Sixteen Experimental Investigations from the Harvard Psychological Laboratory, Hugo Münsterberg [top fiction books of all time TXT] 📗
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When the pendulum is not swinging, a hole in the shield lies behind
ON and exactly corresponds with it. Another in the background does
the same. The eye can thus see straight through to the light L.
Each of these three holes has grooves to take an opaque card, x,
y, or z; there are two cards for the three grooves, and they are
pierced with holes to correspond to i and tt of Fig. 4. The
background BB has a second groove to take a piece of milk-glass M.
These cards are shown in Fig. 6 (Plate II.) Card I bears a hole 5
cm. high and shaped like a dumb-bell. The diameter of the end-circles
(e, e) is 1.3 cm., and the width of the handle h is 0.2 cm. Card
T is pierced by two slits EE, EE, each 9 cm. long and 1.3 cm.
high, which correspond to the two ends of the dumb-bell. These slits
are connected by a perforation H, 1.5 cm. wide, which corresponds to
the handle of the dumb-bell. This opening EEHEE is covered by a
piece of ground-glass which serves as a radiating surface for the
light.
[Illustration: Fig. 5.]
The distance EA (Fig. 5) is 56 cm., and PP‘ is 40 cm.; so that the
arc of eye-movement, that is, the angle PEP‘, is very nearly 40°,
of which the 9-cm. opening ON 9° 11’. SS is 2 cm. behind ON, and
BB 2 cm. behind SS; these distances being left to allow the
pendulum to swing freely.
It is found under these conditions that the natural speed made by the
eye in passing the 9-cm. opening ON is very well approximated by the
pendulum if the latter is allowed to fall through 23.5° of its arc,
the complete swing being therefore 47°. The middle point of the
pendulum is then found to move from O to N in 110[sigma][19]. If
the eye sweeps from O to N in the same time, it will be moving at
an angular velocity of 1° in 11.98[sigma] (since the 9 cm. are 9° 11’
of eye-movement). This rate is much less than that found by Dodge and
Cline (op. cit., p. 155), who give the time for an eye-movement of
40° as 99.9[sigma], which is an average of only 2.49[sigma] to the
degree. Voluntary eye-movements, like other voluntary movements, can
of course be slow or fast according to conditions. After the pendulum
has been swinging for some time, so that its amplitude of movement has
fallen below the initial 47° and therewith its speed past the middle
point has been diminished, the eye in its movements back and forth
between the fixation-points can still catch the after-image of i
perfectly distinct and not at all horizontally elongated, as it would
have to be if eye and pendulum had not moved just together. It appears
from this that certain motives are able to retard the rate of
voluntary movements of the eye, even when the distance traversed is
constant.
[19] The speed of the pendulum is measured by attaching a
tuning-fork of known vibration-rate to the pendulum, and
letting it write on smoked paper as the pendulum swings past
the 9-cm. opening.
The experiment is now as follows. The room is darkened. Card T is
dropped into groove z, while I is put in groove y and swings
with the pendulum. One eye alone is used.
Case 1. The eye is fixed in the direction EA. The pendulum is
allowed to swing through its 47°. The resulting visual image is shown
in Fig. 7:1. Its shape is of course like T, Fig. 6, but the part H
is less bright than the rest because it is exposed a shorter time,
owing to the narrowness of the handle of the dumb-bell, which swings
by and mediates the exposure. Sheets of milk-glass are now dropped
into the back groove of BB, until the light is so tempered that
part H (Fig. 7:1) is barely but unmistakably visible as luminous.
The intensity actually used by the writer, relative to that of EE,
is fairly shown in the figure. (See Plate III.)
It is clear, if the eye were now to move with the pendulum, that the
same amount of light would reach the retina, but that it would be
concentrated on a horizontally narrower area. And if the eye moves
exactly with the pendulum, the visual image will be no longer like 1
but like 2 (Fig. 7). We do not as yet know how the intensities of e,
e and h will relatively appear. To ascertain this we must put card
I into groove x, and let card T swing with the pendulum in
groove y. If the eye is again fixed in the direction EA (Fig. 5),
the retina receives exactly the same stimulation that it would have
received before the cards were shifted if it had moved exactly at the
rate of the pendulum. In the experiments described, the handle h of
this image (Fig. 7:2) curiously enough appears of the same brightness
as the two ends e, e, although, as we know, it is stimulated for a
briefer interval. Nor can any difference between e, e and h be
detected in the time of disappearance of their after-images. These
conditions are therefore generous. The danger is that h of the
figure, the only part of the stimulation which could possibly quite
elapse during the movement, is still too bright to do so.
Case 2. The cards are replaced in their first positions, T in groove
z, I in groove y which swings. The subject is now asked to make
voluntary eye-sweeps from P to P’ and back, timing his moment of
starting so as to bring his axis of vision on to the near side of
opening ON at approximately the same time as the pendulum brings I
on the same point. This is a delicate matter and requires practice.
Even then it would be impossible, if the subject were not allowed to
get the rhythm of the pendulum before passing judgment on the
after-images. The pendulum used gives a slight click at each end of
its swing, and from the rhythm of this the subject is soon able to
time the innervation of his eye so that the exposure coincides with
the middle of the eye-movement.
[Illustration: PSYCHOLOGICAL REVIEW. MONOGRAPH SUPPLEMENT, 17. PLATE III.
Fig. 7.
HOLT ON EYE-MOVEMENT.]
It is true that with every swing the pendulum moves more slowly past
ON, and the period of exposure is lengthened. This, however, only
tends to make the retinal image brighter, so that its disappearance
during an anæsthesia would be so much the less likely. The pendulum
may therefore be allowed to ‘run down’ until its swing is too slow for
the eye to move with it, that is, too slow for a distinct,
non-elongated image of i to be caught in transit on the retina.
With these eye-movements, the possible appearances are of two classes,
according to the localization of the after-image. The image is
localized either at A (Fig. 5), or at the final fixation-point (P
or P’, according to the direction of the movement). Localized at
A, the image may be seen in either of two shapes. First, it may be
identical with 1, Fig. 7. It is seen somewhat peripherally, judgment
of indirect vision, and is correctly localized at A. When the
subject’s eye is watched, it is found that in this case it moved
either too soon or too late, so that when the exposure was made, the
eye was resting quietly on one of the fixation-points and so naturally
received the same image as in case 1, except that now it lies in
indirect vision, the eye being directed not toward A (as in case 1)
but towards either P or P’.
Second, the image correctly localized may be like 2 (Fig. 7), and then
it is seen to move past the opening ON. The handle h looks as
bright as e, e. This appearance once obtained generally recurs
with each successive swing of the pendulum, and scrutiny of the
subject’s eye shows it to be moving, not by separate voluntary
innervations from P to P’ and then from P’ to P, but
continuously back and forth with the swing of the pendulum, much as
the eye of a child passively follows a moving candle. This movement is
purely reflex,[20] governed probably by cerebellar centers. It seems
to consist in a rapid succession of small reflex innervations, and is
very different from the type of movement in which one definite
innervation carries the eye through its 42°, and which yielded the
phenomena with the perimeter. A subject under the spell of this reflex
must be exercised in innervating his eye to move from P to P’ and
back in single, rapid leaps. For this, the pendulum is to be
motionless and the eye is not to be stimulated during its movement.
[20] Exner, Sigmund, _Zeitschrift f. Psychologie u. Physiologie
der Sinnesorgane_, 1896, XII., S. 318. ‘Entwurf zu einer
physiologischen Erklärung der psychischen Erscheinungen,’
Leipzig u. Wien, 1894, S. 128. Mach, Ernst, ‘Beiträge zur
Analyse der Empfindungen,’ Jena, 1900, S. 98.
These two cases in which the image is localized midway between P and
P’ interest us no further. Localized on the final fixation-point,
the image is always felt to flash out suddenly in situ, just as in
the case of the ‘correctly localized’ after-image streaks in the
experiments with the perimeter. The image appears in one of four
shapes, Fig. 7: 2 or 3, 4 or 5.
First, the plain or elongated outline of the dumb-bell appears with
its handle on the final fixation-point (2 or 3). The image is plain
and undistorted if the eye moves at just the rate of the pendulum,
elongated if the eye moves more rapidly or more slowly. The point that
concerns us is that the image appears with its handle. Two
precautions must here be observed.
The eye does not perhaps move through its whole 42°, but stops instead
just when the exposure is complete, that is, stops on either O or
N and considerably short of P or P’. It then follows that the
exposure is given at the very last part of the movement, so that the
after-image of even the handle h has not had time to subside. The
experiment is planned so that the after-image of h shall totally
elapse during that part of the movement which occurs after the
exposure, that is, while the eye is completing its sweep of 42°, from
O to P, or else from N to P’. If the arc is curtailed at point
O or N, the handle of the dumb-bell will of course appear. The
fact can always be ascertained by asking the subject to notice very
carefully where the image is localized. If the eye does in fact stop
short at O or N, the image will be there localized, although the
subject may have thoughtlessly said before that it was at P or P’,
the points he had nominally
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