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Perceptual Coherence : Hearing and Seeing

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196 <strong>Perceptual</strong> <strong>Coherence</strong><br />

Up to the late 1800s, motion was thought to be perceived by tracking<br />

one’s own eye movements. But even at that time, it was known that motion<br />

was perceived when the eye did not move. Exner (1875) provided convincing<br />

evidence that motion was a distinct perceptual quality, <strong>and</strong> not a derivative<br />

of static views spread across space <strong>and</strong> time. Exner produced two<br />

slightly displaced sparks, separated by a short time interval. The critical<br />

outcome occurred when the sparks were so close spatially that both sparks<br />

were always seen together (they could not be separated by any type of eye<br />

movement). Even in this case, there was a clear perception of a single spark<br />

moving back <strong>and</strong> forth between locations at intermediate time intervals. To<br />

demonstrate that these apparent movements were not due to small, nonperceptible<br />

eye movements, Wertheimer (1912) constructed an apparatus that<br />

created two out-of-phase motions, for example a red light moving leftright-left<br />

<strong>and</strong> simultaneously a green light moving right-left-right. Observers<br />

saw both motions, <strong>and</strong> Wertheimer argued that the eye could not<br />

move in both directions at once.<br />

One-Dot Apparent Movement<br />

The Gestalt psychologists used apparent motion to denounce what they<br />

claimed was the orthodox sensation + experience theory of perceiving. Actually,<br />

the Gestalt psychologists had constructed a straw man, as no theorist<br />

adhered to the viewpoint that perception emerged only from the compounding<br />

of sensations. The positive outcome was that extensive research<br />

was undertaken to map out the optimal space-time relationships characterizing<br />

apparent motion.<br />

In the simplest case of apparent motion, a single target at position x 1 is<br />

flashed at time t 1 , <strong>and</strong> a second target is flashed at position x 2 at time t 2 . The<br />

basic case occurs when the targets are identical in the two frames <strong>and</strong> are<br />

either brighter or darker than the background. Given the appropriate interval<br />

(t 2 − t 1 ), the target seems to move from x 1 to x 2 , regardless of whether<br />

the target is brighter or darker than the background. The outcomes are more<br />

complex if the two targets differ, <strong>and</strong> those will be discussed later.<br />

Now consider the cases in which the targets are continuously alternated.<br />

Korte (1915) summarized experiments that incorporated three factors:<br />

(1) the discriminability of two lights; (2) the distance between the lights;<br />

<strong>and</strong> (3) the time interval between the onset of each light. Korte originally<br />

used the time interval between the offset of the first light <strong>and</strong> the onset of<br />

the second, but the results are simpler to interpret if the timing between the<br />

onsets is used. (This differs from hearing, in which the offset-to-onset interval<br />

determines some types of organization, as discussed in chapter 9;<br />

Bregman, Ahad, Crum, & O’Reilly, 2000.) The important law here is that<br />

the onset-to-onset interval is directly proportional to the spatial distance. In

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