Assistant Professor: Zhou Yufeng. N , ,

Similar documents
+ r Position Velocity

1. The sphere P travels in a straight line with speed

Chapter 4 Two-Dimensional Motion

Chapter 4 Kinematics in Two Dimensions

Satellite Orbits. Orbital Mechanics. Circular Satellite Orbits

PHYSICS 211 MIDTERM I 22 October 2003

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

( ) ( ) ( ) ( ) ( ) # B x ( ˆ i ) ( ) # B y ( ˆ j ) ( ) # B y ("ˆ ( ) ( ) ( (( ) # ("ˆ ( ) ( ) ( ) # B ˆ z ( k )

Radial geodesics in Schwarzschild spacetime

( ) ( ) Physics 111. Lecture 13 (Walker: Ch ) Connected Objects Circular Motion Centripetal Acceleration Centripetal Force Sept.

1. The 0.1 kg particle has a speed v = 10 m/s as it passes the 30 position shown. The coefficient of kinetic friction between the particle and the

Section 35 SHM and Circular Motion

Physics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468

10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =

Picking Coordinate Axes

1/31/ :33 PM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.

2/2/ :36 AM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.

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

Answers to test yourself questions

Example 2: ( ) 2. $ s ' 9.11" 10 *31 kg ( )( 1" 10 *10 m) ( e)

13.5. Torsion of a curve Tangential and Normal Components of Acceleration

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

2/20/ :21 AM. Chapter 11. Kinematics of Particles. Mohammad Suliman Abuhaiba,Ph.D., P.E.

Chapter 4 Motion in Two and Three Dimensions

This immediately suggests an inverse-square law for a "piece" of current along the line.

r a + r b a + ( r b + r c)

On the Eötvös effect

UNIT VII Central Force: Review Key

SOLUTIONS TO CONCEPTS CHAPTER 11

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

DYNAMICS. Kinetics of Particles: Newton s Second Law VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information

Algebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016

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

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

Rotations 2D & 3D, & about arbitrary axis. Rotation is linear (as in figure)

Central Forces: Circular Motion and Gravitation

Get Solution of These Packages & Learn by Video Tutorials on EXERCISE-1

RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1

Wave Generation by Oscillating Wall in Static Media

CHAPTER 2 ELECTRIC FIELD

Impulse and Momentum

CONTRIBUTIONS TO THE THEORETICAL STUDY OF THE PRECISION SOWING MACHINES DYNAMICS

Two dimensional polar coordinate system in airy stress functions

Lecture 9-3/8/10-14 Spatial Description and Transformation

Path (space curve) Osculating plane

2 / r. Since the speed of the car is constant,

1 Using Integration to Find Arc Lengths and Surface Areas

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics

6. Gravitation. 6.1 Newton's law of Gravitation

Energy Dissipation Gravitational Potential Energy Power

PHY 121 Finals Review FSE Tutoring Centers Spring 2016

AQA Maths M2. Topic Questions from Papers. Circular Motion. Answers

PREVIOUS EAMCET QUESTIONS

Chapter 6 Thermoelasticity

Electric Potential. and Equipotentials

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

FULL MECHANICS SOLUTION

Integral Expression of EM Fields Summary

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

Winter 2004 OSU Sources of Magnetic Fields 1 Chapter 32

U>, and is negative. Electric Potential Energy

Solutions to Midterm Physics 201

JEE(Advanced) 2018 TEST PAPER WITH SOLUTION PHYSICS. (HELD ON SUNDAY 20 th MAY, 2018) PART-1 : PHYSICS. (C) L = mkr ALLEN

Course Updates. Reminders: 1) Assignment #8 available. 2) Chapter 28 this week.

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

ELECTRO - MAGNETIC INDUCTION

defined on a domain can be expanded into the Taylor series around a point a except a singular point. Also, f( z)


Class #16 Monday, March 20, 2017

N for static friction and N

CHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD

SPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.

Electric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin

4. Two and Three Dimensional Motion

Chapters 5-8. Dynamics: Applying Newton s Laws

4.2 Boussinesq s Theory. Contents

SURFACE TENSION. e-edge Education Classes 1 of 7 website: , ,

Chapter 5 Applications of Newton s Laws

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

Physics 604 Problem Set 1 Due Sept 16, 2010

AP Physics Centripetal Acceleration

Collection of Formulas

Spring-Pendulum Dynamic System

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 18: System of Particles II. Slide 18-1

Friedmannien equations

Lecture 11: Potential Gradient and Capacitor Review:

7.5-Determinants in Two Variables

MAGNETIC EFFECT OF CURRENT & MAGNETISM

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Plane Motion of Rigid Bodies: Forces and Accelerations. Seventh Edition CHAPTER

AP Calculus AB Exam Review Sheet B - Session 1

of Technology: MIT OpenCourseWare). (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike.

Plane curvilinear motion is the motion of a particle along a curved path which lies in a single plane.

1. A man pulls himself up the 15 incline by the method shown. If the combined mass of the man and cart is 100 kg, determine the acceleration of the

2. The Laplace Transform

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

Cartesian Coordinate System and Vectors

NARAYANA I I T / P M T A C A D E M Y. C o m m o n Pr a c t i c e T e s t 0 9 XI-IC SPARK Date: PHYSICS CHEMISTRY MATHEMATICS

Transcription:

Aitnt Pofeo: Zhou Yufeng N3.-0-5, 6790-448, yfzhou@ntu.edu.g http://www3.ntu.edu.g/home/yfzhou/coue.html

. A pojectile i fied t flling tget hown. The pojectile lee the gun t the me intnt tht the tget dopped fom et. Auming tht the gun i initilly imed t the tget, how tht the pojectile will hit the tget. (One etiction i tht the pojectile mut ech the tget befoe the tget tike the floo. Set up efeence fme, the initil condition of two pticle ( fo the pojectile, fo the tget e (x (0, y (0=(0,0, nd (x (0, y (0 = (L, L tn y ( 0 0 in, x (0 0 co, y (0 0 whee i contnt. We e ked to poe tht when x = L, y = y

(i The motion of the pojectile cn be expeed co t ( y ( t in t gt x ( t 0 (ii The motion of the tget cn be expeed 0 ( x ( t L (3 (iii when x = L, fom ( we he y( t gt L tn (4 t* L 0 co (5 Subtituting (5 into ( nd (4 yield y ( t* L tn gt * y( t* L tn gt * Poed!

. At gien intnt the jet plne h peed of 0 nd n cceletion of cting in the diection hown. Detemine the te of incee in the plne peed nd the diu of cutue of the pth. Set up the efeence fme, nd expe the gien ecto 060(, ˆ i 0 ( So we cn he the tngentil cceletion t co 60 eˆ t 0.560( which i the tio of the chnge of peed. And the noml cceletion i n Since co 30 n eˆ n, we he 0 79( m 8.9 n 8.9 30(

3. A motoit i teling on cued potion of high wy of diu 350 m t peed of 7 kh. The bke e uddenly pplied, cuing the peed to decee t contnt te of.5. Detemine the mgnitude of the totl cceletion of the utomobile ( immeditely fte the bke he been pplied, (b 4 lte. Show the pth coodinte, nd expe the gien cl 0 7( k h 0(, t.5(, 350( m ( When t = 0 n 0.49( m / 350 0 (b When t = 4 0 tt 0.54 5( n t n.694( 5 0.6486( m / 350 0 t n.406(

4. The ottion of od OA bout O i defined by the eltion t, whee i expeed in din nd t in econd. Coll B lide long the od in uch wy tht it ditnce fom O i, whee i expeed in millimete. When t =, detemine ( the elocity of the coll, (b the totl cceletion of the coll, (c the cceletion of the coll eltie to the od. (i the motion of the od to be t, 4t, 4 (ii the motion of coll eltie to the od to be 3 60t 0t, 0t 60t, 0 0t So, t t =, we he 3 60t 0t, 4, 4 40, 60, 0 ˆ e coiˆ inˆj 0.46ˆ i 0.9093ˆj eˆ co( ˆ i in( ˆj 0.9093ˆ i 0.46ˆj

( the elocity of the coll i the elocity combintion B B f ( / B' the eltie elocity of B eltie to the od (f e ˆ 60ˆ e 4.97ˆ i B/ f 54.56 ˆj ( the entined elocity of B B ' eˆ (40 4ˆ e 45.49ˆ i 66.58 ˆj (3 Combining ( nd (3 gie B 70.46ˆ i.0 ˆj 70.984.03( m (4

(b the totl cceletion of the coll i the cceletion combintion C B B/ f B' B (5 the eltie cceletion of B eltie to the od (f eˆ B / f 0 (6 the entined cceletion of B i B' eˆ eˆ 60ˆ e 640eˆ (7 the Coiolo cceletion C kˆ 8kˆ (60ˆ e B B/ f B/ f 480eˆ (8 Combining (6 nd (7 nd (8 gie B 640ˆ e 640ˆ e 640( 0.493ˆ i.354 ˆ j 905.0849.6( m (9

5. A ocket i fied eticlly fom lunching pd t B. It flight i tcked by d fom point A. Detemine ( the elocity of the ocket in tem of b, nd, (b the cceletion of the ocket in tem of b,,, nd. Setup the efeence fme, decibe the poition of P by P(x P, y P x P b con tn t x P 0, x P 0 y P b tn Uing the definition of elocity gie d y ( btn bec P dt Uing the definition of cceletion gie d y P dt b(ec d ( b tn dt b(ec b ec tn

6. The pin t B i fee to lide long the cicul lot DE nd long the otting od OC. Auming tht the od OC otte t contnt te, ( detemine the cceletion of pin B, (b detemine the eltie liding elocity nd cceletion of the pin eltie to the otting od OC. Setup two fixed efeence fme O-xy, A-x y, fo the ngul poition of B, we he =. Theefoe. Since i contnt, we cn he contnt nd 0 ( Meuing the motion of B in A-x y : b e ˆ b eˆ b eˆ B theefoe B b eˆ B b ' c ( b ( ( b ( (4b ( which i pointing to point A.

(b Obeed fom the fme (f fixed on od OC, the eltie motion of B i decibed by e, eˆ ˆ B/ f B/ f Expeing in tem of by bco we cn deie bin bin bco Hence B/ f bin e B/ f bin bco e whee e co i in j