( ) ( ) ( ) ( ) ( ) ( )



Similar documents
Scalar versus Vector Quantities. Speed. Speed: Example Two. Scalar Quantities. Average Speed = distance (in meters) time (in seconds) v =

To define concepts such as distance, displacement, speed, velocity, and acceleration.

Calculating average acceleration from velocity change and time

= f x 1 + h. 3. Geometrically, the average rate of change is the slope of the secant line connecting the pts (x 1 )).

Phys222 Winter 2012 Quiz 4 Chapters Name

Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

F f v 1 = c100(10 3 ) m h da 1h 3600 s b =

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. Dr Tay Seng Chuan

Presentation of problem T1 (9 points): The Maribo Meteorite

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion

Newton s Laws. Physics 1425 lecture 6. Michael Fowler, UVa.

XI / PHYSICS FLUIDS IN MOTION 11/PA

3.1 MAXIMUM, MINIMUM AND INFLECTION POINT & SKETCHING THE GRAPH. In Isaac Newton's day, one of the biggest problems was poor navigation at sea.

1.3.1 Position, Distance and Displacement

circular motion & gravitation physics 111N

Physics 121 Sample Common Exam 3 NOTE: ANSWERS ARE ON PAGE 6. Instructions: 1. In the formula F = qvxb:

Physics 41 HW Set 1 Chapter 15

Motion Graphs. Plotting distance against time can tell you a lot about motion. Let's look at the axes:

W i f(x i ) x. i=1. f(x i ) x = i=1

Experiment 2 Free Fall and Projectile Motion

Physics Notes Class 11 CHAPTER 3 MOTION IN A STRAIGHT LINE

1 of 10 7/29/2014 7:28 AM 2 of 10 7/29/2014 7:28 AM

Version A Page The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart.

Physics Kinematics Model

1. Metric system- developed in Europe (France) in 1700's, offered as an alternative to the British or English system of measurement.


Chapter 28 Fluid Dynamics

Ch 7 Kinetic Energy and Work. Question: 7 Problems: 3, 7, 11, 17, 23, 27, 35, 37, 41, 43

2 ONE- DIMENSIONAL MOTION

Name Class Period. F = G m 1 m 2 d 2. G =6.67 x Nm 2 /kg 2

2After completing this chapter you should be able to

Despite its enormous mass (425 to 900 kg), the Cape buffalo is capable of running at a top speed of about 55 km/h (34 mi/h).

Physics 111: Lecture 4: Chapter 4 - Forces and Newton s Laws of Motion. Physics is about forces and how the world around us reacts to these forces.

HW 3 Due Sep 12, Wed

Problem Solving: Kinematics and One Dimensional Motion. Experiment One: Introduction to to Data Studio

Worked Examples from Introductory Physics Vol. I: Basic Mechanics. David Murdock Tenn. Tech. Univ.

Copyright 2013 wolfssl Inc. All rights reserved. 2

CHAPTER 15 FORCE, MASS AND ACCELERATION

Chapter 3.8 & 6 Solutions

Chapter 19 Magnetic Forces and Fields

Catapult Engineering Pilot Workshop. LA Tech STEP

F = ma. F = G m 1m 2 R 2

STATICS. Introduction VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Answer the questions in this problem using words from the following list:

Chapter Test B. Chapter: Measurements and Calculations

SPEED, VELOCITY, AND ACCELERATION

11. Rotation Translational Motion: Rotational Motion:

PHY121 #8 Midterm I

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

Physics 2B. Lecture 29B

x 1 ' = x 1 vt 1 x 1 ' = 4.0 m t 1 = 1.0 s x 2 vt 2 ' = 4.0 m t 2 ' = x 2 = 3.0 s x 1 = x 2 x 1 ' + vt 1 ' + vt 2 v (t 1 t 2 ) = x 2 ' x 1 ' = x 2

Exam 1 Review Questions PHY Exam 1

1 of 7 9/5/2009 6:12 PM

momentum change per impact The average rate of change of momentum = Time interval between successive impacts 2m x 2l / x m x m x 2 / l P = l 2 P = l 3

How To Understand The Physics Of A Charge Charge

US FMVSS 202 Final Rule

Modern Physics Laboratory e/m with Teltron Deflection Tube

Orbital Mechanics. Angular Momentum

226 Chapter 15: OSCILLATIONS

Learning Outcomes. Distinguish between Distance and Displacement when comparing positions. Distinguish between Scalar and Vector Quantities

SOLUTIONS TO CONCEPTS CHAPTER 15

Solution: F = kx is Hooke s law for a mass and spring system. Angular frequency of this system is: k m therefore, k

SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS

Mini slide, Series MSN narrow version Ø 6-16 mm double-acting with magnetic piston cushioning: elastic with integrated ball rail guide

How To Powertrain A Car With A Hybrid Powertrain

Speed A B C. Time. Chapter 3: Falling Objects and Projectile Motion

PHYSICS 111 HOMEWORK SOLUTION #10. April 8, 2013

Solutions to old Exam 1 problems

Quiz: Work and Energy

PARTICLE SIMULATION ON MULTIPLE DUST LAYERS OF COULOMB CLOUD IN CATHODE SHEATH EDGE

10.1 Quantitative. Answer: A Var: 50+

Problem Set 1 Solutions

CHARGED PARTICLES & MAGNETIC FIELDS - WebAssign

Physics: Principles and Applications, 6e Giancoli Chapter 2 Describing Motion: Kinematics in One Dimension

Exam 2 is at 7 pm tomorrow Conflict is at 5:15 pm in 151 Loomis

Review Chapters 2, 3, 4, 5

Millikan Oil Drop Experiment Matthew Norton, Jurasits Christopher, Heyduck William, Nick Chumbley. Norton 0

1 One Dimensional Horizontal Motion Position vs. time Velocity vs. time

CBE 6333, R. Levicky 1 Review of Fluid Mechanics Terminology

Graphing Motion. Every Picture Tells A Story

Chapter 4 One Dimensional Kinematics

8. As a cart travels around a horizontal circular track, the cart must undergo a change in (1) velocity (3) speed (2) inertia (4) weight

Kyu-Jung Kim Mechanical Engineering Department, California State Polytechnic University, Pomona, U.S.A.

AS COMPETITION PAPER 2007 SOLUTIONS

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

2. Orbits. FER-Zagreb, Satellite communication systems 2011/12

Three-dimensional figure showing the operation of the CRT. The dotted line shows the path traversed by an example electron.

4 Impulse and Impact. Table of contents:

HSC Mathematics - Extension 1. Workshop E4

( )( 10!12 ( 0.01) 2 2 = 624 ( ) Exam 1 Solutions. Phy 2049 Fall 2011

Name Period WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS. 1. Stored energy or energy due to position is known as energy.

Acceleration Due to Gravity

Newton s Laws Quiz Review

Mechanics 1: Conservation of Energy and Momentum

Some Comments on the Derivative of a Vector with applications to angular momentum and curvature. E. L. Lady (October 18, 2000)

Chapter 21. Magnetic Forces and Magnetic Fields

Physics 53. Kinematics 2. Our nature consists in movement; absolute rest is death. Pascal

v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

Cambridge International Examinations Cambridge International Advanced Subsidiary and Advanced Level

CHAPTER: 6 FLOW OF WATER THROUGH SOILS

Transcription:

Problem (Q1): Evaluate each of the following to three significant figures and express each answer in SI units: (a) (0.631 Mm)/(8.60 kg) 2 (b) (35 mm) 2 *(48 kg) 3 (a) 0.631 Mm / 8.60 kg 2 6 0.631 10 m 8532 m = = 2 2 2 8.60 kg kg = 8.53 10 m / kg = 8.53 km / kg 3 2 2 2 2 2 3 2 2 3 (b) 35 mm 48 kg = 35 10 m 48 kg = 135 m / kg

12 25. A sphere is fired downwards into a medium with an initial speed of 27 m>s. If it experiences a deceleration of a = (-6t) m>s 2, where t is in seconds, determine the distance traveled before it stops. Velocity: v 0 = 27 m>s at t 0 = 0 s. Applying Eq. 12 2, we have A+TB dv =adt v t dv = -6tdt L27 v = A27-3t 2 B m>s (1) At v = 0, from Eq. (1) Distance Traveled: s at. Using the result v = 27-3t 2 0 = 0 m t 0 = 0 s and applying Eq. 12 1, we have A+TB At t = 3.00 s, from Eq. (2) 0 = 27-3t 2 t = 3.00 s ds =vdt s t ds = A27-3t 2 Bdt L0 s = A27t -t 3 B m s = 27(3.00) - 3.00 3 = 54.0 m (2) This work is protected by United States copyright laws

12 27. A particle is moving along a straight line such that when it is at the origin it has a velocity of 4 m>s. If it begins to decelerate at the rate of a =1-1.5v 1>2 2 m>s 2, wherevis in m>s, determine the distance it travels before it stops. a = dv dt = -1.5v1 2 v t v - 1 2 dv = -1.5dt L4 2v 1 2 v 4 = -1.5tt 0 2av 1 2-2b = -1.5t v = (2-0.75t) 2 m>s (1) s t t ds = (2-0.75t) 2 dt = (4-3t + 0.5625t 2 )dt L0 laws s = 4t - 1.5t 2 + 0.1875t 3 (2) copyright From Eq. (1), the particle will stop when States 0 = (2-0.75t) United 2 t = 2.667 s s t=2.667 = 4(2.667) - 1.5(2.667) 2 + 0.1875(2.667) 3 = 3.56by 3.56 m This work is protected

*12 28. A particle travels to the right along a straight line with a velocity v = [5>14 +s2] m>s, where s is in meters. Determine its deceleration when s = 2 m. v = v dv = a ds dv = 5 4 + s -5 ds (4 + s) 2 5 (4 + s) a - 5 ds (4 + s) 2b = a ds a = - 25 (4 + s) 3 When s = 2 m a = -0.116 m>s 2 This work is protected by United States copyright laws

12 30. As a train accelerates uniformly it passes successive kilometer marks while traveling at velocities of 2 m>s and then 10 m>s. Determine the train s velocity when it passes the next kilometer mark and the time it takes to travel the 2-km distance. Kinematics: For the first kilometer of the journey, v 0 = 2 m>s, v = 10 m>s, s 0 = 0, and s = 1000 m. Thus, A: + B v 2 =v 2 0 + 2a c (s -s 0 ) 10 2 = 2 2 + 2a c (1000-0) a c = 0.048 m>s 2 For the second kilometer, v 0 = 10 m>s, s 0 = 1000 m, s = 2000 m, and a 0.048 m>s 2 c =. Thus, A: + B v 2 =v 2 0 + 2a c (s -s 0 ) v 2 = 10 2 + 2(0.048)(2000-1000) v = 14 m>s For the whole journey, v, v = 14 m>s, and 0.048 m>s 2 0 = 2 m>s a c =. Thus, A: + B v =v 0 +a c t 14 = 2 + 0.048t t = 250 s work is protected by United States copyright laws and is provided solely for the use of instructors Ain teaching