Table XXXII.—Diurnal Variation of Disturbances (Sabine’s numbers).

Hour. Parc St Maur. Batavia.
D. H. V. D. H. V.
E. W. + + E. W. + +
 0-3 10.1 20.3  9.0  8.3  5.7  9.2  1.1  5.8 13.1  6.6  4.0  7.4
 3-6 12.3  8.2  8.4  8.0  6.4 10.4  7.6  7.3 14.2  4.8  6.3 10.0
 6-9 15.7  3.8 14.1 12.5  7.2  9.0 24.9 16.8 12.1  9.9 21.2 21.7
 9-noon 16.2  5.1 18.0 15.6 12.9 15.4 38.5 33.0  8.6 15.8 19.8 16.4
 noon-3 19.3  6.7 15.3 16.5 18.2 18.3 18.8 24.7 16.8 21.1 23.5 22.1
 3-6 14.8  9.7 12.5 15.4 22.9 21.8  6.4  5.4 13.3 16.9 12.6 12.7
 6-9  5.7 21.2 11.4 13.2 18.9 11.2  2.3  3.4  9.9 13.6  7.1  4.1
 9-12  5.9 25.0 11.2 10.5  7.8  4.7  0.4  3.8 12.0 11.1  5.6  5.4
Mean number
 per day
0.88 0.72 1.15 1.56 1.04 0.96 0.46 0.44 1.62 1.61 1.19 1.13
Mean size · · · · · · · · · · · · 1.72 1.69 18.0 19.5 16.7 15.5

§ 32. From the point of view of the surveyor there is a good deal to be said for Sabine’s definition of disturbance, but it is less satisfactory from other standpoints. One objection has been already indicated, viz. the arbitrariness of applying the same limiting value at a station irrespective of the size of the normal diurnal range at the time. Similarly it is arbitrary to apply the same limit between 10 a.m. and noon, when the regular diurnal variation is most rapid, as between 10 p.m. and midnight, when it is hardly appreciable. There seems a distinct difference of phase between the diurnal inequalities on different types of days at the same season; also the phase angles in the Fourier terms vary continuously throughout the year, and much more rapidly at some stations and at some seasons than at others. Thus there may be a variety of phenomena which one would hesitate to regard as disturbances which contribute to the annual and diurnal variations in Tables XXX. to XXXII.

Sabine, as we have seen, confined his attention to the departure of the hourly reading from the mean for that hour. Another and equally natural criterion is the apparent character of the magnetograph curve. At Potsdam curves are regarded as “1” quiet, “2” moderately disturbed, or “3” highly disturbed. Any hourly value to which the numeral 3 is attached is treated as disturbed, and the annual Potsdam publication contains tables giving the annual and diurnal variations in the number of such disturbed hours for D, H and V. According to this point of view, the extent to which the hourly value departs from the mean for that hour is immaterial to the results. It is the greater or less sinuosity and irregularity of the curve that counts. Tables XXXIII. and XXXIV. give an abstract of the mean Potsdam results from 1892 to 1901. The data are percentages: in Table XXXIII. of the mean monthly total, in Table XXXIV. of the total for the day. So far as the annual variation is concerned, the results in Table XXXIII. are fairly similar to those in Table XXX. for Parc St Maur. There are pronounced maxima near the equinoxes, especially the spring equinox. The diurnal variations, however, in Tables XXXII. and XXXIV. are dissimilar. Thus in the case of H the largest disturbance numbers at Parc St Maur occurred between 6 a.m. and 6 p.m., whereas in Table XXXIV. they occur between 4 p.m. and midnight. Considering the comparative proximity of Parc St Maur and Potsdam, one must conclude that the apparent differences between the results for these two stations are due almost entirely to the difference in the definition of disturbance.

Table XXXIII.—Annual Variation of Potsdam Disturbances.

Element.Jan.Feb.Mar.April.May.June.July.Aug.Sept.Oct.Nov.Dec.
D129170149 90 86576264591189482
H109133131102109829491891017584
V10617117010812156647493 877870
Mean115158150100105657376941028279

Table XXXIV.—Diurnal Variation of Potsdam Disturbances.

Hours.1-3.4-6.7-9.10-noon.1-3.4-6.7-9.10-12.
D14.911.18.05.2 5.713.122.519.5
H10.5 8.48.08.511.317.619.216.5
V13.5 9.75.74.7 8.517.221.519.2
Mean13.0 9.77.26.1 8.516.021.118.4

Table XXXV.—Disturbed Day less ordinary Day Inequality (Unit 1′, + to West).

Hour.123456789101112
a.m.−3.4−2.6−2.0−0.3+1.6+1.9+2.3+2.0+2.1+2.0+1.6+1.8
p.m.+1.8+2.2+2.1+1.7+1.40.0−1.3−2.8−3.5−2.6−3.5−2.4