jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
|
|
- Jacob Golden
- 5 years ago
- Views:
Transcription
1 Phone : , Kinematics Pae: 1 fo/u fopkjr Hkh# tu] uha kjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k fla ladyi dj] lrs foifr usd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth ekjkt KINEMATICS Some questions (Assertion Reason type) are ien below. Each question contains STATEMENT 1 (Assertion) and (Reason). Each question has 4 choices (A), (B), (C) and (D) out of which ONLY ONE is correct. So select the correct choice : Choices are : (A) Statement 1 is True, Statement is True; Statement is a correct explanation for Statement 1. (B) Statement 1 is True, Statement is True; Statement is NOT a correct explanation for Statement 1. (C) Statement 1 is True, Statement is False. (D) Statement 1 is False, Statement is True. 9. STATEMENT 1 The instantaneous elocity does not depend on instantaneous position ector. The instantaneous elocity and aerae elocity of a particle are always same. 10. STATEMENT 1 A man who can swim at a speed relatie to water wants to cross the rier of width d, flowin with speed u. He cannot reach a point P opposite him across the rier if u >. The time to reach the opposite point P across the rier is imainary. d u and if u > time will come out to be 11. STATEMENT 1 A balloon ascends from the surface of earth with constant speed. When it was at a heiht 50 m aboe the round, a packet is dropped from it. To an obserer on the balloon, the displacement of the packet, from the moment it is dropped to the moment it reaches the surface of earth, is 50 m. Displacement (ector) depends upon the reference frame used to measure it. 1. STATEMENT 1 If two particles, moin with constant elocities are to meet, the relatie elocity must be alon the line joinin the two particles. Relatie elocity means motion of one particle as iewed from the other. 13. STATEMENT 1 Two balls are dropped one after the other from a tall tower. The distance between them increases linearly with time (elapsed after the second ball is dropped and before the first hits round). Relatie acceleration is zero, whereas relatie elocity non zero in the aboe situation. 14. STATEMENT 1 x t raph, for a particle underoin rectilinear motion, can be as shown in the fiure.
2 Phone : , Kinematics Pae: x Infinitesimal chanes in elocity are physically possible only in infinitesimal time. 15. STATEMENT 1 When a particle moes alon a straiht line manitude of its aerae elocity is equal to its aerae speed oer any time interal. For one dimensional motion displacement and distance both are same. 16. STATEMENT 1 d is equal to d. Here has its usual meanin. dt dt If a particle is acted upon by a external force its momentum must chane. 17. STATEMENT 1 Area under elocity time raph ies displacement. Area under acceleration time raph ies elocity. 18. STATEMENT 1 When a particle is thrown obliquely from the surface of the Earth, it always moes in a parabolic path, proided the air resistance is neliible. A projectile motion is a two dimensional motion. 19. STATEMENT 1 The aerae speed and aerae elocity of the particle are different physical quantities. The aerae speed and aerae elocity hae same dimensions. 0. STATEMENT 1 Two different particles are projected horizontally with different speeds, they reach the round simultaneously. (Assumin is constant) The ertical component of the initial elocity is zero. t 1. STATEMENT 1 Two particles starts moin with elocities V 1 & V respectiely in xy plane. They can meet only if component of their elocity perpendicular to line joinin them are equal. Relatie elocity of a body w.r.t. other body is calculated alon line joinin two bodies.. STATEMENT 1 A man can cross rier of width d in minimum time t. On increasin rier elocity, minimum time to cross the rier by man will remain unchaned.
3 Phone : , Kinematics Pae: 3 Velocity of rier is perpendicular to width of rier. So time to cross the rier is independent of elocity of rier. 3. STATEMENT 1 When a body is dropped or thrown horizontally from the same heiht, it reaches the round at the same time. They hae same acceleration and same initial speed in ertical direction. 4. STATEMENT 1 : The maximum rane alon the inclined plane, when thrown downward is reater than that when thrown upward alon the same inclined plane with constant elocity. : The maximum rane alon inclined plane is independent of anle of inclination. 5. STATEMENT 1 : If particle is moin in straiht line with constant acceleration or retardation its elocity may be zero at particular instant. : If particle moes alon a straiht line it may be accelerated, decelerated or can moe with a constant elocity. 6. STATEMENT 1 : In uniform circular motion acceleration is constant. : In uniform circular motion manitude of acceleration is the centre. V r and direction is always towards 7. STATEMENT 1 : A particle is projected at an anle θ ( < 90) to horizontal, with a elocity u. When particle strikes the round its speed is aain u. : Velocity alon horizontal direction remains same but elocity alon ertical direction is chaned. When particle strikes the round, manitude of final ertical elocity is equal to manitude of initial ertical elocity. 8. STATEMENT 1 : Two particles of different mass, projected with same elocity at same anles. The maximum heiht attained by both the particles will be same. : The maximum heiht of projectile is independent of particle mass 9. STATEMENT 1 : When a particle moes in a circle with a uniform speed, its elocity and acceleration both chanes. : The centripetal acceleration in circular motion is dependent on anular elocity of the body. 30. STATEMENT 1 : The net acceleration of a particle in circular motion is always directed radially inward. : Wheneer a particle moes in a circular path an acceleration exists which is directed towards the centre. 31 STATEMENT 1 : A coin is allowed to fall in a train moin with constant elocity. Its trajectory is parabola as seen by obserer attached to the train. : An obserer on round will see the path of coin as a parabola. 3. STATEMENT 1 : In a projectile motion from round R=H at θ = tan 1 (4). 1 : Max rane of projectile is proportional to (elocity) and. 33. STATEMENT 1 : When speed of projection of a body is made n-times, its time of fliht becomes n times. : This is because rane of projectile become n times. 34. STATEMENT 1 : In a uniformly accelerated motion, acceleration time raph is straiht line with positie slope. : Acceleration is rate of chane of elocity.
4 Phone : , Kinematics Pae: STATEMENT 1 : Horizontal elocity in projectile motion remains constant. :Acceleration due to raity is ertical. 36. STATEMENT 1 : In uniform circular motion acceleration is constant. : In uniform circular motion speed is constant. 37. STATEMENT 1 : A particle is moin on a horizontal surface. Its path will be straiht line if initial elocity and acceleration are alon same horizontal surface. : Anle between u and a determine path therefore, it may be accelerated or retarded curilinear. 38. STATEMENT 1 : If air resistance is considered then time of ascent and time of descent will be different. : Manitudes of acceleration will be different in upwards and downward motion. 39. STATEMENT 1 : For maximum heiht H of a projectile when the maximum rane is R the only alid relation is that H is 50% of R. u sin θ u sin θ : R = and H =. 40. STATEMENT 1 :A particle in motion may not hae ariable speed but constant elocity. : A particle hain non zero acceleration may moe with constant speed. 41. STATEMENT 1 : A body, whateer its motion, is always at rest in a frame of reference which is fixed to the body itself. : The relatie elocity of a body with respect to itself is zero. 4. STATEMENT 1 : A body hain non zero acceleration can hae a constant elocity. : Acceleration is the rate of chane of elocity. 43. STATEMENT 1 : Durin a turn, the alue of centripetal force should be less than the limitin frictional force. : The centripetal force is proided by the frictional force between the tyre and the road. Hint & Solution 9. (C) 10. (A) 11. (D) 1. (A) 13. (A) 14. (D) 15. Both statements are false. 16. (D) 17. (C) 18. (D) 19. (B) 0. (A) 1. (C). (A) 3. (A) 4. (C) 5. (B) 6. (D) 7. (A) 8. (A) 9. (B) 30. (D) 31. (D) 3. (B) 33. (C) 34. (D) 35. (A) 36. (D) 37. (D) 38. (A) 39. (A) 40. (B) 41. (A) 4. (D) 43. (A) d s 9. As =, hence statement 1 is correct. dt Instantaneous elocity is same always to aerae elocity if the particle is moin with constant elocity. 10. Time to cross the rier t = d u.
5 Phone : , Kinematics Pae: 5 u P 11. To an obserer on the balloon, the round is moin. d 1. Suppose motion of 1 is iewed from then as is stationary. If 1 is to meet it, it 1 must come straiht towards i.e., the relatie elocity must be alon At the hih point of the raph elocity (slope of x t cure) chares suddenly from a positie to a neatie alue. This is physically impossible. A - u 17. Area under acceleration time raph ies chane in elocity and not elocity. 18. The particle will moe in a parabolic path till acceleration (due to raity) is constant. For this the particle should be near the surface of the Earth and air resistance should be neliible. 6. In uniform circular motion direction of acceleration is always alon the radial direction. As particle is rotatin so radial ector keeps on chanin. 7. U x = 0, a x = 0 V x = U x + a x T = U x U y = u sin θ; a y = V y = u sin θ t u sin θ = u sin θ. ; V y = u sin θ. 8. u sin θ H = i.e., it is independent of mass of projectile. 9. In uniform circular motion, the manitude of elocity and acceleration remains same, but due to chane in direction of motion, the direction of elocity and acceleration chanes. Also the centripetal acceleration is ien by a = ω r. 30. In case of non uniform circular motion, net acceleration will not be directed towards centre. 31. For the obserer attached with train, the initial horizontal elocity of coin and train are same, thus obserer will find its path as a straiht line. u sin θ 3. Use R = Rane in a function of θ also. u sin θ nu sin θ 33. As T = T = T = nt R = u cosθt R = nu cos θ.nt R = n R 34. Positie slope indicates that acceleration increases uniformly with time. It is not uniform. 35. Since no force is present as horizontal direction elocity of constant. 36. Direction of acceleration chanes. 37.
6 Phone : , Kinematics Pae: 6 a a u accelerated curilinear u retarded curilinear a u straiht line. 38. F(air resistance) m Motion Motion F(air resistance) m 39. Because R max u = [for θ = 45º] u and Hmax = H max can be 50% of rane. 41. A body has no relatie motion with respect to itself. Hence if a frame of reference of the body is fixed, then the bodies will be always at relatiely rest in this frame of reference. So a is correct. dν 4. Acceleration is the rate of chane of elocity i.e., a = dt 43. If the alue of frictional force µm is less than centripetal force, then it is not possible for a ehicle to take twin and the bicycle would take a oer turn. Thus condition for no oer turnin is mν µ m r So statement I and statement II are correct and statement II is the correct explanation of statement I. Hence (a) is correct.
jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : 0 903 903 7779, 98930 58881 Rotational Motion Page: 1 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks]
More informationjfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : 0 903 903 7779, 98930 58881 Laws of Motion Page: 1 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks]
More informationjfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : 0 903 903 7779, 98930 58881 Impulse and Momentum Page: 1 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s;
More informationGet Solution of These Packages & Learn by Video Tutorials on PROJECTILE MOTION
FREE Download Study Packae from website: www.tekoclasses.com & www.mathsbysuha.com Get Solution of These Packaes & Learn by Video Tutorials on www.mathsbysuha.com. BASIC CONCEPT :. PROJECTILE PROJECTILE
More informationSTUDY PACKAGE. Subject : PHYSICS Topic : KINEMATICS. Available Online :
fo/u fopkjr Hkh# tu] uha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k fla ladyi dj] lrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth
More informationjfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : 93 93 7779, 9893 58881 Sount & Waves Page: 9 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj
More informationjfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : 0 903 903 7779, 98930 58881 Modern Physics Page: 55 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks]
More information(a) 1m s -2 (b) 2 m s -2 (c) zero (d) -1 m s -2
11 th Physics - Unit 2 Kinematics Solutions for the Textbook Problems One Marks 1. Which one of the followin Cartesian coordinate system is not followed in physics? 5. If a particle has neative velocity
More informationPhys207: Lecture 04. Today s Agenda 3-D Kinematics Independence of x and y components Baseball projectile Shoot the monkey Uniform circular motion
Phys7: Lecture 4 Reminders All Discussion and Lab sections start meetin this week Homework is posted on course website Solutions to preious hwks will be posted Thursday mornins Today s Aenda 3-D Kinematics
More informationUNDERSTAND MOTION IN ONE AND TWO DIMENSIONS
SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference
More informationjfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt
Phone : (0755) 00 000, 9890 5888 WhatsApp 9009 60 559 QUADRATIC EQUATIONS PART OF fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^
More informationXI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.com https://promotephysics.wordpress.com [MOTION IN TWO DIMENSIONS] CHAPTER NO. 4 In this chapter we are oin to discuss motion in projectile
More informationKINEMATICS PREVIOUS EAMCET BITS ENGINEERING PAPER
KINEMATICS PREVIOUS EAMCET BITS ENGINEERING PAPER. A body is projected vertically upwards at time t = 0 and is seen at a heiht at time t and t seconds durin its fliht. The maximum heiht attained is [ =
More informationthe equations for the motion of the particle are written as
Dynamics 4600:203 Homework 02 Due: ebruary 01, 2008 Name: Please denote your answers clearly, ie, box in, star, etc, and write neatly There are no points for small, messy, unreadable work please use lots
More informationSTUDY PACKAGE. Subject : Mathematics Topic : INVERSE TRIGONOMETRY. Available Online :
fo/u fopkjr Hkh# tu] ugha vkjehks dke] for ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs for vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez iz.ksrk ln~q# Jh j.knksm+nklth
More informationChapter 1: Kinematics of Particles
Chapter 1: Kinematics of Particles 1.1 INTRODUCTION Mechanics the state of rest of motion of bodies subjected to the action of forces Static equilibrium of a body that is either at rest or moes with constant
More informationSTUDY PACKAGE. Subject : Mathematics Topic : Trigonometric Ratio & Identity
fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksMs rqjar e/;e eu dj ';ke iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksMs /;s; dks] j?kqcj jk[ks Vsd jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksmnklth
More informationGround Rules. PC1221 Fundamentals of Physics I. Position and Displacement. Average Velocity. Lectures 7 and 8 Motion in Two Dimensions
PC11 Fundamentals of Physics I Lectures 7 and 8 Motion in Two Dimensions Dr Tay Sen Chuan 1 Ground Rules Switch off your handphone and paer Switch off your laptop computer and keep it No talkin while lecture
More informationISSUED BY K V - DOWNLOADED FROM KINEMATICS
KINEMATICS *rest and Motion are relative terms, nobody can exist in a state of absolute rest or of absolute motion. *One dimensional motion:- The motion of an object is said to be one dimensional motion
More informationSubject : Mathematics Topic : Trigonometric Ratio & Identity
fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';ke iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks Vsd jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth
More informationVISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION
VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION Predict Obsere Explain Exercise 1 Take an A4 sheet of paper and a heay object (cricket ball, basketball, brick, book, etc). Predict what will
More information(C) 7 s. (C) 13 s. (C) 10 m
NAME: Ms. Dwarka, Principal Period: #: WC Bryant HS Ms. Simonds, AP Science Base your answers to questions 1 throuh 3 on the position versus time raph below which shows the motion of a particle on a straiht
More informationv( t) g 2 v 0 sin θ ( ) ( ) g t ( ) = 0
PROJECTILE MOTION Velocity We seek to explore the velocity of the projectile, includin its final value as it hits the round, or a taret above the round. The anle made by the velocity vector with the local
More informationClass 11 Physics NCERT Exemplar Solutions Motion in a Straight Line
Class 11 Physics NCERT Exemplar Solutions Motion in a Straight Line Multiple Choice Questions Single Correct Answer Type Q1. Among the four graphs shown in the figure, there is only one graph for which
More informationREVIEW: Going from ONE to TWO Dimensions with Kinematics. Review of one dimension, constant acceleration kinematics. v x (t) = v x0 + a x t
Lecture 5: Projectile motion, uniform circular motion 1 REVIEW: Goin from ONE to TWO Dimensions with Kinematics In Lecture 2, we studied the motion of a particle in just one dimension. The concepts of
More informationPhysics 4A Solutions to Chapter 4 Homework
Physics 4A Solutions to Chapter 4 Homework Chapter 4 Questions: 4, 1, 1 Exercises & Problems: 5, 11, 3, 7, 8, 58, 67, 77, 87, 11 Answers to Questions: Q 4-4 (a) all tie (b) 1 and tie (the rocket is shot
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVRSITY OF SASKATCHWAN Department of Physics and nineerin Physics Physics 115.3 MIDTRM TST October 3, 009 Time: 90 minutes NAM: (Last) Please Print (Given) STUDNT NO.: LCTUR SCTION (please check): 01
More information(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2.
Chapter 3. Since the trip consists of two parts, let the displacements during first and second parts of the motion be x and x, and the corresponding time interals be t and t, respectiely. Now, because
More informationMotion in Two Dimensions Sections Covered in the Text: Chapters 6 & 7, except 7.5 & 7.6
Motion in Two Dimensions Sections Covered in the Tet: Chapters 6 & 7, ecept 7.5 & 7.6 It is time to etend the definitions we developed in Note 03 to describe motion in 2D space. In doin so we shall find
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVRSITY OF SASKATCHWAN Department of Physics and nineerin Physics Physics 115.3 MIDTRM TST Alternative Sittin October 009 Time: 90 minutes NAM: (Last) Please Print (Given) STUDNT NO.: LCTUR SCTION (please
More informationPhysics Department Tutorial: Motion in a Circle (solutions)
JJ 014 H Physics (9646) o Solution Mark 1 (a) The radian is the angle subtended by an arc length equal to the radius of the circle. Angular elocity ω of a body is the rate of change of its angular displacement.
More informationSTUDY PACKAGE. Subject : PHYSICS Topic : OPTICAL INSTRUMENTS. Available Online :
fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth
More informationMotion in Two Dimensions. 1.The Position, Velocity, and Acceleration Vectors 2.Two-Dimensional Motion with Constant Acceleration 3.
Motion in Two Dimensions 1.The Position, Velocity, and Acceleration Vectors 2.Two-Dimensional Motion with Constant Acceleration 3.Projectile Motion The position of an object is described by its position
More informationPHYS 100: Lecture 4 PROJECTILE MOTION. y = (v 0 /v T ) x (g/2v T2 )x 2. Velocity of Train v T. Physics 100 Lecture 4, Slide y(m)
PHYS : Lecture 4 PROJECTILE MOTION.4. Velocity of Train T y(m).8.6.4. 5 5 x(m) y ( / T ) x (/ T )x Physics Lecture 4, Slide Music Who is the Artist? A) Miles Dais B) Wynton Marsalis C) Chris Botti D) Nina
More informationLinear Motion. Miroslav Mihaylov. February 13, 2014
Linear Motion Miroslav Mihaylov February 13, 2014 1 Vector components Vector A has manitude A and direction θ with respect to the horizontal. On Fiure 1 we chose the eastbound as a positive x direction
More informationPSI AP Physics C Kinematics 2D. Multiple Choice Questions
PSI AP Physics C Kinematics D Multiple Choice Questions 1. A tennis ball is thrown off a cliff 10 m above the round with an initial horizontal velocity of 5 m/s as shown above. The time between the ball
More information1 CHAPTER 7 PROJECTILES. 7.1 No Air Resistance
CHAPTER 7 PROJECTILES 7 No Air Resistance We suppose that a particle is projected from a point O at the oriin of a coordinate system, the y-axis bein vertical and the x-axis directed alon the round The
More informationPhysics 1: Mechanics
Physics 1: Mechanics Đào Ngọc Hạnh Tâm Office: A1.53, Email: dnhtam@hcmiu.edu.n HCMIU, Vietnam National Uniersity Acknowledgment: Most of these slides are supported by Prof. Phan Bao Ngoc credits (3 teaching
More information(a) Taking the derivative of the position vector with respect to time, we have, in SI units (m/s),
Chapter 4 Student Solutions Manual. We apply Eq. 4- and Eq. 4-6. (a) Taking the deriatie of the position ector with respect to time, we hae, in SI units (m/s), d ˆ = (i + 4t ˆj + tk) ˆ = 8tˆj + k ˆ. dt
More informationDYNAMICS. Kinematics of Particles Engineering Dynamics Lecture Note VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER
27 The McGraw-Hill Companies, Inc. All rights resered. Eighth E CHAPTER 11 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdinand P. Beer E. Russell Johnston, Jr. Kinematics of Particles Lecture Notes: J.
More informationLecture 12! Center of mass! Uniform circular motion!
Lecture 1 Center of mass Uniform circular motion Today s Topics: Center of mass Uniform circular motion Centripetal acceleration and force Banked cures Define the center of mass The center of mass is a
More informationMotion in Two or Three Dimensions
Chapter 3 Motion in Two or Three Dimensions PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 3 To use vectors
More informationSKAA 1213 Engineering Mechanics
SKAA 113 Engineering Mechanic TOPIC 8 KINEMATIC OF PARTICLES Lecturer: Roli Anang Dr. Mohd Yunu Ihak Dr. Tan Cher Siang Outline Introduction Rectilinear Motion Curilinear Motion Problem Introduction General
More informationVelocity and Accceleration in Different Coordinate system
Velocity & cceleration in different coordinate system Chapter Velocity and ccceleration in Different Coordinate system In physics basic laws are first introdced for a point partile and then laws are etended
More informationvector of point will be and if the point P is in a space and its coordinates are (x, y, z) then position vector can be expressed as
2.1 Motion in One Dimension : Position Position of any point is completely expressed by two factors : Its distance from the observer and its direction with respect to observer. That is why position is
More informationLesson 3: Free fall, Vectors, Motion in a plane (sections )
Lesson 3: Free fall, Vectors, Motion in a plane (sections.6-3.5) Last time we looked at position s. time and acceleration s. time graphs. Since the instantaneous elocit is lim t 0 t the (instantaneous)
More informationDO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton.
DO PHYSICS ONLINE DISPLACEMENT VELOCITY ACCELERATION The objects that make up space are in motion, we moe, soccer balls moe, the Earth moes, electrons moe, - - -. Motion implies change. The study of the
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationChapter 2 One-Dimensional Kinematics. Copyright 2010 Pearson Education, Inc.
Chapter 2 One-Dimensional Kinematics Units of Chapter 2 Position, Distance, and Displacement Average Speed and Velocity Instantaneous Velocity Acceleration Motion with Constant Acceleration Applications
More informationKinematics of Particles
nnouncements Recitation time is set to 8am eery Monday. Participation i credit will be gien to students t who uploads a good question or good answer to the Q& bulletin board. Suggestions? T s and I will
More informationCIRCULAR MOTION EXERCISE 1 1. d = rate of change of angle
CICULA MOTION EXECISE. d = rate of change of angle as they both complete angle in same time.. c m mg N r m N mg r Since r A r B N A N B. a Force is always perpendicular to displacement work done = 0 4.
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationChapter 4. Motion in Two Dimensions. With modifications by Pinkney
Chapter 4 Motion in Two Dimensions With modifications by Pinkney Kinematics in Two Dimensions covers: the vector nature of position, velocity and acceleration in greater detail projectile motion a special
More informationP6.5 (a) static friction. v r. = r ( 30.0 cm )( 980 cm s ) P6.15 Let the tension at the lowest point be T.
Q65 The speed chanes The tanential orce component causes tanential acceleration Q69 I would not accept that statement or two reasons First, to be beyond the pull o raity, one would hae to be ininitely
More informationMotion in Two and Three Dimensions
PH 1-1D Spring 013 Motion in Two and Three Dimensions Lectures 5,6,7 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter
More informationCHAPTER 3: Kinematics in Two Dimensions; Vectors
HAPTER 3: Kinematics in Two Dimensions; Vectors Solution Guide to WebAssign Problems 3.1 [] The truck has a displacement of 18 + (16) blocks north and 1 blocks east. The resultant has a magnitude of +
More informationChapter 3 Kinematics in Two Dimensions; Vectors
Chapter 3 Kinematics in Two Dimensions; Vectors Vectors and Scalars Addition of Vectors Graphical Methods (One and Two- Dimension) Multiplication of a Vector by a Scalar Subtraction of Vectors Graphical
More informationRutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 4. Home Page. Title Page. Page 1 of 35.
Rutgers Uniersit Department of Phsics & Astronom 01:750:271 Honors Phsics I Fall 2015 Lecture 4 Page 1 of 35 4. Motion in two and three dimensions Goals: To stud position, elocit, and acceleration ectors
More informationLinear Momentum and Collisions Conservation of linear momentum
Unit 4 Linear omentum and Collisions 4.. Conseration of linear momentum 4. Collisions 4.3 Impulse 4.4 Coefficient of restitution (e) 4.. Conseration of linear momentum m m u u m = u = u m Before Collision
More informationChapter 4. Motion in Two Dimensions. Position and Displacement. General Motion Ideas. Motion in Two Dimensions
Motion in Two Dimensions Chapter 4 Motion in Two Dimensions Using + or signs is not always sufficient to fully describe motion in more than one dimension Vectors can be used to more fully describe motion
More informationComponents of a Vector
Vectors (Ch. 1) A vector is a quantity that has a magnitude and a direction. Examples: velocity, displacement, force, acceleration, momentum Examples of scalars: speed, temperature, mass, length, time.
More informationChapter 4. Motion in Two Dimensions. Professor Wa el Salah
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail. Will treat projectile motion and uniform circular
More informationDynamics 4600:203 Homework 03 Due: February 08, 2008 Name:
Dynamics 4600:03 Homework 03 Due: ebruary 08, 008 Name: Please denote your answers clearly, i.e., bo in, star, etc., and write neatly. There are no points for small, messy, unreadable work... please use
More informationMotion in Two and Three Dimensions
PH 1-A Fall 014 Motion in Two and Three Dimensions Lectures 4,5 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationDownloaded from 3. Motion in a straight line. Study of motion of objects along a straight line is known as rectilinear motion.
3. Motion in a straight line IMPORTANT POINTS Study of motion of objects along a straight line is known as rectilinear motion. If a body does not change its position with time it is said to be at rest.
More informationONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.6 MOTION IN A CIRCLE
ONLINE: MAHEMAICS EXENSION opic 6 MECHANICS 6.6 MOION IN A CICLE When a particle moes along a circular path (or cured path) its elocity must change een if its speed is constant, hence the particle must
More informationPY1008 / PY1009 Physics Rotational motion
PY1008 / PY1009 Physics Rotational motion M.P. Vaughan Learning Objecties Circular motion Rotational displacement Velocity Angular frequency, frequency, time period Acceleration Rotational dynamics Centripetal
More informationProblem Set: Fall #1 - Solutions
Problem Set: Fall #1 - Solutions 1. (a) The car stops speedin up in the neative direction and beins deceleratin, probably brakin. (b) Calculate the averae velocity over each time interval. v av0 v 0 +
More information1. Linear Motion. Table of Contents. 1.1 Linear Motion: Velocity Time Graphs (Multi Stage) 1.2 Linear Motion: Velocity Time Graphs (Up and Down)
. LINEAR MOTION www.mathspoints.ie. Linear Motion Table of Contents. Linear Motion: Velocity Time Graphs (Multi Stage). Linear Motion: Velocity Time Graphs (Up and Down).3 Linear Motion: Common Initial
More informationPrince Sultan University Physics Department First Semester 2012 /2013. PHY 105 First Major Exam Allowed Time: 60 min
Prince Sultan University Physics Department First Semester 01 /01 PHY 105 First Major Exam Allowed Time: 60 min Student Name: 1. Write your name in the specified space NOW.. Any paper without name will
More informationA. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged
IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS CHAPTER B TEST REVIEW. A rocket is fired ertically. At its highest point, it explodes. Which one of the following describes what happens
More informationMAGNETIC EFFECTS OF CURRENT-3
MAGNETIC EFFECTS OF CURRENT-3 [Motion of a charged particle in Magnetic field] Force On a Charged Particle in Magnetic Field If a particle carrying a positie charge q and moing with elocity enters a magnetic
More informationGet the frictional force from the normal force. Use dynamics to get the normal force.
. L F n µ k L =00 t µ k = 0.60 = 0 o = 050 lb F n +y +x x = sin y = cos = µf n Is the initial elocity o the car reater than 30 mph? Approach: Use conseration o enery. System: car Initial time: beore you
More informationAP Physics C: Mechanics Ch. 2 Motion. SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.
Name: Period: Date: AP Physics C: Mechanics Ch. Motion SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question. ) Car A is traveling at twice the speed of car
More information1. A sphere with a radius of 1.7 cm has a volume of: A) m 3 B) m 3 C) m 3 D) 0.11 m 3 E) 21 m 3
1. A sphere with a radius of 1.7 cm has a volume of: A) 2.1 10 5 m 3 B) 9.1 10 4 m 3 C) 3.6 10 3 m 3 D) 0.11 m 3 E) 21 m 3 2. A 25-N crate slides down a frictionless incline that is 25 above the horizontal.
More information2.2 Differentiation and Integration of Vector-Valued Functions
.. DIFFERENTIATION AND INTEGRATION OF VECTOR-VALUED FUNCTIONS133. Differentiation and Interation of Vector-Valued Functions Simply put, we differentiate and interate vector functions by differentiatin
More informationNewton's laws of motion
Episode No - 5 Date: 03-04-2017 Faculty: Sunil Deshpande Newton's laws of motion * A plank with a box on it at one end is slowly raised about the other end. As the anle with the horizontal slowly reaches
More informationMOTION IN A PLANE. Chapter Four MCQ I. (a) 45 (b) 90 (c) 45 (d) 180
Chapter Four MOTION IN A PLANE MCQ I 4.1 The angle between A = ˆi + ˆj and B = ˆi ˆj is (a) 45 (b) 90 (c) 45 (d) 180 4.2 Which one of the following statements is true? (a) A scalar quantity is the one
More informationMotion in Two Dimension (Projectile Motion)
Phsics Motion in Two Dimension (Projectile Motion) www.testprepkart.com Table of Content. Introdction.. Projectile. 3. Assmptions of projectile motion. 4. Principle of phsical independence of motions.
More informationAP Physics Chapter 9 QUIZ
AP Physics Chapter 9 QUIZ Name:. The graph at the right shows the force on an object of mass M as a function of time. For the time interal 0 to 4 seconds, the total change in the momentum of the object
More informationN12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES
N1/4/PHYSI/SPM/ENG/TZ0/XX 8816504 Physics Standard leel Paper 1 Tuesday 13 Noember 01 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES Do not open this examination paper until instructed to do so. Answer
More informationYour Thoughts. What is the difference between elastic collision and inelastic collision?
Your Thoughts This seemed pretty easy...before we got the checkpoint questions What is the difference between elastic collision and inelastic collision? The most confusing part of the pre lecture was the
More informationMOTION IN 2-DIMENSION (Projectile & Circular motion And Vectors)
MOTION IN -DIMENSION (Projectile & Circular motion nd Vectors) INTRODUCTION The motion of an object is called two dimensional, if two of the three co-ordinates required to specif the position of the object
More informationStatus: Unit 2, Chapter 3
1 Status: Unit, Chapter 3 Vectors and Scalars Addition of Vectors Graphical Methods Subtraction of Vectors, and Multiplication by a Scalar Adding Vectors by Components Unit Vectors Vector Kinematics Projectile
More informationChapter 2: 1D Kinematics Tuesday January 13th
Chapter : D Kinematics Tuesday January 3th Motion in a straight line (D Kinematics) Aerage elocity and aerage speed Instantaneous elocity and speed Acceleration Short summary Constant acceleration a special
More informationFeb 6, 2013 PHYSICS I Lecture 5
95.141 Feb 6, 213 PHYSICS I Lecture 5 Course website: faculty.uml.edu/pchowdhury/95.141/ www.masteringphysics.com Course: UML95141SPRING213 Lecture Capture h"p://echo36.uml.edu/chowdhury213/physics1spring.html
More informationStudent s Name : Class Roll No. ADDRESS: R-1, Opp. Raiway Track, New Corner Glass Building, Zone-2, M.P. NAGAR, Bhopal
fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj jk[ks VsdAA jfpr% ekuo /kez izksrk ln~q# Jh jknksm+nklth
More informationwhen the particle is moving from D to A.
PRT PHYSICS THE GRPHS GIVEN RE SCHEMTIC ND NOT DRWN TO SCE. student measures the time period of oscillations of a simple pendulum four times. The data set is 9s, 9s, 95s and 9s. If the minimum diision
More informationLesson 2: Kinematics (Sections ) Chapter 2 Motion Along a Line
Lesson : Kinematics (Sections.-.5) Chapter Motion Along a Line In order to specify a position, it is necessary to choose an origin. We talk about the football field is 00 yards from goal line to goal line,
More informationChapter 11 Collision Theory
Chapter Collision Theory Introduction. Center o Mass Reerence Frame Consider two particles o masses m and m interacting ia some orce. Figure. Center o Mass o a system o two interacting particles Choose
More informationa by a factor of = 294 requires 1/T, so to increase 1.4 h 294 = h
IDENTIFY: If the centripetal acceleration matches g, no contact force is required to support an object on the spinning earth s surface. Calculate the centripetal (radial) acceleration /R using = πr/t to
More informationFiring an Ideal Projectile
92 Chapter 13: Vector-Valued Functions and Motion in Space 13.2 Modelin Projectile Motion 921 r at time t v v cos i a j (a) v sin j Newton s second law of motion sas that the force actin on the projectile
More informationPhysics 11 Fall 2012 Practice Problems 2 - Solutions
Physics 11 Fall 01 Practice Problems - s 1. True or false (inore any effects due to air resistance): (a) When a projectile is fired horizontally, it takes the same amount of time to reach the round as
More informationContents. Objectives Circular Motion Velocity and Acceleration Examples Accelerating Frames Polar Coordinates Recap. Contents
Physics 121 for Majors Today s Class You will see how motion in a circle is mathematically similar to motion in a straight line. You will learn that there is a centripetal acceleration (and force) and
More informationMCAT Physics - Problem Drill 06: Translational Motion
MCAT Physics - Problem Drill 06: Translational Motion Question No. 1 of 10 Instructions: (1) Read the problem and answer choices carefully () Work the problems on paper as 1. An object falls from rest
More informationPlanar Motion with Constant Acceleration
Planar Motion with Constant Acceleration 1. If the acceleration vector of an object is perpendicular to its velocity vector, which of the following must be true? (a) The speed is changing. (b) The direction
More informationDYNAMICS. Kinematics of Particles VECTOR MECHANICS FOR ENGINEERS: Tenth Edition CHAPTER
Tenth E CHAPTER 11 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P. Self California Polytechnic State Uniersity Kinematics
More informationGround Rules. PC1221 Fundamentals of Physics I. Position and Displacement. Average Velocity. Lectures 7 and 8 Motion in Two Dimensions
PC11 Fndamentals of Physics I Lectres 7 and 8 Motion in Two Dimensions A/Prof Tay Sen Chan 1 Grond Rles Switch off yor handphone and paer Switch off yor laptop compter and keep it No talkin while lectre
More informationJames T. Shipman Jerry D. Wilson Charles A. Higgins, Jr. Omar Torres. Chapter 2 Motion Cengage Learning
James T. Shipman Jerry D. Wilson Charles A. Higgins, Jr. Omar Torres Chapter 2 Motion Defining Motion Motion is a continuous change in position can be described by measuring the rate of change of position
More information