The following tables are specimen sets made by the subjects C, O, and D.
I. (a) F. 80x10, V. 160x10.
F. V. C. O. D.
40 62, 120 166, 130 28, 24 80 70, 110 104, 102 80, 126 120 46, X 70, 46 68,—44, 128* 160 26, 96 50, 25 85, 196,—88* 200 20, X 55, X —46, 230,* 220,—110*
I. (b) F. 160x10, V. 80x10.
F. V. C. O. D.
40 74, 64 60, 96 27, 34 80 76, 65 72, 87 55, 138 120 60, 56 48, 82 70, 174 160 29, 74 16, 77 —114, 140, 138, 200 200 96, 36 25, 36 177,—146,—148, 230
Now, on Dr. Pierce’s theory, the variable in the first set should be nearer the center, since it is twice the size of the fixed line;—but the choices V. 120, 166, 130 for F. 40; V. 110, 104, 102, 126 for F. 80; V. 128 for F. 120; V. 196 for F. 160; V. 230, 220 for F. 200, show that other forces are at work. If these variations from the expected were slight, or if the presence of second choices did not show a certain opposition or contrast between the two positions, they might disappear in an average. But the position of F. 40, over against V. 120, 166, 130, is evidently not a chance variation. Still more striking are the variations for I. (b). Here we should expect the variable, being smaller, to be farther from the center. But for F. 40, we have V. 27, 34; for F. 80, all nearer but two; for F. 120, V. 60, 56, 48, 82, 70; for F. 160, V. 29, 74, 16, 77, 138, and for F. 200, V. 96, 36, 25, 36, 177—while several positions on the same side of the center as the constant show a point of view quite irreconcilable with mechanical balance.