there is no special reason why the value of y should be fixed at y = 0.3. Any y such that

Size: px
Start display at page:

Download "there is no special reason why the value of y should be fixed at y = 0.3. Any y such that"

Transcription

1 25. More on bivariate functions: partial erivatives integrals Although we sai that the graph of photosynthesis versus temperature in Lecture 16 is like a hill, in the real worl hills are three-imensional objects that can be climbe in several irections. So the sie of a real hill looks more like Figure 1(a), where the bivariate function P efine by P(x,y) y /2 is graphe on [0.1, 1] [0.1, 1]. As iscusse in Lecture 24, P(x, y) represents the power in kilowatts neee to keep an x-kilogram bir with a y-meter wing span in steay flight at the spee that minimizes fuel consumption over a given istance. In Figure 1, a possible path up the sie of the hill inclues KL, a possible path own inclues MN. The curve KL is the curve in which surface z P(x, y) meets vertical plane y 0., so KL has equation P(x, 0.) (0.) /2 0.21x 5/. Thus KL is the graph z f(x) of the orinary function f efine on [0.1, 1] by x 5/, which escribes how power requirement varies with mass in birs with a 0 cm wing span; see Figure 2(a). To etermine its graient f, we apply (22.1) with β 5/: f The graph of f also appears in Figure 2(a). Note that f is concave up f is concave own, in agreement with Exercise 2.2. Similarly, the curve MN is the curve in which surface z P(x, y) meets vertical plane x 0.8, so MN has equation P(0.8, y) y / y /2. Thus MN is the graph z g(y) of the orinary function g efine on [0.1, 1] by y /2, which escribes how power requirement varies with wing span in 800 gm birs; see Figure 2(b). To etermine its graient g, we apply (22.1) with β /2: g 250 (0.8)5/ y 5/ y 5/2. The graph of g also appears in Figure 2(b); again, in agreement with Exercise 2.2, g g are concave up concave own, respectively. Now, for climbing the sie of Figure 1's hill in a irection parallel to the x-axis, there is no special reason why the value of y shoul be fixe at y 0.. Any y such that 0.1 y 1 woul o, say y k. The corresponing curve KL woul be that in which surface z P(x, y) meets vertical plane y k, KL woul have equation 250 x5/ (25.1) z 250 x5/ (25.2) f(x) 250 (0.) /2 (25.) (x) (0.) /2 { x5/ } 250 (0.) /2 x x5/ (25.4) (0.) /2 x(5/ 1) 50 (0.) /2 x 2/ 0.65x 2/. z 250 (0.8)5/ (25.5) g(y) 250 (0.8)5/ (25.6) (y) 250 (0.8)5/ y y /2 { } (25.7) 2 y( /2 1) (0.8)5/

2 z P(x, k) M. Mesterton-Gibbons: Biocalculus, Lecture 25, Page x5/ k /2, (25.8) KL woul be the graph of the orinary function f efine on [0.1, 1] by f(x) 250 k /2 x 5/, (25.) instea of by (). Similarly, for escening in a irection parallel to the y-axis, there is no special reason why the value of x shoul be fixe at x 0.8. Any x such that 0.1 x 1 woul o, say x m. The corresponing curve MN woul be that in which surface z P(x, y) meets vertical plane x m, MN woul have equation z P(m, y) 250 m5/ y /2, (25.10) MN woul be the graph of the orinary function g efine on [0.1, 1] by g(y) 250 m5/ y /2, (25.11) instea of by (6). To obtain the graient along KL, all we nee o is to replace 0. by k in (4); to obtain the graient along MN, all we nee o is to replace 0.8 by m in (7). Thus we obtain in place of (4), f (x) 50 k /2 x 2/ g (y) m5/ y 5/2 (25.12) (25.1) in place of (7). Comparing (12)-(1) with (8)-(11), we observe that f (x) is z/x for KL g (y) is z/y for MN. Use of the symbol z/x implies that z epens only on x, whereas use of the symbol z/y implies that z epens only on y. Isn't this a contraiction? The answer is no, not really, because even though z epens on both x y in general, on KL the value of y is fixe, so that z epens only on x; whereas on MN the value of x is fixe, so z epens only on y. Nevertheless, there is potential for confusion, so we introuce some new notation. For a bivariate function P, we use z/x to enote the erivative of z P(x, y) with respect to x alone, i.e., with y hel fixe; we use z/y to enote the erivative of z P(x, y) with respect to y alone, i.e., with x hel fixe. That is, by analogy with (16.1b), we efine z x P(x + h,y) P(x,y) lim h 0 h (25.14) z y lim P(x,y + h) P(x,y). (25.15) h 0 We refer to z/x, i.e., the graient of z in a irection parallel to the x-axis, as the partial erivative of z with respect to x; to z/y, i.e., the graient of z in a irection parallel to the y-axis, as the partial erivative of z with respect to y. For example, in the case of Figure 1, where k enotes an arbitrary y-value m an arbitrary x-value, we can replace k by y in (12) to obtain z x we can replace m by x in (1) to obtain h 50 y /2 x 2/, (25.16)

3 M. Mesterton-Gibbons: Biocalculus, Lecture 25, Page z y x5/ y 5/2. (25.17) The partial erivatives of z P(x, y) yiel two new bivariate functions, say Q R. 1 That is, P(x + P(x,y) Q(x, y) lim h,y) h 0 h P(x,y + h) P(x,y) R(x, y) lim h 0 h For example, in the case of Figure 1, we have Q(x, y) 50 x2/ y /2 R(x,y) x5/ y 5/2 (25.18). (25.1) (25.20) (25.21) from (16)-(17). An important special case occurs when the function P is separable, i.e., when orinary functions F G exist such that P(x, y) F(x)G(y) (25.22) for any relevant x or y. Then (18) implies (1) implies or, in mixe notation, F(x + F(x)G(y) Q(x, y) lim h)g(y) h 0 h F(x + h) F(x) lim h 0 h F(x)G(y + F(x)G(y) R(x, y) lim G(yx + h) G(y) h 0 h) h 0 h F(x)lim h { x F(x)G(y) } F (x)g(y), 250 y /2 (25.2) G(y) F (x)g(y) F(x) G (y) (25.24) { y F(x)G(y) } F(x) G (y). (25.25) For example, P efine by (1) is separable; so, from z x 5/ y /2 /250, we calculate z x x x5/ 250 y /2 ( ) x x5/ 250 y /2 5 (25.26) x2/ 50 x2/ y /2 in agreement with (16), 1 If P has omain [, ] [a2, b2], then the omains of Q R are, respectively, [, ) [a2, b2] [, ] [a2, b2), by (1.25); i.e., x is, strictly speaking, exclue from the omain of Q, whereas y b2 is exclue from the omain of R. In practice, however, both omains can be extene to [, ] [a2, b2] by analogy with (1.26), i.e., by agreeing that Q(, y) is the limit of Q(x, y) as x R(x, b2) is the limit of R(x, y) as y b2.

4 z y y 250 x5/ 250 x5/ y /2 2 y 5/2 M. Mesterton-Gibbons: Biocalculus, Lecture 25, Page 4 ( ) 250 x5/ y y / x5/ y 5/2. (25.27) in agreement with (17). Furthermore, because Q is itself a bivariate function, it has its own partial erivatives, which are secon partial erivatives of z. We write 2 z x 2 x z x Q(x + h,y) Q(x,y) lim h 0 h 2 z z yx y x For example, in the case of Figure 1, (25)-(26) imply 2 z x 2 x 2 x 1/ whereas (25) (27) imply 2 z yx y 50 x2/ y /2 50 y /2 Q(x,y + h) Q(x,y) lim h 0 50 x2/ y /2 h { } x x2/ 50 y / x 1/ y /2, { } 50 x2/ y y /2 (25.28). (25.2) 50 x2/ 2 y 5/2 100 x2/ y 5/2. Likewise, because R is a bivariate function, we have secon partial erivatives 2 z xy x z y R(x + h,y) R(x,y) lim h 0 h 2 z 2 y z R(x,y + h) R(x,y) y y lim h 0 h In particular, in the case of Figure 1, (25)-(26) imply 2 z xy x x5/ y 5/2 x x5/ 5 x2/ y 5/2 whereas (25) (27) imply 2 z y 2 y x5/ y 5/ x5/ 5 2 y 7/2 by Exercise 1. Note that (1) (4) imply 2 z yx { } x2/ y 5/2, (25.0) (25.1) (25.2). (25.) 500 y 5/2 27 { } 500 x5/ y y 5/ x5/ y 7/2 (25.4) (25.5) 2 z xy. (25.6)

5 M. Mesterton-Gibbons: Biocalculus, Lecture 25, Page 5 This result hols not only for z in Figure 1, but also in general. 2 Thus, although in principle a bivariate function has four secon erivatives, efine by (28), (2), (2) (), in practice there are only three, because (6) makes (2) (2) equal. Now, from Lecture 24, if a bivariate function P has a global minimum on the interior of its omain at ( ˆx,ŷ), then ˆx must minimize the orinary function f efine by f(x) P(x, ŷ), whose graph is a vertical section through the graph of P along y ŷ; ŷmust minimize the orinary function g efine by g(y) P( ˆx, y), whose graph is a vertical section through the graph of P along x ˆx. Thus the partial erivative of P with respect to x along y ŷ must change sign from negative to positive at x ˆx, the partial erivate of P with respect to y along x ˆx must change sign from negative to positive at y ŷ. In other wors, Q( ˆx, ŷ) 0 R( ˆx, ŷ), (25.7) where Q R are efine by (18)-(1); or, in ifferential notation, z x x ˆx yŷ 0 z y x ˆx yŷ. (25.8) This pair of equations is sometimes useful for fining global minima. For example, in Appenix 2A we require the global minimum of S efine by S(α,β) α α β + 667αβ + 7β 2. (25.) Here, with z S(α, β), we have z α (4.26) 155 (α) α α α (α2 ) α z β β (β) α (αβ) + 7 α (β2 ) α β α + 667β (25.40) (4.26) 155 β (α) β (α2 ) β (β) β (αβ) + 7 β (β2 ) α + 7 2β α + 14β, (25.41) so that (8) yiels 601α + 667β α + 14β This pair of equations is reaily solve to yiel ˆα / ˆβ 26751/ , yieling a global minimum of S( ˆα, ˆβ) It is well to remember, however, that (8) isn't always so useful; for example, it wouln't have helpe much in Lecture 24. We conclue by broaching the concept of a partial integral, which is important in probability theory. Partial integration is the opposite of partial ifferentiation, in the sense that a partial erivative is the erivative of a bivariate function with respect to one variable, whereas a partial integral is the integral of a bivariate function with respect to one variable. Now, you know from Lecture 12 that the result of integrating P(x) between x x is inepenent of x, so the result of integrating P(x, y) between x x must also be inepenent of x. The ifference is simply that if P is orinary then Int(P, [, ]) epens only on, whereas if P is 2 More precisely, whenever z represents the height of a smooth surface, which is usually the case in practice. The result is sometimes calle Clairaut's Theorem. See Exercise 2 for an important special case.

6 M. Mesterton-Gibbons: Biocalculus, Lecture 25, Page 6 bivariate then Int(P, [, ]) can also epen on y. So enote it by W(y). Then, by analogy with (12.20), we efine the partial integral of P with respect to x by W(y) P(x, y)x lim P(x,y)δx δx 0. (25.42) [,b 1 ] Corresponingly, the partial integral of P with respect to y is efine by b 2 U(x) P(x, y)y lim P(x,y)δy δy 0. (25.4) a 2 [a 2,b2 ] Both U W are orinary functions, in Appenix 28C we will require an expression for their erivatives. It is simplest to obtain if we assume that P is separable. Then, by (22), orinary functions F G exist such that P(x, y) F(x)G(y). If we are integrating with respect to x, then G(y) behaves like a constant, so from (42) (12.25) with u F, k G(y) we have W (y) y F(x)G(y)x y G(y) F(x)x. (25.44) But if we are ifferentiating with respect to y, then Int(F, [, ]) behaves like a constant, so from (44) (16.17) with k Int(F, [, ]) we have W (y) G (y) F(x)x G (y)f(x)x (25.45) after applying (12.25) again, but this time with k G (y), which behaves like a constant if we are integrating with respect to x. Now, applying (25) to (45), we obtain W (y) F(x) G (y)x In other wors, on using (42), { y F(x)G(y) }x { y P(x,y) }x. (25.46) P(x, y)x y { y P(x,y) }x. (25.47a) A parallel argument establishes that b 2 P(x, y)y x x P(x,y) a (see Exercise 2). Inee (47a) (47b) are in essence the same result; although we have establishe it only for the case where P is separable, it can be shown to hol more { }y (25.47b) 2 generally. b 2 a 2 Exercises Establish (6) for the special case of a separable function, i.e., for z F(x)G(y) Establish (47b) for the special case where P is separable, i.e., P(x, y) F(x)G(y). Hint: Differentiate U in (4) with respect to x use (12.25) (16.17).

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

P(x) = 1 + x n. (20.11) n n φ n(x) = exp(x) = lim φ (x) (20.8) Our first task for the chain rule is to find the derivative of the exponential

P(x) = 1 + x n. (20.11) n n φ n(x) = exp(x) = lim φ (x) (20.8) Our first task for the chain rule is to find the derivative of the exponential 20. Derivatives of compositions: the chain rule At the en of the last lecture we iscovere a nee for the erivative of a composition. In this lecture we show how to calculate it. Accoringly, let P have omain

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

Exam 2 Review Solutions

Exam 2 Review Solutions Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

IMPLICIT DIFFERENTIATION

IMPLICIT DIFFERENTIATION IMPLICIT DIFFERENTIATION CALCULUS 3 INU0115/515 (MATHS 2) Dr Arian Jannetta MIMA CMath FRAS Implicit Differentiation 1/ 11 Arian Jannetta Explicit an implicit functions Explicit functions An explicit function

More information

Linear and quadratic approximation

Linear and quadratic approximation Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

05 The Continuum Limit and the Wave Equation

05 The Continuum Limit and the Wave Equation Utah State University DigitalCommons@USU Founations of Wave Phenomena Physics, Department of 1-1-2004 05 The Continuum Limit an the Wave Equation Charles G. Torre Department of Physics, Utah State University,

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

The Chain Rule. d dx x(t) dx. dt (t)

The Chain Rule. d dx x(t) dx. dt (t) The Chain Rule The Problem You alreay routinely use the one imensional chain rule t f xt = f x xt x t t in oing computations like t sint2 = cost 2 2t In this example, fx = sinx an xt = t 2. We now generalize

More information

MATH 1300 Lecture Notes Wednesday, September 25, 2013

MATH 1300 Lecture Notes Wednesday, September 25, 2013 MATH 300 Lecture Notes Wenesay, September 25, 203. Section 3. of HH - Powers an Polynomials In this section 3., you are given several ifferentiation rules that, taken altogether, allow you to quickly an

More information

Calculus and optimization

Calculus and optimization Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function

More information

II. First variation of functionals

II. First variation of functionals II. First variation of functionals The erivative of a function being zero is a necessary conition for the etremum of that function in orinary calculus. Let us now tackle the question of the equivalent

More information

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling.

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling. Chapter 8 Analytic Functions Stuents nee encouragement. So if a stuent gets an answer right, tell them it was a lucky guess. That way, they evelop a goo, lucky feeling. 1 8.1 Complex Derivatives -Jack

More information

Integration Review. May 11, 2013

Integration Review. May 11, 2013 Integration Review May 11, 2013 Goals: Review the funamental theorem of calculus. Review u-substitution. Review integration by parts. Do lots of integration eamples. 1 Funamental Theorem of Calculus In

More information

Introduction to variational calculus: Lecture notes 1

Introduction to variational calculus: Lecture notes 1 October 10, 2006 Introuction to variational calculus: Lecture notes 1 Ewin Langmann Mathematical Physics, KTH Physics, AlbaNova, SE-106 91 Stockholm, Sween Abstract I give an informal summary of variational

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Implicit Differentiation Using the Chain Rule In the previous section we focuse on the erivatives of composites an saw that THEOREM 20 (Chain Rule) Suppose that u = g(x) is ifferentiable

More information

Implicit Differentiation. Lecture 16.

Implicit Differentiation. Lecture 16. Implicit Differentiation. Lecture 16. We are use to working only with functions that are efine explicitly. That is, ones like f(x) = 5x 3 + 7x x 2 + 1 or s(t) = e t5 3, in which the function is escribe

More information

23 Implicit differentiation

23 Implicit differentiation 23 Implicit ifferentiation 23.1 Statement The equation y = x 2 + 3x + 1 expresses a relationship between the quantities x an y. If a value of x is given, then a corresponing value of y is etermine. For

More information

Further Differentiation and Applications

Further Differentiation and Applications Avance Higher Notes (Unit ) Prerequisites: Inverse function property; prouct, quotient an chain rules; inflexion points. Maths Applications: Concavity; ifferentiability. Real-Worl Applications: Particle

More information

Math 115 Section 018 Course Note

Math 115 Section 018 Course Note Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of

More information

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1 Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information

A. Incorrect! The letter t does not appear in the expression of the given integral

A. Incorrect! The letter t does not appear in the expression of the given integral AP Physics C - Problem Drill 1: The Funamental Theorem of Calculus Question No. 1 of 1 Instruction: (1) Rea the problem statement an answer choices carefully () Work the problems on paper as neee (3) Question

More information

Solutions to Practice Problems Tuesday, October 28, 2008

Solutions to Practice Problems Tuesday, October 28, 2008 Solutions to Practice Problems Tuesay, October 28, 2008 1. The graph of the function f is shown below. Figure 1: The graph of f(x) What is x 1 + f(x)? What is x 1 f(x)? An oes x 1 f(x) exist? If so, what

More information

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v Math Fall 06 Section Monay, September 9, 06 First, some important points from the last class: Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v passing through

More information

Chapter 2. Exponential and Log functions. Contents

Chapter 2. Exponential and Log functions. Contents Chapter. Exponential an Log functions This material is in Chapter 6 of Anton Calculus. The basic iea here is mainly to a to the list of functions we know about (for calculus) an the ones we will stu all

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

1 Lecture 13: The derivative as a function.

1 Lecture 13: The derivative as a function. 1 Lecture 13: Te erivative as a function. 1.1 Outline Definition of te erivative as a function. efinitions of ifferentiability. Power rule, erivative te exponential function Derivative of a sum an a multiple

More information

Many problems in physics, engineering, and chemistry fall in a general class of equations of the form. d dx. d dx

Many problems in physics, engineering, and chemistry fall in a general class of equations of the form. d dx. d dx Math 53 Notes on turm-liouville equations Many problems in physics, engineering, an chemistry fall in a general class of equations of the form w(x)p(x) u ] + (q(x) λ) u = w(x) on an interval a, b], plus

More information

Lagrangian and Hamiltonian Mechanics

Lagrangian and Hamiltonian Mechanics Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical

More information

4.2 First Differentiation Rules; Leibniz Notation

4.2 First Differentiation Rules; Leibniz Notation .. FIRST DIFFERENTIATION RULES; LEIBNIZ NOTATION 307. First Differentiation Rules; Leibniz Notation In this section we erive rules which let us quickly compute the erivative function f (x) for any polynomial

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments Problem F U L W D g m 3 2 s 2 0 0 0 0 2 kg 0 0 0 0 0 0 Table : Dimension matrix TMA 495 Matematisk moellering Exam Tuesay December 6, 2008 09:00 3:00 Problems an solution with aitional comments The necessary

More information

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0. Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?

More information

0.1 The Chain Rule. db dt = db

0.1 The Chain Rule. db dt = db 0. The Chain Rule A basic illustration of the chain rules comes in thinking about runners in a race. Suppose two brothers, Mark an Brian, hol an annual race to see who is the fastest. Last year Mark won

More information

Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS

Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS. An isosceles triangle, whose base is the interval from (0, 0) to (c, 0), has its verte on the graph

More information

Lecture 4 : General Logarithms and Exponentials. a x = e x ln a, a > 0.

Lecture 4 : General Logarithms and Exponentials. a x = e x ln a, a > 0. For a > 0 an x any real number, we efine Lecture 4 : General Logarithms an Exponentials. a x = e x ln a, a > 0. The function a x is calle the exponential function with base a. Note that ln(a x ) = x ln

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

The Principle of Least Action

The Principle of Least Action Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of

More information

Survival Facts from Quantum Mechanics

Survival Facts from Quantum Mechanics Survival Facts from Quantum Mechanics Operators, Eigenvalues an Eigenfunctions An operator O may be thought as something that operates on a function to prouce another function. We enote operators with

More information

Differentiation ( , 9.5)

Differentiation ( , 9.5) Chapter 2 Differentiation (8.1 8.3, 9.5) 2.1 Rate of Change (8.2.1 5) Recall that the equation of a straight line can be written as y = mx + c, where m is the slope or graient of the line, an c is the

More information

REAL ANALYSIS I HOMEWORK 5

REAL ANALYSIS I HOMEWORK 5 REAL ANALYSIS I HOMEWORK 5 CİHAN BAHRAN The questions are from Stein an Shakarchi s text, Chapter 3. 1. Suppose ϕ is an integrable function on R with R ϕ(x)x = 1. Let K δ(x) = δ ϕ(x/δ), δ > 0. (a) Prove

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

On the number of isolated eigenvalues of a pair of particles in a quantum wire

On the number of isolated eigenvalues of a pair of particles in a quantum wire On the number of isolate eigenvalues of a pair of particles in a quantum wire arxiv:1812.11804v1 [math-ph] 31 Dec 2018 Joachim Kerner 1 Department of Mathematics an Computer Science FernUniversität in

More information

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations Characterizing Real-Value Multivariate Complex Polynomials an Their Symmetric Tensor Representations Bo JIANG Zhening LI Shuzhong ZHANG December 31, 2014 Abstract In this paper we stuy multivariate polynomial

More information

Calculus in the AP Physics C Course The Derivative

Calculus in the AP Physics C Course The Derivative Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0. Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?

More information

February 21 Math 1190 sec. 63 Spring 2017

February 21 Math 1190 sec. 63 Spring 2017 February 21 Math 1190 sec. 63 Spring 2017 Chapter 2: Derivatives Let s recall the efinitions an erivative rules we have so far: Let s assume that y = f (x) is a function with c in it s omain. The erivative

More information

and from it produce the action integral whose variation we set to zero:

and from it produce the action integral whose variation we set to zero: Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Vectors in two dimensions

Vectors in two dimensions Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication

More information

Optimization Notes. Note: Any material in red you will need to have memorized verbatim (more or less) for tests, quizzes, and the final exam.

Optimization Notes. Note: Any material in red you will need to have memorized verbatim (more or less) for tests, quizzes, and the final exam. MATH 2250 Calculus I Date: October 5, 2017 Eric Perkerson Optimization Notes 1 Chapter 4 Note: Any material in re you will nee to have memorize verbatim (more or less) for tests, quizzes, an the final

More information

Section 7.2. The Calculus of Complex Functions

Section 7.2. The Calculus of Complex Functions Section 7.2 The Calculus of Complex Functions In this section we will iscuss limits, continuity, ifferentiation, Taylor series in the context of functions which take on complex values. Moreover, we will

More information

Zachary Scherr Math 503 HW 5 Due Friday, Feb 26

Zachary Scherr Math 503 HW 5 Due Friday, Feb 26 Zachary Scherr Math 503 HW 5 Due Friay, Feb 26 1 Reaing 1. Rea Chapter 9 of Dummit an Foote 2 Problems 1. 9.1.13 Solution: We alreay know that if R is any commutative ring, then R[x]/(x r = R for any r

More information

Applications of the Wronskian to ordinary linear differential equations

Applications of the Wronskian to ordinary linear differential equations Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.

More information

First Order Linear Differential Equations

First Order Linear Differential Equations LECTURE 6 First Orer Linear Differential Equations A linear first orer orinary ifferential equation is a ifferential equation of the form ( a(xy + b(xy = c(x. Here y represents the unknown function, y

More information

Chapter 3 Definitions and Theorems

Chapter 3 Definitions and Theorems Chapter 3 Definitions an Theorems (from 3.1) Definition of Tangent Line with slope of m If f is efine on an open interval containing c an the limit Δy lim Δx 0 Δx = lim f (c + Δx) f (c) = m Δx 0 Δx exists,

More information

Partial Differential Equations

Partial Differential Equations Chapter Partial Differential Equations. Introuction Have solve orinary ifferential equations, i.e. ones where there is one inepenent an one epenent variable. Only orinary ifferentiation is therefore involve.

More information

1 Heisenberg Representation

1 Heisenberg Representation 1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.

More information

Math Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis

Math Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis Math 231 - Chapter 2 Essentials of Calculus by James Stewart Prepare by Jason Gais Chapter 2 - Derivatives 21 - Derivatives an Rates of Change Definition A tangent to a curve is a line that intersects

More information

The Ehrenfest Theorems

The Ehrenfest Theorems The Ehrenfest Theorems Robert Gilmore Classical Preliminaries A classical system with n egrees of freeom is escribe by n secon orer orinary ifferential equations on the configuration space (n inepenent

More information

Chapter 6: Integration: partial fractions and improper integrals

Chapter 6: Integration: partial fractions and improper integrals Chapter 6: Integration: partial fractions an improper integrals Course S3, 006 07 April 5, 007 These are just summaries of the lecture notes, an few etails are inclue. Most of what we inclue here is to

More information

Computing Derivatives

Computing Derivatives Chapter 2 Computing Derivatives 2.1 Elementary erivative rules Motivating Questions In this section, we strive to unerstan the ieas generate by the following important questions: What are alternate notations

More information

13.1: Vector-Valued Functions and Motion in Space, 14.1: Functions of Several Variables, and 14.2: Limits and Continuity in Higher Dimensions

13.1: Vector-Valued Functions and Motion in Space, 14.1: Functions of Several Variables, and 14.2: Limits and Continuity in Higher Dimensions 13.1: Vector-Value Functions an Motion in Space, 14.1: Functions of Several Variables, an 14.2: Limits an Continuity in Higher Dimensions TA: Sam Fleischer November 3 Section 13.1: Vector-Value Functions

More information

Math 1B, lecture 8: Integration by parts

Math 1B, lecture 8: Integration by parts Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores

More information

The Natural Logarithm

The Natural Logarithm The Natural Logarithm -28-208 In earlier courses, you may have seen logarithms efine in terms of raising bases to powers. For eample, log 2 8 = 3 because 2 3 = 8. In those terms, the natural logarithm

More information

Mathcad Lecture #5 In-class Worksheet Plotting and Calculus

Mathcad Lecture #5 In-class Worksheet Plotting and Calculus Mathca Lecture #5 In-class Worksheet Plotting an Calculus At the en of this lecture, you shoul be able to: graph expressions, functions, an matrices of ata format graphs with titles, legens, log scales,

More information

Topic 2.3: The Geometry of Derivatives of Vector Functions

Topic 2.3: The Geometry of Derivatives of Vector Functions BSU Math 275 Notes Topic 2.3: The Geometry of Derivatives of Vector Functions Textbook Sections: 13.2 From the Toolbox (what you nee from previous classes): Be able to compute erivatives scalar-value functions

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

Balancing Expected and Worst-Case Utility in Contracting Models with Asymmetric Information and Pooling

Balancing Expected and Worst-Case Utility in Contracting Models with Asymmetric Information and Pooling Balancing Expecte an Worst-Case Utility in Contracting Moels with Asymmetric Information an Pooling R.B.O. erkkamp & W. van en Heuvel & A.P.M. Wagelmans Econometric Institute Report EI2018-01 9th January

More information

Rules of Differentiation

Rules of Differentiation LECTURE 2 Rules of Differentiation At te en of Capter 2, we finally arrive at te following efinition of te erivative of a function f f x + f x x := x 0 oing so only after an extene iscussion as wat te

More information

Chapter Primer on Differentiation

Chapter Primer on Differentiation Capter 0.01 Primer on Differentiation After reaing tis capter, you soul be able to: 1. unerstan te basics of ifferentiation,. relate te slopes of te secant line an tangent line to te erivative of a function,.

More information

Chapter 9 Method of Weighted Residuals

Chapter 9 Method of Weighted Residuals Chapter 9 Metho of Weighte Resiuals 9- Introuction Metho of Weighte Resiuals (MWR) is an approimate technique for solving bounary value problems. It utilizes a trial functions satisfying the prescribe

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

Physics 115C Homework 4

Physics 115C Homework 4 Physics 115C Homework 4 Problem 1 a In the Heisenberg picture, the ynamical equation is the Heisenberg equation of motion: for any operator Q H, we have Q H = 1 t i [Q H,H]+ Q H t where the partial erivative

More information

Fall 2016: Calculus I Final

Fall 2016: Calculus I Final Answer the questions in the spaces provie on the question sheets. If you run out of room for an answer, continue on the back of the page. NO calculators or other electronic evices, books or notes are allowe

More information

Abstract A nonlinear partial differential equation of the following form is considered:

Abstract A nonlinear partial differential equation of the following form is considered: M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent

More information

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs Problem Sheet 2: Eigenvalues an eigenvectors an their use in solving linear ODEs If you fin any typos/errors in this problem sheet please email jk28@icacuk The material in this problem sheet is not examinable

More information

1 Lecture 20: Implicit differentiation

1 Lecture 20: Implicit differentiation Lecture 20: Implicit ifferentiation. Outline The technique of implicit ifferentiation Tangent lines to a circle Derivatives of inverse functions by implicit ifferentiation Examples.2 Implicit ifferentiation

More information

Short Intro to Coordinate Transformation

Short Intro to Coordinate Transformation Short Intro to Coorinate Transformation 1 A Vector A vector can basically be seen as an arrow in space pointing in a specific irection with a specific length. The following problem arises: How o we represent

More information

Chaos, Solitons and Fractals Nonlinear Science, and Nonequilibrium and Complex Phenomena

Chaos, Solitons and Fractals Nonlinear Science, and Nonequilibrium and Complex Phenomena Chaos, Solitons an Fractals (7 64 73 Contents lists available at ScienceDirect Chaos, Solitons an Fractals onlinear Science, an onequilibrium an Complex Phenomena journal homepage: www.elsevier.com/locate/chaos

More information

5.4 Fundamental Theorem of Calculus Calculus. Do you remember the Fundamental Theorem of Algebra? Just thought I'd ask

5.4 Fundamental Theorem of Calculus Calculus. Do you remember the Fundamental Theorem of Algebra? Just thought I'd ask 5.4 FUNDAMENTAL THEOREM OF CALCULUS Do you remember the Funamental Theorem of Algebra? Just thought I' ask The Funamental Theorem of Calculus has two parts. These two parts tie together the concept of

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides Reference 1: Transformations of Graphs an En Behavior of Polynomial Graphs Transformations of graphs aitive constant constant on the outsie g(x) = + c Make graph of g by aing c to the y-values on the graph

More information

Function Spaces. 1 Hilbert Spaces

Function Spaces. 1 Hilbert Spaces Function Spaces A function space is a set of functions F that has some structure. Often a nonparametric regression function or classifier is chosen to lie in some function space, where the assume structure

More information

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes Implicit Differentiation 11.7 Introuction This Section introuces implicit ifferentiation which is use to ifferentiate functions expresse in implicit form (where the variables are foun together). Examples

More information