. There are 20 marks in Section A and 30 in Section B.

From Newton to Einstein. Mid-Term Test, 12a.m. Thur. 13 th Nov Duration: 50 minutes. There are 20 marks in Section A and 30 in Section B. Fom Newton to Einstein Mid-Tem Test, a.m. Thu. 3 th Nov. 008 Duation: 50 minutes. Thee ae 0 maks in Section A and 30 in Section B. Use g = 0 ms in numeical calculations. You ma use the following epessions

More information

2013 Checkpoints Chapter 6 CIRCULAR MOTION

2013 Checkpoints Chapter 6 CIRCULAR MOTION 013 Checkpoints Chapte 6 CIRCULAR MOTIO Question 09 In unifom cicula motion, thee is a net foce acting adially inwads. This net foce causes the elocity to change (in diection). Since the speed is constant,

More information

PHYS 1114, Lecture 21, March 6 Contents:

PHYS 1114, Lecture 21, March 6 Contents: PHYS 1114, Lectue 21, Mach 6 Contents: 1 This class is o cially cancelled, being eplaced by the common exam Tuesday, Mach 7, 5:30 PM. A eview and Q&A session is scheduled instead duing class time. 2 Exam

More information

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.

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. Chapte 5 Fiction When an object is in motion it is usually in contact with a viscous mateial (wate o ai) o some othe suface. So fa, we have assumed that moving objects don t inteact with thei suoundings

More information

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

) 1.510 11 m. ( )( 1.99 10 30 kg) Exaple 1: a.) What i the foce of gaity between a gazelle with a a of 100 kg and a lion with a a that i 50 kg if the lion i lying in wait 100 ete fo the gazelle? b.) What would happen to the foce of gaity

More information

Chapter 5: Uniform Circular Motion

Chapter 5: Uniform Circular Motion Chapte 5: Unifom Cicula Motion Motion at constant speed in a cicle Centipetal acceleation Banked cuves Obital motion Weightlessness, atificial gavity Vetical cicula motion Centipetal Foce Acceleation towad

More information

b) (5) What average force magnitude was applied by the students working together?

b) (5) What average force magnitude was applied by the students working together? Geneal Physics I Exam 3 - Chs. 7,8,9 - Momentum, Rotation, Equilibium Nov. 3, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults

More information

Physics 2001 Problem Set 5 Solutions

Physics 2001 Problem Set 5 Solutions Physics 2001 Poblem Set 5 Solutions Jeff Kissel Octobe 16, 2006 1. A puck attached to a sting undegoes cicula motion on an ai table. If the sting beaks at the point indicated in the figue, which path (A,

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights

More information

Physics 181. Assignment 4

Physics 181. Assignment 4 Physics 181 Assignment 4 Solutions 1. A sphee has within it a gavitational field given by g = g, whee g is constant and is the position vecto of the field point elative to the cente of the sphee. This

More information

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

AP Physics 1 - Circular Motion and Gravitation Practice Test (Multiple Choice Section) Answer Section AP Physics 1 - Cicula Motion and Gaitation Pactice est (Multiple Choice Section) Answe Section MULIPLE CHOICE 1. B he centipetal foce must be fiction since, lacking any fiction, the coin would slip off.

More information

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

Quiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible) Name: Class: Date: ID: A Quiz 6--Wok, Gavitation, Cicula Motion, Toque. (60 pts available, 50 points possible) Multiple Choice, 2 point each Identify the choice that best completes the statement o answes

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion constant speed Pick a point in the objects motion... What diection is the velocity? HINT Think about what diection the object would tavel if the sting wee cut Unifom Cicula Motion

More information

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

Chapter 5. Uniform Circular Motion. a c =v 2 /r Chapte 5 Unifom Cicula Motion a c =v 2 / Unifom cicula motion: Motion in a cicula path with constant speed s v 1) Speed and peiod Peiod, T: time fo one evolution Speed is elated to peiod: Path fo one evolution:

More information

Physics 201, Lecture 6

Physics 201, Lecture 6 Physics 201, Lectue 6 Today s Topics q Unifom Cicula Motion (Section 4.4, 4.5) n Cicula Motion n Centipetal Acceleation n Tangential and Centipetal Acceleation q Relatie Motion and Refeence Fame (Sec.

More information

Chap13. Universal Gravitation

Chap13. Universal Gravitation Chap13. Uniesal Gaitation Leel : AP Physics Instucto : Kim 13.1 Newton s Law of Uniesal Gaitation - Fomula fo Newton s Law of Gaitation F g = G m 1m 2 2 F21 m1 F12 12 m2 - m 1, m 2 is the mass of the object,

More information

3.2 Centripetal Acceleration

3.2 Centripetal Acceleration unifom cicula motion the motion of an object with onstant speed along a cicula path of constant adius 3.2 Centipetal Acceleation The hamme thow is a tack-and-field event in which an athlete thows a hamme

More information

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

ΣF = r r v. Question 213. Checkpoints Chapter 6 CIRCULAR MOTION Unit 3 Physics 16 6. Cicula Motion Page 1 of 9 Checkpoints Chapte 6 CIRCULAR MOTION Question 13 Question 8 In unifom cicula motion, thee is a net foce acting adially inwads. This net foce causes the elocity

More information

AE 245 homework #9 solutions

AE 245 homework #9 solutions AE 245 homewok #9 olution Tim Smith 13 Apil 2000 1 Poblem1 In the Apollo miion fom the Eath to the Moon, the Satun thid tage povided the tan-luna inetion bun that tanfeed the Apollo pacecaft fom a low

More information

Physics 110. Exam #1. September 30, 2016

Physics 110. Exam #1. September 30, 2016 Phyic 110 Exa #1 Septebe 30, 016 Nae Pleae ead and follow thee intuction caefully: Read all poble caefully befoe attepting to olve the. You wok ut be legible, and the oganization clea. You ut how all wok,

More information

Chap 5. Circular Motion: Gravitation

Chap 5. Circular Motion: Gravitation Chap 5. Cicula Motion: Gavitation Sec. 5.1 - Unifom Cicula Motion A body moves in unifom cicula motion, if the magnitude of the velocity vecto is constant and the diection changes at evey point and is

More information

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

Example 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example 014-11-18 Centipetal Aeleation 13 Exaple with full olution Exaple 1 A 1500 kg a i oing on a flat oad and negotiate a ue whoe adiu i 35. If the oeffiient of tati fition between the tie and the oad i 0.5,

More information

Physics 207 Lecture 5. Lecture 5

Physics 207 Lecture 5. Lecture 5 Lectue 5 Goals: Addess sstems with multiple acceleations in 2- dimensions (including linea, pojectile and cicula motion) Discen diffeent efeence fames and undestand how the elate to paticle motion in stationa

More information

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4. ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae

More information

Objective Notes Summary

Objective Notes Summary Objective Notes Summay An object moving in unifom cicula motion has constant speed but not constant velocity because the diection is changing. The velocity vecto in tangent to the cicle, the acceleation

More information

Last time RC circuits. Exam 2 is Tuesday Oct. 27 5:30-7 pm, Birge 145. Magnetic force on charged particle. Magnetic force on electric charges

Last time RC circuits. Exam 2 is Tuesday Oct. 27 5:30-7 pm, Birge 145. Magnetic force on charged particle. Magnetic force on electric charges Eam is Tuesda Oct. 7 5:0-7 pm, ige 45 Last time RC cicuits Students w / scheduled academic conflict please sta afte class TODAY to aange altenate time. Coes: all mateial since eam ook sections: Chap 7,

More information

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

rt () is constant. We know how to find the length of the radius vector by r( t) r( t) r( t) Cicula Motion Fom ancient times cicula tajectoies hae occupied a special place in ou model of the Uniese. Although these obits hae been eplaced by the moe geneal elliptical geomety, cicula motion is still

More information

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion Reading Assignment: Lab #9: The Kinematics & Dynamics of Cicula Motion & Rotational Motion Chapte 6 Section 4 Chapte 11 Section 1 though Section 5 Intoduction: When discussing motion, it is impotant to

More information

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

Thomas Whitham Sixth Form Mechanics in Mathematics. Rectilinear Motion Dynamics of a particle Projectiles Vectors Circular motion Thomas Whitham Sith om Mechanics in Mathematics Unit M Rectilinea Motion Dynamics of a paticle Pojectiles Vectos Cicula motion . Rectilinea Motion omation and solution of simple diffeential equations in

More information

MAGNETIC FIELD INTRODUCTION

MAGNETIC FIELD INTRODUCTION MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),

More information

Kinematics in 2-D (II)

Kinematics in 2-D (II) Kinematics in 2-D (II) Unifom cicula motion Tangential and adial components of Relative velocity and acceleation a Seway and Jewett 4.4 to 4.6 Pactice Poblems: Chapte 4, Objective Questions 5, 11 Chapte

More information

PHYS Summer Professor Caillault Homework Solutions. Chapter 5

PHYS Summer Professor Caillault Homework Solutions. Chapter 5 PHYS 1111 - Summe 2007 - Pofesso Caillault Homewok Solutions Chapte 5 7. Pictue the Poblem: The ball is acceleated hoizontally fom est to 98 mi/h ove a distance of 1.7 m. Stategy: Use equation 2-12 to

More information

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

Circular-Rotational Motion Mock Exam. Instructions: (92 points) Answer the following questions. SHOW ALL OF YOUR WORK. AP Physics C Sping, 2017 Cicula-Rotational Motion Mock Exam Name: Answe Key M. Leonad Instuctions: (92 points) Answe the following questions. SHOW ALL OF YOUR WORK. ( ) 1. A stuntman dives a motocycle

More information

Phys 201A. Homework 5 Solutions

Phys 201A. Homework 5 Solutions Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by

More information

= v 2. a c. = G m m 1 2. F g G = Review 5: Gravitation and Two-Dimensional Motion

= v 2. a c. = G m m 1 2. F g G = Review 5: Gravitation and Two-Dimensional Motion Review 5: Gavitation and Two-Dimensional Motion Review 5 Gavitation and Two-Dimensional Motion 2 d = 1 2 at F = ma 1. A busy waitess slides a plate of apple pie alon a counte to a huny custome sittin nea

More information

SAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b,

SAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b, SAMPLE QUIZ 3 - PHYSICS 1301.1 his is a closed book, closed notes quiz. Calculatos ae pemitted. he ONLY fomulas that may be used ae those given below. Define all symbols and justify all mathematical expessions

More information

NEETIIT.COM. Angular Displacement. Page - 1

NEETIIT.COM. Angular Displacement. Page - 1 - Download ou andoid App. 1. ANGULA DISPLACEMENT Intoduction : Angle subtended by position ecto of a paticle moing along any abitay path w..t. some fixed point is called angula displacement. (a) Paticle

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Have you eve idden on the amusement pak ide shown below? As it spins you feel as though you ae being pessed tightly against the wall. The ide then begins to tilt but you emain glued

More information

Kepler's 1 st Law by Newton

Kepler's 1 st Law by Newton Astonom 10 Section 1 MWF 1500-1550 134 Astonom Building This Class (Lectue 7): Gavitation Net Class: Theo of Planeta Motion HW # Due Fida! Missed nd planetaium date. (onl 5 left), including tonight Stadial

More information

FI 2201 Electromagnetism

FI 2201 Electromagnetism FI Electomagnetim Aleande A. Ikanda, Ph.D. Phyic of Magnetim and Photonic Reeach Goup ecto Analyi CURILINEAR COORDINAES, DIRAC DELA FUNCION AND HEORY OF ECOR FIELDS Cuvilinea Coodinate Sytem Cateian coodinate:

More information

Math Section 4.2 Radians, Arc Length, and Area of a Sector

Math Section 4.2 Radians, Arc Length, and Area of a Sector Math 1330 - Section 4. Radians, Ac Length, and Aea of a Secto The wod tigonomety comes fom two Geek oots, tigonon, meaning having thee sides, and mete, meaning measue. We have aleady defined the six basic

More information

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi

ENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi ENGI 44 Non-Catesian Coodinates Page 7-7. Conesions between Coodinate Systems In geneal, the conesion of a ecto F F xi Fy j Fzk fom Catesian coodinates x, y, z to anothe othonomal coodinate system u,,

More information

Cartesian Coordinate System and Vectors

Cartesian Coordinate System and Vectors Catesian Coodinate System and Vectos Coodinate System Coodinate system: used to descibe the position of a point in space and consists of 1. An oigin as the efeence point 2. A set of coodinate axes with

More information

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn Chapte 6 16. (a) In this situation, we take f s to point uphill and to be equal to its maximum value, in which case f s, max = μsf applies, whee μ s = 0.5. pplying ewton s second law to the block of mass

More information

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion AH Mechanics Checklist (Unit ) AH Mechanics Checklist (Unit ) Cicula Motion No. kill Done 1 Know that cicula motion efes to motion in a cicle of constant adius Know that cicula motion is conveniently descibed

More information