Mahler Expansions

Total Page:16

File Type:pdf, Size:1020Kb

Mahler Expansions MAHLER EXPANSIONS KEITH CONRAD 1. Introduction The set C([0; 1]; R) of all continuous functions f : [0; 1] ! R is a basic example of a function space in real analysis, and its p-adic analogue is the set C(Zp; Qp) of all continuous functions f : Zp ! Qp. These are analogues both because [0; 1] and Zp are compact and because R and Qp are both complete. Examples of continuous functions are polynomials on [0; 1] with real coefficients and polynomials on Zp with p-adic coefficients. A metric can be put on C([0; 1]; R) and C(Zp; Qp) by measuring the distance between two functions as the largest distance between their values: 8 < max jf(x) − g(x)j if f; g : [0; 1] ! R; (1.1) d(f; g) = x2[0;1] :max jf(x) − g(x)jp if f; g : Zp ! Qp: x2Zp The maximum really occurs because jf(x) − g(x)j in the real case and jf(x) − g(x)jp in the p-adic case are continuous functions [0; 1] ! R and Zp ! R, and any real-valued continuous function on a compact metric space has a maximum value (Extreme Value Theorem). Theorem 1.1. The function d in (1:1) is a metric and the spaces C([0; 1]; R) and C(Zp; Qp) are complete with respect to it. Proof. See the appendix. In both C([0; 1]; R) and C(Zp; Qp), the polynomial functions are a dense subset: (1) if f : [0; 1] ! R is continuous and " > 0 there is a polynomial p(x) with real coefficients such that jf(x) − p(x)j < " for all x 2 [0; 1]. (2) if f : Zp ! Qp is continuous and " > 0 there is a polynomial p(x) with coefficients in Qp such that jf(x) − p(x)j < " for all x 2 Zp. In the real case, the denseness of polynomials in C([0; 1]; R) is due to Weierstrass1 (1885). The denseness of polynomials in C(Zp; Qp) was first proved by Dieudonne (1944). While there is no nice description of all the functions in C([0; 1]; R) (they are not describable as power series, since power series are infinitely differentiable and a continuous function need not be even once differentiable everywhere), in 1958 Mahler [3] gave a very nice description of all functions in C(Zp; Qp) using infinite series of special polynomials. Theorem 1.2 (Mahler). Every continuous function f : Zp ! Qp can be written in the form X x x x (1.2) f(x) = a = a + a x + a + a + ··· n n 0 1 2 2 3 3 n≥0 1This was later generalized by Stone to a result now called the Stone{Weierstrass theorem, describing conditions under which a suitable collection of continuous real or complex-valued functions on a compact space is dense in the set of all continuous functions on that space. 1 2 KEITH CONRAD for all x 2 Zp, where an 2 Qp and an ! 0 as n ! 1. We'll see there is a formula for the coefficients an in terms of values of f that is reminiscent of Taylor's formula for the coefficients of a power series, but it must be stressed that (1.2) represents an arbitrary continuous function, not a function expressible by a power series. x Just because each n is differentiable (even infinitely differentiable) does not mean the series in (1.2) has that property too. This is similar to the \paradox" of Fourier series, where continuous functions [0; 1] ! R have a representation as an infinite series of sines and cosines, but need not be differentiable even though sin(nx) and cos(nx) are differentiable. The expansion (1.2) is called the Mahler expansion of f and the numbers an are called PN x the Mahler coefficients of f. If fN (x) is the polynomial n=0 an n then jf(x) − fN (x)jp = P x j n≥N+1 an n jp ≤ maxn≥N+1 janjp since binomial coefficients at p-adic integers are p-adic integers. This maximum goes to 0 as N ! 1 since an ! 0, so Mahler's theorem is an explicit (and useful!) way of approximating continuous functions Zp ! Qp by polynomials. 2. Continuity and coefficient formula Before we show every continuous function Zp ! Qp has a Mahler expansion, let's see P x why an infinite series n≥0 an n with an ! 0 in Qp is a continuous function on Zp. P x Step 1: When an ! 0 in Qp, the infinite series n≥0 an n converges for all x 2 Zp. x The key point is that even though n = x(x − 1) ··· (x − (n − 1))=n! has n! in the denominator, which would ordinarily be bad p-adically (because n! is very small p-adically x as n grows), it is not bad when x 2 Zp because n 2 Zp by p-adic continuity of polynomials x x and its values on the dense subset N. Thus j n jp ≤ 1 for x 2 Zp, so jan n jp ≤ janjp, which x P x proves jan n jp ! 0 from janjp ! 0. Therefore n≥0 an n converges in Qp for each x 2 Zp. P x Step 2: When an ! 0 in Qp, the function f : Zp ! Qp defined by f(x) = n≥0 an n is continuous. For x0 2 Zp we want to prove f is continuous at x0. Pick " > 0. Since an ! 0, there is an x N such that janjp < " for n ≥ N. Each of the finitely many functions n for 0 ≤ n ≤ N − 1 is continuous at x0, so by picking the minimal δ used for each of them in the "-δ definition of continuity at x0, there is a single δ > 0 such that x x0 (2.1) jx − x0jp < δ =) − < " n n p for n 2 f0; 1;:::;N − 1g. If jx − x0jp < δ, X x x0 x x0 jf(x) − f(x0)jp = an − ≤ max janjp − : n n n≥0 n n n≥0 p p x x0 x x0 Since n − n 2 Zp we have janjpj n − n jp ≤ janjp < " for n ≥ N. For the terms x x0 preceding the Nth term, we instead say janjp n − n p ≤ janjp" by (2.1). Let A = maxn≥0 janjp (this exists since the an's tend to 0), so janjp ≤ A for all n. Thus jx − x0jp < δ =) jf(x) − f(x0)jp ≤ max("; A") = max(1;A)"; so f is continuous at x0. As x0 was arbitrary, f is continuous on Zp. MAHLER EXPANSIONS 3 P x Next we will derive a formula for the coefficients in f(x) = n≥0 an n if an ! 0 in Qp. It is easy to get the value of the constant term: setting x = 0 in (1.2) we obtain a0 = f(0) since all terms vanish in the Mahler expansion except the one at n = 0. Similarly, if x = 1 then all terms in (1.2) vanish except for the first two: f(1) = a0 +a1, so a1 = f(1)−a0 = f(1)−f(0). Setting x = 2, all terms in (1.2) vanish except the first three: f(2) = a0 + 2a1 + a2, so a2 = f(2) − a0 − 2a1 = f(2) − f(0) − 2(f(1) − f(0)) = f(2) − 2f(1) + f(0): These formulas suggest we can write an in terms of f(0); f(1); : : : ; f(n), and we will see this is true. The basic mechanism behind a formula for an is the discrete difference operator ∆: for any function f : Zp ! Qp, define ∆f : Zp ! Qp by (∆f)(x) = f(x + 1) − f(x): n This is also a function Zp ! Qp, and it can be iterated to have functions ∆ f for n ≥ 2: ∆2f = ∆(∆f), and more generally ∆nf = ∆(∆n−1f). Set ∆0f = f, which is analogous to the zeroth derivative f (0) of a function f being the function itself. The discrete difference operator ∆ behaves nicely on the binomial coefficient polynomials x x x because it shifts them down by one: ∆ n = n−1 for n ≥ 1, and ∆ 0 = ∆(1) is the zero function. Indeed, by the Pascal's triangle recursion for binomial coefficients, if n ≥ 1 then x x + 1 x x x x x ∆ = − = + − = : n n n n − 1 n n n − 1 This resembles the effect of differentiation on xn:(xn)0 = nxn−1 for n ≥ 1, and (xn)0 = 0 for n = 0. (A more accurate analogy would be with differentiation on the functions xn=n!, n−1 whose derivative is x =(n − 1)! for n ≥ 1.) Applying ∆ to a function f : Zp ! Qp having P x a Mahler expansion n≥0 an n where an ! 0, X x + 1 X x X x + 1 x X x (∆f)(x) = a − a = a − = a ; n n n n n n n n n − 1 n≥0 n≥0 n≥0 n≥1 where a0 drops out and other coefficients shift down one position. Reindexing the series to start at n = 0, X x X x x x ∆ a = a = a + a x + a + a + ··· : n n n+1 n 1 2 3 2 4 3 n≥0 n≥0 The effect of applying ∆ to a Mahler expansion m times is to shift coefficients m positions: X x X x x x ∆m a = a = a + a x + a + a + ··· : n n n+m n m m+1 m+2 2 m+3 3 n≥0 n≥0 Setting x = 0 leaves only the constant term am, so we have proved the following theorem.
Recommended publications
  • Selected Solutions to Assignment #1 (With Corrections)
    Math 310 Numerical Analysis, Fall 2010 (Bueler) September 23, 2010 Selected Solutions to Assignment #1 (with corrections) 2. Because the functions are continuous on the given intervals, we show these equations have solutions by checking that the functions have opposite signs at the ends of the given intervals, and then by invoking the Intermediate Value Theorem (IVT). a. f(0:2) = −0:28399 and f(0:3) = 0:0066009. Because f(x) is continuous on [0:2; 0:3], and because f has different signs at the ends of this interval, by the IVT there is a solution c in [0:2; 0:3] so that f(c) = 0. Similarly, for [1:2; 1:3] we see f(1:2) = 0:15483; f(1:3) = −0:13225. And etc. b. Again the function is continuous. For [1; 2] we note f(1) = 1 and f(2) = −0:69315. By the IVT there is a c in (1; 2) so that f(c) = 0. For the interval [e; 4], f(e) = −0:48407 and f(4) = 2:6137. And etc. 3. One of my purposes in assigning these was that you should recall the Extreme Value Theorem. It guarantees that these problems have a solution, and it gives an algorithm for finding it. That is, \search among the critical points and the endpoints." a. The discontinuities of this rational function are where the denominator is zero. But the solutions of x2 − 2x = 0 are at x = 2 and x = 0, so the function is continuous on the interval [0:5; 1] of interest.
    [Show full text]
  • 2.4 the Extreme Value Theorem and Some of Its Consequences
    2.4 The Extreme Value Theorem and Some of its Consequences The Extreme Value Theorem deals with the question of when we can be sure that for a given function f , (1) the values f (x) don’t get too big or too small, (2) and f takes on both its absolute maximum value and absolute minimum value. We’ll see that it gives another important application of the idea of compactness. 1 / 17 Definition A real-valued function f is called bounded if the following holds: (∃m, M ∈ R)(∀x ∈ Df )[m ≤ f (x) ≤ M]. If in the above definition we only require the existence of M then we say f is upper bounded; and if we only require the existence of m then say that f is lower bounded. 2 / 17 Exercise Phrase boundedness using the terms supremum and infimum, that is, try to complete the sentences “f is upper bounded if and only if ...... ” “f is lower bounded if and only if ...... ” “f is bounded if and only if ...... ” using the words supremum and infimum somehow. 3 / 17 Some examples Exercise Give some examples (in pictures) of functions which illustrates various things: a) A function can be continuous but not bounded. b) A function can be continuous, but might not take on its supremum value, or not take on its infimum value. c) A function can be continuous, and does take on both its supremum value and its infimum value. d) A function can be discontinuous, but bounded. e) A function can be discontinuous on a closed bounded interval, and not take on its supremum or its infimum value.
    [Show full text]
  • Two Fundamental Theorems About the Definite Integral
    Two Fundamental Theorems about the Definite Integral These lecture notes develop the theorem Stewart calls The Fundamental Theorem of Calculus in section 5.3. The approach I use is slightly different than that used by Stewart, but is based on the same fundamental ideas. 1 The definite integral Recall that the expression b f(x) dx ∫a is called the definite integral of f(x) over the interval [a,b] and stands for the area underneath the curve y = f(x) over the interval [a,b] (with the understanding that areas above the x-axis are considered positive and the areas beneath the axis are considered negative). In today's lecture I am going to prove an important connection between the definite integral and the derivative and use that connection to compute the definite integral. The result that I am eventually going to prove sits at the end of a chain of earlier definitions and intermediate results. 2 Some important facts about continuous functions The first intermediate result we are going to have to prove along the way depends on some definitions and theorems concerning continuous functions. Here are those definitions and theorems. The definition of continuity A function f(x) is continuous at a point x = a if the following hold 1. f(a) exists 2. lim f(x) exists xœa 3. lim f(x) = f(a) xœa 1 A function f(x) is continuous in an interval [a,b] if it is continuous at every point in that interval. The extreme value theorem Let f(x) be a continuous function in an interval [a,b].
    [Show full text]
  • Chapter 12 Applications of the Derivative
    Chapter 12 Applications of the Derivative Now you must start simplifying all your derivatives. The rule is, if you need to use it, you must simplify it. 12.1 Maxima and Minima Relative Extrema: f has a relative maximum at c if there is some interval (r, s) (even a very small one) containing c for which f(c) ≥ f(x) for all x between r and s for which f(x) is defined. f has a relative minimum at c if there is some interval (r, s) (even a very small one) containing c for which f(c) ≤ f(x) for all x between r and s for which f(x) is defined. Absolute Extrema f has an absolute maximum at c if f(c) ≥ f(x) for every x in the domain of f. f has an absolute minimum at c if f(c) ≤ f(x) for every x in the domain of f. Extreme Value Theorem - If f is continuous on a closed interval [a,b], then it will have an absolute maximum and an absolute minimum value on that interval. Each absolute extremum must occur either at an endpoint or a critical point. Therefore, the absolute max is the largest value in a table of vales of f at the endpoints and critical points, and the absolute minimum is the smallest value. Locating Candidates for Relative Extrema If f is a real valued function, then its relative extrema occur among the following types of points, collectively called critical points: 1. Stationary Points: f has a stationary point at x if x is in the domain of f and f′(x) = 0.
    [Show full text]
  • Calculus Terminology
    AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential
    [Show full text]
  • MA123, Chapter 6: Extreme Values, Mean Value
    MA123, Chapter 6: Extreme values, Mean Value Theorem, Curve sketching, and Concavity • Apply the Extreme Value Theorem to find the global extrema for continuous func- Chapter Goals: tion on closed and bounded interval. • Understand the connection between critical points and localextremevalues. • Understand the relationship between the sign of the derivative and the intervals on which a function is increasing and on which it is decreasing. • Understand the statement and consequences of the Mean Value Theorem. • Understand how the derivative can help you sketch the graph ofafunction. • Understand how to use the derivative to find the global extremevalues (if any) of a continuous function over an unbounded interval. • Understand the connection between the sign of the second derivative of a function and the concavities of the graph of the function. • Understand the meaning of inflection points and how to locate them. Assignments: Assignment 12 Assignment 13 Assignment 14 Assignment 15 Finding the largest profit, or the smallest possible cost, or the shortest possible time for performing a given procedure or task, or figuring out how to perform a task most productively under a given budget and time schedule are some examples of practical real-world applications of Calculus. The basic mathematical question underlying such applied problems is how to find (if they exist)thelargestorsmallestvaluesofagivenfunction on a given interval. This procedure depends on the nature of the interval. ! Global (or absolute) extreme values: The largest value a function (possibly) attains on an interval is called its global (or absolute) maximum value.Thesmallestvalueafunction(possibly)attainsonan interval is called its global (or absolute) minimum value.Bothmaximumandminimumvalues(ifthey exist) are called global (or absolute) extreme values.
    [Show full text]
  • OPTIMIZATION 1. Optimization and Derivatives
    4: OPTIMIZATION STEVEN HEILMAN 1. Optimization and Derivatives Nothing takes place in the world whose meaning is not that of some maximum or minimum. Leonhard Euler At this stage, Euler's statement may seem to exaggerate, but perhaps the Exercises in Section 4 and the Problems in Section 5 may reinforce his views. These problems and exercises show that many physical phenomena can be explained by maximizing or minimizing some function. We therefore begin by discussing how to find the maxima and minima of a function. In Section 2, we will see that the first and second derivatives of a function play a crucial role in identifying maxima and minima, and also in drawing functions. Finally, in Section 3, we will briefly describe a way to find the zeros of a general function. This procedure is known as Newton's Method. As we already see in Algorithm 1.2(1) below, finding the zeros of a general function is crucial within optimization. We now begin our discussion of optimization. We first recall the Extreme Value Theorem from the last set of notes. In Algorithm 1.2, we will then describe a general procedure for optimizing a function. Theorem 1.1. (Extreme Value Theorem) Let a < b. Let f :[a; b] ! R be a continuous function. Then f achieves its minimum and maximum values. More specifically, there exist c; d 2 [a; b] such that: for all x 2 [a; b], f(c) ≤ f(x) ≤ f(d). Algorithm 1.2. A procedure for finding the extreme values of a differentiable function f :[a; b] ! R.
    [Show full text]
  • Calc. Transp. Correl. Chart
    Calculus Transparencies to Accompany LARSON/HOSTETLER/EDWARDS •Calculus with Analytic Geometry, Seventh Edition •Calculus with Analytic Geometry, Alternate Sixth Edition •Calculus: Early Transcendental Functions, Third Edition Calculus: Early Calculus, Transcendental Transparency Calculus, Alternate Functions, Third Figure Seventh Edition Sixth Edition Edition Number Transparency Title Figure Figure Figure 1The Distance Formula A.16 1.16 A.16 A.17 1.17 A.17 2 Symmetry of a Graph P. 7 1.30 P. 7 3 Rise in Atmospheric Carbon Dioxide P. 11 1.34 P. 11 ----- 1.35 ----- 4The Slope of a Line P. 12 1.38 P. 12 P. 14 1.40 P. 14 5Parallel and Perpendicular Lines P. 19 1.44 P. 19 6Vertical Line Test for Functions P. 26 1.50 P. 26 7 Eight Basic Functions P. 27 1.51 P. 27 8 Shifts and Reflections P. 28 1.52 P. 28 ----- 1.53 ----- 9Trigonometric Functions A.37 8.13 A.37 10 The Tangent Line Problem 1.2 2.2 1.2 11 A Formal Definition of Limit 1.12 2.29 1.12 12 Two Special Trigonometric Limits 1.22 8.20 1.22 Proof of Proof of Proof of Thm 1.9 Thm 8.2 Thm 1.9 13 Continuity 1.25 2.14 1.25 ----- 2.15 ----- 14 Intermediate Value Theorem 1.35 2.20 1.35 1.36 2.21 1.36 15 Infinite Limits 1.40 2.24 1.40 16 The Tangent Line as the Limit of the 2.3 3.3 2.3 Secant Line 2.4 3.4 2.4 17 The Mean Value Theorem 3.12 4.10 3.12 18 The First Derivative Test Proof of Proof of Proof of Thm 3.6 Thm 4.6 Thm 3.6 19 Concavity 3.24 4.20 3.24 20 Points of Inflection 3.28 4.24 3.28 21 Limits at Infinity 3.34 4.30 3.34 22 Oxygen Level in a Pond 3.41 4.34 3.41 23 Finding Minimum Length 3.57 4.47 3.58 3.58 Tech p.
    [Show full text]
  • Calculus Formulas and Theorems
    Formulas and Theorems for Reference I. Tbigonometric Formulas l. sin2d+c,cis2d:1 sec2d l*cot20:<:sc:20 +.I sin(-d) : -sitt0 t,rs(-//) = t r1sl/ : -tallH 7. sin(A* B) :sitrAcosB*silBcosA 8. : siri A cos B - siu B <:os,;l 9. cos(A+ B) - cos,4cos B - siuA siriB 10. cos(A- B) : cosA cosB + silrA sirrB 11. 2 sirrd t:osd 12. <'os20- coS2(i - siu20 : 2<'os2o - I - 1 - 2sin20 I 13. tan d : <.rft0 (:ost/ I 14. <:ol0 : sirrd tattH 1 15. (:OS I/ 1 16. cscd - ri" 6i /F tl r(. cos[I ^ -el : sitt d \l 18. -01 : COSA 215 216 Formulas and Theorems II. Differentiation Formulas !(r") - trr:"-1 Q,:I' ]tra-fg'+gf' gJ'-,f g' - * (i) ,l' ,I - (tt(.r))9'(.,') ,i;.[tyt.rt) l'' d, \ (sttt rrJ .* ('oqI' .7, tJ, \ . ./ stll lr dr. l('os J { 1a,,,t,:r) - .,' o.t "11'2 1(<,ot.r') - (,.(,2.r' Q:T rl , (sc'c:.r'J: sPl'.r tall 11 ,7, d, - (<:s<t.r,; - (ls(].]'(rot;.r fr("'),t -.'' ,1 - fr(u") o,'ltrc ,l ,, 1 ' tlll ri - (l.t' .f d,^ --: I -iAl'CSllLl'l t!.r' J1 - rz 1(Arcsi' r) : oT Il12 Formulas and Theorems 2I7 III. Integration Formulas 1. ,f "or:artC 2. [\0,-trrlrl *(' .t "r 3. [,' ,t.,: r^x| (' ,I 4. In' a,,: lL , ,' .l 111Q 5. In., a.r: .rhr.r' .r r (' ,l f 6. sirr.r d.r' - ( os.r'-t C ./ 7. /.,,.r' dr : sitr.i'| (' .t 8. tl:r:hr sec,rl+ C or ln Jccrsrl+ C ,f'r^rr f 9.
    [Show full text]
  • The Extreme Value Theorem: If Is Continuous on a Closed Interval
    AP Calculus 4.1 Notes Maximum and Minimum Values Goal: Apply derivatives to calculate extreme values. Identify the maxima and minima of the following graph. Find the maxima and minima Example 1:푓(푥) = 푐표푠 푥 Example 2: 푓(푥) = 푥2 Example 3: 푓(푥) = 푥3 Example 4: 푓(푥) = 3푥4 − 16푥3 + 18푥2; 1 ≤ 푥 ≤ 4 The Extreme Value Theorem: If 푓 is continuous on a closed interval [푎, 푏], then 푓 attains an absolute maximum value 푓(푐) and an absolute minimum value 푓(푑) at some numbers of 푐 and 푑 in [푎, 푏] Examples: Non-Examples Fermat’s Theorem: If 푓 has a local maximum or minimum at c, and if 푓′(푐) exists, then 푓′(푐) = 0. Careful! When 푓′(푥) = 0 it doesn’t automatically mean there is a maximum or minimum! In other words the converse of Fermat’s Theorem is not true. Critical Numbers: A critical number of a function f is a number c in the domain of f such that either 푓′(푐) = 0 or 푓′(푐) does not exist. Example 5: Find the critical numbers 푓(푥) = 3푥2 − 2푥 푓(푥) = 푥2/3 + 1 If f has a local maximum or minimum at c then c is a critical number of f. To find an absolute maximum or minimum of a continuous function on a closed interval, we note that either it is local (in which case it occurs at a critical number) or it occurs at an endpoint of the interval. Thus the following three-step method ALWAYS works.
    [Show full text]
  • Proof of the Extreme Value Theorem
    Proof of the Extreme Value Theorem Theorem: If f is a continuous function defined on a closed interval [a; b], then the function attains its maximum value at some point c contained in the interval. Proof: There will be two parts to this proof. First we will show that there must be a finite maximum value for f (this was not done in class); second, we will show that f must attain this maximum value. Note that the methods in the two parts are very similar. Part I First we show that there must be a finite maximum value. We will accomplish this by assuming that there is no such value, and then deriving a contradiction. Assume there is no maximum value; then certainly this means that the function attains larger and larger values. In particular, there must be some point c1 with f(c1) > 1, and a point c2 with f(c2) > 2, and a point c3 with f(c3) > 3,... Now look at all of these points c1; c2; :::. It is certainly not clear that they converge to some single point in [a; b]; in fact they probably don’t. We will however be able to find a ”subsequence” that does converge to a single point; this will prove useful at the end of the proof. We find the subsequence as follows. First, split the interval [a; b] into two equally sized pieces. We notice that there are infinitely many points cn in [a; b]– so, therefore, there must be infinitely many cn’s in either the left half or the right half.
    [Show full text]
  • 4.1 Extreme Values of Functions Objective: Able to Determine the Local Or Global Extreme Values of a Function
    AP Calculus BC 4.1 Extreme Values of Functions Objective: able to determine the local or global extreme values of a function. Absolute (Global) Extreme Values Let f be a function with domain Dfc. Then ( ) is the (a) absolute maximum value on D if and only if fxfc( )≤ ( ) for all xD in . (b) absolute minimum value on D if and only if fxfc( )≥ ( ) for all xD in . 1. Function Rule Domain D Absolute Extrema on D 2 a. y = – x + 1 −, b. y = – x 2 + 1 [-2, 0] c. y = – x 2 + 1 [-2, 0) d. y = – x 2 + 1 (-2, 0) Extreme Value Theorem If f is continuous on a closed interval [ a, b], then f has both a maximum value and a minimum value on the interval. The maximum and minimum values may occur at interior points or endpoints. Local (Relative) Extreme Values Let c be an interior point of the domain of the function f. Then f( c ) is a (a) local maximum value at c if and only if fxfc( )≤ ( ) for all x in some open interval containing c. (b) local minimum value at c if and only if fxfc( )≥ ( ) for all x in some open interval containing c. A function f has a local maximum or local minimum at an endpoint c if the appropriate inequality holds for all x in some half-op en domain interval containing c. Local Extreme Value Theorem If a function f has a local maximum value or a local minimum value at an interior point c of its domain, and if f' exists at cfc, then '( )= 0.
    [Show full text]