Some approximation theorems in Math 522. I. Approximations of continuous functions by smooth functions
|
|
- Kelly Thornton
- 5 years ago
- Views:
Transcription
1 Some approximation theorems in Math 522 I. Approximations of continuous functions by smooth functions The goal is to approximate continuous functions vanishing at ± by smooth functions. In a previous homewor problem a C -function φ was constructed with the property that φ is positive on (, and φ(t = 0 for t. If we divide by a suitable constant we may achieve and assume and we may also write Now for s > 0 define φ(tdt = φ(tdt = since φ vanishes off [,]. φ s (t = s φ( t. s Then we also have φ s (tdt =, by the substitution u = t/s. Graph the function φ s for small values of the parameter s. Definition. For continuous f C(R we define A s f(x = φ s (x tf(tdt. We shall be interested in the behavior of A s f for s 0. Note that the t-integral extends over a compact interval depending on x, s. The integral is also called a convolution of the functions φ s and f. Exercise: Let f C(R. Show that for every s > 0 the function x A s f is a C function on (,. If lim x f(x = 0 then show also that lim x A s f(x = 0. Theorem. (a Let f C(R and let J be any compact interval. Then, as s 0, A s f converges to f uniformly on J. (b Let f be as in (a and assume in addition that lim x f(x = 0. Then A s f converges to f uniformly on R. Proof. We shall only prove part (b. As an exercise you can prove part (a in the same way, or alternatively, deduce it from part (b. One may change variables to write A s f(x = φ s (tf(x tdt. TheconvolutionoftwofunctionsdefinedonRisgivenbyf g(x = f(yg(x ydy whenever this maes sense; one checs f g = g f.
2 2 Since φ s (tdt = we see that A s f(x f(x = φ s (t[f(x t f(x]dt. Note that, since φ s (t = 0 for t > s, the t integral is really an integral over [ s,s]. The assumptions that f is continuous and that lim x f(x = 0 imply that f is uniformly continuous on R (prove this!. Thus given ε > 0 there is a δ > 0 so that f(x t f(x < ε/2 for all t with t δ and for all x R. If 0 < s < δ we have by the nonnegativity of φ s A s f(x f(x for all x R. s sφ s (t f(x t f(x dt ε 2 s sφ s (tdt = ε 2 Terminology: The linear transformations (aa as linear operators A s are called approximations of the identity. The identity operator Id is simply given by Id(f = f, and the above Theorem says that the operators A s approximate in a certain sense the identity operator as s 0. One can use other approximations of the identity defined lie the one above where φ is replaced by a not necessarily compactly supported function. If one drops the compact support the proofs get slightly more involved. Other types of approximations of the identity (with a parameter n are given by the families of linear operators L n in II below and B n in III below. For each f these linear operators will produce families of polynomials depending on f. II. The Weierstrass approximation theorem Theorem. Let f be a continuous function on an interval [a, b]. Then f can be uniformly approximated by polynomials on [a, b]. In other words: Given ε > 0 there exists a polynomial P (depending on ε so that max f(x P(x ε. x [a,b] Here f may be complex valued and then a polynomial is a function of the form N =0 a x with complex coefficients a (considered for x [a,b]. If f is real-valued, the polynomial can be chosen real-valued. Define The Landau polynomials. Q n (x = c n ( x 2 n where c n = ( ( s2 n ds so that Q n(tdt =.
3 Let f be continuous on the interval [ /2, /2]. The sequence of Landau polynomials associated to f is defined by L n f(x = /2 /2 f(tq n (t xdt. Verify that L n f is a polynomial of degree at most 2n. We shall prove the Weierstrass approximation theorem for the interval I γ := [ 2 +γ, 2 γ] for small γ > 0, by using the Landau Polynomials. By a change of variable one can then use the Weierstrass approximation theorem on any compact interval [a,b]. See the last paragraph in this section. Our first concrete version of the Weierstrass approximation theorem is Theorem. Let γ > 0 and let I γ = [ /2+γ,/2 γ]. The sequence L n f converges to f, uniformly on the interval I γ, i.e. max L N f(x f(x 0. x I γ 3 Proof. 2 We first need some information about the size of the polynomials Q n. Consider c n = ( s2 n ds. We use the inequality ( x 2 n nx 2, for 0 x. To see this let h(x = ( x 2 n +nx 2. The derivative of h is h (x = 2xn( x 2 n +2nx = 2nx( ( x 2 n which is positive for x [0,]. Thus h is increasing on [0,] and since h(0 = 0 we see that h(x 0 for x [0,]. Since h is even we have h(x 0 for x [,]. We use the last displayed inequality in the integral defining the constant c n and get n = ( x 2 n dx = 2 c and from this we obtain 2 ( x 2 n dx 2 0 n /2 0 n /2 ( nx 2 dx > n /2 ( Q n (x n( x 2 n. 0 ( x 2 n dx Given ε > 0 the goal is to show that max x Iγ L n f(x f(x < ε for sufficiently large n. Let ε > 0. Since f is uniformly continuous on [ /2,/2] we can find δ > 0 so that δ < γ and so that for all x I γ and all t with t δ we have that f(x+t f(x < ε/4. 2 The proof here is essentially the same as the proof of Weierstrass theorem in Theorem 7.26 of W. Rudin s boo.
4 4 Write (with a change of variables /2 /2 f(sq n (s xds = 2 +x 2 +x f(t+xq n (tdt Since x I γ = [ /2 + γ,/2 γ] and since δ < γ we have /2 + x < < δ < /2+x. We may thus split the integral as /2+x x δ f(t+xq n (tdt. The idea is that the first and the third term will be small for large n. We modify the middle integral further to write f(t+xq n (tdt = and finally (using Q n(tdt = f(x Q n (tdt = f(x f(x Putting it all together we get where Estimate I n (x = II n (x = [f(t+x f(x]q n (tdt+f(x Q N (tdt f(x L n f(x f(x = I n (x+ii n (x+iii n (x [f(t+x f(x]q n (tdt /2+x III n (x = f(x I n (x = f(t+xq n (tdt+ Q N (tdt f(x 2 +x δ f(t+x f(x Q n (tdt δ δ Q n (tdt Q N (tdt. f(t+xq n (tdt Q N (tdt. ε N (tdt 4 Q ε Q N (tdt = ε 4 4 ; this estimate is true for all n. Now let M = max x [ /2,/2] f(x. Then by our estimate (* for Q n we see that II n (x + III n (x 2M max Q n(t 2M n( 2 n t [,] [δ,] and since 2M n( 2 n tends to 0 as n we see that there is N so that for n N we have max x Iγ II n (x+iii n (x < ε/2 for n N. If we combine this with the estimate for I n (x we see that L n f(x f(x < ε for n > N and all x I γ.
5 5 Arbitrary compact intervals. Consider an interval[a, b] and let f C([a, b]. Let l(t = Ct + D so that l( 2 + γ = a and l( 2 γ = b (you can compute that C, D explicitly and C 0, the inverse of l is given by l (x = C x C D. The function g l is in C(I γ. Thus there exists a polynomial P such that max g(l(t P(t < ε t I γ and therefore if we set Q(x = P(l (x then Q is a polynomial and we have max g(x Q(x < ε. x [a,b] Remar: A much more general version of the Weierstrass approximation theorem is due to Marshall Stone, the Stone-Weierstrass theorem. We will prove it in class and the proof can be found in Rudin s boo. III. The Bernstein polynomials: A second proof of Weierstrass theorem Here we consider the interval [0,]. For n =,2,... define B n f(t = f( ( n n t ( t n, =0 the sequence of Bernstein polynomials associated to f. Here ( n = n!!(n!, the binomial coefficients. For each n, B n f is a polynomial of degree at most n. Theorem. If f C([0,] then the polynomials B n f converge to f uniformly on [0,]. For the proof we will use the following auxiliary Lemma. ( ( n n t2 t ( t n n. 0 n We shall first prove the Theorem based on the Lemma and then give a proof of the Lemma. There is also a probabilistic interpretation of the Lemma which is appended below. Proof of the theorem. By the binomial theorem ( n = (t+( t n = t ( t n =0
6 6 and thus we may write B n f(t f(t = = f( ( n n t ( t n f(t =0 =0 0 n n t δ [ f( n f(t] ( n t ( t n Given ε > 0 find δ > 0 so that f(t+h f(t ε/4 if t,t +h [0,] and h < δ. For the terms with n t δ we will exploit the smallness of f( n f(t] and for the terms with n t > δ we will exploit the smallness of the term in the Lemma, for large n. We thus split B n f(t f(t = I n (t+ii n (t where I n (t = ( [ n f( n f(t] t ( t n II n (t = 0 n n t >δ [ f( n f(t] ( n t ( t n the decomposition depends of course on δ but δ does not depend on n. We show that I n (t ε/4 for all n = 2,3,... Indeed, since f( n f(t ε/4 for n t δ we compute I n (t f( ( n n f(t t ( t n ε 4 0 n n t δ 0 n ( n t ( t n = ε 4 where we have used again the binomial theorem. Concerning II n we observe that δ 2 ( n t2 for n t δ and estimate f( n f(t 2max f. Thus II n (t δ 2 ( ( n t2 n f( n f(t t ( t n 0 n n t >δ δ 2 2max f 0 n ( n t2 ( n t ( t n By the Lemma II n (t (4n δ 2 2max f and for sufficiently large n this is ε/2 and we are done.
7 Proof of the Lemma. We set ψ 0 (t =, ψ (t = t and ψ 2 (t = t 2, etc. Then we can explicitly compute the polynomials B n ψ 0, B n ψ, B n ψ 2 for n =,2,... First, by the binomial theorem (as used before ( n B n ψ 0 (t = t ( t n = =0 =0 thus B n ψ 0 = ψ 0. Next for n B n ψ (t = n ( n t ( t n (n! = (!(n! t ( t n = ( n = t t ( t n ( = n ( n = t t j ( t n j = t j j=0 which means B n ψ = ψ for n. To compute B n ψ 2 we observe that B ψ 2 (t = ψ 2 (0( t+ψ 2 (t = t = ψ (t and, for n 2 B n ψ 2 (t = =0 2 n 2 ( n t ( t n + (n! = n (!(n! t ( t n = = ( ( n 2 t 2 (n t 2 ( t n 2 ( 2 n 2 =2 ( n +t t ( t n ( = = (n t2 +t = t 2 + t t2 n n. We summarize: For n 2 we have B n ψ 0 = ψ 0, B n ψ = ψ, B n ψ 2 = ψ 2 + n (ψ ψ 2. To prove the assertion in the Lemma lets multiply out ( n t2 = ( n 2 2t n +t2 7
8 8 and use that the transformation f B n f(t is linear (i.e we have B n [c f + c 2 f 2 ](x = c B n f (x+c 2 B n f 2 (x for functions f,f 2 and scalars c,c 2. We compute, for n 2 ( ( n n t2 t ( t n 0 n = B n ψ 2 (t 2tB n ψ (t+t 2 = t 2 + t t2 2t t+t 2 = t t2 n n and since max 0 t t t 2 = /4 we get the assertion of the Lemma. Remar. Let s consider an arbitrary compact interval [a, b] and let f C([a, b]. Then the polynomials ( n (x a P n f(x = f(a+ n (b a (b x n (b a n =0 converge to f uniformly on [a,b]. Using a change of variable derive this statement from the above theorem.
9 9 Addendum: Probabilistic interpretation of the Bernstein polynomials. You might have seen the expressions B n f(t in a course on probability. In what follows the parameter t is a parameter for a probability (between 0 and. Let s consider a series of trials of an experiment. Each trial may is supposed to have two possible outcomes (either success or failure. Each integer in X n := {,...,n} represents a trial; we label the jth trial as T j. Let t [0,] be fixed. In each trial the probability of success is assumed to be t, and the probability of failure is then ( t. The trials are supposed to be independent. Let A be a specific subset of {,...,n} which is of cardinality, i.e. A is of the form {j,j 2,...,j } for mutually different integers j,...,j ; if = 0 then A =. Then the event Ω A that for each j A the trial T j results in a successandforeach j X N \A thetrial T j resultsinafailurehasprobability t ( t n. There are exactly ( n subsets A of Xn which have cardinality and they represent mutually exclusive (aa disjoint events. Let Ω be the event that the n trials result in successes, then the probability of Ω is ( n P(Ω = t ( t n. The probabilities of the mutually exclusive events Ω add up to ; P(Ω = ; =0 (cf. the binomial theorem. Let now X be the number of successes in a series of n trials (X is a random variable which depends on the outcome of each trial. The event Ω is just the event that X assumes the value (one writes P(Ω also as P(X =. The random variable X/n is the ratio of successes and total numberoftrials, andit taes values in[0,] (moreprecisely in{0, n,..., n n }. The expected value of X/n is by definition =0 E[X/n] = =0 n P(Ω and in the proof of the Lemma we computed it to ( n E[X/n] = t ( t n = B n ψ (t = t. n Generally, if f is a function of t, the expected value of f(x/n is equal to E[f(X/n] = f ( P(Ω = f( ( n n n t ( t n ; =0 =0
10 0 that gives the probabilistic interpretation of the Bernstein polynomials evaluated at t; B n f(t = E[f(X/n]. The Variance of X/n is given by E [( X n E[X n ] 2] = ( ( n t n t2 ( t n = t t2 n, =0 as computed in the proof of the lemma. Letδ > 0beasmallnumber. Theprobabilitythatthenumberofsuccesses deviates from the expected value tn by more than δn is given by 0 n nt δn P(Ω = 0 n nt δn ( n t ( t n. The smallness of this quantity (uniformly in t played an important role in the Bernstein proof of Weierstrass theorem. It was estimated by [ ( X E[X] ] 2 E = δ 2 ( ( n t δn n t2 ( t n = t t2 δ 2 n. =0 Thus,bythestatementoftheLemma, theeventthatthenumberofsuccesses deviates fromtheexpectedvaluetnbymorethanδnhasprobabilitynomore than (4δ 2 n. IV. Approximation by trigonometrical polynomials. Prelude: Basic facts and formulas for the partial sum operator for Fourier series. Consider the partial sums of the Fourier series S n f(x = c e ix = n where c = f(te it dt are the Fourier coefficients. We can write π S n f(x = f(ye iy dye ix = n = f(yd n (x ydy where D n (t = = n e it. Definition. The convolution of two periodic functions f, g is defined as f g(x = f(yg(x ydy.
11 Note that the convolution of periodic continuous functions is well defined and is again a -periodic continuous function. and we also have the commutativity property f g(x = g f(x To see we first note that for a periodic inegrable functione we have F(tdt = a+π a F(tdt for any a. The commutativity property follows if in the definition of f g we change variables t = x y (with dt = dy and get f g(x = = x+π x f(yg(x ydy = f(x tg(tdt = x x+π f(x tg(t( dt g(tf(x tdt = g f(x where in the last formula we have used the -periodicity of f and g. Going bac to the partial sum of the Fourier series we have S n f(x = f D n (x = D n f(x where D n (t = e it. = n Below we will need a more explicit expression for D n, namely To see this we use n e i(n+t D n (t = sin(n+ 2 t sin t 2 =0 eit = ei(n+t e it and = n eit = n = e it = andthesecondsumcanbesimplifiedto e int. ThusD e it e it n (t =. Multiplying numerator and denominator with e it/2 yields e i(n+t e int e it D n (t = ei(n+/2t e i(n+/2t e it/2 e it/2 and this yields the displayed formula. Fejér s theorem We would lie to prove that every continuous function can be approximated by trigonometric polynomials, uniformly on [, π]. One may thin that, in view of Theorem 8. in Rudin s boo, the partial sums S n f of the Fourier series are good candidates for such an approximation. Unfortunately for merely continuous f, given x, the partial sums S n f(x may not converge to f(x (and then of course S n f cannot converge uniformly. 3 3 The situation is even worse. Given x [,π] one can show that in a certain sense the convergence of S nf(x fails for typical f. I hope to return to this point later in the class.
12 2 However instead of S n f we consider the better behaved arithmetic means (or Cesàro means of the partial sums. Define σ N f(x = N + N S n f(x. The means σ N f are also called the Fejér means of the Fourier series, in tribute to the Hungarian mathematician Leopold Fejér who in 900 published the following Theorem. Let f be a continuous -periodic function. Then the means σ N f converge to f uniformly, i.e. n=0 max x R σ Nf(x f(x 0, as N. If we use the convolution formula S n f = D n f then it follows that where σ N f(x = K N f(x = = K N (t = N + K N (x yf(ydy K N (tf(x tdt N D n (t n=0 K N is called the Nth Fejér ernel. We need the following properties of K N. Lemma. (a Explicit formulas for K N on [,π] are given by K N (x = cos(n +x N + cosx ( sin N+ 2 = x 2, 2(N + sin x 2 if x is not an integer multiple of. Also K N (0 = N +. (b K N (x 0 for all x 0. (c π K N (tdt =. (d K N (x ( 2 for 0 < δ x π. N + cosδ By (c, (d most of K N is concentrated near 0 for large N. Properties (b, (c, (d are important, the explicit expressions for K N much less so.
13 Proof of the Lemma. We use and rewrite the above explicit formula for the Dirichlet ernel namely D n (x = sin(n+ 2 x sin x 2 = sin x 2 sin(n+ 2 x sin 2 x. 2 Observe that 2sinasinb = cos(a b cos(a + b and apply this with a = (n+ 2 x, b = x 2 to get Thus D n (x = cosnx cos(n+x 2sin 2 x. 2 K N (x = N + = N + = N + N D n (x n=0 N n=0 cosnx cos(n+x 2sin 2 x 2 cos(n +x 2sin 2 x 2 Now recall the formula cos2a = cos 2 a sin 2 a = 2sin 2 a, hence 2sin 2 a = cos2a. If we use this for a = x/2 we get the first claimed formula for K N, and if we use it for a = (N + x 2 then we get the second claimed formula. Compute the limit as x 0, this yields K N (0 = N +. Property (d is immediate from the first explicit formula. Estimate cos(n + x 2 and ( cosx cosδ for δ x π and also use that the cosine is an even function to get the same estimate for x. The nonnegativity of K N is also clear from the explicit formulas. The property (c follows from D n(tdt = (and taing the arithmetic mean of s gives a. Proof of Fejér s theorem. Given ε > 0 we have to show that there is M = M(ε so that for all N M, Now we write σ N f(x f(x = = σ N f(x f(x ε for all x. K N (tf(x tdt f(x K N (t [ f(x t f(x ] dt; here we have used property (c. f is continuous and therefore uniformly continuous on any compact interval. Since f is also -periodic, f is uniformly continuous on R. This means 3
14 4 that there is a δ > 0 such that f(x t f(x ε 4 for t δ, and allx R. We split the integral into two parts: where K N (t [ f(x t f(x ] dt = I N (x+ii N (x I N (x = II N (x = K N (t [ f(x t f(x ] dt, [,π]\[,δ] K N (t [ f(x t f(x ] dt. We give an estimate of I N which holds for all N. Namely I N (x K N (t f(x t f(x dt K N (t ε 4 dt K N (t ε 4 dt = ǫ 4, by (b and (c. Since this estimate holds for all N we may now choose N large to estimate the second term II N (x. We use property (d to estimate the integral for x [δ,π] [,]. We crudely bound f(x t f(x f(x t + f(x 2max f. Thus II N (x 2max f N + ( 4max f cosδ [,π]\[,δ]. N + ( 2 cosδ dt As N+ 0 as N we may choose N 0 so that for N N 0 the quantity ( 4max f N+ cos δ is less than ε/4. Thus for N N0 both quantities I N (x and II N (x are ε/4 for all x and thus we conclude that max x R σ Nf(x f(x ε/2 for N N 0. An application for the partial sum operator Theorem. Let f be a continuous -periodic function. Then ( /2 S n f(x f(x dx 2 = 0 lim n
15 i.e., S n f converges to f in the L 2 -norm in the space of square-integrable functions. 4 Proof. By Theorem 8. in Rudin (which is linear algebra we have S N t M = t M for every trigonometric polynomial t M (x = M = M γ e it provided that N M. Now let ε > 0. By Fejér s theorem we can find such a trigonometric polynomial t M (of some degree M depending on ǫ so that max f(x t M (x ε. Then for n > M we have S n f f = S n (f t M (f t M. We also have SN (f t M 2 f t M 2 this is just (76 in 8.3 in Rudin. Thus S n f f S n (f t M + f t M 2 f t M. 5 But we have ( π /2 f(x t M (x 2 dx max f tm < ε 2 and we are done. Fejér s theorem implies the Weierstrass approximation theorem A very short proof of the Weierstrass approximation theorem can be given assuming Fejér s theorem. By a change of variable it suffices to consider the interval [a,b] = [ π 2, π 2 ]. Extend the function f to a continuous function F on [,π] so that F(x = f(x on [ π 2, π 2 ] and F( = F(π = 0. Then we can extend F to a continuous periodic function on R. Let ε > 0. By Fejér s theorem we can find a trigonometric polynomial N T(x = a 0 + [a cosx+b sinx] = so that max F(x T(x < ε/2. x R Now the Taylor series for cos and sin converge uniformly on every compact interval. Thus we can find a polynomial P so that max T(x P(x < ε/2. x [.π] Combining the two estimates (and using that f = F on [ π 2, π 2 ] yields max f(x P(x = max F(x P(x < ε. x π/2 x π/2 4 ( Recall: This norm is given by f = f(x 2 dx /2 and is derived from the scalar product f,g = π f(xg(xdx.
be the set of complex valued 2π-periodic functions f on R such that
. Fourier series. Definition.. Given a real number P, we say a complex valued function f on R is P -periodic if f(x + P ) f(x) for all x R. We let be the set of complex valued -periodic functions f on
More information7: FOURIER SERIES STEVEN HEILMAN
7: FOURIER SERIES STEVE HEILMA Contents 1. Review 1 2. Introduction 1 3. Periodic Functions 2 4. Inner Products on Periodic Functions 3 5. Trigonometric Polynomials 5 6. Periodic Convolutions 7 7. Fourier
More information1 + lim. n n+1. f(x) = x + 1, x 1. and we check that f is increasing, instead. Using the quotient rule, we easily find that. 1 (x + 1) 1 x (x + 1) 2 =
Chapter 5 Sequences and series 5. Sequences Definition 5. (Sequence). A sequence is a function which is defined on the set N of natural numbers. Since such a function is uniquely determined by its values
More informationINTRODUCTION TO REAL ANALYSIS II MATH 4332 BLECHER NOTES
INTRODUCTION TO REAL ANALYSIS II MATH 433 BLECHER NOTES. As in earlier classnotes. As in earlier classnotes (Fourier series) 3. Fourier series (continued) (NOTE: UNDERGRADS IN THE CLASS ARE NOT RESPONSIBLE
More informationMATH 5640: Fourier Series
MATH 564: Fourier Series Hung Phan, UMass Lowell September, 8 Power Series A power series in the variable x is a series of the form a + a x + a x + = where the coefficients a, a,... are real or complex
More information1 Taylor-Maclaurin Series
Taylor-Maclaurin Series Writing x = x + n x, x = (n ) x,.., we get, ( y ) 2 = y ( x) 2... and letting n, a leap of logic reduces the interpolation formula to: y = y + (x x )y + (x x ) 2 2! y +... Definition...
More informationIowa State University. Instructor: Alex Roitershtein Summer Homework #5. Solutions
Math 50 Iowa State University Introduction to Real Analysis Department of Mathematics Instructor: Alex Roitershtein Summer 205 Homework #5 Solutions. Let α and c be real numbers, c > 0, and f is defined
More informationREAL AND COMPLEX ANALYSIS
REAL AND COMPLE ANALYSIS Third Edition Walter Rudin Professor of Mathematics University of Wisconsin, Madison Version 1.1 No rights reserved. Any part of this work can be reproduced or transmitted in any
More informationMath 321 Final Examination April 1995 Notation used in this exam: N. (1) S N (f,x) = f(t)e int dt e inx.
Math 321 Final Examination April 1995 Notation used in this exam: N 1 π (1) S N (f,x) = f(t)e int dt e inx. 2π n= N π (2) C(X, R) is the space of bounded real-valued functions on the metric space X, equipped
More informationThe Space of Continuous Functions
Chapter 3 The Space of Continuous Functions dddddddddddddddddddddddddd dddd ddddddddddddddddddddd dddddddddddddddddd ddddddd ddddddddddddddddddddddddd ddddddddddddddddddddddddd dddddddddddddd ddddddddddd
More informationFourier Series. ,..., e ixn ). Conversely, each 2π-periodic function φ : R n C induces a unique φ : T n C for which φ(e ix 1
Fourier Series Let {e j : 1 j n} be the standard basis in R n. We say f : R n C is π-periodic in each variable if f(x + πe j ) = f(x) x R n, 1 j n. We can identify π-periodic functions with functions on
More informationExercises from other sources REAL NUMBERS 2,...,
Exercises from other sources REAL NUMBERS 1. Find the supremum and infimum of the following sets: a) {1, b) c) 12, 13, 14, }, { 1 3, 4 9, 13 27, 40 } 81,, { 2, 2 + 2, 2 + 2 + } 2,..., d) {n N : n 2 < 10},
More informationFurther Mathematical Methods (Linear Algebra) 2002
Further Mathematical Methods (Linear Algebra) Solutions For Problem Sheet 9 In this problem sheet, we derived a new result about orthogonal projections and used them to find least squares approximations
More informationAnalysis Qualifying Exam
Analysis Qualifying Exam Spring 2017 Problem 1: Let f be differentiable on R. Suppose that there exists M > 0 such that f(k) M for each integer k, and f (x) M for all x R. Show that f is bounded, i.e.,
More informationLecture 32: Taylor Series and McLaurin series We saw last day that some functions are equal to a power series on part of their domain.
Lecture 32: Taylor Series and McLaurin series We saw last day that some functions are equal to a power series on part of their domain. For example f(x) = 1 1 x = 1 + x + x2 + x 3 + = ln(1 + x) = x x2 2
More informationFourier Series. 1. Review of Linear Algebra
Fourier Series In this section we give a short introduction to Fourier Analysis. If you are interested in Fourier analysis and would like to know more detail, I highly recommend the following book: Fourier
More information1.1 Appearance of Fourier series
Chapter Fourier series. Appearance of Fourier series The birth of Fourier series can be traced back to the solutions of wave equation in the work of Bernoulli and the heat equation in the work of Fourier.
More informationFinite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product
Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )
More information2 Sequences, Continuity, and Limits
2 Sequences, Continuity, and Limits In this chapter, we introduce the fundamental notions of continuity and limit of a real-valued function of two variables. As in ACICARA, the definitions as well as proofs
More informationTHE GAMMA FUNCTION AND THE ZETA FUNCTION
THE GAMMA FUNCTION AND THE ZETA FUNCTION PAUL DUNCAN Abstract. The Gamma Function and the Riemann Zeta Function are two special functions that are critical to the study of many different fields of mathematics.
More informationTaylor and Maclaurin Series
Taylor and Maclaurin Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Background We have seen that some power series converge. When they do, we can think of them as
More informationMath 421, Homework #9 Solutions
Math 41, Homework #9 Solutions (1) (a) A set E R n is said to be path connected if for any pair of points x E and y E there exists a continuous function γ : [0, 1] R n satisfying γ(0) = x, γ(1) = y, and
More informatione x = 1 + x + x2 2! + x3 If the function f(x) can be written as a power series on an interval I, then the power series is of the form
Taylor Series Given a function f(x), we would like to be able to find a power series that represents the function. For example, in the last section we noted that we can represent e x by the power series
More informationMath 115 ( ) Yum-Tong Siu 1. Derivation of the Poisson Kernel by Fourier Series and Convolution
Math 5 (006-007 Yum-Tong Siu. Derivation of the Poisson Kernel by Fourier Series and Convolution We are going to give a second derivation of the Poisson kernel by using Fourier series and convolution.
More informationMath The Laplacian. 1 Green s Identities, Fundamental Solution
Math. 209 The Laplacian Green s Identities, Fundamental Solution Let be a bounded open set in R n, n 2, with smooth boundary. The fact that the boundary is smooth means that at each point x the external
More informationCharacteristic Functions and the Central Limit Theorem
Chapter 6 Characteristic Functions and the Central Limit Theorem 6.1 Characteristic Functions 6.1.1 Transforms and Characteristic Functions. There are several transforms or generating functions used in
More informationMATH NEW HOMEWORK AND SOLUTIONS TO PREVIOUS HOMEWORKS AND EXAMS
MATH. 4433. NEW HOMEWORK AND SOLUTIONS TO PREVIOUS HOMEWORKS AND EXAMS TOMASZ PRZEBINDA. Final project, due 0:00 am, /0/208 via e-mail.. State the Fundamental Theorem of Algebra. Recall that a subset K
More informationSome analysis problems 1. x x 2 +yn2, y > 0. g(y) := lim
Some analysis problems. Let f be a continuous function on R and let for n =,2,..., F n (x) = x (x t) n f(t)dt. Prove that F n is n times differentiable, and prove a simple formula for its n-th derivative.
More informationSection 5.8. Taylor Series
Difference Equations to Differential Equations Section 5.8 Taylor Series In this section we will put together much of the work of Sections 5.-5.7 in the context of a discussion of Taylor series. We begin
More informationMathematics 324 Riemann Zeta Function August 5, 2005
Mathematics 324 Riemann Zeta Function August 5, 25 In this note we give an introduction to the Riemann zeta function, which connects the ideas of real analysis with the arithmetic of the integers. Define
More informationIntroduction to Fourier Analysis
Lecture Introduction to Fourier Analysis Jan 7, 2005 Lecturer: Nati Linial Notes: Atri Rudra & Ashish Sabharwal. ext he main text for the first part of this course would be. W. Körner, Fourier Analysis
More informationTopics in Fourier analysis - Lecture 2.
Topics in Fourier analysis - Lecture 2. Akos Magyar 1 Infinite Fourier series. In this section we develop the basic theory of Fourier series of periodic functions of one variable, but only to the extent
More informationNumerical Analysis: Interpolation Part 1
Numerical Analysis: Interpolation Part 1 Computer Science, Ben-Gurion University (slides based mostly on Prof. Ben-Shahar s notes) 2018/2019, Fall Semester BGU CS Interpolation (ver. 1.00) AY 2018/2019,
More information1 Homework. Recommended Reading:
Analysis MT43C Notes/Problems/Homework Recommended Reading: R. G. Bartle, D. R. Sherbert Introduction to real analysis, principal reference M. Spivak Calculus W. Rudin Principles of mathematical analysis
More informationNotes on uniform convergence
Notes on uniform convergence Erik Wahlén erik.wahlen@math.lu.se January 17, 2012 1 Numerical sequences We begin by recalling some properties of numerical sequences. By a numerical sequence we simply mean
More informationFOURIER SERIES WITH THE CONTINUOUS PRIMITIVE INTEGRAL
Real Analysis Exchange Summer Symposium XXXVI, 2012, pp. 30 35 Erik Talvila, Department of Mathematics and Statistics, University of the Fraser Valley, Chilliwack, BC V2R 0N3, Canada. email: Erik.Talvila@ufv.ca
More informationIB Mathematics HL Year 2 Unit 11: Completion of Algebra (Core Topic 1)
IB Mathematics HL Year Unit : Completion of Algebra (Core Topic ) Homewor for Unit Ex C:, 3, 4, 7; Ex D: 5, 8, 4; Ex E.: 4, 5, 9, 0, Ex E.3: (a), (b), 3, 7. Now consider these: Lesson 73 Sequences and
More informationHARMONIC ANALYSIS TERENCE TAO
HARMONIC ANALYSIS TERENCE TAO Analysis in general tends to revolve around the study of general classes of functions (often real-valued or complex-valued) and operators (which take one or more functions
More informationMa 530 Power Series II
Ma 530 Power Series II Please note that there is material on power series at Visual Calculus. Some of this material was used as part of the presentation of the topics that follow. Operations on Power Series
More informationExercise 1. Let f be a nonnegative measurable function. Show that. where ϕ is taken over all simple functions with ϕ f. k 1.
Real Variables, Fall 2014 Problem set 3 Solution suggestions xercise 1. Let f be a nonnegative measurable function. Show that f = sup ϕ, where ϕ is taken over all simple functions with ϕ f. For each n
More informationd(x n, x) d(x n, x nk ) + d(x nk, x) where we chose any fixed k > N
Problem 1. Let f : A R R have the property that for every x A, there exists ɛ > 0 such that f(t) > ɛ if t (x ɛ, x + ɛ) A. If the set A is compact, prove there exists c > 0 such that f(x) > c for all x
More informationChapter 3a Topics in differentiation. Problems in differentiation. Problems in differentiation. LC Abueg: mathematical economics
Chapter 3a Topics in differentiation Lectures in Mathematical Economics L Cagandahan Abueg De La Salle University School of Economics Problems in differentiation Problems in differentiation Problem 1.
More information2) Let X be a compact space. Prove that the space C(X) of continuous real-valued functions is a complete metric space.
University of Bergen General Functional Analysis Problems with solutions 6 ) Prove that is unique in any normed space. Solution of ) Let us suppose that there are 2 zeros and 2. Then = + 2 = 2 + = 2. 2)
More information7. Let X be a (general, abstract) metric space which is sequentially compact. Prove X must be complete.
Math 411 problems The following are some practice problems for Math 411. Many are meant to challenge rather that be solved right away. Some could be discussed in class, and some are similar to hard exam
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION APPLICATIONS 5 (Maclaurin s and Taylor s series) A.J.Hobson
JUST THE MATHS UNIT NUMBER.5 DIFFERENTIATION APPLICATIONS 5 (Maclaurin s and Taylor s series) by A.J.Hobson.5. Maclaurin s series.5. Standard series.5.3 Taylor s series.5.4 Exercises.5.5 Answers to exercises
More informationh(x) lim H(x) = lim Since h is nondecreasing then h(x) 0 for all x, and if h is discontinuous at a point x then H(x) > 0. Denote
Real Variables, Fall 4 Problem set 4 Solution suggestions Exercise. Let f be of bounded variation on [a, b]. Show that for each c (a, b), lim x c f(x) and lim x c f(x) exist. Prove that a monotone function
More informationDepartment of Mathematics
Department of Mathematics Ma 3/103 KC Border Introduction to Probability and Statistics Winter 2017 Lecture 8: Expectation in Action Relevant textboo passages: Pitman [6]: Chapters 3 and 5; Section 6.4
More informationMa 221 Final Exam Solutions 5/14/13
Ma 221 Final Exam Solutions 5/14/13 1. Solve (a) (8 pts) Solution: The equation is separable. dy dx exy y 1 y0 0 y 1e y dy e x dx y 1e y dy e x dx ye y e y dy e x dx ye y e y e y e x c The last step comes
More information11.8 Power Series. Recall the geometric series. (1) x n = 1+x+x 2 + +x n +
11.8 1 11.8 Power Series Recall the geometric series (1) x n 1+x+x 2 + +x n + n As we saw in section 11.2, the series (1) diverges if the common ratio x > 1 and converges if x < 1. In fact, for all x (
More informationRecall that any inner product space V has an associated norm defined by
Hilbert Spaces Recall that any inner product space V has an associated norm defined by v = v v. Thus an inner product space can be viewed as a special kind of normed vector space. In particular every inner
More informationMATH MEASURE THEORY AND FOURIER ANALYSIS. Contents
MATH 3969 - MEASURE THEORY AND FOURIER ANALYSIS ANDREW TULLOCH Contents 1. Measure Theory 2 1.1. Properties of Measures 3 1.2. Constructing σ-algebras and measures 3 1.3. Properties of the Lebesgue measure
More informationSyllabus Fourier analysis
Syllabus Fourier analysis by T. H. Koornwinder, 1996 University of Amsterdam, Faculty of Science, Korteweg-de Vries Institute Last modified: 7 December 2005 Note This syllabus is based on parts of the
More informationTHE STONE-WEIERSTRASS THEOREM AND ITS APPLICATIONS TO L 2 SPACES
THE STONE-WEIERSTRASS THEOREM AND ITS APPLICATIONS TO L 2 SPACES PHILIP GADDY Abstract. Throughout the course of this paper, we will first prove the Stone- Weierstrass Theroem, after providing some initial
More informationX n D X lim n F n (x) = F (x) for all x C F. lim n F n(u) = F (u) for all u C F. (2)
14:17 11/16/2 TOPIC. Convergence in distribution and related notions. This section studies the notion of the so-called convergence in distribution of real random variables. This is the kind of convergence
More informationProblem Set 5: Solutions Math 201A: Fall 2016
Problem Set 5: s Math 21A: Fall 216 Problem 1. Define f : [1, ) [1, ) by f(x) = x + 1/x. Show that f(x) f(y) < x y for all x, y [1, ) with x y, but f has no fixed point. Why doesn t this example contradict
More informationQF101: Quantitative Finance August 22, Week 1: Functions. Facilitator: Christopher Ting AY 2017/2018
QF101: Quantitative Finance August 22, 2017 Week 1: Functions Facilitator: Christopher Ting AY 2017/2018 The chief function of the body is to carry the brain around. Thomas A. Edison 1.1 What is a function?
More informationON GENERALIZATIONS OF BOEHMIAN SPACE AND HARTLEY TRANSFORM. C. Ganesan and R. Roopkumar. 1. Introduction
MATEMATIČKI VESNIK MATEMATIQKI VESNIK 69, 2 (2017, 133 143 June 2017 originalni nauqni rad research paper ON GENERALIZATIONS OF BOEHMIAN SPACE AND HARTLEY TRANSFORM C. Ganesan and R. Roopkumar Abstract.
More informationChapter 2: Functions, Limits and Continuity
Chapter 2: Functions, Limits and Continuity Functions Limits Continuity Chapter 2: Functions, Limits and Continuity 1 Functions Functions are the major tools for describing the real world in mathematical
More information1.4 Techniques of Integration
.4 Techniques of Integration Recall the following strategy for evaluating definite integrals, which arose from the Fundamental Theorem of Calculus (see Section.3). To calculate b a f(x) dx. Find a function
More informationFourier Integral. Dr Mansoor Alshehri. King Saud University. MATH204-Differential Equations Center of Excellence in Learning and Teaching 1 / 22
Dr Mansoor Alshehri King Saud University MATH4-Differential Equations Center of Excellence in Learning and Teaching / Fourier Cosine and Sine Series Integrals The Complex Form of Fourier Integral MATH4-Differential
More informationSolutions to Tutorial 11 (Week 12)
THE UIVERSITY OF SYDEY SCHOOL OF MATHEMATICS AD STATISTICS Solutions to Tutorial 11 (Week 12) MATH3969: Measure Theory and Fourier Analysis (Advanced) Semester 2, 2017 Web Page: http://sydney.edu.au/science/maths/u/ug/sm/math3969/
More informationf (r) (a) r! (x a) r, r=0
Part 3.3 Differentiation v1 2018 Taylor Polynomials Definition 3.3.1 Taylor 1715 and Maclaurin 1742) If a is a fixed number, and f is a function whose first n derivatives exist at a then the Taylor polynomial
More informationFourth Week: Lectures 10-12
Fourth Week: Lectures 10-12 Lecture 10 The fact that a power series p of positive radius of convergence defines a function inside its disc of convergence via substitution is something that we cannot ignore
More informationMath 181, Exam 2, Study Guide 2 Problem 1 Solution. 1 + dx. 1 + (cos x)2 dx. 1 + cos2 xdx. = π ( 1 + cos π 2
Math 8, Exam, Study Guide Problem Solution. Use the trapezoid rule with n to estimate the arc-length of the curve y sin x between x and x π. Solution: The arclength is: L b a π π + ( ) dy + (cos x) + cos
More information11.10a Taylor and Maclaurin Series
11.10a 1 11.10a Taylor and Maclaurin Series Let y = f(x) be a differentiable function at x = a. In first semester calculus we saw that (1) f(x) f(a)+f (a)(x a), for all x near a The right-hand side of
More informationON A WEIGHTED INTERPOLATION OF FUNCTIONS WITH CIRCULAR MAJORANT
ON A WEIGHTED INTERPOLATION OF FUNCTIONS WITH CIRCULAR MAJORANT Received: 31 July, 2008 Accepted: 06 February, 2009 Communicated by: SIMON J SMITH Department of Mathematics and Statistics La Trobe University,
More informationSolutions to Homework 2
Solutions to Homewor Due Tuesday, July 6,. Chapter. Problem solution. If the series for ln+z and ln z both converge, +z then we can find the series for ln z by term-by-term subtraction of the two series:
More informationFourier series
11.1-11.2. Fourier series Yurii Lyubarskii, NTNU September 5, 2016 Periodic functions Function f defined on the whole real axis has period p if Properties f (t) = f (t + p) for all t R If f and g have
More informationMath 350 Fall 2011 Notes about inner product spaces. In this notes we state and prove some important properties of inner product spaces.
Math 350 Fall 2011 Notes about inner product spaces In this notes we state and prove some important properties of inner product spaces. First, recall the dot product on R n : if x, y R n, say x = (x 1,...,
More informationMath 320: Real Analysis MWF 1pm, Campion Hall 302 Homework 8 Solutions Please write neatly, and in complete sentences when possible.
Math 320: Real Analysis MWF pm, Campion Hall 302 Homework 8 Solutions Please write neatly, and in complete sentences when possible. Do the following problems from the book: 4.3.5, 4.3.7, 4.3.8, 4.3.9,
More informationTHEOREMS, ETC., FOR MATH 515
THEOREMS, ETC., FOR MATH 515 Proposition 1 (=comment on page 17). If A is an algebra, then any finite union or finite intersection of sets in A is also in A. Proposition 2 (=Proposition 1.1). For every
More informationAP Calculus Testbank (Chapter 9) (Mr. Surowski)
AP Calculus Testbank (Chapter 9) (Mr. Surowski) Part I. Multiple-Choice Questions n 1 1. The series will converge, provided that n 1+p + n + 1 (A) p > 1 (B) p > 2 (C) p >.5 (D) p 0 2. The series
More informationA glimpse of Fourier analysis
Chapter 7 A glimpse of Fourier analysis 7.1 Fourier series In the middle of the 18th century, mathematicians and physicists started to study the motion of a vibrating string (think of the strings of a
More informationMetric Spaces. Exercises Fall 2017 Lecturer: Viveka Erlandsson. Written by M.van den Berg
Metric Spaces Exercises Fall 2017 Lecturer: Viveka Erlandsson Written by M.van den Berg School of Mathematics University of Bristol BS8 1TW Bristol, UK 1 Exercises. 1. Let X be a non-empty set, and suppose
More informationReal Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi
Real Analysis Math 3AH Rudin, Chapter # Dominique Abdi.. If r is rational (r 0) and x is irrational, prove that r + x and rx are irrational. Solution. Assume the contrary, that r+x and rx are rational.
More information8.5 Taylor Polynomials and Taylor Series
8.5. TAYLOR POLYNOMIALS AND TAYLOR SERIES 50 8.5 Taylor Polynomials and Taylor Series Motivating Questions In this section, we strive to understand the ideas generated by the following important questions:
More information1.5 Approximate Identities
38 1 The Fourier Transform on L 1 (R) which are dense subspaces of L p (R). On these domains, P : D P L p (R) and M : D M L p (R). Show, however, that P and M are unbounded even when restricted to these
More information4 Divergence theorem and its consequences
Tel Aviv University, 205/6 Analysis-IV 65 4 Divergence theorem and its consequences 4a Divergence and flux................. 65 4b Piecewise smooth case............... 67 4c Divergence of gradient: Laplacian........
More informationMath 141: Lecture 11
Math 141: Lecture 11 The Fundamental Theorem of Calculus and integration methods Bob Hough October 12, 2016 Bob Hough Math 141: Lecture 11 October 12, 2016 1 / 36 First Fundamental Theorem of Calculus
More informationMATH 522 ANALYSIS II LECTURE NOTES UW MADISON - FALL 2018
MATH 522 ANALYSIS II LECTURE NOTES UW MADISON - FALL 2018 JORIS ROOS Contents 0. Review: metric spaces, uniform convergence, power series 3 0.0. Metric spaces 3 0.1. Uniform convergence 3 0.2. Power series
More informationMath 489AB A Very Brief Intro to Fourier Series Fall 2008
Math 489AB A Very Brief Intro to Fourier Series Fall 8 Contents Fourier Series. The coefficients........................................ Convergence......................................... 4.3 Convergence
More informationMATH 117 LECTURE NOTES
MATH 117 LECTURE NOTES XIN ZHOU Abstract. This is the set of lecture notes for Math 117 during Fall quarter of 2017 at UC Santa Barbara. The lectures follow closely the textbook [1]. Contents 1. The set
More informationRiemann integral and volume are generalized to unbounded functions and sets. is an admissible set, and its volume is a Riemann integral, 1l E,
Tel Aviv University, 26 Analysis-III 9 9 Improper integral 9a Introduction....................... 9 9b Positive integrands................... 9c Special functions gamma and beta......... 4 9d Change of
More information2. Function spaces and approximation
2.1 2. Function spaces and approximation 2.1. The space of test functions. Notation and prerequisites are collected in Appendix A. Let Ω be an open subset of R n. The space C0 (Ω), consisting of the C
More informationContinuous functions that are nowhere differentiable
Continuous functions that are nowhere differentiable S. Kesavan The Institute of Mathematical Sciences, CIT Campus, Taramani, Chennai - 600113. e-mail: kesh @imsc.res.in Abstract It is shown that the existence
More information2.2 The derivative as a Function
2.2 The derivative as a Function Recall: The derivative of a function f at a fixed number a: f a f a+h f(a) = lim h 0 h Definition (Derivative of f) For any number x, the derivative of f is f x f x+h f(x)
More informationFACULTY OF SCIENCE FINAL EXAMINATION MATHEMATICS MATH 355. Analysis 4. Examiner: Professor S. W. Drury Date: Tuesday, April 18, 2006 INSTRUCTIONS
FACULTY OF SCIENCE FINAL EXAMINATION MATHEMATICS MATH 355 Analysis 4 Examiner: Professor S. W. Drury Date: Tuesday, April 18, 26 Associate Examiner: Professor K. N. GowriSankaran Time: 2: pm. 5: pm. INSTRUCTIONS
More informationSuccessive Derivatives and Integer Sequences
2 3 47 6 23 Journal of Integer Sequences, Vol 4 (20, Article 73 Successive Derivatives and Integer Sequences Rafael Jaimczu División Matemática Universidad Nacional de Luján Buenos Aires Argentina jaimczu@mailunlueduar
More informationIn terms of measures: Exercise 1. Existence of a Gaussian process: Theorem 2. Remark 3.
1. GAUSSIAN PROCESSES A Gaussian process on a set T is a collection of random variables X =(X t ) t T on a common probability space such that for any n 1 and any t 1,...,t n T, the vector (X(t 1 ),...,X(t
More informationPrinciple of Mathematical Induction
Advanced Calculus I. Math 451, Fall 2016, Prof. Vershynin Principle of Mathematical Induction 1. Prove that 1 + 2 + + n = 1 n(n + 1) for all n N. 2 2. Prove that 1 2 + 2 2 + + n 2 = 1 n(n + 1)(2n + 1)
More informationWe denote the space of distributions on Ω by D ( Ω) 2.
Sep. 1 0, 008 Distributions Distributions are generalized functions. Some familiarity with the theory of distributions helps understanding of various function spaces which play important roles in the study
More informationthe convolution of f and g) given by
09:53 /5/2000 TOPIC Characteristic functions, cont d This lecture develops an inversion formula for recovering the density of a smooth random variable X from its characteristic function, and uses that
More informationMAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9
MAT 570 REAL ANALYSIS LECTURE NOTES PROFESSOR: JOHN QUIGG SEMESTER: FALL 204 Contents. Sets 2 2. Functions 5 3. Countability 7 4. Axiom of choice 8 5. Equivalence relations 9 6. Real numbers 9 7. Extended
More informationSPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT
SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT Abstract. These are the letcure notes prepared for the workshop on Functional Analysis and Operator Algebras to be held at NIT-Karnataka,
More informationAn idea how to solve some of the problems. diverges the same must hold for the original series. T 1 p T 1 p + 1 p 1 = 1. dt = lim
An idea how to solve some of the problems 5.2-2. (a) Does not converge: By multiplying across we get Hence 2k 2k 2 /2 k 2k2 k 2 /2 k 2 /2 2k 2k 2 /2 k. As the series diverges the same must hold for the
More informationLecture 4: Fourier Transforms.
1 Definition. Lecture 4: Fourier Transforms. We now come to Fourier transforms, which we give in the form of a definition. First we define the spaces L 1 () and L 2 (). Definition 1.1 The space L 1 ()
More information8.7 Taylor s Inequality Math 2300 Section 005 Calculus II. f(x) = ln(1 + x) f(0) = 0
8.7 Taylor s Inequality Math 00 Section 005 Calculus II Name: ANSWER KEY Taylor s Inequality: If f (n+) is continuous and f (n+) < M between the center a and some point x, then f(x) T n (x) M x a n+ (n
More informationChapter 11 - Sequences and Series
Calculus and Analytic Geometry II Chapter - Sequences and Series. Sequences Definition. A sequence is a list of numbers written in a definite order, We call a n the general term of the sequence. {a, a
More informationFormulas for probability theory and linear models SF2941
Formulas for probability theory and linear models SF2941 These pages + Appendix 2 of Gut) are permitted as assistance at the exam. 11 maj 2008 Selected formulae of probability Bivariate probability Transforms
More informationMATH 819 FALL We considered solutions of this equation on the domain Ū, where
MATH 89 FALL. The D linear wave equation weak solutions We have considered the initial value problem for the wave equation in one space dimension: (a) (b) (c) u tt u xx = f(x, t) u(x, ) = g(x), u t (x,
More information