Can a watch-sized electromagnet deflect a bullet? (from James Bond movie)

Size: px
Start display at page:

Download "Can a watch-sized electromagnet deflect a bullet? (from James Bond movie)"

Transcription

1 Can a peon be blown away by a bullet? et' ay a bullet of a 0.06 k i ovin at a velocity of 300 /. And let' alo ay that it ebed itelf inide a peon. Could thi peon be thut back at hih peed (i.e. blown away)? To olve thi aue the a of the peon i, ay, 70 k. Apply conevation of linea oentu to the bullet and peon, between the point jut befoe the bullet tike the peon, and afte it ebed inide the peon (o that bullet + peon both have the ae final velocity). We have, 0.06(300) +70(0) = ( )V whee V i the velocity of the bullet + peon afte the bullet ebed in the peon. Solve fo V = 0.6 /. Thi peed i fa too low to caue the peon to be "blown away". Can a watch-ized electoanet deflect a bullet? (fo Jae Bond ovie) To analyze thi let' ay a bullet flie pat a watch a hown in the fiue below, with dienion a hown. bullet anet V l F d V h Fo exaple, let' ay the bullet ove at Vh = 300 / and we wih to deflect it a inificant aount o that it ie it ak copletely. f the intended taet of the bullet i the one weain the anetic watch then the bullet would have to deflect a eat deal to avoid hittin the taet. So let' eaonably ay the bullet would have to be deflected by an anle of 45. Thi ean that the lateal peed of the bullet (Vl) would be equal to the hoizontal bullet peed (Vh). So Vl = 300 /. Befoe the bullet pae by the watch, it lateal peed i zeo. A it pae by the watch the lateal bullet peed would have to be inceaed to 300 /. Thi ean that the anetic foce of attaction F between bullet and watch would have to be vey lae in ode to caue uch a apid lateal peed inceae in the hot tie peiod it take the bullet to pa by the watch. To

2 axiize the anetic foce the bullet would have to pa a cloe a poible to the watch, o d would have to be a all a poible. f we uppoe the watch i =.5 c in diaete, then it take the bullet 0.05/300 = 8.33x0-5 econd to pa by the watch. et' alo uppoe the a of the bullet i 0.06 k. To olve fo the foce F we can ue the ipule and oentu equation: Ft = v v, whee F i the aveae lateal foce pullin on the bullet duin the bullet pa, t i the tie duation of the pa, i the a of the bullet, v i the lateal bullet peed befoe the pa, and v i the lateal bullet peed afte the pa. Uin the vaiable iven peviouly, we have F(8.33x0-5 ) = 0.06(300) 0.06(0). Solvin fo F we et F = 6,000 N. Thi i equal to ton! Clealy a watch ized anet cannot even coe cloe to ufficiently deflectin a bullet. Note that a anetic foce vaie with the invee cube of the ditance fo the anet. Thi ean that the anetic foce F can only be hih when the bullet i in vey cloe poxiity to the watch. Thi poxiity equieent i appoxiately odeled by auin that the anetic foce F i only actin on the bullet while it pae ove the watch. n eality the anetic foce would alo be actin on the bullet while it i oe ditance away fo the watch, but in the calculation we aue that the foce i only actin on the bullet a it pae ove the watch, which i a eaonably ood appoxiation. Could a kydive whoe paachute failed to open hit a playound eeaw and end a all il flyin even toie hih, and he could till uvive? We hall aue a conevative cae whee the kydive doe not ebound off the eeaw and intead "tick" to it iht afte ipact. We can apply conevation of anula oentu to analyze thi poble between tae () and () a hown in the fiue below, with vaiable hown. The lae ball on the iht epeent the kydive. The alle ball on the left epeent the il. The anle i all, which i a ood appoxiation fo the typical eeaw.

3 JUST BEFORE MACT V () JUST AFTER MACT V () V w Apply the conevation of anula oentu equation about point, between tae () and () V Whee: V V w i the a of the kydive i the a of the il V i the velocity of the kydive jut befoe he ipact the eeaw V i the velocity of the kydive (and il) jut afte the kydive ipact the eeaw 3

4 i the ditance fo the pivot point to the end of the eeaw whee the kydive and il ae located i the otational inetia of the eeaw about point, which coincide with the cente of a of the eeaw (by auption) w i the anula velocity of the eeaw jut afte ipact Now, w = V/ fo the eoety. The above equation then becoe V V V ( V / ) Solve fo V. V V / A a eaonable appoxiation teat the eeaw a a lende od, whee () 3 whee i the a of the eeaw. t follow that V V 3 Suppoe we have V = 0 ph (appoxiate teinal peed of kydive), = 80 k, = 30 k, and = 00 k. Then fo the above equation we have V = 67 ph. The fiue below how the takeoff point of the il. Thi i tae (3). 4

5 V 3 takeoff V 3 (3) At takeoff, the il leave the eeaw at V3 = V (appoxiately). Thee i vey little tie fo the velocity of the il on the eeaw to chane beyond V iven the hih V velocity afte ipact (which quickly otate the eeaw). Thi eult in a neliible velocity chane fo the il, between the tie the ipact occu and when the il take off. Since we ae conidein a conevative cae (tickin upon ipact) then V3 i the inial takeoff velocity of the il. Now, 67 ph = 30 /, which eult in a peak heiht eached of 46 ete, auin neliible ai eitance and the il flyin taiht up (a ood appoxiation iven a all anle ). Thi heiht i uch eate than even toie o the yth i indeed poible. Howeve, unle he land oewhee oft he i unlikely to uvive the fall. Thi i in addition to the udden upwad acceleation, at takeoff, which can fatally injue he a well 5

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12

LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12 CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental

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 1401 Homework Solutions - Walker, Chapter 9

( ) Physics 1401 Homework Solutions - Walker, Chapter 9 Phyic 40 Conceptual Quetion CQ No Fo exaple, ey likely thee will be oe peanent deoation o the ca In thi cae, oe o the kinetic enegy that the two ca had beoe the colliion goe into wok that each ca doe on

More information

SOLUTIONS TO CONCEPTS CHAPTER 12

SOLUTIONS TO CONCEPTS CHAPTER 12 SOLUTONS TO CONCEPTS CHPTE. Given, 0c. t t 0, 5 c. T 6 sec. So, w sec T 6 t, t 0, 5 c. So, 5 0 sin (w 0 + ) 0 sin Sin / 6 [y sin wt] Equation of displaceent (0c) sin (ii) t t 4 second 8 0 sin 4 0 sin 6

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

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

Universal Gravitation

Universal Gravitation Add Ipotant Univeal Gavitation Pae: 7 Note/Cue Hee Unit: Dynaic (oce & Gavitation Univeal Gavitation Unit: Dynaic (oce & Gavitation NGSS Standad: HS-PS-4 MA Cuiculu aewok (00:.7 AP Phyic Leanin Objective:.B..,.B..,

More information

Perhaps the greatest success of his theory of gravity was to successfully explain the motion of the heavens planets, moons, &tc.

Perhaps the greatest success of his theory of gravity was to successfully explain the motion of the heavens planets, moons, &tc. AP Phyic Gavity Si Iaac Newton i cedited with the dicovey of gavity. Now, of coue we know that he didn t eally dicove the thing let face it, people knew about gavity fo a long a thee have been people.

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

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

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

r dt dt Momentum (specifically Linear Momentum) defined r r so r r note: momentum is a vector p x , p y = mv x = mv y , p z = mv z

r dt dt Momentum (specifically Linear Momentum) defined r r so r r note: momentum is a vector p x , p y = mv x = mv y , p z = mv z Moentu, Ipulse and Collisions Moentu eeyday connotations? physical eaning the tue easue of otion (what changes in esponse to applied foces) d d ΣF ( ) dt dt Moentu (specifically Linea Moentu) defined p

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

3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard

3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honors Physics Impulse-Momentum Theorem. Name: Answer Key Mr. Leonard 3pt3pt 3pt3pt0pt 1.5pt3pt3pt Honor Phyic Impule-Momentum Theorem Spring, 2017 Intruction: Complete the following workheet. Show all of you work. Name: Anwer Key Mr. Leonard 1. A 0.500 kg ball i dropped

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

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

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

Momentum and the Flow of Mass Challenge Problems Solutions

Momentum and the Flow of Mass Challenge Problems Solutions Poblem 1: Steam Bouncing off Wall Momentum and the Flow of Ma Challenge Poblem Solution A team of paticle of ma m and epaation d hit a pependicula uface with peed v. The team ebound along the oiginal line

More information

AP Physics Momentum AP Wrapup

AP Physics Momentum AP Wrapup AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol

More 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

1121 T Question 1

1121 T Question 1 1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed

More information

Homework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x

Homework Set 4 Physics 319 Classical Mechanics. m m k. x, x, x, x T U x x x x l 2. x x x x. x x x x Poble 78 a) The agangian i Hoewok Set 4 Phyic 319 Claical Mechanic k b) In te of the cente of a cooinate an x x1 x x1 x xc x x x x x1 xc x xc x x x x x1 xc x xc x, x, x, x T U x x x x l 1 1 1 1 1 1 1 1

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

Spring 2002 Test 2 Solutions. Problem 1 (Short Answer: 15 points)

Spring 2002 Test 2 Solutions. Problem 1 (Short Answer: 15 points) Spin 2002 Test 2 Solutions Poble 1 (Shot Answe: 15 points) A sled on ice oves in the was descibed in questions 1-7 below. Fiction is so sall that it can be inoed. A peson weain spiked shoes standin on

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

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

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

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided

More information

Momentum. Momentum. Impulse. Impulse Momentum Theorem. Deriving Impulse. v a t. Momentum and Impulse. Impulse. v t

Momentum. Momentum. Impulse. Impulse Momentum Theorem. Deriving Impulse. v a t. Momentum and Impulse. Impulse. v t Moentu and Iule Moentu Moentu i what Newton called the quantity of otion of an object. lo called Ma in otion The unit for oentu are: = oentu = a = elocity kg Moentu Moentu i affected by a and elocity eeding

More information

Second Law of Motion. Force mass. Increasing mass. (Neglect air resistance in this example)

Second Law of Motion. Force mass. Increasing mass. (Neglect air resistance in this example) Newton Law of Motion Moentu and Energy Chapter -3 Second Law of Motion The acceleration of an object i directly proportional to the net force acting on the object, i in the direction of the net force,

More 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

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003 avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive

More information

5.5. Collisions in Two Dimensions: Glancing Collisions. Components of momentum. Mini Investigation

5.5. Collisions in Two Dimensions: Glancing Collisions. Components of momentum. Mini Investigation Colliion in Two Dienion: Glancing Colliion So ar, you have read aout colliion in one dienion. In thi ection, you will exaine colliion in two dienion. In Figure, the player i lining up the hot o that the

More information

Lecture 23: Central Force Motion

Lecture 23: Central Force Motion Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces

More information

SPH4U Magnetism Test Name: Solutions

SPH4U Magnetism Test Name: Solutions SPH4U Magneti et Nae: Solution QUESION 1 [4 Mak] hi and the following two quetion petain to the diaga below howing two cuent-caying wie. wo cuent ae flowing in the ae diection (out of the page) a hown.

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

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle

LINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle LINEAR MOMENTUM Physical quantities that we have been using to chaacteize the otion of a paticle v Mass Velocity v Kinetic enegy v F Mechanical enegy + U Linea oentu of a paticle (1) is a vecto! Siple

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

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr Flipping Phyic Lecture Note: Introduction to Acceleration with Priu Brake Slaing Exaple Proble a Δv a Δv v f v i & a t f t i Acceleration: & flip the guy and ultiply! Acceleration, jut like Diplaceent

More information

5.4 Conservation of Momentum in Two Dimensions

5.4 Conservation of Momentum in Two Dimensions Phyic Tool bo 5.4 Coneration of Moentu in Two Dienion Law of coneration of Moentu The total oentu before a colliion i equal to the total oentu after a colliion. Thi i written a Tinitial Tfinal If the net

More information

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts.

Then the number of elements of S of weight n is exactly the number of compositions of n into k parts. Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to

More information

Conservation of Energy

Conservation of Energy Add Iportant Conervation of Energy Page: 340 Note/Cue Here NGSS Standard: HS-PS3- Conervation of Energy MA Curriculu Fraework (006):.,.,.3 AP Phyic Learning Objective: 3.E.., 3.E.., 3.E..3, 3.E..4, 4.C..,

More information

Practice Midterm #1 Solutions. Physics 6A

Practice Midterm #1 Solutions. Physics 6A Practice Midter # Solution Phyic 6A . You drie your car at a peed of 4 k/ for hour, then low down to k/ for the next k. How far did you drie, and what wa your aerage peed? We can draw a iple diagra with

More information

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

r ˆr F = Section 2: Newton s Law of Gravitation m 2 m 1 Consider two masses and, separated by distance Gravitational force on due to is

r ˆr F = Section 2: Newton s Law of Gravitation m 2 m 1 Consider two masses and, separated by distance Gravitational force on due to is Section : Newton s Law of Gavitation In 1686 Isaac Newton published his Univesal Law of Gavitation. This explained avity as a foce of attaction between all atte in the Univese, causin e.. apples to fall

More information

4 Conservation of Momentum

4 Conservation of Momentum hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding

More information

Lab 10: Newton s Second Law in Rotation

Lab 10: Newton s Second Law in Rotation Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have

More information

CHAPTER 5: Circular Motion; Gravitation

CHAPTER 5: Circular Motion; Gravitation CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal

More information

1131 T Question 1

1131 T Question 1 1131 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, taelling on the sae path in the sae diection as you, at a constant speed

More information

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection

More information

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin technical proof TP A.30 The effect of cue tip offet, cue weight, and cue peed on cue all peed and pin technical proof upporting: The Illutrated Principle of Pool and Billiard http://illiard.colotate.edu

More information

Physics 30 Lesson 3 Impulse and Change in Momentum

Physics 30 Lesson 3 Impulse and Change in Momentum Phyic 30 Leon 3 Ipule and Change in Moentu I. Ipule and change in oentu According to Newton nd Law of Motion (Phyic Principle 1 on the Data Sheet), to change the otion (i.e. oentu) of an object an unbalanced

More information

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) = 8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt

More information

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4.

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4. Chapter 5 Newton Law Practice Proble Solution Student Textbook page 163 1. Frae the Proble - Draw a free body diagra of the proble. - The downward force of gravity i balanced by the upward noral force.

More information

How can you find the dimensions of a square or a circle when you are given its area? When you multiply a number by itself, you square the number.

How can you find the dimensions of a square or a circle when you are given its area? When you multiply a number by itself, you square the number. 7. Finding Squae Root How can you find the dimenion of a quae o a cicle when you ae given it aea? When you multiply a numbe by itelf, you quae the numbe. Symbol fo quaing i the exponent. = = 6 quaed i

More information

What is the length of the pendulum? Period = T = 12.0 s

What is the length of the pendulum? Period = T = 12.0 s Eaple: hen visitin an office buildin you notice that it has an atiu with an enoous pendulu with one end attached to the oof of the buildin and the othe end nealy eachin the floo. You obseve that the pendulu

More information

Orbital Angular Momentum Eigenfunctions

Orbital Angular Momentum Eigenfunctions Obital Angula Moentu Eigenfunctions Michael Fowle 1/11/08 Intoduction In the last lectue we established that the opeatos J Jz have a coon set of eigenkets j J j = j( j+ 1 ) j Jz j = j whee j ae integes

More information

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115;

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115; WEEK-3 Recitation PHYS 3 eb 4, 09 Ch. 4: OC 9, 3,, 8. Pobles 0, 4, 38, 48, 77, 83 & 5; Ch. 4: OC Questions 9, 3,, 8. 9. (e) Newton s law of gavitation gives the answe diectl. ccoding to this law the weight

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

Related Rates section 3.9

Related Rates section 3.9 Related Rate ection 3.9 Iportant Note: In olving the related rate proble, the rate of change of a quantity i given and the rate of change of another quantity i aked for. You need to find a relationhip

More information

Estimation and Confidence Intervals: Additional Topics

Estimation and Confidence Intervals: Additional Topics Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:

More information

Physics 20 Lesson 16 Friction

Physics 20 Lesson 16 Friction Phyic 0 Leon 16 riction In the previou leon we learned that a rictional orce i any orce that reit, retard or ipede the otion o an object. In thi leon we will dicu how riction reult ro the contact between

More information

Lecture 52. Dynamics - Variable Acceleration

Lecture 52. Dynamics - Variable Acceleration Dynamics - Vaiable Acceleation Lectue 5 Example. The acceleation due to avity at a point outside the eath is invesely popotional to the squae of the distance x fom the cente, i.e., ẍ = k x. Nelectin ai

More information

AP CHEM WKST KEY: Atomic Structure Unit Review p. 1

AP CHEM WKST KEY: Atomic Structure Unit Review p. 1 AP CHEM WKST KEY: Atoic Structure Unit Review p. 1 1) a) ΔE = 2.178 x 10 18 J 1 2 nf 1 n 2i = 2.178 x 10 18 1 1 J 2 2 6 2 = 4.840 x 10 19 J b) E = λ hc λ = E hc = (6.626 x 10 34 J )(2.9979 x 10 4.840 x

More information

15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object.

15 N 5 N. Chapter 4 Forces and Newton s Laws of Motion. The net force on an object is the vector sum of all forces acting on that object. Chapter 4 orce and ewton Law of Motion Goal for Chapter 4 to undertand what i force to tudy and apply ewton irt Law to tudy and apply the concept of a and acceleration a coponent of ewton Second Law to

More information

Tidal forces. m r. m 1 m 2. x r 2. r 1

Tidal forces. m r. m 1 m 2. x r 2. r 1 Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.

More information

Physics 6A. Practice Final (Fall 2009) solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6A. Practice Final (Fall 2009) solutions. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic 6A Practice inal (all 009) olution or Capu Learning Aitance Service at UCSB . A locootive engine of a M i attached to 5 train car, each of a M. The engine produce a contant force that ove the train

More information

THE BICYCLE RACE ALBERT SCHUELLER

THE BICYCLE RACE ALBERT SCHUELLER THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The

More 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

Name: Answer Key Date: Regents Physics. Energy

Name: Answer Key Date: Regents Physics. Energy Nae: Anwer Key Date: Regent Phyic Tet # 9 Review Energy 1. Ue GUESS ethod and indicate all vector direction.. Ter to know: work, power, energy, conervation of energy, work-energy theore, elatic potential

More 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

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 C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet Linea and angula analogs Linea Rotation x position x displacement v velocity a T tangential acceleation Vectos in otational motion Use the ight hand ule to detemine diection of the vecto! Don t foget centipetal

More information

PHY 171 Practice Test 3 Solutions Fall 2013

PHY 171 Practice Test 3 Solutions Fall 2013 PHY 171 Practice et 3 Solution Fall 013 Q1: [4] In a rare eparatene, And a peculiar quietne, hing One and hing wo Lie at ret, relative to the ground And their wacky hairdo. If hing One freeze in Oxford,

More information

Formula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m.

Formula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m. A Lit of foulae fo ecanical engineeing pinciple Foula Foula ybol Unit Ste Stain applied foce co ectionalaea cange in lengt oiginal lengt F A e x L Young odulu of elaticity te tain Stiffne foce extenion

More information

PHYSICS: MIDTERM MATHEMATICAL MODELS NAME: TYPE OF PHYSICAL QUANTITY Distance d m - How far an object is located from the origin.

PHYSICS: MIDTERM MATHEMATICAL MODELS NAME: TYPE OF PHYSICAL QUANTITY Distance d m - How far an object is located from the origin. HYSCS: MDTERM MATHEMATCAL MODELS NAME: CHATER NTRODUCTON TO HYSCS HYSCAL QUANTTY SYMBOL UNTS MATH MODEL DEFNTON TYE OF HYSCAL QUANTTY Ditance - How fa an object i locate fo the oiin. Scala oition x o -

More information

3-7 FLUIDS IN RIGID-BODY MOTION

3-7 FLUIDS IN RIGID-BODY MOTION 3-7 FLUIDS IN IGID-BODY MOTION S-1 3-7 FLUIDS IN IGID-BODY MOTION We ae almost eady to bein studyin fluids in motion (statin in Chapte 4), but fist thee is one cateoy of fluid motion that can be studied

More information

Physics Exam 3 Formulas

Physics Exam 3 Formulas Phyic 10411 Exam III November 20, 2009 INSTRUCTIONS: Write your NAME on the front of the blue exam booklet. The exam i cloed book, and you may have only pen/pencil and a calculator (no tored equation or

More information

Sir Isaac Newton. 1. Calculate the gravitational force on an object in a gravitational

Sir Isaac Newton. 1. Calculate the gravitational force on an object in a gravitational Chapte 8: Gavity I can calculate the otion of heavenly bodies, but not the adness of people. Si Isaac Newton Objectives 1. Calculate the avitational foce on an object in a avitational field.. Utilize Newton

More information

FARADAY'S LAW dt

FARADAY'S LAW dt FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,

More information

Solution to Theoretical Question 1. A Swing with a Falling Weight. (A1) (b) Relative to O, Q moves on a circle of radius R with angular velocity θ, so

Solution to Theoretical Question 1. A Swing with a Falling Weight. (A1) (b) Relative to O, Q moves on a circle of radius R with angular velocity θ, so Solution to Theoretical uetion art Swing with a Falling Weight (a Since the length of the tring Hence we have i contant, it rate of change ut be zero 0 ( (b elative to, ove on a circle of radiu with angular

More information

PHYS Summer Professor Caillault Homework Solutions. Chapter 9

PHYS Summer Professor Caillault Homework Solutions. Chapter 9 PHYS - Summe 007 - Pofesso Caillault Homewok Solutions Chapte 9 3. Pictue the Poblem The owne walks slowly towad the notheast while the cat uns eastwad and the dog uns nothwad. Stategy Sum the momenta

More information

Lecture 13. Rotational motion Moment of inertia

Lecture 13. Rotational motion Moment of inertia Lectue 13 Rotational motion Moment of inetia EXAM 2 Tuesday Mach 6, 2018 8:15 PM 9:45 PM Today s Topics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics

More information

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018 Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining

More information

Lecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell

Lecture 15 - Current. A Puzzle... Advanced Section: Image Charge for Spheres. Image Charge for a Grounded Spherical Shell Lecture 15 - Current Puzzle... Suppoe an infinite grounded conducting plane lie at z = 0. charge q i located at a height h above the conducting plane. Show in three different way that the potential below

More information

Physics 6A. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6A. Angular Momentum. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Phyic 6A Angular Momentum For Campu earning Angular Momentum Thi i the rotational equivalent of linear momentum. t quantifie the momentum of a rotating object, or ytem of object. f we imply tranlate the

More information

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2. Chapte answes Heineann Physics 1 4e Section.1 Woked exaple: Ty youself.1.1 CALCULATING APPARENT WEIGHT A 79.0 kg student ides a lift down fo the top floo of an office block to the gound. Duing the jouney

More information

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

V V The circumflex (^) tells us this is a unit vector Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude

More information

Constant Force: Projectile Motion

Constant Force: Projectile Motion Contant Force: Projectile Motion Abtract In thi lab, you will launch an object with a pecific initial velocity (magnitude and direction) and determine the angle at which the range i a maximum. Other tak,

More information

Holt Physics Problem 3E

Holt Physics Problem 3E NAME DATE CLASS Holt Phyic Problem 3E PROJECTILES LAUNCHED AT AN ANGLE PROBLEM SOLUTION 1. DEFINE. PLAN A flying fih leap out of the water with a peed of 15.3. Normally thee fih ue winglike fin to glide

More information

Answer keys. EAS 1600 Lab 1 (Clicker) Math and Science Tune-up. Note: Students can receive partial credit for the graphs/dimensional analysis.

Answer keys. EAS 1600 Lab 1 (Clicker) Math and Science Tune-up. Note: Students can receive partial credit for the graphs/dimensional analysis. Anwer key EAS 1600 Lab 1 (Clicker) Math and Science Tune-up Note: Student can receive partial credit for the graph/dienional analyi. For quetion 1-7, atch the correct forula (fro the lit A-I below) to

More information

PHYSICS 211 MIDTERM II 12 May 2004

PHYSICS 211 MIDTERM II 12 May 2004 PHYSIS IDTER II ay 004 Exa i cloed boo, cloed note. Ue only your forula heet. Write all wor and anwer in exa boolet. The bac of page will not be graded unle you o requet on the front of the page. Show

More information

( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s.

( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s. THE VIBRATION ABSORBER Preable - A NEED arie: Lui San Andre (c) 8 MEEN 363-617 Conider the periodic forced repone of a yte (Kp-Mp) defined by : 1 1 5 lbf in : 1 3 lb (t) It natural frequency i: : ec F(t)

More information

Niraj Sir. circular motion;; SOLUTIONS TO CONCEPTS CHAPTER 7

Niraj Sir. circular motion;; SOLUTIONS TO CONCEPTS CHAPTER 7 SOLUIONS O CONCEPS CHAPE 7 cicula otion;;. Distance between Eath & Moon.85 0 5 k.85 0 8 7. days 4 600 (7.) sec.6 0 6 sec.4.85 0 v 6.6 0 8 05.4/sec v (05.4) a 0.007/sec.7 0 /sec 8.85 0. Diaete of eath 800k

More information

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving Physics 11 Chapte 3: Vectos and Motion in Two Dimensions The only thing in life that is achieved without effot is failue. Souce unknown "We ae what we epeatedly do. Excellence, theefoe, is not an act,

More information

Ch 11 Particulate suspensions

Ch 11 Particulate suspensions Ch 11 Paticulate upenion Iue Stability (dipeion) edientation igation wall lip Had phee Only igid epulion peent when paticle coe into contact Zeo hea vicoity ( 1+. φ) 5 1+.5φ + 6.φ d.5 ( φ) dφ exp( 5φ /

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

Sample Problems. Lecture Notes Related Rates page 1

Sample Problems. Lecture Notes Related Rates page 1 Lecture Note Related Rate page 1 Sample Problem 1. A city i of a circular hape. The area of the city i growing at a contant rate of mi y year). How fat i the radiu growing when it i exactly 15 mi? (quare

More information

SPH4U Unit 6.3 Gravitational Potential Energy Page 1 of 9

SPH4U Unit 6.3 Gravitational Potential Energy Page 1 of 9 SPH4 nit 6.3 Gavitational Potential negy Page of Notes Physics ool box he gavitational potential enegy of a syste of two (spheical) asses is diectly popotional to the poduct of thei asses, and invesely

More information

AP Physics with the Physics Kahuna: Gravity

AP Physics with the Physics Kahuna: Gravity AP Phyic with the Phyic Kahuna: Gavity Si Iaac Newton i cedited with the dicovey of gavity. Now, of coue we know that he didn t eally dicove the thing let face it, people knew about gavity fo a long a

More information