Physics Numericals. Subtopic wise numericals with solutions. Shortcuts to enable quick problem solving.

Size: px
Start display at page:

Download "Physics Numericals. Subtopic wise numericals with solutions. Shortcuts to enable quick problem solving."

Transcription

1 Physics Numeicals SD. XII Sci. Salient Featues Subtopic wise numeicals with solutions. Shotcuts to enable quick poblem soling. Pactice poblems fo eey subtopic. Includes soled boad numeicals. Numeical based multiple choice questions fo effectie pepaation. Solutions/hints to pactice poblems and multiple choice questions aailable in downloadable PDF fomat at Pinted at: Repo Knowledgecast Ltd., Mumbai aget Publications Pt. Ltd. No pat of this book may be epoduced o tansmitted in any fom o by any means, C.D. ROM/Audio Video Cassettes o electonic, mechanical including photocopying; ecoding o by any infomation stoage and etieal system without pemission in witing fom the Publishe. P.O. No _JUP

2 Peface In the case of good books, the point is not how many you can get though, but athe how many can get though to you. SD XII Sci.: PHYSICS NUMERICALS is a complete and thoough guide to the numeical aspect of the HSC pepaation. he book is pepaed as pe the Mahaashta State Boad syllabus.subtopic wise segegation of Soled Numeicals in each chapte help the student to gain knowledge of the boad spectum of poblems in each subtopic Fomulae which fom a ital pat of poblem-soling ae poided in eey chapte. Solutions and calculations hae been boken down to the simplest fom possible (with log calculation poided wheee needed) so that the student can tackle each and eey poblem with ease. Poblems fo pactice ae poided to test the igilance and aletness of the students and build thei confidence. Boad Numeicals till the latest yea hae been poided to help the student get accustomed to the diffeent standads of boad numeicals. Numeical based multiple choice questions ae coeed sub-topic-wise to pepae the student on a competitie leel. Solution/hints to pactice poblems and multiple choice questions can be downloaded in PDF fomat fom ou website www. tagetpublications.og he jouney to ceate a complete book is stewn with tiumphs, failues and nea misses. If you think we e nealy missed something o want to applaud us fo ou tiumphs, we d loe to hea fom you. Please wite to us on : mail@tagetpublications.og A book affects etenity; one can nee tell whee its influence stops. Yous faithfully Authos Edition: Second Best of luck to all the aspiants! Disclaime his book is intended to be study mateial expessing iews and elaboating concepts fo ease of undestanding fo students and puely fo thei benefits. We make no epesentations as to accuacy, completeness, coectness, suitability, o alidity of any infomation though this study mateial. And, shall not be held liable o esponsible fo any eos, omissions, o diffeences in this infomation o any losses, injuies o damages aising fom its use. All infomation is poided on as it is basis depending upon the undestanding of the autho and his/he elaboation of such concepts along with adoption and inspiation fom aious othe texts in elation to the topics as mentioned in this study mateial. It is the eade s esponsibility to eify thei own facts. hough this study mateial we ae only explaining and elaboating aious concepts as may be necessay fo the students in the pesent famewok and context. he iews and opinions expessed in this study mateial ae puely as pe the undestanding of the authos and do not necessaily eflect the official policy o position of any othe agency, oganization, employe o company. Assumptions made in this analysis ae not eflectie of the position of any othe than the authos - and since we ae citically thinking human beings with pesonified opinions, these iews ae always subject to change, eision and ethinking at any time. Please do not hold us to them in pepetuity. Reades shall not misconceie this wok with any othe wok. his wok is puely inspied upon the couse wok as suggested and pescibed by the Mahaashta State Boad of Seconday and Highe Seconday Education, Pune. All the facts and figues so stated hae been puely adopted fom aious eseach points puely fo the pupose of epesentation and explaining the students and eades at lage as a pat of fai dealing. By poducing anything and eeything in this book the autho does not intend to claim copyights on any such mateial but has been puely adopted and used fo the pupose of epesentation and fo bette undestanding of the students with a pue intention to educate the public at lage fo a bette India.

3 01 Cicula Motion Chapte 01: Cicula Motion Fomulae Section 1: Angula Displacement, Relation Between Linea Velocity and Angula Velocity 1. Angula elocity: i. = whee, = linea elocity = adius of the cicle along which paticle pefoms cicula motion. ii. = t whee, = angula displacement of the paticle in cicula motion duing time inteal t. iii. = n whee, n = fequency of eolution of paticle in cicula motion. i. = whee, = peiod of eolution of paticle pefoming cicula motion.. Angula displacement: = t 3. ime peiod: i. = ii. 4. Fequency of eolution: n = 1 = 5. Linea elocity: i. = ii. = n Section : Angula Acceleation 1. Angula acceleation: i. = t whee, = change in the angula elocity of a paticle in cicula motion duing a time inteal t. ii. n = t whee, n = change in fequency of the paticle in cicula motion duing a time inteal t. Section 3: Centipetal and angential Acceleation 1. Centipetal (o adial) acceleation: a = = =. angential acceleation: a = 3. Resultant o total acceleation: a = at a ata cos whee, = angle made by a with a t a = a a when = Fo U.C.M.: a = a = = a t = 0 t Section 4: Centipetal and Centifugal Foces 1. Centipetal foce: i. F c = ii. F c = iii. F c = m i. F c = 4 mn. 4 m F c = whee, m = mass of paticle pefoming cicula motion Section 5: Motion of a Vehicle along a Cued Unbanked Road 1. he necessay centipetal foce: F c = mg = whee, m = mass of ehicle = elocity of the ehicle = adius of the cue oad 1

4 Std. XII Sci.: Physics Numeicals = coefficient of fiction between the tyes of the ehicle and the suface of the oad.. he maximum elocity with which a ehicle can take a tun safely without skidding: = g 3. he maximum angula elocity with which a ehicle can take a tun safely without skidding: g = Section 6: Banking of Roads Fo motion of ehicles along a banked cue oad: 1. he pope elocity o optimum elocity: = g tan whee, = angle of banking. he maximum elocity without skidding: s tan max = g 1 s tan whee, s = coefficient of fiction between the tyes of the ehicle and suface of the oad 3. Angle of banking: = tan 1 o tan = g g 4. Height of inclined oad: h = d sin whee, d = distance between the two font o ea wheels. 5. he maximum elocity with which a ehicle can go on a banked cued oad without toppling: d = g H whee, H = height of cente of gaity (C.G.) of the ehicle fom the oad. Section 7: Conical Pendulum 1. Linea speed of bob: = g tan. Angula elocity: = g l cos 3. Peiodic time: = l cos = = g gtan = h g whee, l = length of conical pendulum h = the height of the fixed suppot fom the cente of the cicle o axial height of the cone = semietical angle of the cone. 4. ension in the sting: mg = cos Section 8: Vetical Cicula Motion 1. Velocity at any point in etical cicula motion: i. P = L g (1 cos) ii. L = 5g iii. H = g i. M = 3g whee, P = elocity of the paticle at any point P along the cicle. L = Minimum elocity at the lowest point on the cicle so that it can safely tael along the etical cicle (looping the loop). H = Minimum elocity of the paticle at the highest point on the cicle so that the sting will not be slackened. M = Minimum elocity of the paticle at a mid-way point so that it can tael along the cicle. = adius of the etical cicle. = angle between the position ectos at the gien position of paticle and that of the lowest point on the etical cicle.

5 Chapte 01: Cicula Motion. Relation between elocities at diffeent points in etical cicula motion: i. L = H + 4g ii. = + g M H 3. ension at: i. Any point P, P = + mg cos ii. Lowest point L, L = L + mg = H + 5mg iii. Highest point H, H = H mg = i. Midway point M, M = M = L 5 mg L mg 4. otal enegy at any point: E = 1 + mg (1 cos ) = 5 mg Section 9: Kinematical Equations Analogy between tanslatoy motion and cicula motion No. anslatoy Motion Cicula Motion 1. Linea elocity = d dt Angula elocity = d dt. Linea acceleation d d a= dt dt Angula acceleation d d = dt dt 3. Linea momentum p = m Angula momentum L = I 4. Linea impulse = F (t) = p Angula impulse = (t) = L 5. Foce F = m a oque = I 6. Wok W = F. Wok W =. 7. Kinetic enegy of tanslation E t = 1 Kinetic enegy of otation E = 1 I 8. Equations of linea motion Equations of otational motion i. = u + at i. = 1 + t ii. s = ut + 1 at ii. = 1 t + 1 t iii. u = as iii. 1 = i. s n = u + a (n 1) i. n = 1 + (n 1) 3

6 Std. XII Sci.: Physics Numeicals Shotcuts 1. Angula acceleation (): If numbe of otations o eolutions is gien, then = (n n 1 ) ad/s t. If linea elocity is gien, apply a = 4 and if angula elocity is gien, apply a = to find a. 3. If numbe of eolutions in a paticula time is gien, apply a = 4 n. 4. If some mass is placed on a otating body, then angula motion changes due to fictional foce between the mass and the body. Coefficient of fiction can be calculated by applying the fomula, = mg o = = g = 4 n g g 5. Beaking tension is the maximum centipetal foce which is gien by the elation, F = = m 6. Speed of a ehicle on a banked oad o cicula tun depends upon the cuatue of the oad. tan = g 7. o aoid skidding, g whee is the coefficient of fiction between the tyes and oad. d = h whee d is the distance between two wheels. 8. In case of conical pendulum if l be the length and be the adius of the hoizontal cicle then height of the igid point of suspension is calculated by the fomula, h = l 9. Use the expessions, L = 5g and = g fo the following cases: i. Bucket full of wate whiled in a etical cicle. ii. Moto cyclist iding in a etical cicle in hollow sphee. 10. Fo looping the loop of adius, the minimum height fom which the body should be eleased is gien by, h = i. Fo a ehicle moing oe a conex bidge which is in the shape of an ac of a cicle, N = mg ii. Fo the moto cyclist at the uppe most point in the globe of death in a cicus, N = mg whee, N = nomal eaction acting on the ehicle o the motocycle. Soled Examples Section 1: Angula Displacement, Relation Between Linea Velocity and Angula Velocity Example 1.1 A wheel of adius mete is making 60 eolutions pe minute. Calculate the angula elocity of any point on the im. Gien: n = 60.p.m. = 60/60 = 1 ps, = m o find: Angula elocity () Fomula: = n Calculation: Fom fomula, = 1 = ad/s Ans: he angula elocity of any point on the im of the wheel is ad/s. Example 1. Find the angula displacement of a paticle moing on a cicle with angula elocity (/3) ad/s in 15 s. Gien: t = 15 s, = (/3) ad/s o find: Angula displacement () Fomula: = t Calculation: Fom fomula, = 15 3 = 10 π ad Ans: he angula displacement of the paticle is 10 ad.

7 Chapte 01: Cicula Motion Example 1.3 What is the angula speed of the second hand of a clock? If the second hand is 10 cm long, then find the linea speed of its tip. Gien: = 10 cm = 10 1 m, = 60 s o find: i. Angula speed () ii. Linea speed () Fomulae: i. = ii. = Calculation: Fom fomula (i), = 3. = 6014 = ad/s Fom fomula (ii), = = = m/s. Ans: i. he angula speed of the second hand of a clock is ad/s. ii. he linea speed of the tip of the second hand is m/s. Example 1.4 If a body otates in a hoizontal cicle of adius 15 cm with an angula elocity of 0.8 ad/s, then what is its linea elocity? Gien: = 15 cm = 0.15 m, = 0.8 ad/s o find: Linea elocity () Fomula: = Calculation: Fom fomula, = = 0.1 m/s. Ans: he linea elocity of the otating body is 0.1 m/s. Example 1.5 he linea elocity of a body is 0. m/s. If it otates in a hoizontal cicle haing adius 0.5 m, what is its angula elocity? Gien: = 0.5 m, = 0. m/s o find: Angula elocity () Fomula: = Calculation: Fom fomula, = = = 0.4 ad/s Ans: he angula elocity of the otating body is 0.4 ad/s. Example 1.6 A paticle is eoling in a cicle of adius 10 cm with linea speed of 0 m/s. Find (i) its peiod of eolution and (ii) fequency. Gien: = 10 cm = m, = 0 m/s o find: i. Peiod of eolution () ii. Fomulae: i. = Fequency (n) ii. n = 1 Calculation: Fom fomula (i), = 0 = = s Fom fomula (ii), n = 1 = n = s 1 Ans: i. he peiod of eoling paticle is s ii. he fequency of the paticle is n = s 1. Example 1.7 What is the angula elocity of the minute hand of a clock? If the minute hand is 5 cm long, what is the linea elocity of its tip? [Oct 04] Gien: R = 5 cm = 5 10 m, = 1h = 3600 s o find: i. Angula elocity () ii. Linea elocity of the tip () Fomulae: i. = ii. = Calculation: Fom fomula (i), = 3.14 = 3600 = ad/s Fom fomula (ii), = = m/s Ans: Fo the minute hand of the clock, i. he angula elocity is ad/s. ii. he linea elocity of the tip is m/s. 5

Written as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.

Written as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune. Witten as pe e evised syllabus pescibed by e Mahaashta State oad of Seconday and Highe Seconday Education, Pune. Pecise Physics I SD. XII Sci. Salient Featues Concise coveage of syllabus in Question nswe

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

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

Shree Datta Coaching Classes, Contact No Circular Motion

Shree Datta Coaching Classes, Contact No Circular Motion Shee Datta Coaching Classes, Contact No. 93698036 Pof. Deepak Jawale Cicula Motion Definition : The motion of the paticle along the cicumfeence of a cicle is called as cicula motion. Eg. i) Motion of eath

More information

STD. XII Sci. Triumph Physics

STD. XII Sci. Triumph Physics Useful fo all Agicultual, Medical, Phamacy and Engineeing Entance Examinations held acoss India. SD. XII Sci. iumph Physics Based on Mahaashta Boad Syllabus Fouth Edition: June 05 Salient Featues Exhaustie

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

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

SAMPLE QUESTION PAPER CLASS NAME & LOGO XII-JEE (MAINS)-YEAR Topic Names: Cicula motion Test Numbe Test Booklet No. 000001 110001 Wite/Check this Code on you Answe Sheet : IMPORTANT INSTRUCTIONS : Wite

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

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

Circular Motion. Subtopics. Introduction. Angular displacement. acceleration. Relation between linear velocity and angular velocity Chapte 0 : Cicula Motion 0 Cicula Motion Subtopics.0 Intoduction. Angula displacement. Angula elocity acceleation.3 Relation between linea elocity and angula elocity.4 Unifom cicula motion.5 Acceleation

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

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

Motion in a Circle. Content 1. Kinematics of uniform circular motion 2. Centripetal acceleration 3. Centripetal force. JJ 014 H PHYSICS (9646) Motion in a Cicle Motion in a Cicle Content 1. Kinematics of unifom cicula motion. Centipetal acceleation 3. Centipetal foce Leaning Outcomes Candidates should be able to: (a) expess

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

Hoizontal Cicula Motion 1. A paticle of mass m is tied to a light sting and otated with a speed v along a cicula path of adius. If T is tension in the sting and mg is gavitational foce on the paticle then,

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

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

CIRCULAR MOTION. Particle moving in an arbitrary path. Particle moving in straight line 1 CIRCULAR MOTION 1. ANGULAR DISPLACEMENT Intoduction: Angle subtended by position vecto of a paticle moving along any abitay path w..t. some fixed point is called angula displacement. (a) Paticle moving

More information

ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION

ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION POINTS TO REMEMBER 1. Tanslatoy motion: Evey point in the body follows the path of its peceding one with same velocity including the cente of mass..

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 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

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

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

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

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

Physics 1114: Unit 5 Hand-out Homework (Answers) Physics 1114: Unit 5 Hand-out Homewok (Answes) Poblem set 1 1. The flywheel on an expeimental bus is otating at 420 RPM (evolutions pe minute). To find (a) the angula velocity in ad/s (adians/second),

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

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

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

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

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 Section. Cuilinea Motion he study of the motion of a body along a geneal cue. We define u ˆ û the unit ecto at the body, tangential to the cue the unit ecto nomal to the cue Clealy, these unit ectos change

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

Version 1.0. klm. General Certificate of Education June Mathematics. Mechanics 2B. Mark Scheme

Version 1.0. klm. General Certificate of Education June Mathematics. Mechanics 2B. Mark Scheme Vesion.0 klm Geneal Cetificate of Education June 00 Mathematics MMB Mechanics B Mak Scheme Mak schemes ae pepaed by the Pincipal Examine and consideed, togethe with the eleant questions, by a panel of

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

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

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

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

A Level Exam-style Practice Paper

A Level Exam-style Practice Paper A Leel Exam-style Pactice Pape a i The peiod is gien by the time lapse between high tide and low tide which is.5 hous. ii The amplitude is gien by half the total displacement and so is 5 m. b The safe

More information

Chapter 7 Rotational Motion and the Law of Gravity

Chapter 7 Rotational Motion and the Law of Gravity Chapte 7 Rotational Motion and the Law of Gaity What is a Rigid Body? Rotational Kinematics Angula Velocity ω and Acceleation α Unifom Rotational Motion: Kinematics Unifom Cicula Motion: Kinematics and

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

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions ) 06 - ROTATIONAL MOTION Page ) A body A of mass M while falling vetically downwads unde gavity beaks into two pats, a body B of mass ( / ) M and a body C of mass ( / ) M. The cente of mass of bodies B and

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

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

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

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

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

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

Rotatoy Motion Hoizontal Cicula Motion In tanslatoy motion, evey point in te body follows te pat of its pecedin one wit same velocity includin te cente of mass In otatoy motion, evey point move wit diffeent

More information

Physics 107 TUTORIAL ASSIGNMENT #8

Physics 107 TUTORIAL ASSIGNMENT #8 Physics 07 TUTORIAL ASSIGNMENT #8 Cutnell & Johnson, 7 th edition Chapte 8: Poblems 5,, 3, 39, 76 Chapte 9: Poblems 9, 0, 4, 5, 6 Chapte 8 5 Inteactive Solution 8.5 povides a model fo solving this type

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

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

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

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

Chapter 7-8 Rotational Motion

Chapter 7-8 Rotational Motion Chapte 7-8 Rotational Motion What is a Rigid Body? Rotational Kinematics Angula Velocity ω and Acceleation α Unifom Rotational Motion: Kinematics Unifom Cicula Motion: Kinematics and Dynamics The Toque,

More information

Circular Motion. Mr. Velazquez AP/Honors Physics

Circular Motion. Mr. Velazquez AP/Honors Physics Cicula Motion M. Velazquez AP/Honos Physics Objects in Cicula Motion Accoding to Newton s Laws, if no foce acts on an object, it will move with constant speed in a constant diection. Theefoe, if an object

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

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

FREE Download Study Package from website: &

FREE Download Study Package from website:  & FREE Download Study Package fom website: www.tekoclasses.com & www.mathsbysuhag.com Get Solution of These Packages & Lean by Video Tutoials on www.mathsbysuhag.com CIRCULAR MOTION When a paticle moves

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 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

2018 Physics. Advanced Higher. Finalised Marking Instructions

2018 Physics. Advanced Higher. Finalised Marking Instructions National Qualifications 018 018 Physics Advanced Highe Finalised Making Instuctions Scottish Qualifications Authoity 018 The infomation in this publication may be epoduced to suppot SQA qualifications

More information

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets Beyond the Thills excusions Teaches notes Physics is the science of how the wold (and Univese) woks. Luna Pak Sydney is a lage hands-on physics laboatoy full of fee falling objects, otating systems and

More information

ISSUED BY K V - DOWNLOADED FROM CIRCULAR MOTION

ISSUED BY K V - DOWNLOADED FROM  CIRCULAR MOTION K.V. Silcha CIRCULAR MOTION Cicula Motion When a body moves such that it always emains at a fixed distance fom a fixed point then its motion is said to be cicula motion. The fixed distance is called the

More information

4. Two and Three Dimensional Motion

4. Two and Three Dimensional Motion 4. Two and Thee Dimensional Motion 1 Descibe motion using position, displacement, elocity, and acceleation ectos Position ecto: ecto fom oigin to location of the object. = x i ˆ + y ˆ j + z k ˆ Displacement:

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

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

AP * PHYSICS B. Circular Motion, Gravity, & Orbits. Teacher Packet AP * PHYSICS B Cicula Motion, Gavity, & Obits Teache Packet AP* is a tademak of the College Entance Examination Boad. The College Entance Examination Boad was not involved in the poduction of this mateial.

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

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website: Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula

More information

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY Centipetal Foce OBJECTIVE To veify that a mass moving in cicula motion expeiences a foce diected towad the cente of its cicula path. To detemine how the mass, velocity, and adius affect a paticle's centipetal

More information

Translation and Rotation Kinematics

Translation and Rotation Kinematics Tanslation and Rotation Kinematics Oveview: Rotation and Tanslation of Rigid Body Thown Rigid Rod Tanslational Motion: the gavitational extenal foce acts on cente-of-mass F ext = dp sy s dt dv total cm

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

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

SECTION 1. Objectives. Solve problems involving centripetal acceleration. Solve problems involving centripetal force. SECTION 1 Plan and Pepae Peiew Vocabulay Latin Wod Oigins The wod centipetal is ombination of two pats, cente and petal. The second pat of the wod is deied fom the Latin wod petee, which means seeking.

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

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

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

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 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

Physics 231 Lecture 17

Physics 231 Lecture 17 Physics 31 Lectue 17 Main points of today s lectue: Centipetal acceleation: a c = a c t Rotational motion definitions: Δω Δω α =, α = limδ t 0 Δt Δt Δ s= Δ θ;t = ω;at = α Rotational kinematics equations:

More information

Torque, Angular Momentum and Rotational Kinetic Energy

Torque, Angular Momentum and Rotational Kinetic Energy Toque, Angula Moentu and Rotational Kinetic Enegy In ou peious exaples that inoled a wheel, like fo exaple a pulley we wee always caeful to specify that fo the puposes of the poble it would be teated as

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

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

10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11.

10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11. NSWRS - P Physics Multiple hoice Pactice Gavitation Solution nswe 1. m mv Obital speed is found fom setting which gives v whee M is the object being obited. Notice that satellite mass does not affect obital

More information

Unit 6 Test Review Gravitation & Oscillation Chapters 13 & 15

Unit 6 Test Review Gravitation & Oscillation Chapters 13 & 15 A.P. Physics C Unit 6 Test Review Gavitation & Oscillation Chaptes 13 & 15 * In studying fo you test, make sue to study this eview sheet along with you quizzes and homewok assignments. Multiple Choice

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

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

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

Physics 1C Fall 2011: Quiz 1 Version A 1

Physics 1C Fall 2011: Quiz 1 Version A 1 Physics 1C Fall 2011: Quiz 1 Vesion A 1 Depatment of Physics Physics 1C Fall Quate - 2011 D. Mak Paddock INSTRUCTIONS: 1. Pint you full name below LAST NAME FIRST NAME MIDDLE INITIAL 2. You code numbe

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS LSN 10-: MOTION IN A GRAVITATIONAL FIELD Questions Fom Reading Activity? Gavity Waves? Essential Idea: Simila appoaches can be taken in analyzing electical

More information

Chapter 8. Accelerated Circular Motion

Chapter 8. Accelerated Circular Motion Chapte 8 Acceleated Cicula Motion 8.1 Rotational Motion and Angula Displacement A new unit, adians, is eally useful fo angles. Radian measue θ(adians) = s = θ s (ac length) (adius) (s in same units as

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

Chapter 1: Mathematical Concepts and Vectors

Chapter 1: Mathematical Concepts and Vectors Chapte : Mathematical Concepts and Vectos giga G 9 mega M 6 kilo k 3 centi c - milli m -3 mico μ -6 nano n -9 in =.54 cm m = cm = 3.8 t mi = 58 t = 69 m h = 36 s da = 86,4 s ea = 365.5 das You must know

More information

AP Physics C: Electricity and Magnetism 2003 Scoring Guidelines

AP Physics C: Electricity and Magnetism 2003 Scoring Guidelines AP Physics C: Electicity and Magnetism 3 Scoing Guidelines The mateials included in these files ae intended fo use by AP teaches fo couse and exam pepaation; pemission fo any othe use must be sought fom

More information

Multiple choice questions [100 points] As shown in the figure, a mass M is hanging by three massless strings from the ceiling of a room.

Multiple choice questions [100 points] As shown in the figure, a mass M is hanging by three massless strings from the ceiling of a room. Multiple choice questions [00 points] Answe all of the following questions. Read each question caefully. Fill the coect ule on you scanton sheet. Each coect answe is woth 4 points. Each question has exactly

More information

Potential Energy and Conservation of Energy

Potential Energy and Conservation of Energy Potential Enegy and Consevation of Enegy Consevative Foces Definition: Consevative Foce If the wok done by a foce in moving an object fom an initial point to a final point is independent of the path (A

More information

Universal Gravitation

Universal Gravitation Chapte 1 Univesal Gavitation Pactice Poblem Solutions Student Textbook page 580 1. Conceptualize the Poblem - The law of univesal gavitation applies to this poblem. The gavitational foce, F g, between

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

OSCILLATIONS AND GRAVITATION

OSCILLATIONS AND GRAVITATION 1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,

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

Useful for all Engineering Entrance Examinations held across India. STD. XII Sci.

Useful for all Engineering Entrance Examinations held across India. STD. XII Sci. Useful for all Engineering Entrance Examinations held across India. Triumph Maths STD. XII Sci. Salient Features Exhaustive subtopic wise coverage of MCQs. Important formulae provided in each chapter.

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

Exam 3, vers Physics Spring, 2003

Exam 3, vers Physics Spring, 2003 1 of 9 Exam 3, ves. 0001 - Physics 1120 - Sping, 2003 NAME Signatue Student ID # TA s Name(Cicle one): Michael Scheffestein, Chis Kelle, Paisa Seelungsawat Stating time of you Tues ecitation (wite time

More information

( ) ( ) 1.4 m ( ) Section 3.2: Centripetal Acceleration Tutorial 1 Practice, page Given: r = 25 km = m; v = 50.0 m/s. Required: a!

( ) ( ) 1.4 m ( ) Section 3.2: Centripetal Acceleration Tutorial 1 Practice, page Given: r = 25 km = m; v = 50.0 m/s. Required: a! Section 3.2: Centipetal Acceleation Tutoial 1 Pactice, page 118 1. Given: 25 km 2.5 10 4 m; v 50.0 m/s Requied: Analysis: Solution: ( 50.0 m/s) 2 2.5!10 4 m 0.10 m/s 2 Statement: The magnitude of the centipetal

More information

Lecture 13 EXAM 2. Today s Topics: Rotational motion Moment of inertia. Tuesday March 8, :15 PM 9:45 PM

Lecture 13 EXAM 2. Today s Topics: Rotational motion Moment of inertia. Tuesday March 8, :15 PM 9:45 PM Lectue 13 Rotational motion Moment of inetia EXAM uesday Mach 8, 16 8:15 PM 9:45 PM oday s opics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics Angula

More information