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The diurnal variation of sizes of sudden commencements and impulses in the Kodaikanal magneto grams

B. SRINIVASAMURTHY Kodaikanal Observatory, Kodaikanal

(Received 17 February 1959)

ABSTRACT. Combined data of sudden commencements (SCs) and sudden impulses (SIs) recorded at Kodai·

kanal (geomagnetic latitude 6QN) during the period 1949-57 have been analysed in order to study the relationship between the diurnal variation (DV) in the amplitudes of the impulses and the DVin the horizontal component of the earth's magnetic field (the Sq variations in H)_ There is a statistically significant daytime enhancement in

se

sizes similar to the enhancement in Sq variation. Furthermore, this enhancement is larger on days with larger Sf] varia.

tion than on days with smaller Sq variation. These results confirm those obtained by Forbush and Vestine (1955) at Huancayo, another station near t,he geomagnetic equator.

1. Introduction

The diurnal variation of the amplitudes of SOs in relation to the variations in magnetic elements has been studied by several workers.

Ferraro and Unthank (1951) found a simi- larity between the DV of SO sizes in H and the DV of Sq in H at Huancayo. Ferraro (1954), however, found that apart from Huancayo other stations, e.g., Cheltenham, Tucson, San Juan, Honolulu and Watheroo, do not appear to show a daytime augmentation of mean hourly values of

se

impluses. Suguira (1953), comparing the SO sizes at Huancayo and Cheltenham-stations on the same meridian but at different latitudes-found that there is a considerable enhancement in the size of daytime SOs near the geomagnetic equator. He also observed that the ratio of SO sizes at the two stations, increases in the morning, reaches a maximum around 11 hours local time, decreases towards the evening and remains constant throughout the night. This daytime augmentation in SO sizes at Huancayo was later examined in detail and found statistically significant by For- bush and Vestine (1955). A similar analysis was suggested by them for Kodaikanal, as one of particular interest, Kodaikanal being the only other established station near the geomagnetic equator. Sivaramakrisbnan

lVI/J94CP

(1956), concluded frO!Il the data of SOs at Kodaikanal, Alibag and Huancayo for the period 1949-53, that the SO amplitude is largest at local noon and this noon increase in amplitude is maximum at stations near the geomagnetic equator. In the present investi- gation it is proposed to examine statistically the data for 1949-57 available at Kodaikanal in order to verify the significance of the above conclusions. In an earlier paper the author (Srinivasamurthy 1959) had studied the DV in the hourly frequencies of ses and SIs at Kodaikanal.

2. Analysis

The method adopted in the analysis is very similar to that of Forbush and Vestine.

398 SOs and SIs which have been selected after comparison with the reports of other stations (published by the rAGA) have been included in this analysis. The distinction between SOs and SIs has not been retained.

The size of impulse in H, which is generally a rise, and the departure /:,.H of the average value of H for the hour preceding the hour of SO from the previous midnight value were measured from the magnetograms. The smoothed hourly mean values of /:,.H and also of the. size of impulses were determined and plotted in Fig.1 (a). The resemblance

(2)

65 B. SRINIV ASAMURTHY

(

80

~o

-40 _

20

y

40

f

I I I

'i

I I

x X

\

\

l,

\

\

\

\

I"

I

1949101951 x-x ME AN t:,H 0-0 ME-AN SC SIZE

\ X

\

\ \

\

10 IS ZO 24

HOUR 5 (t. oro/ rlm~ )

Fig.i(a)

I x I I

~ ... "t ' \ .

I ~

\

\

Fig. i(e)

\

" \

195210 I~S4 , - , MEAN ;::P

<>--0 MEAN S( SIZE

between the diurnal curves of mean t:,.H and mean size y of the impulses can be clearly seen. Fig. 2 (a) gives the graph of hourly meant:,.H values versus the hourly mean

se

sizes. In spite of a slight scatter of points for the higher values, a linear relationship y

=

12·3~+ 0·21 /::;.H (1) is suggested. A comparison of equation (1) with that obtained by Forbush and Vestine

so

4()

20

O'I,l(,

I ~

,

I

,

~

I I

\ '\

\949!~ 195t x-x MEAN AH CHI MEAN SC SIZE

\~

\

, ,

\

\ .,.

5 10 15 20 24

y

80

60

"

, ,,'-

o :.x-X_)(-)('" )

o 5

HOORS (LOcal rhtu)

Fig.i(b)

I I

,

I

"

I I

,

"

,

I

x ,

\

,

,

..

I

~

\

\ I . \

1955 to 1957

~_x MEAN 5:H

0-0 ME AN SC SIZE:

x

\

,

\ ~

" '~

!;.o::_x_x_x)

10 20

HOURS ( LOcal Thne)

Fig.i(d)

shows that both the night mean size 'a' and the rate of enhancement 'b' with /::,.H are smaller at Kodaikanal than atHuancayo.

From a comparison of the amplitudes of about 70 storm sudden commencements (January 1950-June 1955) at Huancayo . as reported in the .J ournal of Geophysioal Researoh and the corresponding values at Kodaikanal, it is found that the amplitudes are generally higher at Huancayo, where the

(3)

40

50

'"

'" 10

N V)

JO

"

V)

0

\... 20

a

o

1949 to 195-' y = 12'3 +O·.216H

10 20 30 AO 50 60 70 80 90 MeAN t::.HY

JO

Fig.2(a)

1952 to 1954 :>z= 10'1 +0'14 IlH

20 :50 40 so 60

MCAN 6HY Fig. 2(0)

70

\..

50 ,

'" 20

N

~ 10 ~-: 1949 tot9:51

'"". )'t= f3-1 +0·18 l:!.H

... '"

' - - - l

40

!.. 30

'"

~ 20

V)

~ N ~ ~ ~ ~ 00 m

IM~AN MY

Fig.2\b)

o . ..LI_.L...-.-..L...:L-..J

o m ro m w ~ m M 00 ~ ~ MEAN MY

Fig. 2 (d)

,Sq in H is also larger. The local time varia- Yh.

=

13·1

+

0·18 /'::,H

tions of mean values of amplitudes at Huan- (2)

(3) (4) cayo and Kodaikanal are given in Fig. 3. Y2

=

10·1

+

0·14 /'::,H

:3. Dependence of the factors 'a' and 'b' on relative and ,lIa

=

13·9

+

O' 24 £:,.H

sunspot numbers 1

The period under investigation covering almost a solar cyole has been divided into three-year periods 1949-51,1952-54 and 1955- 57, corresponding roughly to the post maxi- mum, minimum and pre-maximUlll periods of the cycle. Hourly smoothed means of £:,.H and the sizes of impulses have been determined for each period. The DV in mean /'::,H has been fitted to the DV in Sq by taking the averages of hourly means of £:,.H and the corresponding hourly means of Sq variation.

(The hourly means of Sq variation were

obt~ined for each three-year period by takIng all days other.than those exceptionally disturbed). £:,.H, thus derived, gives a fair representation of Sq variation in H on· the days (and hours) on which the impulses occurred. Figs. 1 (b), 1 (c) and 1 (d) give the DVin the tiH values and the DV in the mean

se

sizes. From Figs. 2(b), 2(c) and 2(d) the following linear relationships can be obtained

The linear equations (1) to (4) have been derived by the method of least squares.

The equations (2), (3) and (4) correspond to the three-year periods with average relative sunspot numbers 96'0, 16·6 and 190·0 res- pectively. A slight increase in the factors 'a' il.nd 'b' with increase in sunspot numbers is seen from the above equations. The night-time mean size of SOs and the rate of enhancement with£:,.H are least near the period of minimUlll sunspot number, when incidentally, the num- ber of impulses is also small.

4. SC sizes during day and night

The frequency distributions of SO sizes during A: day (0600-1800 LMT) and B: night (1800-0600 LMT) are represented in the histograms of FigA (a). The percentage of SOs and SIs with amplitudes greater than 20,,/ is 48 in group A, whereas it is only 25 in group B; unusually Jarge SOs are noticed

(4)

67 B. SRINIVASAMURTHY

tOO

eo

:< 40

0 1 I I O x : ... JC

20 __ x __ _

1950ro 195'>

o C-O HUANCAYO

x-x KOOAU<ANAl.

o 0

o

o o

o ... x ... --lil

"

°Ok---~S----~,O·----~\~---ILO--~~

HOURS (Locol Mean rime)

Fig. 3

only in group A. The standard deviations of sizes in A and Bare 21"1 a,;nd 12"1 and the means 261' and 17'Y respectively. It is found that the difference in means is about five times as large as the standard deviation 1· 7 "1 of the difference between the two means.

The difference is thus significant; the, mean size of impulses during the sunlit llOurs is greater than that during night.

5. se sizes on days with large and small DV in H

If the DV in SO sizes actually corresponds to DV in H, the day-time enhancement in SO sizes should be more on days with larger variation in H. The SOs and SIs recorded during each hour t in the interval 0800-1600 LMT were classified into groups I and II ac- cording to whether the corresponding 6.Ht values were greater or less than the median6.H for that hour. The frequency distributions of sizes are given in Fig. 4(b). The percentage of SOs with sizes greater than 30"1 is 43 for group I and only 20 in group II. The samples standard deviations are 2· 6)' and 1· 7"1 and the means 29· 8", and 23· I'}' respectively. The difference in the means is nearly 20 times greater than the standard deviation 0·331' 0f the difference and hence is significant.

50

40

~ 30

"

""

<!

'"

v 20

Q:

'"

C\.

10

o

50

40

~ 30

"

i--

::: ~ 20 Q:

'"

Cl 10

o

,.."

r I 1

A B

o 50 100 o so

SIZE: Y

Fig. 4(a). Frequency distribution of se sizes A-For day (0600-1800 LMT) B-For night (1800-0600 LMT)

1 1I

o 50 100 0 so

'S/Z£)I"

Fig.4(b). Frequency distribution of se sizes I-·-For days with !::,.Ht >rnedian II-For daYt:\ with !::,.Ht <median

6. Conclusion

100

The correlation between day-time SO am- plitudes and the range of DV in H at Kodai·

kanal is established beyond doubt. The enhan- cement in size is, however, small com- pared to, that at Huancayo. The close connection between the day-time enchance- ment in SO sizes and the' enhancement in the 8q variation in H suggests that. the seat

(5)

of these two phenomena may be one and the same. As suggested by Forbush and Vestine the currents associated with them may flow in or near the E-region of the ionosphere and enhancement in both cases may be due to tho locally enhanced conductivity of the E-region near the geomagnetie equator.

The possible relationships of these currents tD wind motions have been discussed by Vestine (1954) on the dynamo theory of geomagnetic disturbances. Ferraro (1954) while agreeing to the suggestion that there are undoubtedly atmospheric contributions to the magnetic

storm currents, for instance, in the aurora\

zone, finds it difficult to accept that a charac- teristically world-wide phenomenon like

se

can be generated by winds in the atmosphere as if by trigger action. It is, however, prema- ture to say whether the application of dynamo theory to geomagnetic disturbances can be fully satisfactory; only a beginning in this direction has been made by Vestine, Fuku- shima and others.

7. Acknowledgement

My thanks are due to Dr. A. K. Das and Shri B.N. Bhargava for their suggestions.

REFERENOES

Ferraro, V. C. A.

Ferraro, V.C.A. and Unthank, H. W.

Forbush, S. E. and Vestine, E. H.

Sivaramakrishnan, M. V.

Srinivasamurthy, B.

Snguira, M.

Vestine, E. H.

1954 .1. geophys. Res., 59, p. 311.

1951 Geofis. pur. appl., 20, pp. 3-6.

1955 J. geophys. Res., 60, p. 299.

1956 Indian J. Met. Geophys., 7, 2, p. 137.

1959 Ibid., 10, 2, p. 209.

1953 J. geophys. Res., 58, p. 558.

1954 Ibid., 59, p. 93.

References

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