ch11 - Chapter 11. Supplemental Text Material S11-1. The...

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Chapter 11. Supplemental Text Material S11-1. The Method of Steepest Ascent The method of steepest ascent can be derived as follows. Suppose that we have fit a first- order model ± ±± yx ii i k =+ = ββ 0 1 and we wish to use this model to determine a path leading from the center of the design region x = 0 that increases the predicted response most quickly. Since the first–order model is an unbounded function, we cannot just find the values of the x ’s that maximize the predicted response. Suppose that instead we find the x ’s that maximize the predicted response at a point on a hypersphere of radius r . That is Max subject to ± ± xr i i k i i i k = = = 0 1 2 1 2 The can be formulated as Max Gx x i i k i k r L N M O Q P == ∑∑ λ 0 1 2 1 2 ± where λ is a LaGrange multiplier. Taking the derivatives of G yields =− L N M O Q P = G x xi k G i i i k ± ,, , βλ 21 2 2 1 2 " Equating these derivatives to zero results in i i i i k = = ± β 2 12 2 1 2 " k Now the first of these equations shows that the coordinates of the point on the hypersphere are proportional to the signs and magnitudes of the regression coefficients (the quantity 2 λ is a constant that just fixes the radius of the hypersphere). The second equation just states that the point satisfies the constraint. Therefore, the heuristic description of the method of steepest ascent can be justified from a more formal perspective.
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S11-2. The Canonical Form of the Second-Order Response Surface Model Equation (11-9) presents a very useful result, the canonical form of the second-order response surface model.
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ch11 - Chapter 11. Supplemental Text Material S11-1. The...

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