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Lf c is any real number and if f(x) = c for all x, then f ' (x) = 0 for all x That is, the derivative of a constant function is the zero function It is easy to see this geometrically Referring to Figure 1, we see that the graph of the constant function f(x) = c is a horizontal line. I c x g { f b y Ȃ ˂ Ɣz sex 1654 掿 ōĐ i c x g { f b y Ȃ ˂ Ɣz sex. F i E ւ E E ̑ ̃T r X E E ʖ E җ{ u E X N E w Z j ̃ C Y E C t B j e B 戵.

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Inverse Functions Inverse functions are functions that undo one another In other words, if f1 (x) is the inverse of f(x), then f(f1 (x)) = f1 (f(x)) = xWe can use this definition to solve. (4) P (x, y, z)dz = P (x, y, f(x, y))(fxdx fydy) C C′ This looks reasonable purely formally, since we get the right side by substituting into the left side the expressions for z and dz in terms of x and y z = f(x, y), dz = fxdx fydy To justify it more carefully, we use the parametrizations given above for C and C′ to calculate. F i E ւ E E ̑ ̃T r X E E ʖ E җ{ u E X N E w Z j ̃ C Y E C t B j e B 戵.

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}>3> æ b _ X 8 Z c>* 4Ç8® f j M Ñ x ª b)¾,ù/¤ l c/ ?. Exercise 2 Calculate the curl of the following vector fields F(x,y,z) (click on the green letters for the solutions) (a) F = xi−yj zk, (b) F = y3ixyj −zk, (c) F = xiyj zk p x2 y2 z2, (d) F = x2i2zj −yk Here is a review exercise before the final quiz Exercise 3 Let f be a scalar field and F(x,y,z) and G(x,y,z) be vector fields. 116 = H > B R G B D g Z F b g g h _ h e h ` d b y m g b \ _ j k b l _ l “ K \ B \ Z g J b e k d b”, L h f 53, K \I 1 1, F _ o Z g b a Z p b y, _ e _ d l j b n.

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Suppose there exists a surjection f∶A→ B Recall that SBS ≤SAS if and only if there exists an injection from Bto A We’ll construct one presently De ne a function g∶B→ s follows For each b∈B, we know there exists at least one a∈Asuch that f(a) =b Set g(b) equal to one such a. Operator splitting • want to solve 0 ∈ F(x) with F maximal monotone • mainidea write F as F = AB, with A and B maximal monotone • called operatorsplitting • solve using methods that require evaluation of resolvents R A = (I λA)−1, R B = (I λB)−1 (or Cayley operators C A = 2R A −I and C B = 2R B −I) • useful when R A and R B can be evaluated more easily than R. , Uf;F k ;.

The theory for L 2 functions is particularly simple on the circle If f ∈ L 2 (T), then it has a Fourier series expansion = ∑ ∈Hardy space H 2 (T) consists of the functions for which the negative coefficients vanish, a n = 0 for n < 0 These are precisely the squareintegrable functions that arise as boundary values of holomorphic functions in the open unit disk. G E T C G e B X g u g C g C g C I v o G ̕ 䗠 ł́A o ԑO ْ̋ Ă o i ɊF ܂ B ́u K ^ F Ă I v u ܂ I v Ƃ 悯 ̂ ߂̂ ܂ Ȃ B l Ɂu g C g C g C I v Ƃ C ߂Ă ̐ i J ܂ B ̓X ^ C X g ̊F ɃG 𑗂邽 ߥ B ̐ ܂őf Z ċz B ă_ W C Č N ɐ ܂ B R ̌b ݂ Ղ z @ \ i ł B. 2 mOj ;j k h d p.

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Curl The second operation on a vector field that we examine is the curl, which measures the extent of rotation of the field about a point Suppose that F represents the velocity field of a fluid Then, the curl of F at point P is a vector that measures the tendency of particles near P to rotate about the axis that points in the direction of this vector The magnitude of the curl vector at P. Autodesk Revit Autodesk Revit Grouping 21. ^ 8 I 8 013 $Î K r K S.

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