POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY

Size: px
Start display at page:

Download "POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY"

Transcription

1 APPLICATIONES MATHEMATICAE 36, (29), pp. 2 Zbigniew Ciesielski (Sopot) Ryszard Zieliński (Warszawa) POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY Abstract. Dvoretzky Kiefer Wolfowitz type inequalities for some polynomial and spline estimators of distribution functions are constructed. Moreover, ints on te corresponding algoritms are given as well.. Introduction. Te family of all continuous probability distribution functions on te real line is denoted by F. If te probability corresponding to F F is supported on te interval I ten we write F F(I). Let X,..., X n be a simple sample corresponding to a distribution F F and let (.) F n () = n n (,] (X j ). j= Te Dvoretzky Kiefer Wolfowitz (DKW) inequality in its final form (see [6]) (.2) P { F n F ε} 2e 2nε2 for all F F, were F n F = sup F n () F (), gives us a powerful tool for statistical applications (testing ypoteses concerning unknown F, confidence intervals for F etc.). It seems, owever, unnatural to estimate a continuous F F by te step function F n. In te abundant literature of te subject one can find different approaces to smooting empirical distribution functions but it turns out tat smooting may spoil te estimator. For classical kernel estimators (see e.g. [8]) no inequality of DKW type eists (Zieliński [9]). Consequently, one cannot tell ow many observations X,..., X n are 2 Matematics Subject Classification: Primary 62G7; Secondary 62G3, 6E5. Key words and prases: nonparametric estimation, distribution estimation, Dvoretzky Kiefer Wolfowitz inequality, polynomial estimators, spline estimators, smooting of empirical distribution function. DOI:.464/am36-- [] c Instytut Matematyczny PAN, 29

2 2 Z. Ciesielski and R. Zieliński needed to guarantee te prescribed accuracy of te kernel estimator. Using te metod from [9] one can prove a similar negative result for some polynomial estimators (see Section 4 below). In wat follows we discuss tree estimators and te DKW type inequalities for tem. Te first one (see Section 3), to be denoted by Φ m,n, is a smoot modification of F n. It is a piecewise polynomial estimator of te class C m F wit knots placed at te sample points X :n,..., X n:n. Te smootness parameter m =, 2,... can be fied by te statistician according to is a priori knowledge of te smootness of te estimated F F. In tis case te DKW type inequality olds in te class F of all continuous probability distribution functions on te real line. Te second one (see Section 4) is te polynomial estimator constructed in Ciesielski [3], and te tird one (see Section 5) is a spline estimator wit equally spaced knots (Ciesielski [2], [4]). In bot cases subclasses of F are eplicitly specified for wic te DKW type inequalities are proved. We start in Section 2 wit preliminaries on specific approimations by algebraic polynomials and by splines wit equally spaced knots. 2. Preliminaries from approimation teory. We recall te necessary ingredients from approimation teory, in particular te basic properties of te Bernstein polynomials and of te related B-splines. Te relation is direct: te Bernstein polynomials are simply te degenerate B-splines. Let us start wit te Bernstein polynomials. For a given integer r let Π m denote te space of real polynomials of degree at most m = r (i.e. of order r). For convenience, bot parameters r and m will be used; m is more natural for polynomials and r for splines. Te basic Bernstein polynomials of degree m are linearly independent and given by te formula (2.) N i,m () = Consequently, ( m i ) i ( ) m i wit i =,..., m. (2.2) Π m = span[n i,m : i =,..., m], and terefore eac w Π m as a unique representation m (2.3) w() = w i N i,m (). i= Now, given te coefficients w i and te (, ) we can calculate te value w() using te Casteljeau algoritm based on te identity (2.4) N i,m () = ( )N i,m () + N i,m (). Te Bernstein polynomials are positive on (, ) and tey form a partition

3 of unity, (2.5) Polynomial and spline estimators 3 m N i,m () = for i =,..., m and (, ). i= On te oter and, te modified Bernstein polynomials (2.6) M i,m () = (m + )N i,m () are normalized in L (, ), i.e. (2.7) M i,m () d =. In our construction of te polynomial estimator, te Durrmeyer kernel m (2.8) R m (, y) = M i,m ()N i,m (y) i= plays an essential role. Te kernel is symmetric and it as te following spectral representation: m (2.9) R m (, y) = λ i,m l i ()l i (y), i= were te eigenfunctions are te ortonormal Legendre polynomials l i and for te corresponding eigenvalues λ i,m we ave (cf. e.g. [5]) (2.) λ,m =, λ i,m = i j= wence, wit te notation λ k = k(k + ), (2.) 2 5 λ j λ k+ λ j,m λ j m + 2 m + j m + + j for i =,..., m, for λ k m < λ k+, j k. Now, for a given function F wic is eiter of bounded variation or continuous on [, ], te value of te underlying smooting operator is a polynomial of degree m + defined by te formula [ (2.2) T m F () = F () + Now, since (2.3) M i,m (y) dy = m+ j=i+ ] R m (y, z) df (y) dz. N j,m+ () for i =,,..., m, te Casteljeau algoritm, in case F = F n, can be applied to calculate te value T m F (). It also follows from (2.2) tat te integrated Legendre

4 4 Z. Ciesielski and R. Zieliński polynomials (2.4) L j () = l j (y) dy for j =,,... are te eigenfunctions for te operators T m wit te corresponding eigenvalues (2.6). For more details on te eigenvalues λ i,m we refer to [3]. An elementary argument gives, for any probability distribution functions F and G, bot supported on [, ], te important inequality (2.5) T m F T m G F G. Moreover, if F is a continuous function on [, ], ten (2.6) T m F 3 F. Proposition 2.. For eac F C[, ] we ave (2.7) F T m F as m. Proof. Te family {T m } of operators on C[, ] is by (2.6) uniformly bounded and terefore by te Banac Steinaus teorem it is sufficient to ceck (2.7) for F = L j wit any fied j. However, in tis case F T m F = L j T m L j = ( λ j,m )L j, and an application of (2.) completes te proof. In wat follows we use te symbol W m p (I) for te Sobolev space of order of smootness m and wit te integrability eponent p. Teorem 2.2. Let F W 2 2 [, ] F[, ], D = d/d and M = D2 F 2. Ten (2.8) F T m F M m /4 for m = 2, 3,.... Proof. For te density f = DF we ave (2.9) (f, ) = wit te usual scalar product (f, g) in L 2 [, ], and (2.2) F () T m F () = (f R m f)(z) dz, were R m is te Durrmeyer operator corresponding to (2.8). It now follows from (2.2) tat (2.2) F T m F f R m f 2. Using te spectral representation of R m we find tat (2.22) f R m f 2 2 = ( λ i,m ) 2 a 2 i, i=

5 Polynomial and spline estimators 5 were te a i s are te Fourier Legendre coefficients and by definition eac λ i,m for i > m is assumed to be. Moreover, (2.23) a i = (f, l i ). Using te notation from (2.4) we get (2.24) a i = (D 2 F, L i ) M L i 2. It remains to estimate L i 2. To tis end apply te identity (2.25) 2L i+ = l i+2 l i, i, (2i + )(2i + 3) (2i + )(2i ) to get (2.26) L i+ 2 2 = ( ) 8λ i 3 ( ) 4λ i 8λ i 3 =, 5λ 4λ i i. Tus, for te unique k satisfying te inequalities λ k m < λ k+ we obtain (2.27) a i 2 M 2 = M 2 5λ i 5 k. i=k+ By te monotonicity in m of f R m f 2 and by (2.) we get k ( ) 2 (2.28) f R m f 2 λi 2 a i 2 + M 2 m k. Now, λ = 2, L 2 2 = /, m/2 k < m, and terefore k ( ) 2 λi (2.29) a i 2 3M 2 m m. i= i= i=k Combining (2.29) and (2.28) we get (2.8). In te construction below of te spline estimator wit random knots, a particular role is played by te following polynomial density function on [, ]: ( ) 2m (2.3) φ m () := M m,2m () = (2m + ) m ( ) m, m were te positive integer m is te given parameter of smootness. Te corresponding polynomial distribution function is (2.3) Φ m () = φ m (y) dy, or else (see (2.3)) (2.32) Φ m () = 2m+ i=m+ N i,2m+ (),

6 6 Z. Ciesielski and R. Zieliński wic permits calculating Φ m () wit te elp of te Casteljeau algoritm. It is also important tat Φ m () solves te two-point Hermite interpolation problem of order m, i.e. (2.33) D k Φ m () = and D k Φ m () = δ k, for k =,..., m. For later convenience we also introduce te transformed polynomial distribution ( ) a (2.34) Φ m (; [a, b]) = Φ m. b a Clearly, Φ m (a; [a, b]) = and Φ m (b; [a, b]) =. On te real line R similar roles to polynomials and Bernstein polynomials on [, ] are played by te cardinal splines and cardinal B-splines, respectively. For a given integer r te space S r of cardinal splines of order r is te space of all functions on R of class C r 2 wose restrictions to (j, j + ) are polynomials of order r, i.e. D r S = on eac (j, j + ) for j =, ±,.... It is known tat tere is a unique B (r) S r (up to a multiplicative constant) positive on (, r) and wit support [, r]. Te function B (r) becomes unique if normalized e.g. so tat (2.35) B (r) (y) dy =. R Te density B (r) can as well be defined probabilistically by te formula (2.36) P {U + + U r < } = B (r) (y) dy were U,..., U r are independent uniformly distributed r.v. on [, ]. We also need te rescaled cardinal B-splines N (r) i, () = B(r) ( i ) and M (r) i, () = B(r) ( i ) for i Z, were > is te so called window parameter. Tey sare te nice properties (2.37) N (r) i, () = and M (r) i, (y) dy =. Clearly, supp N (r) i, formula (2.38) N (r) i, () = i (r) = supp M i, R = [i, (i + r)]. Moreover, te recurrent i (r ) N (r ) i, () + (i + r) (r ) N (r ) i+, () supplies an algoritm for calculating at a given te value of te cardinal

7 spline (2.39) Polynomial and spline estimators 7 i a i N (r) i, () given te coefficients (a i ). Te same algoritm can be used to calculate te value at of te distribution function (2.4) M (r) i, (y) dy = N (r+) i, (). Now, just as in te polynomial case (cf. (2.8)) we introduce te spline kernel (2.4) R (k,r) (, y) = M (k) (r) i+ν, ()N i, (y). i= In wat follows it is assumed tat k r and tat r k is even, i.e. r k = 2ν wit ν being a non-negative integer. It ten follows tat te supports of M (k) (r) i+ν, and of N i, are concentric. Denote by C ±(R) te linear space of all rigt-continuous functions on R wit finite limits at ±, and by BV (R) te linear space of all continuous functions of finite total variation on R. Now, for F C ± (R) BV (R) te value of te operator T (k,r) F is defined by te formula ( ) (2.42) T (k,r) F () = R (k,r) (z, y) F (dz) dy = R i= R j=i M (k) i+ν, df N (r) i, (y) dy. To recall from [4] te direct approimation teorem by te operators T (k,r), te notion of modulus of a given order m is needed: were m t ω m (F ; δ) = sup m t F, t <δ is te mt order progressive difference wit step t, i.e. m ( ) m m t f() = ( ) j+m f( + jt). j j= Now, te following teorem, important for spline estimation, was proved in [4]: Teorem 2.3. Let k r wit r k even and let >. Ten for F C ± (R) BV (R), (2.42) T (r,k) F F,

8 8 Z. Ciesielski and R. Zieliński and for F C ± (R), (2.43) F T (k,r) F 2(4 + (r + k) 2 )ω 2 (F ; ), and in particular for k =, ( (2.44) F T (,r) F ω F ; r + ). 2 Consequently, for eac continuous probability distribution F, (2.45) F T (k,r) F as A smoot modification of F n. We start, for a given positive integer m, wit te polynomial density (2.3) and its polynomial probability distribution (2.3). Let now X :n,..., X n:n wit X :n X n:n be te order statistics from te sample X,..., X n. For tecnical reasons we assume tat X :n < < X n:n ; oterwise one sould consider multiple knots. Moreover, define X :n = ma{, X :n (X 2:n X :n )} = ma{, 2X :n X 2:n }, X n+:n = min{x n:n + (X n:n X n :n ), } = min{2x n:n X n :n, }. Now, for te given sample X,..., X n and for given m a new estimator Φ m,n () for F is defined as follows: it equals for < X :n, for X n+:n, and for i =,..., n + and X i :n < X i:n, (3.) Φ m,n () = n Φ(; [X i :n, X i:n ]) + F n (X i :n ) 2n. We consider Φ m,n () as an estimator of te unknown distribution function F F wic generates te sample X,..., X n. Given te sample, te estimator Φ m,n () may be easily calculated by te Casteljeau algoritm or using te standard incomplete beta functions or distribution functions of beta random variable; te functions are available in numerical computer packages. Summarizing we get Proposition 3.. Te estimator Φ m,n as te following properties:. It is a piecewise polynomial probability distribution supported on [X :n, X n+:n ] wit knots at te sample points. 2. Te function Φ m,n ()+/2n interpolates F n at te sample points, i.e. Φ m,n (X i:n ) + 2n = F n(x i:n ) for i =,..., n. 3. Φ m,n C m (R). 4. D k Φ m,n (X i:n ) = for k =,..., m and i =,..., n. 5. Φ m,n F F n F + /2n.

9 Polynomial and spline estimators 9 6. Moreover, te following DKW type inequality olds: (3.2) P { Φ m,n F ε} 2 e 2n(ε /2n)2, n > 2ε, F F. 4. Estimating by polynomials on [, ]. A polynomial estimator on [, ] (see [3] and cf. (2.2)) can be defined by (4.) F m,n () = T m F n (), were T m transforms distributions on [, ], continuous or not, into distribution functions on [, ] wic are polynomials of degree m +. It turns out tat for te family F[, ] of all continuous distributions supported on [, ], te DKW type inequality for te estimator F m,n does not old. More precisely, we ave te following negative result Teorem 4.. Tere are ε > and η > suc tat for any m and n one can find a distribution function F F[, ] suc tat (4.2) P { F m,n F > ε} > η. To prove (4.2) it is enoug to demonstrate tat for some ε, η > and for every n and for every odd m te following inequality olds: (4.3) P {F m,n (/2) > F (/2) + ε > } > η. We start te proof by writing formula (4.) in te form (4.4) F m,n () = n m N i,m (X j ) M i,m (y) dy, n wence by (2.3), (4.5) F m,n () = n j= i= n j= i= m N i,m (X j ) m+ k=i+ N k,m+ (). Let now {ε k : k =,,...} be a sequence of independent Bernoulli r.v. wit P {ε k = } = /2 = P {ε k = }. Moreover, let ζ m+ = ε + + ε m+ be te binomial r.v. Ten for odd m = 2ν and i ν, (4.6) m+ k=i+ N k,m+ (/2) = P {ζ m+ > i} P {ζ m+ > ν} = P {ζ m+ ν} = /2. Consequently, by (2.3) we obtain, for odd m, (4.7) F m,n (/2) n ν N i,m (X j ) 2n 2n j= i= n j= X j M ν,m (y) dy.

10 Z. Ciesielski and R. Zieliński Now, te continuous function M m () = M ν,m (y) dy is decreasing on [, ], M m () =, and M m (/2) = /2. Consequently, for ε (, /6) tere is δ > suc tat M m (δ + /2) > 4ε. Coose now F F[, ] suc tat F (/2) < ε and F (/2 + δ) > η /n. Tus, by our ypotesis we get, for j =,..., n, P F {X j < /2 + δ} > η /n and P F {M m (X j ) > 4ε} > η /n. Taking into account tat n {M m (X j ) > 4ε} one obtains j= wic proves (4.3). P F { n n j= { n n j= } M m (X j ) > 4ε } M m (X j ) > 4ε > η, To obtain a positive DKW type inequality for te above polynomial estimators we reduce te space F of all continuous distribution functions to a smaller subclass. We sall discuss, for a given constant M, subclass W M of F[, ] suc tat F W M if and only if te density f = F is absolutely continuous and its derivative satisfies (4.8) f () 2 d M. Teorem 4.2. Given constants M >, ε > and η >, one can find eplicit values of m and n suc tat (4.9) P { F m,n F > ε} < η for all F W M. Specifically, it is enoug to coose m and n so tat 2M < ε and 2 ep ( 2 nm 2 ) m/4 m /2 < η. Proof. Let us start wit te identity F F m,n = (F T m F ) + T m (F F n ). Now (see [3]) te triangle inequality and contraction property (2.5) imply (4.) F F m,n F F n + F T m F,

11 Polynomial and spline estimators wence by Teorem 2.2 and by te DKW inequality we get P { F F m,n > ε} P { F F m,n > 2M/m /4 } and tis completes te proof. P { F F n + F T m F > 2M/m /4 } P { F F n + M/m /4 > 2M/m /4 } = P { F F n > M/m /4 } 2 ep ( 2 nm 2 ) < η, m /2 5. Estimating by splines wit equally spaced knots. In tis section we eibit a ric family of subclasses of continuous probability distributions on R for wic te DKW type inequality olds. Te general sceme is very muc like tat in Section 4 (cf. te proof of Teorem 4.2). We start by recalling te generalized Hölder classes. A function ω() on R + is said to be a modulus of smootness if it is bounded, continuous, vanising at, non-decreasing and subadditive, e.g. concave. Suppose we are given integers (k, r) satisfying te conditions formulated just below formula (2.4). Taking into account wat we already know it is reasonable to consider te following Hölder classes of probability distributions: (5.) (5.2) H (k,r) ω,2 = {F F : 2(4 + (r + k) 2 )ω 2 (F ; ) ω() for all > }, ( H (k,r) ω, = {F F : ω F ; r + k ) } ω() for all >. 2 According to our sceme, te spline estimator wit window parameter and wit te given (k, r) is defined by te formula (5.3) F,n = F (k,r),n = T (k,r) F n. For tese estimators we also ave te basic inequality (5.4) F F,n F F n + F T (k,r) F. We are now in a position to state te DKW type inequality for te generalized Hölder classes of continuous distributions. Teorem 5.. Let i =, 2 and k r wit r k even. Ten for all ε > and η > tere are > and n suc tat (5.5) P { F,n F > ε} < η for all F H (k,r) ω,i. It suffices to coose and n suc tat ω() < ε/2 and 2 ep( nε 2 /2) < η. Te proof is immediate from te DKW inequality, (5.4) and Teorem 2.3.

12 2 Z. Ciesielski and R. Zieliński References [] C. de Boor, Linear combinations of B-splines, in: Approimation Teory II, Academic Press, 976, 47. [2] Z. Ciesielski, Local spline approimation and nonparametric density estimation, in: Constructive Teory of Functions 87, Sofia, 988, [3], Nonparametric polynomial density estimation, Probab. Mat. Statist. 9 (988),. [4], Asymptotic nonparametric spline density estimation, ibid. 2 (99), 24. [5] Z. Ciesielski and J. Domsta, Te degenerate B-splines as basis in te space of algebraic polynomials, Ann. Polon. Mat. 46 (985), [6] P. Massart, Te tigt constant in te Dvoretzky Kiefer Wolfowitz inequality, Ann. Probab. 8 (99), [7] I. J. Scoenberg, Cardinal interpolation and spline functions, J. Appro. Teory 2 (969), [8] E. J. Wegman, Kernel estimators, in: Encyclopedia of Statistical Sciences, 2nd ed., Vol. 6, Wiley-Interscience, 26. [9] R. Zieliński, Kernel estimators and te Dvoretzky Kiefer Wolfowitz inequality, Appl. Mat. (Warsaw) 34 (27), Instytut Matematyczny PAN Abraama Sopot, Poland Z.Ciesielski@impan.gda.pl Instytut Matematyczny PAN Śniadeckic Warszawa, Poland R.Zielinski@impan.pl Received on.7.28 (945)

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

2.8 The Derivative as a Function

2.8 The Derivative as a Function .8 Te Derivative as a Function Typically, we can find te derivative of a function f at many points of its domain: Definition. Suppose tat f is a function wic is differentiable at every point of an open

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc

More information

lecture 26: Richardson extrapolation

lecture 26: Richardson extrapolation 43 lecture 26: Ricardson extrapolation 35 Ricardson extrapolation, Romberg integration Trougout numerical analysis, one encounters procedures tat apply some simple approximation (eg, linear interpolation)

More information

Order of Accuracy. ũ h u Ch p, (1)

Order of Accuracy. ũ h u Ch p, (1) Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical

More information

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER*

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER* EO BOUNDS FO THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BADLEY J. LUCIE* Abstract. Te expected error in L ) attimet for Glimm s sceme wen applied to a scalar conservation law is bounded by + 2 ) ) /2 T

More information

MATH745 Fall MATH745 Fall

MATH745 Fall MATH745 Fall MATH745 Fall 5 MATH745 Fall 5 INTRODUCTION WELCOME TO MATH 745 TOPICS IN NUMERICAL ANALYSIS Instructor: Dr Bartosz Protas Department of Matematics & Statistics Email: bprotas@mcmasterca Office HH 36, Ext

More information

Lecture 15. Interpolation II. 2 Piecewise polynomial interpolation Hermite splines

Lecture 15. Interpolation II. 2 Piecewise polynomial interpolation Hermite splines Lecture 5 Interpolation II Introduction In te previous lecture we focused primarily on polynomial interpolation of a set of n points. A difficulty we observed is tat wen n is large, our polynomial as to

More information

Continuity and Differentiability of the Trigonometric Functions

Continuity and Differentiability of the Trigonometric Functions [Te basis for te following work will be te definition of te trigonometric functions as ratios of te sides of a triangle inscribed in a circle; in particular, te sine of an angle will be defined to be te

More information

Chapter 2 Limits and Continuity

Chapter 2 Limits and Continuity 4 Section. Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 6) Quick Review.. f () ( ) () 4 0. f () 4( ) 4. f () sin sin 0 4. f (). 4 4 4 6. c c c 7. 8. c d d c d d c d c 9. 8 ( )(

More information

Math 161 (33) - Final exam

Math 161 (33) - Final exam Name: Id #: Mat 161 (33) - Final exam Fall Quarter 2015 Wednesday December 9, 2015-10:30am to 12:30am Instructions: Prob. Points Score possible 1 25 2 25 3 25 4 25 TOTAL 75 (BEST 3) Read eac problem carefully.

More information

MA455 Manifolds Solutions 1 May 2008

MA455 Manifolds Solutions 1 May 2008 MA455 Manifolds Solutions 1 May 2008 1. (i) Given real numbers a < b, find a diffeomorpism (a, b) R. Solution: For example first map (a, b) to (0, π/2) and ten map (0, π/2) diffeomorpically to R using

More information

Journal of Computational and Applied Mathematics

Journal of Computational and Applied Mathematics Journal of Computational and Applied Matematics 94 (6) 75 96 Contents lists available at ScienceDirect Journal of Computational and Applied Matematics journal omepage: www.elsevier.com/locate/cam Smootness-Increasing

More information

Continuity. Example 1

Continuity. Example 1 Continuity MATH 1003 Calculus and Linear Algebra (Lecture 13.5) Maoseng Xiong Department of Matematics, HKUST A function f : (a, b) R is continuous at a point c (a, b) if 1. x c f (x) exists, 2. f (c)

More information

Differentiation in higher dimensions

Differentiation in higher dimensions Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends

More information

Poisson Equation in Sobolev Spaces

Poisson Equation in Sobolev Spaces Poisson Equation in Sobolev Spaces OcMountain Dayligt Time. 6, 011 Today we discuss te Poisson equation in Sobolev spaces. It s existence, uniqueness, and regularity. Weak Solution. u = f in, u = g on

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x

More information

Semigroups of Operators

Semigroups of Operators Lecture 11 Semigroups of Operators In tis Lecture we gater a few notions on one-parameter semigroups of linear operators, confining to te essential tools tat are needed in te sequel. As usual, X is a real

More information

Derivatives of Exponentials

Derivatives of Exponentials mat 0 more on derivatives: day 0 Derivatives of Eponentials Recall tat DEFINITION... An eponential function as te form f () =a, were te base is a real number a > 0. Te domain of an eponential function

More information

Symmetry Labeling of Molecular Energies

Symmetry Labeling of Molecular Energies Capter 7. Symmetry Labeling of Molecular Energies Notes: Most of te material presented in tis capter is taken from Bunker and Jensen 1998, Cap. 6, and Bunker and Jensen 2005, Cap. 7. 7.1 Hamiltonian Symmetry

More information

Preconditioning in H(div) and Applications

Preconditioning in H(div) and Applications 1 Preconditioning in H(div) and Applications Douglas N. Arnold 1, Ricard S. Falk 2 and Ragnar Winter 3 4 Abstract. Summarizing te work of [AFW97], we sow ow to construct preconditioners using domain decomposition

More information

Continuity and Differentiability Worksheet

Continuity and Differentiability Worksheet Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

On the best approximation of function classes from values on a uniform grid in the real line

On the best approximation of function classes from values on a uniform grid in the real line Proceedings of te 5t WSEAS Int Conf on System Science and Simulation in Engineering, Tenerife, Canary Islands, Spain, December 16-18, 006 459 On te best approximation of function classes from values on

More information

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example,

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example, NUMERICAL DIFFERENTIATION James T Smit San Francisco State University In calculus classes, you compute derivatives algebraically: for example, f( x) = x + x f ( x) = x x Tis tecnique requires your knowing

More information

The derivative function

The derivative function Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative

More information

232 Calculus and Structures

232 Calculus and Structures 3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE

More information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

ERROR BOUNDS FOR FINITE-DIFFERENCE METHODS FOR RUDIN OSHER FATEMI IMAGE SMOOTHING

ERROR BOUNDS FOR FINITE-DIFFERENCE METHODS FOR RUDIN OSHER FATEMI IMAGE SMOOTHING ERROR BOUNDS FOR FINITE-DIFFERENCE METHODS FOR RUDIN OSHER FATEMI IMAGE SMOOTHING JINGYUE WANG AND BRADLEY J. LUCIER Abstract. We bound te difference between te solution to te continuous Rudin Oser Fatemi

More information

Analytic Functions. Differentiable Functions of a Complex Variable

Analytic Functions. Differentiable Functions of a Complex Variable Analytic Functions Differentiable Functions of a Complex Variable In tis capter, we sall generalize te ideas for polynomials power series of a complex variable we developed in te previous capter to general

More information

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015 Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes

More information

HOMEWORK HELP 2 FOR MATH 151

HOMEWORK HELP 2 FOR MATH 151 HOMEWORK HELP 2 FOR MATH 151 Here we go; te second round of omework elp. If tere are oters you would like to see, let me know! 2.4, 43 and 44 At wat points are te functions f(x) and g(x) = xf(x)continuous,

More information

Pre-Calculus Review Preemptive Strike

Pre-Calculus Review Preemptive Strike Pre-Calculus Review Preemptive Strike Attaced are some notes and one assignment wit tree parts. Tese are due on te day tat we start te pre-calculus review. I strongly suggest reading troug te notes torougly

More information

Chapter 1. Density Estimation

Chapter 1. Density Estimation Capter 1 Density Estimation Let X 1, X,..., X n be observations from a density f X x. Te aim is to use only tis data to obtain an estimate ˆf X x of f X x. Properties of f f X x x, Parametric metods f

More information

3.4 Algebraic Limits. Ex 1) lim. Ex 2)

3.4 Algebraic Limits. Ex 1) lim. Ex 2) Calculus Maimus.4 Algebraic Limits At tis point, you sould be very comfortable finding its bot grapically and numerically wit te elp of your graping calculator. Now it s time to practice finding its witout

More information

Convexity and Smoothness

Convexity and Smoothness Capter 4 Convexity and Smootness 4.1 Strict Convexity, Smootness, and Gateaux Differentiablity Definition 4.1.1. Let X be a Banac space wit a norm denoted by. A map f : X \{0} X \{0}, f f x is called a

More information

The Laplace equation, cylindrically or spherically symmetric case

The Laplace equation, cylindrically or spherically symmetric case Numerisce Metoden II, 7 4, und Übungen, 7 5 Course Notes, Summer Term 7 Some material and exercises Te Laplace equation, cylindrically or sperically symmetric case Electric and gravitational potential,

More information

Chapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1

Chapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1 Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 969) Quick Review..... f ( ) ( ) ( ) 0 ( ) f ( ) f ( ) sin π sin π 0 f ( ). < < < 6. < c c < < c 7. < < < < < 8. 9. 0. c < d d < c

More information

How to Find the Derivative of a Function: Calculus 1

How to Find the Derivative of a Function: Calculus 1 Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te

More information

1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)

1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x) Calculus. Gradients and te Derivative Q f(x+) δy P T δx R f(x) 0 x x+ Let P (x, f(x)) and Q(x+, f(x+)) denote two points on te curve of te function y = f(x) and let R denote te point of intersection of

More information

Recall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if

Recall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if Computational Aspects of its. Keeping te simple simple. Recall by elementary functions we mean :Polynomials (including linear and quadratic equations) Eponentials Logaritms Trig Functions Rational Functions

More information

Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series

Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series Lawrence D. Brown, Pilip A. Ernst, Larry Sepp, and Robert Wolpert August 27, 2015 Abstract We consider te class,

More information

A h u h = f h. 4.1 The CoarseGrid SystemandtheResidual Equation

A h u h = f h. 4.1 The CoarseGrid SystemandtheResidual Equation Capter Grid Transfer Remark. Contents of tis capter. Consider a grid wit grid size and te corresponding linear system of equations A u = f. Te summary given in Section 3. leads to te idea tat tere migt

More information

Different Approaches to a Posteriori Error Analysis of the Discontinuous Galerkin Method

Different Approaches to a Posteriori Error Analysis of the Discontinuous Galerkin Method WDS'10 Proceedings of Contributed Papers, Part I, 151 156, 2010. ISBN 978-80-7378-139-2 MATFYZPRESS Different Approaces to a Posteriori Error Analysis of te Discontinuous Galerkin Metod I. Šebestová Carles

More information

arxiv: v1 [math.na] 28 Apr 2017

arxiv: v1 [math.na] 28 Apr 2017 THE SCOTT-VOGELIUS FINITE ELEMENTS REVISITED JOHNNY GUZMÁN AND L RIDGWAY SCOTT arxiv:170500020v1 [matna] 28 Apr 2017 Abstract We prove tat te Scott-Vogelius finite elements are inf-sup stable on sape-regular

More information

A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION

A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION STUDIA UNIV. BABEŞ BOLYAI, MATHEMATICA, Volume XLVIII, Number 3, September 2003 A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION GH. MICULA, E. SANTI, AND M. G. CIMORONI Dedicated to

More information

3.4 Worksheet: Proof of the Chain Rule NAME

3.4 Worksheet: Proof of the Chain Rule NAME Mat 1170 3.4 Workseet: Proof of te Cain Rule NAME Te Cain Rule So far we are able to differentiate all types of functions. For example: polynomials, rational, root, and trigonometric functions. We are

More information

arxiv:math/ v1 [math.ca] 1 Oct 2003

arxiv:math/ v1 [math.ca] 1 Oct 2003 arxiv:mat/0310017v1 [mat.ca] 1 Oct 2003 Cange of Variable for Multi-dimensional Integral 4 Marc 2003 Isidore Fleiscer Abstract Te cange of variable teorem is proved under te sole ypotesis of differentiability

More information

Global Existence of Classical Solutions for a Class Nonlinear Parabolic Equations

Global Existence of Classical Solutions for a Class Nonlinear Parabolic Equations Global Journal of Science Frontier Researc Matematics and Decision Sciences Volume 12 Issue 8 Version 1.0 Type : Double Blind Peer Reviewed International Researc Journal Publiser: Global Journals Inc.

More information

A SHORT INTRODUCTION TO BANACH LATTICES AND

A SHORT INTRODUCTION TO BANACH LATTICES AND CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,

More information

Section 3.1: Derivatives of Polynomials and Exponential Functions

Section 3.1: Derivatives of Polynomials and Exponential Functions Section 3.1: Derivatives of Polynomials and Exponential Functions In previous sections we developed te concept of te derivative and derivative function. Te only issue wit our definition owever is tat it

More information

Mass Lumping for Constant Density Acoustics

Mass Lumping for Constant Density Acoustics Lumping 1 Mass Lumping for Constant Density Acoustics William W. Symes ABSTRACT Mass lumping provides an avenue for efficient time-stepping of time-dependent problems wit conforming finite element spatial

More information

An approximation method using approximate approximations

An approximation method using approximate approximations Applicable Analysis: An International Journal Vol. 00, No. 00, September 2005, 1 13 An approximation metod using approximate approximations FRANK MÜLLER and WERNER VARNHORN, University of Kassel, Germany,

More information

FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS

FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS UNIVERSITATIS IAGELLONICAE ACTA MATHEMATICA, FASCICULUS XL 2002 FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS by Anna Baranowska Zdzis law Kamont Abstract. Classical

More information

University Mathematics 2

University Mathematics 2 University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at

More information

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014 Solutions to te Multivariable Calculus and Linear Algebra problems on te Compreensive Examination of January 3, 24 Tere are 9 problems ( points eac, totaling 9 points) on tis portion of te examination.

More information

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix Opuscula Mat. 37, no. 6 (2017), 887 898 ttp://dx.doi.org/10.7494/opmat.2017.37.6.887 Opuscula Matematica OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS Sandra

More information

LECTURE 14 NUMERICAL INTEGRATION. Find

LECTURE 14 NUMERICAL INTEGRATION. Find LECTURE 14 NUMERCAL NTEGRATON Find b a fxdx or b a vx ux fx ydy dx Often integration is required. However te form of fx may be suc tat analytical integration would be very difficult or impossible. Use

More information

Stability properties of a family of chock capturing methods for hyperbolic conservation laws

Stability properties of a family of chock capturing methods for hyperbolic conservation laws Proceedings of te 3rd IASME/WSEAS Int. Conf. on FLUID DYNAMICS & AERODYNAMICS, Corfu, Greece, August 0-, 005 (pp48-5) Stability properties of a family of cock capturing metods for yperbolic conservation

More information

On convexity of polynomial paths and generalized majorizations

On convexity of polynomial paths and generalized majorizations On convexity of polynomial pats and generalized majorizations Marija Dodig Centro de Estruturas Lineares e Combinatórias, CELC, Universidade de Lisboa, Av. Prof. Gama Pinto 2, 1649-003 Lisboa, Portugal

More information

IEOR 165 Lecture 10 Distribution Estimation

IEOR 165 Lecture 10 Distribution Estimation IEOR 165 Lecture 10 Distribution Estimation 1 Motivating Problem Consider a situation were we ave iid data x i from some unknown distribution. One problem of interest is estimating te distribution tat

More information

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx.

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx. Capter 2 Integrals as sums and derivatives as differences We now switc to te simplest metods for integrating or differentiating a function from its function samples. A careful study of Taylor expansions

More information

158 Calculus and Structures

158 Calculus and Structures 58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you

More information

AN ANALYSIS OF NEW FINITE ELEMENT SPACES FOR MAXWELL S EQUATIONS

AN ANALYSIS OF NEW FINITE ELEMENT SPACES FOR MAXWELL S EQUATIONS Journal of Matematical Sciences: Advances and Applications Volume 5 8 Pages -9 Available at ttp://scientificadvances.co.in DOI: ttp://d.doi.org/.864/jmsaa_7975 AN ANALYSIS OF NEW FINITE ELEMENT SPACES

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

Robotic manipulation project

Robotic manipulation project Robotic manipulation project Bin Nguyen December 5, 2006 Abstract Tis is te draft report for Robotic Manipulation s class project. Te cosen project aims to understand and implement Kevin Egan s non-convex

More information

Basic Nonparametric Estimation Spring 2002

Basic Nonparametric Estimation Spring 2002 Basic Nonparametric Estimation Spring 2002 Te following topics are covered today: Basic Nonparametric Regression. Tere are four books tat you can find reference: Silverman986, Wand and Jones995, Hardle990,

More information

Homework 1 Due: Wednesday, September 28, 2016

Homework 1 Due: Wednesday, September 28, 2016 0-704 Information Processing and Learning Fall 06 Homework Due: Wednesday, September 8, 06 Notes: For positive integers k, [k] := {,..., k} denotes te set of te first k positive integers. Wen p and Y q

More information

Click here to see an animation of the derivative

Click here to see an animation of the derivative Differentiation Massoud Malek Derivative Te concept of derivative is at te core of Calculus; It is a very powerful tool for understanding te beavior of matematical functions. It allows us to optimize functions,

More information

Notes on Multigrid Methods

Notes on Multigrid Methods Notes on Multigrid Metods Qingai Zang April, 17 Motivation of multigrids. Te convergence rates of classical iterative metod depend on te grid spacing, or problem size. In contrast, convergence rates of

More information

Recent Progress in the Integration of Poisson Systems via the Mid Point Rule and Runge Kutta Algorithm

Recent Progress in the Integration of Poisson Systems via the Mid Point Rule and Runge Kutta Algorithm Recent Progress in te Integration of Poisson Systems via te Mid Point Rule and Runge Kutta Algoritm Klaus Bucner, Mircea Craioveanu and Mircea Puta Abstract Some recent progress in te integration of Poisson

More information

REVIEW LAB ANSWER KEY

REVIEW LAB ANSWER KEY REVIEW LAB ANSWER KEY. Witout using SN, find te derivative of eac of te following (you do not need to simplify your answers): a. f x 3x 3 5x x 6 f x 3 3x 5 x 0 b. g x 4 x x x notice te trick ere! x x g

More information

Efficient algorithms for for clone items detection

Efficient algorithms for for clone items detection Efficient algoritms for for clone items detection Raoul Medina, Caroline Noyer, and Olivier Raynaud Raoul Medina, Caroline Noyer and Olivier Raynaud LIMOS - Université Blaise Pascal, Campus universitaire

More information

3.1 Extreme Values of a Function

3.1 Extreme Values of a Function .1 Etreme Values of a Function Section.1 Notes Page 1 One application of te derivative is finding minimum and maimum values off a grap. In precalculus we were only able to do tis wit quadratics by find

More information

2.3 Algebraic approach to limits

2.3 Algebraic approach to limits CHAPTER 2. LIMITS 32 2.3 Algebraic approac to its Now we start to learn ow to find its algebraically. Tis starts wit te simplest possible its, and ten builds tese up to more complicated examples. Fact.

More information

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,

More information

Math 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006

Math 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006 Mat 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006 f(x+) f(x) 10 1. For f(x) = x 2 + 2x 5, find ))))))))) and simplify completely. NOTE: **f(x+) is NOT f(x)+! f(x+) f(x) (x+) 2 + 2(x+) 5 ( x 2

More information

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as

More information

THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS

THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS MATHEMATICS OF COMPUTATION Volume 00, Number 0, Pages 000 000 S 0025-5718XX0000-0 THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS GERHARD DZIUK AND JOHN E. HUTCHINSON Abstract. We solve te problem of

More information

Some Error Estimates for the Finite Volume Element Method for a Parabolic Problem

Some Error Estimates for the Finite Volume Element Method for a Parabolic Problem Computational Metods in Applied Matematics Vol. 13 (213), No. 3, pp. 251 279 c 213 Institute of Matematics, NAS of Belarus Doi: 1.1515/cmam-212-6 Some Error Estimates for te Finite Volume Element Metod

More information

Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS

Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS Opuscula Matematica Vol. 26 No. 3 26 Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS Abstract. In tis work a new numerical metod is constructed for time-integrating

More information

CS522 - Partial Di erential Equations

CS522 - Partial Di erential Equations CS5 - Partial Di erential Equations Tibor Jánosi April 5, 5 Numerical Di erentiation In principle, di erentiation is a simple operation. Indeed, given a function speci ed as a closed-form formula, its

More information

Exercises for numerical differentiation. Øyvind Ryan

Exercises for numerical differentiation. Øyvind Ryan Exercises for numerical differentiation Øyvind Ryan February 25, 2013 1. Mark eac of te following statements as true or false. a. Wen we use te approximation f (a) (f (a +) f (a))/ on a computer, we can

More information

A posteriori error estimates for non-linear parabolic equations

A posteriori error estimates for non-linear parabolic equations A posteriori error estimates for non-linear parabolic equations R Verfürt Fakultät für Matematik, Rur-Universität Bocum, D-4478 Bocum, Germany E-mail address: rv@num1rur-uni-bocumde Date: December 24 Summary:

More information

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these. Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra

More information

Strongly continuous semigroups

Strongly continuous semigroups Capter 2 Strongly continuous semigroups Te main application of te teory developed in tis capter is related to PDE systems. Tese systems can provide te strong continuity properties only. 2.1 Closed operators

More information

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract Superconvergence of energy-conserving discontinuous Galerkin metods for linear yperbolic equations Yong Liu, Ci-Wang Su and Mengping Zang 3 Abstract In tis paper, we study superconvergence properties of

More information

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist Mat 1120 Calculus Test 2. October 18, 2001 Your name Te multiple coice problems count 4 points eac. In te multiple coice section, circle te correct coice (or coices). You must sow your work on te oter

More information

Some Review Problems for First Midterm Mathematics 1300, Calculus 1

Some Review Problems for First Midterm Mathematics 1300, Calculus 1 Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,

More information

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY (Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative

More information

Parameter Fitted Scheme for Singularly Perturbed Delay Differential Equations

Parameter Fitted Scheme for Singularly Perturbed Delay Differential Equations International Journal of Applied Science and Engineering 2013. 11, 4: 361-373 Parameter Fitted Sceme for Singularly Perturbed Delay Differential Equations Awoke Andargiea* and Y. N. Reddyb a b Department

More information

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is Mat 180 www.timetodare.com Section.7 Derivatives and Rates of Cange Part II Section.8 Te Derivative as a Function Derivatives ( ) In te previous section we defined te slope of te tangent to a curve wit

More information

2.11 That s So Derivative

2.11 That s So Derivative 2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point

More information

Cubic Functions: Local Analysis

Cubic Functions: Local Analysis Cubic function cubing coefficient Capter 13 Cubic Functions: Local Analysis Input-Output Pairs, 378 Normalized Input-Output Rule, 380 Local I-O Rule Near, 382 Local Grap Near, 384 Types of Local Graps

More information

MVT and Rolle s Theorem

MVT and Rolle s Theorem AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state

More information

Convexity and Smoothness

Convexity and Smoothness Capter 4 Convexity and Smootness 4. Strict Convexity, Smootness, and Gateaux Di erentiablity Definition 4... Let X be a Banac space wit a norm denoted by k k. A map f : X \{0}!X \{0}, f 7! f x is called

More information

GELFAND S PROOF OF WIENER S THEOREM

GELFAND S PROOF OF WIENER S THEOREM GELFAND S PROOF OF WIENER S THEOREM S. H. KULKARNI 1. Introduction Te following teorem was proved by te famous matematician Norbert Wiener. Wiener s proof can be found in is book [5]. Teorem 1.1. (Wiener

More information

Reflection Symmetries of q-bernoulli Polynomials

Reflection Symmetries of q-bernoulli Polynomials Journal of Nonlinear Matematical Pysics Volume 1, Supplement 1 005, 41 4 Birtday Issue Reflection Symmetries of q-bernoulli Polynomials Boris A KUPERSHMIDT Te University of Tennessee Space Institute Tullaoma,

More information

Polynomials 3: Powers of x 0 + h

Polynomials 3: Powers of x 0 + h near small binomial Capter 17 Polynomials 3: Powers of + Wile it is easy to compute wit powers of a counting-numerator, it is a lot more difficult to compute wit powers of a decimal-numerator. EXAMPLE

More information

1. Introduction. We consider the model problem: seeking an unknown function u satisfying

1. Introduction. We consider the model problem: seeking an unknown function u satisfying A DISCONTINUOUS LEAST-SQUARES FINITE ELEMENT METHOD FOR SECOND ORDER ELLIPTIC EQUATIONS XIU YE AND SHANGYOU ZHANG Abstract In tis paper, a discontinuous least-squares (DLS) finite element metod is introduced

More information