Math 53 Worksheet Solutions- Minmax and Lagrange



Similar documents
(a) We have x = 3 + 2t, y = 2 t, z = 6 so solving for t we get the symmetric equations. x 3 2. = 2 y, z = 6. t 2 2t + 1 = 0,

1 3 4 = 8i + 20j 13k. x + w. y + w

SOLUTIONS. f x = 6x 2 6xy 24x, f y = 3x 2 6y. To find the critical points, we solve

( 1) = 9 = 3 We would like to make the length 6. The only vectors in the same direction as v are those

Solutions for Review Problems

Section 12.6: Directional Derivatives and the Gradient Vector

Linear and quadratic Taylor polynomials for functions of several variables.

SECOND DERIVATIVE TEST FOR CONSTRAINED EXTREMA

5.7 Maximum and Minimum Values

Name: ID: Discussion Section:

Adding vectors We can do arithmetic with vectors. We ll start with vector addition and related operations. Suppose you have two vectors

Math 265 (Butler) Practice Midterm II B (Solutions)

42 CHAPTER 1. VECTORS AND THE GEOMETRY OF SPACE. Figure 1.18: Parabola y = 2x Brief review of Conic Sections

Section 1. Finding Common Terms

This makes sense. t /t 2 dt = 1. t t 2 + 1dt = 2 du = 1 3 u3/2 u=5

FINAL EXAM SOLUTIONS Math 21a, Spring 03

Review Sheet for Test 1

COLLEGE ALGEBRA. Paul Dawkins

Maximizing volume given a surface area constraint

2 Integrating Both Sides

Practice Final Math 122 Spring 12 Instructor: Jeff Lang

Solutions to Homework 10

Math 120 Final Exam Practice Problems, Form: A

1.5. Factorisation. Introduction. Prerequisites. Learning Outcomes. Learning Style

1.7 Graphs of Functions

Practice with Proofs

To give it a definition, an implicit function of x and y is simply any relationship that takes the form:

Limits and Continuity

Exam 1 Sample Question SOLUTIONS. y = 2x

L 2 : x = s + 1, y = s, z = 4s Suppose that C has coordinates (x, y, z). Then from the vector equality AC = BD, one has

Constrained optimization.

correct-choice plot f(x) and draw an approximate tangent line at x = a and use geometry to estimate its slope comment The choices were:

constraint. Let us penalize ourselves for making the constraint too big. We end up with a

Equations Involving Lines and Planes Standard equations for lines in space

1 Lecture: Integration of rational functions by decomposition

Solving DEs by Separation of Variables.

APPLICATIONS. are symmetric, but. are not.

Solutions to Homework 5

MATH 21. College Algebra 1 Lecture Notes

+ 4θ 4. We want to minimize this function, and we know that local minima occur when the derivative equals zero. Then consider

Factoring - Greatest Common Factor

Factoring Flow Chart

Solutions to Practice Problems for Test 4

SOLUTIONS TO HOMEWORK ASSIGNMENT #4, MATH 253

Name Intro to Algebra 2. Unit 1: Polynomials and Factoring

In this section, we will consider techniques for solving problems of this type.

Module 1 : Conduction. Lecture 5 : 1D conduction example problems. 2D conduction

CHAPTER 8, GEOMETRY. 4. A circular cylinder has a circumference of 33 in. Use 22 as the approximate value of π and find the radius of this cylinder.

299ReviewProblemSolutions.nb 1. Review Problems. Final Exam: Wednesday, 12/16/2009 1:30PM. Mathematica 6.0 Initializations

Basic Properties of Rational Expressions

Factor Polynomials Completely

Math 241, Exam 1 Information.

Mathematics Placement

Derive 5: The Easiest... Just Got Better!

ALGEBRA I (Common Core)

Determine whether the following lines intersect, are parallel, or skew. L 1 : x = 6t y = 1 + 9t z = 3t. x = 1 + 2s y = 4 3s z = s

Solutions - Homework sections

FACTORING ax 2 bx c. Factoring Trinomials with Leading Coefficient 1

Unit 1 Equations, Inequalities, Functions

Section 9: Applied Optimization

CAHSEE on Target UC Davis, School and University Partnerships

Lecture L26-3D Rigid Body Dynamics: The Inertia Tensor

SAT Math Facts & Formulas Review Quiz

If Σ is an oriented surface bounded by a curve C, then the orientation of Σ induces an orientation for C, based on the Right-Hand-Rule.

Constrained Optimization: The Method of Lagrange Multipliers:

Lagrange Interpolation is a method of fitting an equation to a set of points that functions well when there are few points given.

Solutions to old Exam 1 problems

Finding the Measure of Segments Examples

Prot Maximization and Cost Minimization

5 Systems of Equations

Two vectors are equal if they have the same length and direction. They do not

2.3. Finding polynomial functions. An Introduction:

The Fourth International DERIVE-TI92/89 Conference Liverpool, U.K., July Derive 5: The Easiest... Just Got Better!

~ EQUIVALENT FORMS ~

Factoring Polynomials

Click on the links below to jump directly to the relevant section

1.1 Practice Worksheet

REVIEW EXERCISES DAVID J LOWRY

Increasing for all. Convex for all. ( ) Increasing for all (remember that the log function is only defined for ). ( ) Concave for all.

Line and surface integrals: Solutions

Simplify the rational expression. Find all numbers that must be excluded from the domain of the simplified rational expression.

Polynomials. Key Terms. quadratic equation parabola conjugates trinomial. polynomial coefficient degree monomial binomial GCF

How To Solve Factoring Problems

3. Solve the equation containing only one variable for that variable.

0.8 Rational Expressions and Equations

5 Double Integrals over Rectangular Regions

Factoring Trinomials of the Form x 2 bx c

Negative Integer Exponents

FACTORING POLYNOMIALS

Understanding Basic Calculus


Definitions 1. A factor of integer is an integer that will divide the given integer evenly (with no remainder).

Math 432 HW 2.5 Solutions

Recognizing Types of First Order Differential Equations E. L. Lady

Math Review. for the Quantitative Reasoning Measure of the GRE revised General Test

CNC Applications. Introduction to Machining Centers

The Theory and Practice of Using a Sine Bar, version 2

8 Polynomials Worksheet

SPECIAL PRODUCTS AND FACTORS

Chapter 7 - Roots, Radicals, and Complex Numbers

Transcription:

Math 5 Worksheet Solutions- Minmax and Lagrange. Find the local maximum and minimum values as well as the saddle point(s) of the function f(x, y) = e y (y x ). Solution. First we calculate the partial derivatives and set them equal to zero. f x (x, y) = xe y = 0, f y (x, y) = e y (y x ) + ye y = 0. For the first equation, e y 0, so we have x = 0. Plugging this in to the second equation, we have e y [y + y] = 0, and since again e y 0, we have y = 0 and y =. So our two critical points are (0, 0) and (0, ). We now must check what kind of critical points these are. To do this we need the second and mixed partials, f xx (x, y) = e y, f yy (x, y) = e y (y x + y) + e y (y + ), f xy (x, y) = xe y. At the point (0, 0), we have and so f xx (0, 0) =, f yy (0, 0) =, f xy (0, 0) = 0, D = f xx (0, 0)f yy (0, 0) [f xy (0, 0)] = 4 < 0, and since f xx (0, 0) < 0, we know that f has a local maximum at (0,0) by the second derivative test. At the point (0, ), we have and so f xx (0, ) = e, f yy (0, ) = e, f xy (0, ) = 0, so f has a saddle point at (0, ). D = f xx (0, )f yy (0, ) [f xy (0, )] = 4 > 0,. Find the absolute maximum and minimum values of f(x, y) = x + y 4 on the set D = {(x, y) x + y }. Solution. Recall the method for find absolute maxima and minima:. Find the critical points of f. No second derivative test is needed.. Find the values of f at the function s critical points.. Find the extreme values of f on the boundary of the region in question. (Don t forget endpoints!) 4. The largest value from () and () is the maximum; the smallest is the minimum.

With these in mind, we re ready to attack the problem. So let s find the critical points by taking partials. f x (x, y) = 6x = 0, f y (x, y) = 4y = 0, so (x, y) = (0, 0) is the only critical point. And note that f(0, 0) = 0. Now we must look at the boundary, the circle x + y =. On this circle, y = x, so define g(x) = f(x, y) = x + ( x ), and we will now find the extra of g(x) as in traditional one-variable calculus. First calculate the derivative and set equal to zero. g (x) = 6x 4x( x ) = 0 = x[x + x ] = 0, and so we have solutions x = 0 and x = ± 9 + 6 =,, but we can ignore the solution x = as we seek to find the extrema of g(x) on the interval [, ]. So we have g(0) =, g( ) = 6. But we still need to check the endpoints of g, since we re finding its extrema on a closed interval! Note that g( ) =, g() =. Looking back at all the values of f(x, y), it turns out that the maximum occurs at (, 0) and the minimum at (, 0). (Remember that g( ) = f(, 0) and g() = f(, 0).). Use Lagrange multipliers to find the maximum and minimum values of the function f(x, y) = x y z subject to the constraint x + y + z =. Solution. The function we re finding extrema of is f(x, y, z) = x y z and the constraint is g(x, y, z) = x + y + z = 0. Then f(x, y, z) = xy z, yx z, zx y, g(x, y, z) = x, y, z, and so we must solve f = λ g. This equation is actually the three equations, xy z = xλ, yx z = yλ, zx y = xλ, along with the constraint equation. Observe that if any one of x, y, z is zero. Then f(x, y, z) = 0, according to the equation for f(x, y, z). If none of the variables is equal to zero, then the equations become λ = y z = x z = x y,

and because x, y, z 0, this indicates that x = y = z. The constraint is then x = 0, or x =. In this case, f (,, ) ( ) 6 = = 7. So the maximum occurs at (x, y, z) = (,, ) and the minimum occurs at any point (x, y, z) where one of the variables is zero. The maximum value is and the 7 minimum value is 0. 4. The plane x + y + z = intersects the paraboloid z = x + y in an ellipse. Find the points on this ellipse that are nearest to and farthest from the origin. Solution. The key here is that we needn t worry about the equation of the ellipse formed by the intersection; instead, we regard the two surfaces as constraints and seek to minimize the distance from the origin. More precisely, we ll minimize f(x, y, z) = x + y + z, the distance squared, since this is minimized precisely when the distance is, and this function is a lot easier to work with. You should remember this trick. The constraints then are We must now solve So we calculate, g(x, y, z) = x + y + z = 0, h(x, y, z) = x + y z = 0. f = λ g + µ h. f = x, y, z, g =,,, h = x, y,. And the equation we must solve becomes three equations, in addition to the two constraints. x = λ + xµ, y = λ + yµ, z = λ µ. Solving five equations for five unknowns can get tricky, to say the least. One idea is to observe that the first two equations above are quite similar. In fact, we can write x xµ = λ = y yµ = (x y)( µ) = 0. And so either µ = or x = y. First consider the case where µ =. Then from the first equation above, λ = 0. Then z =. But then x + y =, and there are clearly no solutions in this case. So now assume x = y. At this point, we can dispense with solving for λ and µ entirely. (Remember, nothing about the problem insists we find their values!) So, going back to the original constraints, we have x + z =, x = z.

These are much simpler! From the first equation, we get z = x, so the second then shows x + x = 0, and this factors as (x )(x + ) = 0, so x = and x = are solutions. So the two critical points are (,, ) and (,, ). Now we just calculate that ( f,, ) =, f(,, ) = 6, 4 and these are the minimum and maximum values, respectively. (Where minimum means the point closest to the origin and maximum is the point furthest.) 5. If the length of the diagonal of a rectangular box must be L, what is the largest possible volume? Solution. It s not hard to see that if the side lengths are x, y, and z, then the length of the diagonal L and the volume V satisfy L = x + y + z, V = xyz. Now, we could use Lagrange multipliers to solve this problem, but let s do it first without such an advanced technique. To implement the constraint, we solve for z in the first equation and get z = L x y, so that we can write V (x, y) = xy L x y. And now we just need to maximize V with the constraints x, y > 0 and x + y L. So, first we find the critical points. V x (x, y) = y x y L x y L x y, Setting the components equal to zero gives L x y [ L x y ] y = 0, V y(x, y) = x xy L x y L x y. and L x y [ L x y ] x = 0. Now x, y 0, as noted above, so we must have L x y = 0, L x y = 0. Write the first equation as y = L x and substitute into the second. We then have L x (L x ) = 0, = x = L, and so x = L. Substituting this into the first equation, it follows that y = L. So the maximum volume is obtained when x = y = z = L, 4

and the volume then is ( ) L V = = L. The problem is indeed easier with Lagrange. Here f(x, y, z) = xyz and g(x, y, z) = x + y + z L = 0. Then f(x, y, z) = yz, xz, xy, g(x, y, z) = x, y, z, and the equations are yz = xλ, xz = yλ, xy = zλ. Then xyz = x λ = y λ = z λ, which we obtain by multiplying each equation by x, y, and z respectively. Thus either λ = 0 or x = y = z, since x, y, z > 0. If λ = 0, then at least one of x, y, z is zero, which cannot happen. So we must have x = y = z and, from the constraint equation, this means we must have x = y = z = L. Then, again, we find that ( ) L V = = L. 5