Section 11.6: Directional Derivatives and the Gradient Vector

Similar documents
2008 AP Calculus BC Multiple Choice Exam

First derivative analysis

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables.

Exponential Functions

Calculus concepts derivatives

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

Note If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Curl, Divergence, Gradient, and Laplacian in Cylindrical and Spherical Coordinate Systems

1973 AP Calculus AB: Section I

Math 34A. Final Review

MATHEMATICS PAPER IB COORDINATE GEOMETRY(2D &3D) AND CALCULUS. Note: This question paper consists of three sections A,B and C.

Chapter 1. Chapter 10. Chapter 2. Chapter 11. Chapter 3. Chapter 12. Chapter 4. Chapter 13. Chapter 5. Chapter 14. Chapter 6. Chapter 7.

MATH 1080 Test 2-SOLUTIONS Spring

Calculus Revision A2 Level

u 3 = u 3 (x 1, x 2, x 3 )

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

Pipe flow friction, small vs. big pipes

1997 AP Calculus AB: Section I, Part A

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C


INTEGRATION BY PARTS

are given in the table below. t (hours)

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

y = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b)

Higher order derivatives

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12

Where k is either given or determined from the data and c is an arbitrary constant.

Sundials and Linear Algebra

DIFFERENTIAL EQUATION

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

4037 ADDITIONAL MATHEMATICS

MSLC Math 151 WI09 Exam 2 Review Solutions

1 Isoparametric Concept

Text: WMM, Chapter 5. Sections , ,

Differentiation of Exponential Functions

Objective Mathematics

Integration by Parts

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

MAXIMA-MINIMA EXERCISE - 01 CHECK YOUR GRASP

Einstein Equations for Tetrad Fields

Thomas Whitham Sixth Form

That is, we start with a general matrix: And end with a simpler matrix:

EAcos θ, where θ is the angle between the electric field and

nd the particular orthogonal trajectory from the family of orthogonal trajectories passing through point (0; 1).

ECE 650 1/8. Homework Set 4 - Solutions

MATHEMATICS PAPER IIB COORDINATE GEOMETRY AND CALCULUS. Note: This question paper consists of three sections A, B and C.

1997 AP Calculus AB: Section I, Part A

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Thomas Whitham Sixth Form

Deepak Rajput

High Energy Physics. Lecture 5 The Passage of Particles through Matter

Basic Polyhedral theory

MATHEMATICS (B) 2 log (D) ( 1) = where z =

Unit 6: Solving Exponential Equations and More

Calculus II (MAC )

Answers & Solutions. for MHT CET-2018 Paper-I (Mathematics) Instruction for Candidates

Mathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration

Addition of angular momentum

6.1 Integration by Parts and Present Value. Copyright Cengage Learning. All rights reserved.

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

y cos x = cos xdx = sin x + c y = tan x + c sec x But, y = 1 when x = 0 giving c = 1. y = tan x + sec x (A1) (C4) OR y cos x = sin x + 1 [8]

Addition of angular momentum

PHYS-333: Problem set #2 Solutions

The Matrix Exponential

A Propagating Wave Packet Group Velocity Dispersion

4 x 4, and. where x is Town Square

Search sequence databases 3 10/25/2016

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

( ) Differential Equations. Unit-7. Exact Differential Equations: M d x + N d y = 0. Verify the condition

The Matrix Exponential

VTU NOTES QUESTION PAPERS NEWS RESULTS FORUMS

cycle that does not cross any edges (including its own), then it has at least

Differential Equations

Exercise 1. Sketch the graph of the following function. (x 2

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

PROBLEM SET Problem 1.

2. Background Material

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

EXST Regression Techniques Page 1

AP Calculus Multiple-Choice Question Collection

10. The Discrete-Time Fourier Transform (DTFT)

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

INC 693, 481 Dynamics System and Modelling: The Language of Bound Graphs Dr.-Ing. Sudchai Boonto Assistant Professor

Announce. ECE 2026 Summer LECTURE OBJECTIVES READING. LECTURE #3 Complex View of Sinusoids May 21, Complex Number Review

The Frequency Response of a Quarter-Wave Matching Network

MATH 319, WEEK 15: The Fundamental Matrix, Non-Homogeneous Systems of Differential Equations

Direct Approach for Discrete Systems One-Dimensional Elements

(1) Then we could wave our hands over this and it would become:

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Massachusetts Institute of Technology Department of Mechanical Engineering

Sec 2.3 Modeling with First Order Equations

The function y loge. Vertical Asymptote x 0.

Collisions between electrons and ions

Differential Equations

Content Skills Assessments Lessons. Identify, classify, and apply properties of negative and positive angles.

Transcription:

Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th surac at th point a b a b in th dirction a b a b a b Slop o th tangnt lin to th surac at th point a b a b in th dirction Instad o rstricting ourslvs to th and ais suppos w want to ind a mthod or inding th slop o th surac in an dsird dirction. Slop in dir Slop in dir D u Slop in u dir θ u < a b >

Lt u < a b > b th unit vctor a vctor o lngth on on th - plan which indicats th dirction w ar moving. Thn w din th ollowing: Dinition o th Dirctional Drivativ Th dirctional drivativ o a unction in th dirction o th unit vctor u < a b > dnotd b is dind th b th ollowing: D u D u a + b Nots. Gomtricall th dirctional drivativ is usd to calculat th slop o th surac. That is to calculat th slop o th surac at th point whr w comput th ollowing: Slop o Surac at point D in dirction o unit vctor u < a. b > u a + b. Th vctor u < a b > must b a unit vctor. I w want to comput th dirctional drivativ o a unction in th dirction o th vctor v and v is not a unit vctor w comput v u v. v v 3. Th dirction o th unit vctor u can b prssd in trms o th angl θ btwn th vctor u and th -ais. In this cas u < cosθ sinθ > not u is a unit vctor sinc u cos θ + sin θ and th dirctional drivativ can b prssd as D u cosθ + sinθ. 4. Computationall th dirctional drivativ rprsnts th rat o chang o th unction in th dirction o th unit vctor u.

3 Eampl : ind th dirctional drivativ o th unction 3 4 + 6 at th π point in th dirction o th unit vctor that maks an angl o θ radians with 3 th -ais. Solution:

4 Eampl : ind th dirctional drivativ o th unction point -3-4 in th dirction o th vctor v i + 3j. 3 4 + 6 at th Solution:

5 Gradint o a unction Givn a unction o two variabls th gradint vctor dnotd b is a vctor in th - plan dnotd b i j + acts about Gradints. Th dirctional drivativ o th unction in th dirction o th unit vctor u < a b > can b prssd in trms o gradint using th dot product. That is D u u < a + > < a b > b. Th gradint vctor givs th dirction o maimum incras o th surac. Th lngth o th gradint vctor is th maimum valu o th dirctional drivativ th maimum rat o chang o. That is Maimum Valu o th Dirctional Drivativ D u 3. Th ngation o th gradint vctor givs th dirction o maimum dcras. o th surac. Th ngation o th lngth o th gradint vctor is th minimum valu o th dirctional drivativ. That is Minimum Valu o th Dirctional Drivativ D u

6 Eampl 3: Givn th unction cos. a. ind th gradint o b. Evaluat th gradint at th point P π. 3 c. Us th gradint to ind a ormula or th dirctional drivativ o in th dirction o th 3 4 vctor u < >. Us th rsult to rsult to ind th rat o chang o at P in th 5 5 dirction o th vctor u. Solution:

7 Dirctional Drivativ and Gradint or unctions o 3 variabls Th dirctional drivativ o a unction o 3 variabls in th dirction o th unit vctor u < a b c > dnotd b D u is dind to b th ollowing: c b a D + + u Th gradint vctor dnotd b is a vctor dnotd b k j i + +

8 Eampl 4: ind th gradint and dirctional drivativ o P 4 in th dirction o th point Q-3. 5 3 + at Solution: W irst comput th irst ordr partial drivativs with rspct to and. Th ar as ollows. 3 + 3 + 3 + 3 + +. Thn th ormula or th gradint is computd as ollows: i + j+ k 3 + i + 3 + j + k Hnc at th point P 4 th gradint is 4 3 + 4 i + 3 + 4 j + k i + j + k < > To ind th dirctional drivativ w must irst ind th unit vctor u spciing th dirction at th point P 4 in th dirction o th point Q-3. To do this w ind th vctor v PQ. This is ound to b v PQ < 3 4 >< 4 >. This must b a unit vctor so w comput th ollowing: u v v 4 + + < 4 > < 4 >< 4 > Thn using th dot product ormula involving th gradint or th dirctional drivativ and th rsults or th gradint at th point P4 and u givn abov w obtain Th dirctional at th point drivativ Du 4 4 u P4 < > < 4 4 + + 48 4 53.6 >

9 Eampl 5: ind th maimum rat o chang o 4 and th dirction in which it occurs. 5 3 + at th point Solution:

Normal Lins to Suracs Rcall that givs a 3D surac in spac. W want to orm th ollowing unctions o 3 variabls Not that th unction is obtaind b moving all trms to on sid o an quation and stting thm qual to ro. W us th ollowing basic act. act: Givn a point on a surac th gradint o at this point i + j + k is a vctor orthogonal normal to th surac.

Eampl 6: ind a unit normal vctor to th surac + + 9 at th point Solution:

Tangnt Plans Using th gradint w can ind a quation o a plan tangnt to a surac and a lin normal to a surac. Considr th ollowing: Rcall that to writ quation o a plan w nd a point on th plan and a normal vctor. Sinc < > rprsnts a normal vctor to th surac and th tangnt plan its componnts can b usd to writ th quation o th tangnt plan at th point. Th quation o th tangnt plan is givn as ollows: + + Rcall to writ th quation o a lin in 3D spac w nd a point and a paralll vctor. Sinc < > is a vctor normal to th surac it would b paralll to an lin normal to th surac at. Thus th paramtric quations o th normal lin ar: t t t + + +.

3 W summari ths rsults as ollows. Tangnt Plan and Normal Lin Equations to a Surac Givn a surac in 3D orm th unction o thr variabls. Thn th quation o th tangnt plan to th surac at th point is givn b + + Th paramtric quations o th normal lin through th point ar givn b t t t + + +. Not: Rcall that to ind th smmtric quations o a lin tak th paramtric quations solv or t and st th rsults qual.

4 Eampl 7: ind th quation o th tangnt plan and th paramtric and smmtric quations or th normal lin to th surac + + 9 at th point. Solution:

5 Not: Th ollowing graph using Mapl shows th graph o th sphr + + 9 with th tangnt plan and normal lin at th point.

6 Eampl 8: ind th quation o th tangnt plan and th paramtric and smmtric quations or th normal lin to th surac at th point. Solution: W start b stting and computing th unction o 3 variabls Rcall that to gt an quation o an plan including a tangnt plan w nd a point and a normal vctor. W ar givn th point. Th normal vctor coms rom computing th gradint vctor o at this point. Rcall that or a givn point th gradint vctor at this point is givn b th ormula k j i + + Computing th ncssar partial drivativs w obtain Th givn point is. Thus sinc and th gradint vctor o at th point is k j k j i + + + W us th componnts o th gradint vctor to writ th quation o th tangnt plan using th ormula continud on nt pag

7 + + At th point this ormula bcoms + + Using th calculations or th partial drivativs givn on th prvious pag this quation bcoms or + + W can pand this quation to gt it in gnral orm. Doing this givs + + and whn combining lik trms w hav th quation o th tangnt plan 3 +. Th paramtric quations o th normal lin through th point ar givn b t t t + + + Using th calculations w computd abov whr that and w obtain + t + t + t which whn simpliid givs continud on nt pag

8 t t I w want to convrt this ths quations to smmtric orm w can tak th last two / quations o th prvious rsult and solv or t. This givs t and t. / Equation givs th smmtric quations o th normal lin. / / Th ollowing displas th graph o th unction and th normal lin at th point. th tangnt plan