Problem set 2 due Friday June 1 by 7 pm in class or in the mailbox. Problem 1. Compute the determinants of the following matrices. (a) 1 0 1 1 0 1 0 1 1 (b) 1 2 0 1 2 3 1 0 4 (c) −6 −3 0 3 1 0 0 0 3 (d) 2 −1 −3 1 4 −1 −1 2 0 (e) 1 −1 −3 2 0 4 1 0 2 (f) −2 0 0 0 2 1 0 −1 2 Hint : Two of those determinants can be directly seen to be 0 because of linear dependence. Two of these matrices are actually block diagonal, and thus you can reduce to computing the determinant of a 2 × 2 matrix. For the other two determinants, you can either use the general formula, or expand the determinant along a well chosen line or column. Problem 2. Let f (x, y) be a nicely behaved function of two variables of which you only know that f (1, 0) = 2, fx (1, 0) = 0 and fy (1, 0) = 1. 1 (a) What’s your best guess for f (1.01, −0.03) ? (b) You are now told that fxx (1, 0) = −1, fxy (1, 0) = 1 and fyy (1, 0) = 1. What is your answer to the previous question now ? Problem 3. Compute the Taylor approximation of order two of the following functions. (a) sin(x) ex at x = 0 (b) ln(x + ey ) at (x, y) = (0, 0) (c) xy at (x, y) = (1, 1) Problem 4. 3 Consider the function f (x) = x3 + 2x2 defined on the closed interval [−5, 5]. Which interior points are local minima ? Which ones are local maxima ? What are the global extrema and what are the minimum and maximum values of f on [−5, 5] ? Hint : Don’t forget the two boundary points. Problem 5. On Fermat’s principle. You’re a lifeguard on the beach at point A of coordinates (0, h1 ), and spot someone seemingly in trouble in the sea at point B = (l, −h2 ). You need to minimize you travel time to this point. The beach/sea interface is the horizontal line y = 0. You’ll run in a straight line to a point P = (x, 0) and from there swim in a straight line to point B. (a) Express d1 , the distance between A and P as a function of the parameters introduced above. Compute similarly d2 , the distance between P and B Hint : You can use Pythagoras’ theorem. (b) Recall that the time of travel is given by length = speed × time. Write down the time t1 it takes you to cover the distance AP on the beach, in terms of d1 and of your running speed, s1 . Compute similarly the time t2 it takes you to cover the distance P B in the sea, knowing your swimming speed is s2 . (c) As a lifeguard, you’re required to minimize your total time of travel T (x) = t1 + t2 by chosing in a clever way the best value for x, i.e. the best position for the point P where you’re going to enter the sea. Consider the incidence angles θ1 and θ2 (in other words, θ1 (respectively θ2 ) is the angle the segment AP (respectively BP ) makes with a vertical line). Check, using trigonometry in relevant triangles, that sin θ1 = x/d1 , and sin θ2 = (l − x)/d2 . Explain using a calculus computation why Snell’s law (s2 sin θ1 = s1 sin θ2 ) is a necessary condition on x for the total time function T (x) to have a local extrema at x. Hint : if you take a derivative, don’t forget that quantities such as d1 or θ1 are functions of x. (d) We now want to prove that T has a unique global minimum. 2 If x < 0 or x > l, show - by a quick common sense argument - that T attains values strictly smaller than T (x) on the interval [0, l]. Show that on [0, l], sin θ1 is increasing in x whereas sin θ2 is decreasing in x. Use this to show that there is a unique point x∗ in [0, l] for which Snell’s law is satisfied (you can for example consider the quantity sin θ1 / sin θ2 ). (e*) Show that T has a unique global minimum, at x∗ . You can for example use the results of (d) and try to adapt to the function T (x) the "compactness" 2 argument given in class for the function of two variables ex + y 2 . Problem 6. A naive approach to a minimization problem with constraint. Consider a rectangular parallelepiped i.e. a box, the faces of which are rectangles. Let us call its edge sizes x, y and z. (a) Express the surface area A (the box is closed : it has six faces), and the volume V of the box as functions of the three edge sizes. (b) We want to minimize the surface area A(x, y, z), for a fixed volume V (x, y, z) = V0 (i.e. we restrict the domain of A to those points (x, y, z) satisfying the equation V (x, y, z) = V0 ). Under the constraint V = V0 , express z as a function of x, y and V0 , and use this to rewrite A as a function of the two variables x and y. Show that A(x, y) admits a unique local minimum. (c**) Discuss globality. You can try a "compactness" argument i.e. mimick what I did in class for 2 the function ex + y 2 . Recall that the core of the argument was to show that out of a region not too big, the function takes values too big to matter when looking for a minimum. For example, you can : - Assume c ≥ x > 0. Check A ≥ V /c. - Show (by a drawing in the xy plane) that the three conditions x ≥ c, y ≥ c and z ≥ c cut out a region fitting our purpose (i.e. a region that stays away from infinity, and from the boundaries x = 0 and y = 0). -Conclude. (d) We would now like to solve a very related problem, namely maximizing the volume V (x, y, z), for a fixed surface area A(x, y, z) = A0 . Express z as a function of x, y and A0 . Notice that it is not a very friendly-looking formula. One can still solve the problem with the technique used in (b) but the computation is quite messy. We’ll thus use a somewhat indirect approach (we’ll see later in class a technique to solve this problem with a direct but much easier computation). (e) Using the result of (b), we’re going to prove that x = y = z = with constraint A = A0 . p A0 /6 is a global maximum of V 0 0 0 0 0 0 Argue by contradition p p: suppose p you can find a point (x , y , z ) satisfying A(x , y , z ) = A0 and 0 0 0 V (x , y , z ) > V ( A0 /6, A0 /6, A0 /6). By rescaling the box (x0 , y 0 , z 0 ), find a contradiction with the result of (b). Conclude. 3
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