Math Lab 10: Differential Equations and Direction Fields Complete before class Wed. Feb. 28; Due noon Thu. Mar. 1 in class

Similar documents
Math Lab 8: Electric Fields Integrating Continuous Charge Distributions II Due noon Thu. Feb. 1 in class

Physics E-1ax, Fall 2014 Experiment 3. Experiment 3: Force. 2. Find your center of mass by balancing yourself on two force plates.

7.1 Indefinite Integrals Calculus

Physics 212E Spring 2004 Classical and Modern Physics. Computer Exercise #2

WISE Regression/Correlation Interactive Lab. Introduction to the WISE Correlation/Regression Applet

1 Review of the dot product

Conservation of Momentum

Successful completion of the core function transformations unit. Algebra manipulation skills with squares and square roots.

INTRODUCTION TO DIFFERENTIATION

1 Newton s 2nd and 3rd Laws

Chapter 14: Finding the Equilibrium Solution and Exploring the Nature of the Equilibration Process

Parabolas and lines

Quadratic Equations Part I

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Lines and Their Equations

Implicit Differentiation Applying Implicit Differentiation Applying Implicit Differentiation Page [1 of 5]

Chapter 1 Functions and Limits

DIFFERENTIAL EQUATIONS

Linear Functions A linear function is a common function that represents a straight line

Exploring Graphs of Polynomial Functions

Lab 4: Gauss Gun Conservation of Energy

18.03SC Practice Problems 2

Linear Motion with Constant Acceleration

Lesson 3-1: Solving Linear Systems by Graphing

Lab 12.1 Calorimetry. Name School Date

This module focuses on the logic of ANOVA with special attention given to variance components and the relationship between ANOVA and regression.

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Quadratic Equations

AP Calculus. Derivatives.

Multiple Representations: Equations to Tables and Graphs Transcript

Chapter 9: Roots and Irrational Numbers

LAB 2 - ONE DIMENSIONAL MOTION

RC Circuits. 1. Designing a time delay circuit. Introduction. In this lab you will explore RC circuits. Introduction

Acceleration, Free Fall, Symmetry

Learning Critical Thinking Through Astronomy: Observing A Stick s Shadow 1

Slope Fields: Graphing Solutions Without the Solutions

Lab 2 Worksheet. Problems. Problem 1: Geometry and Linear Equations

Solving Quadratic & Higher Degree Equations

Boyle s Law and Charles Law Activity

Graphs of Antiderivatives, Substitution Integrals

Math 122 Fall Handout 11: Summary of Euler s Method, Slope Fields and Symbolic Solutions of Differential Equations

PHYSICS LAB: CONSTANT MOTION

Coulomb s Law Mini-Lab

base 2 4 The EXPONENT tells you how many times to write the base as a factor. Evaluate the following expressions in standard notation.

Physics Motion Math. (Read objectives on screen.)

Physics 6A Lab Experiment 6

Experiment 1: The Same or Not The Same?

Math 5a Reading Assignments for Sections

Overlay Analysis II: Using Zonal and Extract Tools to Transfer Raster Values in ArcMap

Predicting the future with Newton s Second Law

Lab Slide Rules and Log Scales

PHYSICS LAB: CONSTANT MOTION

Experiment 0 ~ Introduction to Statistics and Excel Tutorial. Introduction to Statistics, Error and Measurement

Math 112 Group Activity: The Vertical Speed of a Shell

Absolute and Local Extrema

Resonance and response

Vectors. Vector Practice Problems: Odd-numbered problems from

Remember that C is a constant and ë and n are variables. This equation now fits the template of a straight line:

Derivation of Euler's Method - Numerical Methods for Solving Differential Equations

Partner s Name: EXPERIMENT MOTION PLOTS & FREE FALL ACCELERATION

Lesson 7: Classification of Solutions

Finding Limits Graphically and Numerically

( )( b + c) = ab + ac, but it can also be ( )( a) = ba + ca. Let s use the distributive property on a couple of

Horizontal asymptotes

RATES OF CHANGE. A violin string vibrates. The rate of vibration can be measured in cycles per second (c/s),;

LAB Exercise #4 - Answers The Traction Vector and Stress Tensor. Introduction. Format of lab. Preparation reading

School Date. Acceleration, Freefall, Symmetry

1 Implicit Differentiation

Purpose: Materials: WARNING! Section: Partner 2: Partner 1:

7.1 Day 1: Differential Equations & Initial Value Problems (30L)

Distributive property and its connection to areas

Name Date Time to Complete. NOTE: The multimeter s 10 AMP range, instead of the 300 ma range, should be used for all current measurements.

INSTRUCTORS MANUAL: TUTORIAL 8 Spherical Linear Dielectric

Calculus I Homework: The Tangent and Velocity Problems Page 1

VPython Class 2: Functions, Fields, and the dreaded ˆr

{ }. The dots mean they continue in that pattern.

3.4 Pascal s Pride. A Solidify Understanding Task

Lecture 22: The Arrhenius Equation and reaction mechanisms. As we wrap up kinetics we will:

MAPLE Worksheet Number 7 Derivatives in Calculus

MEI Core 1. Basic Algebra. Section 1: Basic algebraic manipulation and solving simple equations. Manipulating algebraic expressions

module, with the exception that the vials are larger and you only use one initial population size.

PHY 101L - Experiments in Mechanics

CHAPTER ONE FUNCTIONS AND GRAPHS. In everyday life, many quantities depend on one or more changing variables eg:

Data and Error Analysis

Name: Date: Partners: LAB 2: ACCELERATED MOTION

Physics 6A Lab Experiment 6

Infinity Unit 2: Chaos! Dynamical Systems

PHY 111L Activity 2 Introduction to Kinematics

INTEGRALS. In Chapter 2, we used the tangent and velocity problems to introduce the derivative the central idea in differential calculus.

Students will explore Stellarium, an open-source planetarium and astronomical visualization software.

The Relation between the Integral and the Derivative Graphs. Unit #10 : Graphs of Antiderivatives, Substitution Integrals

PHY221 Lab 2 - Experiencing Acceleration: Motion with constant acceleration; Logger Pro fits to displacement-time graphs

AP Calculus Worksheet: Chapter 2 Review Part I

MITOCW MITRES18_005S10_DerivOfSinXCosX_300k_512kb-mp4

Introduction to Algebra: The First Week

5.5 Deeper Properties of Continuous Functions

Physics 351 Wednesday, January 10, 2018

Where Is Newton Taking Us? And How Fast?

Sampling Distributions of the Sample Mean Pocket Pennies

Solving Quadratic & Higher Degree Equations

The Physics of Boomerangs By Darren Tan

Algebra. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed.

Transcription:

Matter & Motion Winter 2017 18 Name: Math Lab 10: Differential Equations and Direction Fields Complete before class Wed. Feb. 28; Due noon Thu. Mar. 1 in class Goals: 1. Gain exposure to terminology and notation associated with differential equations. 2. Learn to sketch direction fields and draw solution curves for particular differential equations by hand and by Desmos. 3. Verify proposed solutions to particular differential equations. Instructions: Same as previous labs; see Handout folder in program file share. INTRODUCTION (from Stewart p. 493) Perhaps the most important of all the applications of calculus is to differential equations. When physical scientists or social scientists use calculus, more often than not it is to analyze a differential equation that has arisen in the process of modeling some phenomenon that they are studying. Although it is often impossible to find an explicit formula for the solution of a differential equation, we will see that graphical and numerical approaches provide the needed information. In this Math Lab our last of the quarter, and of the year!, you will gain some further experience with differential equations in advance of our formal study of them in Chapter 7 during weeks 18 and 19. You have already encountered differential equations, frequently in physics, particularly in kinematics and dynamics but also in circuits e.g. the charging/discharging RC circuit, and will encounter them shortly in chemistry in the context of kinetics. Differential equations also synthesize the two main parts of single variable calculus: the relevant rate s of change in the mathematical model involve derivatives, and when there is an analytical solution, it often involves integration. You ve practiced solving differential equations analytically though perhaps those encounters weren t explicitly stated to be solving differential equations and numerically using the Euler Aspel Cromer method, in Physics Lab 9. PART 1: BRIEF PRIMER ON DIFFERENTIAL EQUATIONS Perhaps not surprisingly, a differential equation is an equation that involves a derivative of an unknown function. Solving the differential equation means finding that unknown function or family of functions. For example, say that we know that /, for some known function,, but the function, is unknown. Then solving the differential equation, means finding that unknown function,. 1. Below is one of the simplest differential equations I can think of. Given this differential equation, what does your prior knowledge tell you that? Write down your best proposal for, take its derivative, and show that 1 for your proposed. 1 2. Did you propose where is some constant? If so, great. If you forgot the, go back and fix it now, and write yourself a note in the box that will remind you that in general, a solution to a differential equation is a family of functions. You might recognize that in this case, solving the differential equation involved finding the anti derivative as you have done many times before.

3. Repeat for the following, to determine a family of functions whose is as given: 0 note that this is asking for a function whose derivative is itself 4. Hopefully you got,, and. For the last one, you might have thought it was, but note that in this case. If you re not sure about these, check with your neighbor or with TA/faculty. 5. You saw that there was a solution to the differential equation and. What about for? As a first guess, I would try and see what happens. Try for yourself and confirm that this doesn t work. PART 2: DIRECTION FIELDS, BY HAND It turns out that there is an analytic method to find the solution to the differential equation, but we won t worry about that for now an approach is suggested on the board, should you be interested in trying it after you have completed the lab. Instead, we will explore a graphical method that helps us visualize the shapes of the solutions to a differential equation, a graphical method call direction fields or slope fields. You will learn how to draw direction fields by hand. That method is a bit tedious, but I hope will give you a foundation for understanding what you will see when we use Desmos to draw direction fields for us. 6. Recall that the first derivative gives us the slope of at any point. Consider again. For the point 0, 0, where 0 and 0, then 0. For the point 0, 1, where 0 and 1, then 0 again. For 1,2, then 1, etc. In this simple case, the solution does not depend on the values. Fill out the table below, which has some of the entries already filled in hopefully you will see an interesting pattern that you can use to save some time : 3 3 2 1 0 1 2 3 2 1 1 0 0 1 0 2 3 7. On the graph on the next page, you will plot each slope for each point in pencil. Use a straight edge to draw straight line segments. Draw the slope as accurately as you can, using the grid lines to help. Some are already plotted for you as a model. Note that we are just drawing short line segments to represent the slopes, but those slopes are accurate.

8. Repeat, but this time for. Again, a few entries are filled out for you and again, hopefully you will see an interesting pattern that you can use to save time. 3 2 1 0 1 2 3 3 6 2 1 1 0 0 1 1 2 5 3 0

9. Plot the direction field below, again using pencil. 10. If you haven t already, compare your direction fields to your neighbors. As needed, make any corrections/updates see why I asked you to use pencil?. 11. https://www.youtube.com/watch?v=f7wkjccqeha is a reasonably short video tutorial I found on direction fields that seems acceptable; watch it now and jot down any useful notes in the space below.

PART 3: DIRECTION FIELDS, BY DESMOS It was likely tedious to draw even just a few points of the direction field by hand. Luckily, we can use a computer to plot direction fields for us. We ll use Desmos. You might want to keep the plots you produce in this section; recall that you can do that either by screenshot and then pasting into Word or PowerPoint or equivalent, or you click on the Share Graph icon next to the Help icon and click on export image, which will give you several options for saving the graph and then you can insert it as a picture into Word, PowerPoint, etc. 12. Go to the following Desmos calculator https://www.desmos.com/calculator/422bzlk5yr In input line 2, you should see,, so this should be the direction field slope field corresponding to what you drew by hand for step 7 though for a larger plotting window, and what you saw in the video. Confirm this. 13. Change the entry in input line 2 to be, and confirm that this is matches what you do in step 9 and saw in the video. 14. Return to,. Back in part 1, you showed that the solution to this was. Enter this into what should be the empty input line 3, and turn on the C slider. Adjust the C slider. What do you notice about the solution curves and the direction field? 15. Hopefully you noticed that the direction field suggests the solution curve. Hopefully this makes sense: at any point, the direction field shows the tangent to the function which is one of the solutions to the differential equation. If you draw enough tangent lines, close enough together, you should get a sense of the original functions that are solutions to the differential equation. 16. Change so that, 0 and the solution curve to be you found this in step 3. Adjust the C slider. Any surprises? 17. Change so that, 1 and the solution curve to be you found this in step 1. Adjust the C slider. Any surprises? 18. Change so that, and the solution curve to be you also found this in step 3. Adjust the C slider. Any surprises? 19. Change so that, which you did not do previously, though you may be familiar with it. Look at the direction field, and in particular, compare it to the direction field for,. Can you guess what the solution curve will be? 20. Did you guess? Good. Test it out and see. Any surprises? 21. Return to,. Hide the input in line 3, as we don t yet have a formula for the solution curves. It turns out that 1 is the solution to. By taking the derivative of 1, verify that it is a solution to.

22. In input line 3, enter 1, and adjust the C slider. Any surprises? PART 4: INTEGRATING AND EXTENDING 23. For now, don t use Desmos. Consider the differential equation /. Are you able to quickly write down its solution, like you could for 0, 1,,, or even? If so, do so in the space below, but if not, that s ok; just write Not yet!. 24. Can you picture the direction field in your head? It s ok if not but cool if you can. Enter, / into Desmos. What do you notice about the direction field? What does that suggest about solution curves? 25. Enter into input line 3, turn on the r slider and adjust it. Any surprises? 26. By taking the derivative of, show that these are solutions to / /. Hints: solve for, then take the derivative using the chain rule i.e. use implicit differentiation. 27. Starting from / /, show that. Then, integrate both sides and see what you get.