6
J.di •• . 1. Md . a.ophys. (1972), 23. 2. 189·194 551.590.22 : 525.6 Lunar atmospheric tides in surface winds at six Indian stations* K. N. RAO and S. JEEVA: 'UNDA REDD Y M eteorol ogica lO ffice , Poona (Receirol 21 April 1971) ABSTRACT. Using hourly data for 8 to 10 yealll. the lunar semi-diurnal tldee-c-emplitude (I.) and p.•} in Rurfa.oo winds at. "ix. Indi an "t6 tion'l heve b een determi ned . In working out th e vect or pr ol)abl o erro r. th o' improved method of )bti n and Ch'lpm "lQ(1910) ba'" boon used, Th e ealuee obta ined for amplltude in tho ease of ecat wer d (II) component am in good agreement with t.hc theoretioal value (10m/fl ee), out in the case of lkluLhwl\rd (- ..) eompa nem , th e ealouleted veteee aro aome what lees. Except in a few eeeee, the f1 0Me of eote tt on of the wind vector il1 co nt ra ry to that predicted by the theory . Bu t, however, tho proba ble error values obt ained are in reasoueble limlte, evon though the d'\ta.used are for a.ehcrt. period. Th o Increaac with la titude, of the amplitude here inf erred is in accordance with theory. However f\AJ'lier st udie s (t.U" Haurwitz and Cowley) do not indicate such verietion. The amplitudes obtainodfor eastward (ll)COm- pon cnt Ilylng in the range 0 ·8·}·3 of wind for the six eta tione UIe greeter 1h"D the southward (-u) com- ponent (lying in the range 0·4-0·9 em/sec) of wind and the probab le er rors follow this t-rend. Tho amplitude in J .tlO uon ia greeter than in Dceoeecn at 011 the l ix sta tions. , 1. Introdu oUon Chapman (19!8) evaluated lunar tide. at Mauritius in the Southern Hemisphere and Haur- witz and Cowley (\968) for four American stations in the Northern Hemisphere. In meteorological elements, the lunar semi-diurnal tide is found to be significant. They obtained the amplitude of the lunar semi-diurnal wave as \ em/sec and th e rotation with time of wind vector is opposite in the two hemispheres, which arc both in agreement with theory. But in both t he hemispheres, the sense of rotation of the calculated wind vector is contrary to that expected from theory. In the present paper lunar tide (L,) in surface winds at six Indian stations in different latitudes have been studied. The data considered are the mean hourly values over a period of 8 to 10 years, as detailed in Table I. 2. An&lr ' ls The amplit ude and phase are calculated using Chapman and Miller (19!0) method and the vector probable error evalu at ed by a method due to Malin and Chapman (1970). The data have been analysed for the three seasons and annual, i.e., J = Mi y to August, D = November to February, E = March, April, September & October and Y= Yearly. In case of meteorological d ata stormy day. are very few. The data is therefore, not analysed according to calm and disturbed days as in tho case of gcomagnetio data. The computa- tions were made for J, D, E and Y on IBM 1620 comput er at Poona and on CDV 3600 computer at Bombay. The solar and lunar tides are obtained in th e form, 4 8 = }; s, sin (1" + 8,) (I) p= 1 and t. = }; I, sin [ 1(1l -2) + 2. + A,J (2\ ._1 where. 8 = ""lar tid e, s, and 8, (1' =1 , 2, 3,!) represent amplitudes and phases respectively of the first four harmonics i .e., 24, 12, 8 and 6 solar hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tid e,l , and A, (n =I,2,3,4) represent amplitudes and phases respectively of the first four harmonics, i.e., 24, 12, 8 and 6 lunar hourly waves in lunar tide (24 lunar hours = \ lunar day), t = time in degrees; increases from 0° to 360° from one local transit of the sun (local mid night) to the next, and. = time in degrees; increases from 0° to 360° from one local transit of the moon to the next (one lunar day = \ '03505 solar days). - As the lunar semi-diu rnal wave alone is signi - . ficant in meteorological elements, the above equation for lunar tides can be written as - L = I. sill (2. + \1 (:I) and correspondingly its solar semi-diurnal tide is- s = 8. sin (21 + 8.) (4) Neces.'5ary corrections arc made for and 9 2 , The result s of the analysis are shown in Table 2. In the course of eomputotions of L., solar tide, S, . has also been determined and these are gh'el1 •Acuulltcd for llrcijQlltation a t thoX thAssclllbly, I.u.a.G., in AUGust 1971, Moscow 189

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Page 1: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes

J.di•• .1. Md. a.ophys. (1972), 23. 2. 189·194

551.590.22 : 525.6

Lunar atmospheric tides in surface windsat six Indian stations*

K. N. RAO and S. JEEVA:'UNDA REDD Y

Meteorological Office, Poona

(Receirol 21 April 1971)

ABSTRACT. Using hourly data for 8 to 10 yealll. the lunar semi-diurnal t ldee-c-emplitude (I.) and pha~p.•}in Rurfa.oo winds at. "ix. Ind ian "t6 tion'l heve been determined . In working out th e vector pr ol)ablo erro r. th o'improved method of )btin a nd Ch'lpm "lQ(1910) ba'" boon used, Th e ealuee obtained for amplltude in tho easeof ecat wer d (II) component am in good agreement with t.hc th eoretioal value (10m/flee), out in the case oflkluLhwl\rd (-..) eompa nem , th e ealouleted veteee aro aome what lees. Except in a few eeeee, the f10Me ofeote tt on of the wind vector il1 cont ra ry to that predicted by the theory . Bu t, however, tho probable errorvalues ob tained are in reasoueble limlte, evon thou gh th e d'\ t a. used a re for a.ehc rt. period.

Th o Increaac with latitude, of the amplitude here inferred is in accorda nce with theory. However f\AJ'lierst udie s (t.U" Haurwitz and Cowley) do not indi cat e such ve rietion. Th e ampli tudes obtainod for eastward (ll)COm­poncnt Ilylng in the range 0 ·8·}·3 cm/~c) of wind for the six eta t ione UIe greeter 1h"D the southward (-u) com­ponent (lying in the range 0 ·4-0 ·9 em/sec ) of wind and the probab le er rors follow this t-rend. Tho amplitude inJ .tlOuon ia greeter than in D ceoeecn at 011 the l ix sta t ions.

•,

1. Introdu oUonChapman (19!8) evaluated lunar tide. at

Mauritius in the Southern Hemisphere and Haur­witz and Cowley (\968) for four American stationsin th e Northern Hemisphere. In meteorologicalelements, the lunar semi-diurnal tide is found to besignificant . They obtained the amplitude of thelunar semi-diurnal wave as \ em/sec and th erotation with t ime of wind vector is opposite inthe two hemispheres, which arc both in agreementwith theory. But in both the hemispheres, thesense of rotation of the calculated wind vector iscontrary to that expected from theory.

In the present paper lunar tide (L, ) in surfacewinds at six Indian stations in different latitudeshave been studied. The data considered are themean hourly values over a period of 8 to 10 years,as detailed in Table I.2. An&lr ' ls

The amplitude and phase are calculated usingChapman and Miller (19!0) method and the vectorprobable error evaluat ed by a method due toMalin and Chapman (1970). The data have beenanalysed for the thre e seasons and annual, i.e.,J = Mi y to August, D = November to February,E = March, April , September & October and Y=Yearly. In case of meteorological data stormyday. are very few. The data is therefore, notanalysed according to calm and disturbed daysas in tho case of gcomagnetio data. The computa­tions were made for J , D, E and Y on IBM 1620computer at Poona and on CDV 3600 computerat Bombay.

The solar and lunar tides are obtained in th e form,4

8 = }; s, sin (1" + 8,) (I)p = 1

•and t. = }; I, sin [ 1(1l-2) + 2 . + A, J (2\._1

where. 8 = ""lar tide, s, and 8, (1'=1 , 2, 3,!)represent amplitudes and phases respective ly of thefirst four harmonics i .e., 24, 12, 8 and 6 solarhourly waves in solar factor (24 solar hours =I solar day) . L = Lunar tide,l, and A, (n=I,2,3,4)represent amplitudes and phases respectively ofthe first four harmonics, i.e., 24, 12, 8 and 6 lunarhourly waves in lunar tide (24 lunar hours = \lunar day), t = time in degrees; increases from 0°to 360° from one local transit of the sun (localmid night) to the next, and. = time in degrees;increases from 0° to 360° from one local transitof the moon to the next (one lunar day = \ ' 03505solar days). -

As the lunar semi-diurnal wave alone is signi - .ficant in meteorological elements, the aboveequat ion for lunar tides can be written as -

L = I. sill (2. +\1 (:I)and correspondingly its solar semi-diurnal tide is-

s = 8. sin (21 +8.) (4)

Neces.'5ary corrections arc made for .\~ and 92,

The results of the ana lysis are shown in Table 2.In th e course of eomputotions of L., solar tide,S, . has also been determined and these are gh'el1

•Acuulltcd for llrcijQlltation at tho XthAssclllbly, I.u.a.G., in AUGust 1971, Moscow189

Page 2: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes
Page 3: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes
Page 4: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes
Page 5: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes
Page 6: 1 - metnet.imd.gov.inmetnet.imd.gov.in/mausamdocs/523210.pdf · hourly waves in solar factor (24 solar hours = I solar day). L = Lunar tide,l, and A, (n=I,2,3,4) represent amplitudes