Table 15 family of fractional factorials
Fraction
Generators
When combined with principal
fraction gives:
Principal
I = 124 I = 135 I = 236 I = 1237
. . .
A1 I = -124 I = -135 I = -236 I = -1237
All main effects
A2
I = -124 I = - 135 I = 236 I = -1237
1, 12, 13, 14, 15, 16, 17
A3
I = -124 I = 135 I = -236 I = -1237
2, 12, 23, 24, 25, 26, 27
A4
I = 124 I = -135 I = -236 I = -1237
3, 13, 23, 34, 35, 36, 37
A5
I = -124 I = 135 I = 236 I = 1237
4, 14, 24, 34, 45, 46, 47
A6
I = 124 I = -135 I = 236 I = 1237
5, 15, 25, 35, 45, 56, 57
A7
I = 124 I = 135 I = -236 I = 1237
6, 16, 26, 36, 46, 56, 67
A8
I = 124 I = 135 I = 236 I = -1237 7, 17, 27, 37, 47, 57, 67
Orthogonal Arrays
The theory of fractional factorial designs was first worked out by Finney (Ref 26) and Rao (Ref 27). Many highly
fractionated designs were introduced by Tippett (Ref 28), Plackett and Burman (Ref 29), and others. Some of these were
referred to as magic squares and orthogonal arrays. Two-level and three-level fractional factorial designs gained
widespread attention and industrial application, beginning in the 1950s. Box and Hunter (Ref 7) provided much useful
guidance to the practitioner in the adroit use of these experimental design structures.
In the late 1970s, the use of orthogonal arrays for quality design and improvement by Taguchi (Ref 4) and others gained
widespread acceptance in industry. This has led to considerable discussion concerning the relative merits of these designs
and the methods of design selection vis-à-vis the methodology of the more general class of fractional factorial designs. In
particular, it is important to examine the philosophical framework and interpretation of these similar (often identical)
design structures.
Issue of Confounding. To many, the most significant property of the designs is orthogonality, that is, the ability to
separate out the individual effects of several variables on a response of interest. The term orthogonal arrays as used by
Taguchi implies having this property of orthogonality or producing effects that are not confounded. In fact, whenever
anything less than a full factorial is under consideration, confounding or mixing of effects is present by definition. Such
confounding can only be removed by assumptions made about the physical system and confirmed through some analyses
of the results.
Similarly, when two-level factorials are fractionated, the ability to determine all the interactions among a set of factors is
lost. However, judicious fractionation leads to the ability to obtain knowledge on low-order interactions under the
assumption that higher-order interactions are of negligible importance. Because the orthogonal arrays, as applied to
Taguchi methods, are highly fractionated factorial designs, the information these arrays produce is a function of two
elements: the nature of their confounding patterns and the assumptions made about the physical system they are applied