Goos and Jones · 2011
Optimal Design of Experiments: A Case Study Approach
- Matches
- Very close
- Close
- Differs
Factorial gives the book's answers. Where they differ, this page says why: some are misprints in the book, and for some the reason is not known yet.
Examples
Each example, and how closely Factorial gives its answers.
Pages 1 to 99
- Comparing the mean cable thickness of two machines in 12 runs: every split of the runs, equal variancesDesign · p. 4Matches
- Comparing the mean cable thickness of two machines in 12 runs: every split of the runs, machine 2 nine times as variableDesign · pp. 5, 7Matches
- Comparing the mean cable thickness of two machines in 12 runs: every split of the runs, machine 2 twice as variableDesign · p. 6Matches
- Comparing two treatments when a run of treatment 1 costs twice as much: every split of a budget of 24Design · pp. 6, 7Matches
- Extraction of an antimicrobial lipopeptide from Bacillus subtilis cultures: four solvents, pH and time in a 12-run orthogonal designExample · pp. 10-21, 31-32, 40-41Very close
- The 12-run design for the extraction experiment in coded units, made by an algorithm for D-optimal designsDesign · pp. 12-13Matches
- The bias of the methanol main effect by the ethanol-by-propanol interaction, worked as the average of x1 x2 x3Design · pp. 18-19Matches
- Four runs for the main effects of three two-level factors, and the alias matrix that confounds each with an interactionDesign · pp. 31, 33Matches
- The coordinate-exchange algorithm worked by hand: a random start of four runs for two continuous factors, turned element by element into the 2^2 factorialDesign · pp. 37-40Matches
- A 12-run D-optimal design for six two-level factors when the ethanol-by-propanol interaction is in the model from the startDesign · pp. 41-42Misprint found
- The extraction experiment augmented with eight D-optimal runs, to tell nine competing models apartExample · pp. 47-65Not yet explained
- Peel strength of a hermetic package seal: temperature, pressure and speed, made robust to three suppliers of packaging materialExample · pp. 70-82Close
- A 24-run I-optimal design for peel strength: a full quadratic in temperature, pressure and speed, with three suppliersDesign · pp. 72-78Differs
- A 24-run D-optimal design for peel strength: a full quadratic in temperature, pressure and speed, with three suppliersDesign · pp. 74-78Close
- Yield of a reaction A to B to C over a 3 x 3 factorial in time and temperature, with a full quadratic modelExample · pp. 96-99Matches
- Yield of a reaction over a hexagonal region of time and temperature: a 15-run D-optimal design for a cubic modelExample · pp. 99-112Matches
Pages 100 to 199
- Reflectivity of aluminium sheet from three rolling mills, whose reductions in thickness sum to one, with two coolant settingsExample · pp. 114-125Matches
- A 16-run half fraction of the 2^5 factorial for the rolling mill, infeasible because each run's three thickness reductions must sum to 1Design · pp. 117-118Matches
- Expansion of pastry dough: a 28-run D-optimal response surface design in seven blocks (days) of four runsExample · pp. 136-160Not yet explained
- A three-factor central composite design in three orthogonal blocks: two half fractions of the cube with two centre runs each, and the axial runs with twoDesign · pp. 137-159Matches
- A duplicated 2^3 factorial in four blocks of four runs, each replicate split by the sign of x1 x2 x3Design · pp. 138-139Matches
- Stability of riboflavin in light: a 32-run D-optimal screening design in eight blocks (days) of four for six two-level factorsExample · pp. 164-179Matches
- Dr. Xu's 2^(6-1) design in eight blocks of four, which confounds three two-factor interactions with the blocksDesign · pp. 165-166Matches
- A random 32-run design in eight blocks of four for six two-level factors, which estimates every effect but poorlyDesign · pp. 165-169Matches
- A 64-run design in 16 blocks of four: Dr. Xu's half fraction twice, blocked differently each timeDesign · pp. 171-175Matches
- The 64-run design in 16 blocks of four printed as D-optimal for the main effects and two-factor interactionsDesign · pp. 172-175Misprint found
- Surface tension of polypropylene after a gas plasma treatment: an 18-run D-optimal design with three covariates chosen from samples in stockExample · pp. 188-206Very close
- The 40 polypropylene samples in stock: their EPDM and ethylene proportions and whether they contain EVADesign · pp. 188-190Matches
- The polypropylene experiment with EPDM, ethylene and EVA treated as ordinary two-level factors: an 18-run D-optimal designDesign · pp. 196-197Not yet explained
Pages 200 to 299
- A 2^3 factorial in a run order robust to a linear time trend, for a main-effects modelDesign · pp. 212-213Matches
- A D- and Dβ-optimal run order of the 2^3 factorial for main effects and two-factor interactions with a linear time trendDesign · pp. 213-214Matches
- Drag, lift and efficiency of a race car in a wind tunnel: a 50-run I-optimal split-plot design in ten whole plots, two hard-to-change factorsExample · pp. 220-247Not yet explained
- Dr. Cavendish's first wind tunnel design: a 2^2 master design with its centre, each setting twice, crossed with the 2^2 and its centreDesign · pp. 223-224Matches
- Dr. Cavendish's second wind tunnel design: a 3^2 master design with its centre twice, ten whole plots of five runsDesign · pp. 224-231Misprint found
- A two-level split-plot design with eight whole plots of two runs: one hard-to-change factor and three easy-to-change factorsDesign · pp. 244-246Matches
- Open circuit voltage of battery cells: a 48-run D-optimal two-way split-plot design, 16 lots by six curing cycles, for six two-level factorsExample · pp. 255-267Matches
- Pino's two-way split-plot design for a battery cell: the 2^6 factorial as 16 lots by four curing cyclesDesign · pp. 256-259Matches
- A 12-run two-way split-plot design in four rows and four columns for two row factors and one column factorDesign · pp. 270-273Matches
Misprints
Misprints found in the book, by page. Each shows what the book prints and what its own data give.
T value: pHp. 19
Book −4.29Data -3.4723
The t ratio is the estimate over its standard error, -2.4758/0.7130 = -3.47, whose p value on 5 residual degrees of freedom is the 0.0178 the table prints; a t ratio of -4.29 would have a p value of 0.0078
T value: Timep. 19
Book 8.37Data 7.32
The t ratio is the estimate over its standard error, 5.2158/0.7130 = 7.32, whose p value on 5 residual degrees of freedom is the 0.0007 the table prints; a t ratio of 8.37 would have a p value of 0.0004
Vif: intercept, x2, x3 and x2 x3p. 41
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Vif: intercept, x2, x3 and x2 x3p. 41
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Vif: intercept, x2, x3 and x2 x3p. 41
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Show the rest
Vif: intercept, x2, x3 and x2 x3p. 41
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Vif: Interceptp. 42
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Vif: Ethanolp. 42
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Vif: Propanolp. 42
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Book 1.25Data 1.12
Table 2.11's runs give 12 × 3/32 = 1.125: the runs at the four combinations of x2 and x3 number 4, 4, 2 and 2, and the intercept, x2, x3 and x2 x3, orthogonal to the other four columns, each have the variance (1/16)(1/4 + 1/4 + 1/2 + 1/2) = 3/32 in units of σ². A coordinate exchange from 3,000 random starts finds no 12-run design with a larger |X'X| for this model than Table 2.11's 339,738,624, and that best design's VIFs are 1.125 too
Book >1.5Data 1.06662
The reduced model of Table 3.7, fitted to the 20 runs, has an RMSE of 1.07; the RMSE above one and a half is that of the model fitted to the 12 original runs (Table 3.6), 1.56
Xtx: the augmented design, Equation 3.5, the block's rowp. 64
The block's row of X'X is the products of the block column with each column of Equation 3.13, which that equation prints: 4 2 2 -2 2 2 0 0 2 0 2 -2 2 20; the first entry is the 12 original runs at +1 less the 8 follow-up runs at -1. The printed row and column differ from these in every entry but the diagonal, by 2
Determinant: the augmented design, Equation 3.5p. 64
Book 6.5541e17Data 6.92428e+17
|X'X| for the runs of Equation 3.13 is 6.9243e17, and Table 3.10's variances are its inverse's diagonal; the matrix printed in Equation 3.14, whose block row is wrong, has the determinant 6.5246e17, so 6.5541e17 is the determinant of neither
Determinant: I-optimal designp. 77
Book 1.5121e20Data 2.08428e+18
The designs of Tables 4.2 and 4.3, whose relative variances Table 4.4 prints, have determinants in the ratio 0.4113 under any coding of the supplier (D-optimal 5.0672e18 and I-optimal 2.0843e18 with the supplier coded +1, 0 and -1 as here; 4.1045e20 and 1.6883e20 with JMP's orthonormal coding), so the relative D-efficiency is 0.952; the printed determinants are in the ratio 0.2828
Relative d efficiency: I-optimal design versus D-optimal designp. 77
Book 0.93Data 0.95
The designs of Tables 4.2 and 4.3, whose relative variances Table 4.4 prints, have determinants in the ratio 0.4113 under any coding of the supplier (D-optimal 5.0672e18 and I-optimal 2.0843e18 with the supplier coded +1, 0 and -1 as here; 4.1045e20 and 1.6883e20 with JMP's orthonormal coding), so the relative D-efficiency is 0.952; the printed determinants are in the ratio 0.2828
Relative d efficiency: I-optimal design versus D-optimal designp. 77
Book 0.93Data 0.95
The designs of Tables 4.2 and 4.3, whose relative variances Table 4.4 prints, have determinants in the ratio 0.4113 under any coding of the supplier (D-optimal 5.0672e18 and I-optimal 2.0843e18 with the supplier coded +1, 0 and -1 as here; 4.1045e20 and 1.6883e20 with JMP's orthonormal coding), so the relative D-efficiency is 0.952; the printed determinants are in the ratio 0.2828
Determinant: D-optimal designp. 77
Book 5.3467e20Data 5.06723e+18
The designs of Tables 4.2 and 4.3, whose relative variances Table 4.4 prints, have determinants in the ratio 0.4113 under any coding of the supplier (D-optimal 5.0672e18 and I-optimal 2.0843e18 with the supplier coded +1, 0 and -1 as here; 4.1045e20 and 1.6883e20 with JMP's orthonormal coding), so the relative D-efficiency is 0.952; the printed determinants are in the ratio 0.2828
Relative d efficiency: Table 8.7 versus Table 8.6p. 172
Book 1.03Data 1.00
The design printed as Table 8.7 holds the same 64 runs as Table 8.6, in another order: its blocks 1 to 8 confound x1 x2, x3 x4 and x5 x6 and its blocks 9 to 16 x1 x6, x2 x3 and x4 x5, as Peter's construction does, so the two have the same |X'X| and a relative D-efficiency of 1
Relative d efficiency: the I-optimal design's gainp. 228
Book 12.1Data 9.4
The designs of Figure 10.2 and Table 10.2 give a relative D-efficiency of 91.4%, 9.4% more information for the I-optimal design; like Table 10.3's I-optimal column, the 89.2% belongs to an I-optimal design other than the one printed
Relative d efficiency: against the I-optimal designp. 228
Book 89.2%Data 91.378
The designs of Figure 10.2 and Table 10.2 give a relative D-efficiency of 91.4%, 9.4% more information for the I-optimal design; like Table 10.3's I-optimal column, the 89.2% belongs to an I-optimal design other than the one printed
Variance: yaw angle and grille coveragep. 229
Book 0.032Data 0.034
The I-optimal design printed in Table 10.2 gives 0.0340: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: yaw angle and grille coveragep. 229
Book 0.032Data 0.033
The I-optimal design printed in Table 10.2 gives 0.0333: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: the other interaction effectsp. 229
Book 0.046Data 0.048
The I-optimal design printed in Table 10.2 gives 0.0485: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: the other interaction effectsp. 229
Book 0.046Data 0.047
The I-optimal design printed in Table 10.2 gives 0.0466: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: the other interaction effectsp. 229
Book 0.046Data 0.049
The I-optimal design printed in Table 10.2 gives 0.0487: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: the other interaction effectsp. 229
Book 0.046Data 0.047
The I-optimal design printed in Table 10.2 gives 0.0468: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Interceptp. 230
Book 0.454Data 0.447
The I-optimal design printed in Table 10.2 gives 0.4471: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Yaw anglep. 230
Book 0.032Data 0.034
The I-optimal design printed in Table 10.2 gives 0.0340: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Grille coveragep. 230
Book 0.032Data 0.033
The I-optimal design printed in Table 10.2 gives 0.0333: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: FRH × Yaw anglep. 230
Book 0.046Data 0.048
The I-optimal design printed in Table 10.2 gives 0.0485: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: FRH × Grille coveragep. 230
Book 0.046Data 0.047
The I-optimal design printed in Table 10.2 gives 0.0466: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: RRH × Yaw anglep. 230
Book 0.046Data 0.049
The I-optimal design printed in Table 10.2 gives 0.0487: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: RRH × Grille coveragep. 230
Book 0.046Data 0.047
The I-optimal design printed in Table 10.2 gives 0.0468: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Yaw angle × Grille coveragep. 230
Book 0.042Data 0.049
The I-optimal design printed in Table 10.2 gives 0.0487: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: FRH × FRHp. 230
Book 0.523Data 0.524
The I-optimal design printed in Table 10.2 gives 0.5242: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: RRH × RRHp. 230
Book 0.523Data 0.524
The I-optimal design printed in Table 10.2 gives 0.5235: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Yaw angle × Yaw anglep. 230
Book 0.102Data 0.100
The I-optimal design printed in Table 10.2 gives 0.1001: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Variance: Grille coverage × Grille coveragep. 230
Book 0.102Data 0.105
The I-optimal design printed in Table 10.2 gives 0.1050: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Average variance: excluding the interceptp. 230
Book 0.160Data 0.161
The I-optimal design printed in Table 10.2 gives 0.1614: Table 10.3's I-optimal column, symmetric in the two ride heights and in the two easy-to-change factors, is not that of the printed design, which reproduces its own average prediction variance 0.512 (p. 231); a coordinate-exchange search finds many I-optimal split-plot designs with this master design and an average prediction variance of 0.5125 to 0.513, whose variances differ in the third decimal, and no single changed run of Table 10.2 gives the column
Df: β0, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β1, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β2, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β3, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β4, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β12, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β13, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β14, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β23, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β24, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β34, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β11, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β22, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β33, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Df: β44, ordinary least squaresp. 237
Book 45Data 35
The full quadratic model has 15 parameters, so ordinary least squares on the 50 runs leaves 35 residual degrees of freedom; the table's p values are those of 35 (the t ratio 0.93 of β12 has p 0.3592 on 35 and 0.3575 on 45)
Squares: (Yaw angle)² and (Grille coverage)²p. 247
The first run of whole plot 6 has yaw angle 1, whose square is 1; the table prints 0
Not yet
Answers the book prints that Factorial cannot compute yet, by what it lacks.
- The library's power leaves out the intercept; its relative variance, 0.058, is the block's, whose power of 0.930 is checkedp. 55
- An average over the simplex of the mills' pseudocomponents and the two levels of each process variable, which the library's regions (a mixture or a box) do not hold together; sampled with 400,000 points it is 0.483, and 0.372 with the process variables continuous between -1 and +1p. 120
- A property of the design among all designs of its size, which the library's optimal design search does not cover for two crossed random effectsp. 271
- A property found by searching for each ratiop. 273