v v at 1 2 d vit at v v 2a d

Similar documents
a = Acceleration Linear Motion Acceleration Changing Velocity All these Velocities? Acceleration and Freefall Physics 114

Kinematics Quantities. Linear Motion. Coordinate System. Kinematics Quantities. Velocity. Position. Don t Forget Units!

x=0 x=0 Positive Negative Positions Positions x=0 Positive Negative Positions Positions

1 cos. where v v sin. Range Equations: for an object that lands at the same height at which it starts. v sin 2 i. t g. and. sin g

E-Companion: Mathematical Proofs

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1

Let us look at a linear equation for a one-port network, for example some load with a reflection coefficient s, Figure L6.

8. INVERSE Z-TRANSFORM

? plate in A G in

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Quiz: Experimental Physics Lab-I

DCDM BUSINESS SCHOOL NUMERICAL METHODS (COS 233-8) Solutions to Assignment 3. x f(x)

PHYSICS 211 MIDTERM I 22 October 2003

Dynamics of Linked Hierarchies. Constrained dynamics The Featherstone equations

PHYS 100 Worked Examples Week 05: Newton s 2 nd Law

Projectile Motion. Parabolic Motion curved motion in the shape of a parabola. In the y direction, the equation of motion has a t 2.

CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS

5.1 How do we Measure Distance Traveled given Velocity? Student Notes

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Variable time amplitude amplification and quantum algorithms for linear algebra. Andris Ambainis University of Latvia

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:

Big idea in Calculus: approximation

Model Fitting and Robust Regression Methods

6 Roots of Equations: Open Methods

7.1 Integral as Net Change and 7.2 Areas in the Plane Calculus

1. Find the derivative of the following functions. a) f(x) = 2 + 3x b) f(x) = (5 2x) 8 c) f(x) = e2x

Physics 120. Exam #1. April 15, 2011

Applied Statistics Qualifier Examination

Analysis of Variance and Design of Experiments-II

Physics 111. CQ1: springs. con t. Aristocrat at a fixed angle. Wednesday, 8-9 pm in NSC 118/119 Sunday, 6:30-8 pm in CCLIR 468.

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives

ECE470 EXAM #3 SOLUTIONS SPRING Work each problem on the exam booklet in the space provided.

UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II

Math Calculus with Analytic Geometry II

ψ ij has the eigenvalue

Math 116 Calculus II

An Ising model on 2-D image

Position and Speed Control. Industrial Electrical Engineering and Automation Lund University, Sweden

2 b. , a. area is S= 2π xds. Again, understand where these formulas came from (pages ).

AP Calculus. Fundamental Theorem of Calculus

Chapters 4 & 5 Integrals & Applications

ECEN 5807 Lecture 26

Introduction to Numerical Integration Part II

x = b a n x 2 e x dx. cdx = c(b a), where c is any constant. a b

ME306 Dynamics, Spring HW1 Solution Key. AB, where θ is the angle between the vectors A and B, the proof

Section 6.4 Graphs of the sine and cosine functions

Student Session Topic: Particle Motion

Math 1431 Section M TH 4:00 PM 6:00 PM Susan Wheeler Office Hours: Wed 6:00 7:00 PM Online ***NOTE LABS ARE MON AND WED

Name: SID: Discussion Session:

20.2. The Transform and its Inverse. Introduction. Prerequisites. Learning Outcomes

Math 2142 Homework 2 Solutions. Problem 1. Prove the following formulas for Laplace transforms for s > 0. a s 2 + a 2 L{cos at} = e st.

The Fundamental Theorem of Calculus, Particle Motion, and Average Value

Lecture 4: Piecewise Cubic Interpolation

2009 Physics Bowl Solutions

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

ragsdale (zdr82) HW6 ditmire (58335) 1 the direction of the current in the figure. Using the lower circuit in the figure, we get

Jens Siebel (University of Applied Sciences Kaiserslautern) An Interactive Introduction to Complex Numbers

Electrochemical Thermodynamics. Interfaces and Energy Conversion

Math 8 Winter 2015 Applications of Integration

Section 6.3 The Fundamental Theorem, Part I

7.2 Volume. A cross section is the shape we get when cutting straight through an object.

MA123, Chapter 10: Formulas for integrals: integrals, antiderivatives, and the Fundamental Theorem of Calculus (pp.

Abhilasha Classes Class- XII Date: SOLUTION (Chap - 9,10,12) MM 50 Mob no

Work and Energy (Work Done by a Varying Force)

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )

Thermodynamics Lecture Series

When current flows through the armature, the magnetic fields create a torque. Torque = T =. K T i a

Problems (Show your work!)

Read section 3.3, 3.4 Announcements:

Mathematics Extension 2

1 The fundamental theorems of calculus.

Section 6: Area, Volume, and Average Value

1 The fundamental theorems of calculus.

Mathematics Extension 1

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve

R(3, 8) P( 3, 0) Q( 2, 2) S(5, 3) Q(2, 32) P(0, 8) Higher Mathematics Objective Test Practice Book. 1 The diagram shows a sketch of part of

Quick Visit to Bernoulli Land

PHYS 2421 Fields and Waves

Partially Observable Systems. 1 Partially Observable Markov Decision Process (POMDP) Formalism

INTERPOLATION(1) ELM1222 Numerical Analysis. ELM1222 Numerical Analysis Dr Muharrem Mercimek

Artificial Intelligence Markov Decision Problems

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007

4.4 Areas, Integrals and Antiderivatives

Integrals - Motivation

i-clicker i-clicker A B C a r Work & Kinetic Energy

Exponents and Powers

6.2 CONCEPTS FOR ADVANCED MATHEMATICS, C2 (4752) AS

2. Work each problem on the exam booklet in the space provided.

Unit #10 De+inite Integration & The Fundamental Theorem Of Calculus

The Fundamental Theorem of Calculus. The Total Change Theorem and the Area Under a Curve.

Definition of Tracking

AP * Calculus Review

SOLUTIONS TO CONCEPTS CHAPTER 6

Section Areas and Distances. Example 1: Suppose a car travels at a constant 50 miles per hour for 2 hours. What is the total distance traveled?

CHAPTER 10 ROTATIONAL MOTION

MATH 144: Business Calculus Final Review

COMP 465: Data Mining More on PageRank

Fact: All polynomial functions are continuous and differentiable everywhere.

Review: Velocity: v( t) r '( t) speed = v( t) Initial speed v, initial height h, launching angle : 1 Projectile motion: r( ) j v r

Designing Information Devices and Systems I Discussion 8B

Transcription:

SPH3UW Unt. Accelerton n One Denon Pge o 9 Note Phyc Inventory Accelerton the rte o chnge o velocty. Averge ccelerton, ve the chnge n velocty dvded by the te ntervl, v v v ve. t t v dv Intntneou ccelerton the ccelerton t ny prtculr ntnt. l. t 0 t dt The lope o curve on velocty-te grph repreent the ccelerton. The re under the curve on n ccelerton-te grph repreent the chnge n velocty. There re 5 vrble nvolved n the thetcl nly o oton wth contnt ccelerton:, v, v, d, t There re 5 equton tht llow you to olve oton proble wth contnt ccelerton: d x x 0 v v t d vt t v v d d v v t d v t t You cn olve ll proble you ue both equton ultneouly: v v t d vt t Accelerton the rte t whch velocty chnge. Jut we dd or velocty, we cn dene verge ccelerton over n ntervl or ntntneou ccelerton t pecc oent n te. Averge ccelerton: ve v t v v t Intntneou ccelerton: v l t 0 t dv dt I you re gven grph o velocty veru te, the verge ccelerton over n ntervl jut the lope o the lne connectng the two end o the ntervl (ecnt lne), nd the ntntneou ccelerton the lpe o the tngent lne drwn to the grph t the gven te. The net re under the velocty veru te grph jut the dplceent, the re totl dtnce trvelled. d. The bolute vlue o

SPH3UW Unt. Accelerton n One Denon Pge o 9 Note o Cuton: Keep n nd tht negtve ccelerton doe not necerly en tht n object lowng down. I the ccelerton negtve, nd the velocty negtve, the object peedng up! Exple A cr peed up wth n verge ccelerton wth gntude o 6., deterne t velocty ter.7 t ntl w 3 E.

SPH3UW Unt. Accelerton n One Denon Pge 3 o 9 Soluton: Fro ve v v v t t The nl velocty 4 E Exple Snce ccelerton peedng up, t n the e drecton velocty [E].. v 3 E 6. E.7 0.54 3 0.54 E 3 E v v 4.54 E 4 E E v E gncnt dgt. Fro the ollowng velocty v te grph: ) generte the correpondng poton-te grph b) generte the correpondng ccelerton-te grph c) deterne the ntntneou velocty t t= econd nd t=4 econd

SPH3UW Unt. Accelerton n One Denon Pge 4 o 9 ) b)

SPH3UW Unt. Accelerton n One Denon Pge 5 o 9 c) The ntntneou velocty t t= 6 / The ntntneou velocty t t=4 9 / Thee 5 equton ut be eorzed nd prctced wth nee. Equton or oton wth Contnt Accelerton Equton Mng Quntty * v v0 t x x0 * x x0 v0t t v 0 0 v v x x t x x0 v0 vt x x vt t 0 0 v The two equton wth n * cn be ued to olve ny proble. You olve both equton ultneouly nd cobne. Exple Obervng trc lowdown, you brke your cr ro peed o 00 k/h to peed o 80.0 k/h durng dplceent o 88.0, t contnt ccelerton. ) Wht tht ccelerton? b) How uch te requred or the gven decree n peed?

SPH3UW Unt. Accelerton n One Denon Pge 6 o 9 Soluton: We re gven: x x0 88.0 k h 000 v0 00 7.8 h 3600 k t? ) Method? Ung v v0 t nd k h 000 v v 80.0. h 3600 k x x0 v0t t v v t. 7.8 t 5.6 t 0 nd ubttute nto x x0 v0t t 5.6 5.6 88.0 7.8 55.68 5.68 88.0 40 88.0 40 88.0.59 Thu the ccelerton (n the oppote drecton velocty) -.59 /.

SPH3UW Unt. Accelerton n One Denon Pge 7 o 9 Method Snce we wnt the ccelerton nd the ng vrble t, thereore we cn ply ue v v x x 0 0 v v x x 0 0. 7.8 88.0.59 b) We hve ll pece o norton or the equton o oton o we cn ue ny equton. Let ue the eet orul: v v t 0.. 7.8.59 t t 3.5 Exple: The velocty o prtcle ovng long the x x vre n te ccordng to the expreon vx 50 4t /,,where t n econd. ) Fnd the verge ccelerton n the te ntervl t =0 to t=.0 b) Deterne the ccelerton t t =.0. Soluton: ) v v 50 4 0 50 50 4 46 x v 46 50 v 4 t t 0 The negtve gn rend u tht nce nl velocty ller thn ntl, t lowng down.

SPH3UW Unt. Accelerton n One Denon Pge 8 o 9 b) We recll tht x v l t 0 t v 50 4t We lo note tht 50 4 50 4 8 4 v t t t t t Cobnng: x v l t 0 t v v l t 0 t t t 0 50 4t 8t 4 t 50 4t l t 0 t 8t 4 l t 0 t l8 4t 8 t Becue the velocty o the prtcle potve nd the ccelerton negtve, the prtcle lowng down.

SPH3UW Unt. Accelerton n One Denon Pge 9 o 9 Extr Note nd Coent