“…The amount of excitation produced by a probe in a neighboring detector should be inversely related to the distance between the probe and the detector. There are reasons to suppose that the function relating measured discrimination time to distance between the objects to be discriminated (e.g., Henmon, 1906;Moyer & Landauer, 1967) or between a test object and the discrimination boundary (e.g., DeRosa & Morin, 1970;Fish, 1981;Levy et al, 1980) becomes asymptotically flat for large distances and, indeed, may approximate a reciprocal (hyperbolic) function (e.g., Curtis, Paulos, & Rule, 1973;Shepard et al, 1975;Shepard, Note 1). However, as a simpler first approximation, we suppose here that at least over a suitably limited range, the theoretically postulated excitation in detector i can be taken as falling off roughly linearly with its Euclidean distance, 'd\., from the probed square: e\ = bad.…”