Sixteen Experimental Investigations from the Harvard Psychological Laboratory by Hugo Münsterberg (100 books to read .txt) 📕
[5] Dodge, Raymond, PSYCHOLOGICAL REVIEW, 1900, VII., p. 456.
[6] Graefe, A., Archiv f. Ophthalmologie, 1895, XLI., 3, S. 136.
This explanation of Graefe is not to be admitted, however, since in the case of eye-movement there are muscular sensations of one's own activity, which are not present when one merely sits in a coach. These sensations of eye-movement are in all cases so intimately connected with our perception of the movement of objects, that they may not be in this case simpl
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Total judgments, 113; Errors (B = 31), A = 57.
The relatively meager results set forth in the preceding section are
corroborated in the present set of experiments. That such a variation
of intensity introduced into an otherwise undifferentiated auditory
series, while it affects the time-values of both preceding and
following intervals, has a much greater influence on the latter than
on the former, is as apparent here as in the previous test. The number
of errors, irrespective of extent, for the two intervals are: B, 82.3
per cent, of total judgments; A, 90.7 per cent. When the mean and
extreme sign displacements are estimated on the quantitative basis
given above these percentages become B, 64.5; A, 90.7, respectively—a
ratio of 0.711:1.000.
The direction of error, likewise, is the same as in the preceding
section. Since the actual values of the two intervals here are
throughout of extreme sign—one always greater, the other always
less—only errors which lie in a single direction are discriminable.
Illusions lying in this direction will be clearly exhibited, since the
differences of interval introduced are in every case above the
threshold of discrimination when the disturbing element of variations
in intensity has been removed and the series of sounds made
intensively uniform. In case of a tendency to underestimate B or
overestimate A, errors would not be shown. This problem, however, is
not to be met here, as the results show; for there is recorded a
proportion of 82.3 per cent. of errors in judgment of interval B, and
of 90.7 per cent. in judgment of interval A, all the former being
errors of overestimation, all of the latter of underestimation.
The influence of position in the series on the effect exerted by such
a change of intensity in a single member can be stated only
tentatively. The number of experiments with the louder sound in
position five was smaller than in the other cases, and the relation
which there appears cannot be absolutely maintained. It may be also
that the number of intervals following that concerning which judgment
is to be given, and with which that interval may be compared, has an
influence on the accuracy of the judgment made. If we abstract from
this last set of results, the tendency which appears is toward an
increase in accuracy of perception of comparative durations from the
beginning to the end of the series, a tendency which appears more
markedly in the relations of the interval preceding the louder sound
than in those of the interval which follows it. This conclusion is
based on the succession of values which the proportion of errors to
total judgments presents, as in the annexed table.
TABLE XXX.
Percentage of Errors for Each Position.
Interval. I II III IV V
B. 83.3 76.9 69.2 (100) Irrespective
A. 85.7 91.6 91.6 84.6 (100) of extent.
B. 73.3 71.9 53.8 (60) Estimated
A. 85.7 91.6 91.6 84.6 (100) quantitatively.
Next, the relation of the amount of increase in intensity introduced
at a single position in such a series to the amount of error thereby
occasioned in the apprehension of the adjacent intervals was taken up.
Two sets of experiments were carried out, in each of which five of
the sounds were of equal intensity, while one, occurring in the midst
of the series, was louder; but in one of the sets this louder sound
was occasioned by a fall of the hammer through a distance of 0.875
inch, while in the other the distance traversed was 2.00 inches. In
both cases the extent of fall in the remaining hammers was uniformly
0.25 inch. The results are given in the following table:
TABLE XXXI.
Interval B.¹ Interval A.
Ratio of Interval 0.875 in. 2.00 in. 0.875 in. 2.00 in.
B to Interval A. + = - + = - + = - + = -
1.000 : 1.000 0 6 0 0 4 2 0 5 1 0 0 6
0.909 : 1.000 2 4 0 0 4 2 0 2 4 2 2 2
0.833 : 1.000 0 6 0 0 4 2 4 0 2 1 3 2
0.770 : 1.000 0 6 0 2 2 2 2 4 0 4 0 2
0.714 : 1.000 0 6 0 1 5 0 6 0 0 2 2 2
Totals, 2 28 3 19 8 12 11 7 9 7 14
T.E., T.J., 2 30 11 30 13 30 21 30
and per cent., 6.6% 36.6% 60.0% 70.0%
¹Interval B in these experiments is of the same duration as all
others but that following the louder sound; hence, judgments in
the second column are correct.
Again the markedly greater influence of increased intensity on the
interval following than on that preceding it appears, the percentage
of errors being, for B (both intensities), 21.6 per cent.; for A, 56.6
per cent. Also, in these latter experiments the direction of error is
more definite in the case of interval A than in that of interval B.
The influence of changes in intensity on the amount of error produced
is striking. Two intensities only were used for comparison, but the
results of subsequent work in various other aspects of the general
investigation show that this correlation holds for all ranges of
intensities tested, and that the amount of underestimation of the
interval following a louder sound introduced into an otherwise uniform
series is a function of the excess of the former over the latter. The
law holds, but not with equal rigor, of the interval preceding the
louder sound. So far as these records go, the influence of such an
increase of intensity is more marked in the case of interval B than in
that of interval A. It is to be noted, however, that the absolute
percentage of errors in the case of A is several times greater than in
that of B. I conclude that A is much more sensitive than B to such
influences, and that there is here presented, in passing from
intensity I. to intensity II., the rise of conditions under which the
influence of the louder sound on B is first distinctly felt—that is,
the appearance of a threshold—and that the rate of change manifested
might not hold for higher intensities.
Lastly, the rate at which the sounds of the series succeeded one
another was varied, in order to determine the relation which the
amount of influence exerted bore to the absolute value of the
intervals which it affected. Three rates were adopted, the whole
series of sounds occupying respectively 2.50 secs., 2.20 secs, and
1.80 secs. The results are summed in the following table:
TABLE XXXII.
Rate: 2.5 secs. Rate: 2.2 secs. Rate: 1.8 secs.
Ratio of Interval B B A B A B A
to Interval A. + = - + = - + = - + = - + = - + = -
1.000 : 1.000 2 8 0 0 8 2 0 8 2 0 2 8 0 4 0 0 2 2
0.917 : 1.000 0 8 2 4 6 0 3 8 0 0 8 3 2 2 0 0 2 2
0.846 : 1.000 1 9 0 5 4 1 3 8 0 3 7 1 6 5 0 1 8 2
0.786 : 1.000 1 10 0 11 0 0 6 6 0 7 3 4 6 2 2 2 6 2
0.733 : 1.000 4 2 0 4 0 2 4 6 0 8 0 2
0.687 : 1.000 5 3 1 6 1 2 2 6 0 7 0 1
Totals 4 35 2 20 18 3 21 35 3 20 21 20 20 25 2 18 18 11*
*Transcriber’s Note: Original “1”.
These results are converted into percentages of the total number of
judgments in the following table:
TABLE XXXIII.
Rate of B A
Success. + = - Errors. + = - Errors.
2.5 secs 10 85 5 15 49 44 7 51
2.2 ” 36 59 5 41 33 34 33 67
1.8 ” 43 53 4 47 38 38 24 62
In the case of interval A the direction of the curve of error changes
in passing from Rate II. to Rate III. In the case of interval B the
increase is continuous.
This increase in the percentage of error is, further, distinctly in
the direction of an accentuation of the overestimation of the
interval B, as is shown in the percentage of cases in which this
interval appeared greater than the rest of the series for each of the
three rates.
If the three rates be combined in the one set of results, the
difference in the effects produced on the interval following the
louder sound and on that which precedes it becomes again apparent.
This is done in the table below.
TABLE XXXIV.
B A B A
Ratio + = - + = - T.E. T.J. % T.E. T.J. %
I. 2 20 2 0 12 12 2 24 8.5 12 24 50.0
II. 5 18 2 4 16 5 5 25 20.0 21 25 84.4
III. 10 22 0 9 19 4 10 32 31.0 23 32 72.0
IV. 13 18 2 20 9 8 13 33 39.0 17 37 46.0
V. 8 8 0 12 0 4 8 16 50.0 4 16 25.0
VI. 7 9 1 13 1 3 7 17 41.0 4 17 24.0
The overestimation of the interval before the louder sound also tends
to increase in extent with the actual increase in duration of the
interval following that sound over the other intervals of the series.
Thus, the form which the sensible time-relations of such a limited
series of sounds present is found to be intimately dependent on the
intensive preponderance of certain elements within it, on the degree
of increased stress which such elements receive, on their local
position in the series, and on the rate at which the stimulations
succeed one another. The knowledge of these facts prepares us for the
whole series of relations manifested in the special quantitative
investigations reported in the sections which follow. In the first of
these is presented the time-relations obtaining among the successive
reactions of the various rhythm types discussed in the preceding
division of this part, the section, namely, on the distribution of
intensities.
In the first group of reactions the series was not to be consciously
accented, nor to be divided into groups by the introduction of pauses.
The reactor was required only to conceive it as a succession of
two-beat groups continuously repeated, the way in which the groups
should be defined, whether by counting or otherwise, being left to his
own discretion. The experimental group was composed of five subjects.
The following table presents the quantitative results of an analysis
of the material in series of ten successive pairs of reactions, upon
the basis of unity as the value of the first element.
TABLE XXXV.
Quantities. I II III IV V VI VII VIII IX X
Whole Meas., 1.000 0.894 1.035 0.912 1.000 0.877 1.070 0.877 1.070 0.841
First Inter., 1.000 1.142 1.071 1.142 1.000 1.285 1.000 1.214 1.000 1.214
Second Inter., 1.000 0.837 1.023 0.860 1.000 0.744 1.093 0.767 1.093 0.790
Within the limits of the calculation no progressive change appears,
either of acceleration or of retardation, whether in general or on the
part of individual reactors. In narrower ranges the inconstancy of the
periods is very marked, and their variations of clearly defined
rhythmical character. The duration of the total measures of two beats
is throughout alternately longer and shorter, the average of their
values presenting a ratio of 1.000:0.847. The order of this
arrangement, namely, that the longer period precedes the shorter in
the larger group, is drawn from the
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