Math 202 Project Diving Deception Pass. The problem This problem is concerned with the behavior of water as its flowing through the Deception Pass which.

Slides:



Advertisements
Similar presentations
Physics: Principles with Applications, 6th edition
Advertisements

Relationship between First Derivative, Second Derivative and the Shape of a Graph 3.3.
POSITION AND DISPLACEMENT A particle travels along a straight-line path defined by the coordinate axis s. The position of the particle at any instant,
PROJECT 1 DIVING DECEPTION PASS.
APPLICATIONS OF DIFFERENTIATION
RELATED RATES PROBLEMS
Chapter 2 Motion in One Dimension. Dynamics The branch of physics involving the motion of an object and the relationship between that motion and other.
1 Basic Differentiation Rules and Rates of Change Section 2.2.
Ch 3.8: Mechanical & Electrical Vibrations
Quadratic Functions and Equations
APPLICATIONS OF DIFFERENTIATION
Introduction Creating equations from context is important since most real-world scenarios do not involve the equations being given. An equation is a mathematical.
Copyright © 2013, 2009, 2005 Pearson Education, Inc. 1 3 Polynomial and Rational Functions Copyright © 2013, 2009, 2005 Pearson Education, Inc.
What is speed? The speed of an object is the distance the object moves per unit of time. Speed may be written as an equation.
In The Name of ALLAH Project Of Chapter 1 Diving Deception Pass WELCOME.
APPLICATIONS OF DIFFERENTIATION
PARAMETRIC EQUATIONS AND POLAR COORDINATES 9. Usually, we use Cartesian coordinates, which are directed distances from two perpendicular axes. Here, we.
Finding a free maximum Derivatives and extreme points Using second derivatives to identify a maximum/minimum.
Copyright © Cengage Learning. All rights reserved.
What is a function? Quite simply, a function is a rule which takes certain values as input values and assigns to each input value exactly one output value.
1)Domain for optimization 1)Domain for optimization Done by: Fatema Al Hebabi Student ID: Serial no:05.
INTRODUCTION & RECTILINEAR KINEMATICS: CONTINUOUS MOTION Today’s Objectives: Students will be able to: 1.Find the kinematic quantities (position, displacement,
Describing Motion: Kinematics in One Dimension
Linear Motion Physics. Linear Motion Linear Motion refers to “motion in a line”. The motion of an object can be described using a number of different.
APPLICATIONS OF DIFFERENTIATION 4. Many applications of calculus depend on our ability to deduce facts about a function f from information concerning.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Managerial Decision Making and Problem Solving
Introduction : In this chapter we will introduce the concepts of work and kinetic energy. These tools will significantly simplify the manner in which.
Chapter 5 Quadratic Functions Review. Question 1a Identify the vertex, the axis of symmetry, create a table, then graph. y = x² - 8x + 5.
3.4 b) Particle Motion / Rectilinear Motion
Integrals  In Chapter 2, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.  In much the.
Math Jeopardy Quad. Functions And Square Roots Graphing Quad. Equations Solving Quad. Equations Vertical Motion “Algebra – Chapter 9” Critical Values.
Parametric Equations. You throw a ball from a height of 6 feet, with an initial velocity of 90 feet per second and at an angle of 40º with the horizontal.
Chapter 2 Describing Motion: Kinematics in One Dimension.
Do Now Describe your position in the classroom using a reference point and a set of reference directions. Record your response in your science journal.
Notes on Motion VI Free Fall A Special type of uniform acceleration.
APPLICATIONS OF DIFFERENTIATION 4. Many applications of calculus depend on our ability to deduce facts about a function f from information concerning.
Copyright Sautter General Problem Solving Steps (1) Read the problem more than once (three of four times is preferable) (2) Decide what is to be.
Notes on Motion VI Free Fall A Special type of uniform acceleration.
Unit 1: Linear Motion Mrs. Jennings Physics.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Notes on Motion IV Acceleration a What do you think of when someone says acceleration? If you think speeding up – then you are almost completely correct!!!!
Chapter 2 Describing Motion: Kinematics in One Dimension © 2014 Pearson Education, Inc.
Is she moving clockwise or
1 Chapter 6 Flow Analysis Using Differential Methods ( Differential Analysis of Fluid Flow)
 You can use weighted averages to solve uniform motion problems when the objects you are considering are moving at constant rates or speeds.
 In this packet we will look at:  The meaning of acceleration  How acceleration is related to velocity and time  2 distinct types acceleration  A.
RECTILINEAR KINEMATICS: CONTINUOUS MOTION
Applications of Differentiation Section 4.9 Antiderivatives
Wave motion over uneven surface Выпускная работа In work consider two problems about the impact of bottom shape on the profile of the free boundary. 1.
In Chapters 6 and 8, we will see how to use the integral to solve problems concerning:  Volumes  Lengths of curves  Population predictions  Cardiac.
Math 3120 Differential Equations with Boundary Value Problems
An Overview of Mechanics Statics: The study of bodies in equilibrium. Dynamics: 1. Kinematics – concerned with the geometric aspects of motion 2. Kinetics.
Section 4.2 Graphing Polynomial Functions Copyright ©2013, 2009, 2006, 2001 Pearson Education, Inc.
Speed & Velocity Aim: How can we differentiate between speed and velocity?
Chapter 3 Describing Motion: Kinematics in One Dimension.
Chapter 4 Integration 4.1 Antidifferentiation and Indefinate Integrals.
A train traveling at 20 m/s
Introduction Creating equations from context is important since most real-world scenarios do not involve the equations being given. An equation is a mathematical.
Average Rate of Change of a Function
Chapter 2 Describing Motion: Kinematics in One Dimension
Section 3: Acceleration
Introduction Creating equations from context is important since most real-world scenarios do not involve the equations being given. An equation is a mathematical.
Chapter 2 Describing Motion: Kinematics in One Dimension
Topic 6 - Square Root Functions & Equations
Chapter 2 Describing Motion: Kinematics in One Dimension
10.4 Parametric Equations.
4.2 Graphing Polynomial Functions
Describing Motion: Kinematics in One Dimension
Presentation transcript:

Math 202 Project Diving Deception Pass

The problem This problem is concerned with the behavior of water as its flowing through the Deception Pass which is a narrow channel between two islands near Seattle, Washington.

The problem is divided into 6 questions. Each one of those questions represents a solution of a certain part of the main problem.

Problem 1 Suppose that the initial velocity v(0) of the current under bridge is 7 mph. Convert it to ft/s and find the velocity of the current 600 ft west of the bridge. Likewise find the velocity of the current 200 ft east of the bridge, and 800 ft east of the bridge.

The Equation needed for this part (1)

Converting the velocity form mph to ft/s: 7 mph= ft/s Now we will use equation 1 : For x=600 to the west V=2.98 ft/s For x=200 ft to the east V=9.78 ft/s For x=800 ft to the west V=2.98 ft/s

Problem 2 Under the assumptions of Problem 1, where is the current fastest?

The analysis of the data shows that the point where the maximum velocity of the current will occur at x=100 ft which is located east of the bridge. X’)ft/s)X (ft)

Problem 3 Use the deception pass tool on the de tools cd to see how your motion changes depending on where you start. In words describe your motion if you enter the channel 1000 feet to the west of the bridge and compare it to the motion if you start 1000 feet east of the bridge.

The DE Tools CD contains a visual representation of the motion of the diver during the entire trip. In this part of the problem we will use two concepts to distinguish between the two cases. The first is equation 1 and the second is the fact that the maximum velocity of the current will occur at the narrowest point of the channel.

For the first case were the diver dives 1000 feet west of the bridge he will be moving with an initial velocity that well keep increasing as the channel gets narrower in tell he reaches the maximum velocity 100 feet east of the bridge which is the narrowest part of the channel. After that the velocity will start decreasing as the channel gets wider in tell the end of the motion.

In contrary if the diver starts his motion 1000 feet east of the bridge he will start with an initial velocity that well decrease in tell the end of the motion due to the fact that the channel is getting wider. The difference between the two cases is that in case 1 the diver will swim through the point of maximum velocity which is 100 feet east of the bridge unlike case 2 where the diver will start after that point and in this case the velocity will keep going down.

Velocity during the trip

Problem 4 Suppose that the time t=0 corresponds to slack water, compute the velocity of the current near your entry point 1000 feet west of the bridge, that is, with x=-1000,when you started your dive one hour after slack water.remember that time is given in seconds.

Equation 3

In order to determine the velocity of the current 1000 feet west of the bridge and one hour after the slack water we will have to use equation 2 which is the correction of equation 1 but we need to convert the time into seconds: Time= 1 hour  3600 s X=-1000 So x' = v0 sin (π *3600/23400) / (1+( )^2/200000)=0.89 ft/s

Problem 5 You want to compute your likely position relative to the bridge from the time you entered the water (1 hour after the slack water and 1000 feet west of the bridge). What initial value problem would you solve to do so.

This part of the problem needs the use of the initial value concept so we will have to settle on the parameters of our unknowns that we need to find and what information do we have in order to design the required initial value problem. Essentially we will have to use equation 2 as our main differential equation but we need to determine the initial value condition.

What do we have in our disposal of information are the initial position and the time at which we want to find the required position. Since equation 2 gives the velocity in terms of the time then we have the value of one of the needed parameters which is the time however what we need is a condition that contains both time and position.

This can be explained by the fact that the integral of the velocity is the position which we have so the needed condition will be x (3600) = And the needed equation in this case to be solved along with this condition is equation (3) in the book

Problem 6 Show that the model given in the book (4) gives opposite signs for the velocity of the current at x = -300 and x = 300. What does this mean physically discuss the physical validity of this differential equation in view of the sign of the channel-size function S(x).

The correction model for the velocity equation ( Equation 3)

Equation 3 well be used to calculate the corrected velocity at the following cases: 1)X = )X= 300

Using equation 3: 1)x'= 2.73 ft/s 2)x'= ft/s Here both velocities are measured with using the correctional model (5) and this results confirms the range of validity of this correctional model which is from x= to x=0

Case1 in the first case the positive result of the velocity at x= -300 confirm the fact that at that point the correctional model S (x) is valid and yields the expected positive velocity

Case 2 however in this case it pretty clear that the result obtained for the velocity confirms that the point x= 300 is beyond the range of the correctional model of S (x)

The legitimacy of these results agrees with the sings of channel-size function which gives positive sign for the first case and a negative sign for the second case which lie beyond the range of validity of S (x) which varies from x= to x =0 and form here we conclude the physical meaning of this variation of values which clearly show that the range of the correctional model was exceeded

Q & A Done by: Al-Bassam, A.M Al-Bassam, R.A Al-Dukair, A.M