Co-ordinated observations of VHF scintillations in...

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Indian Journal of Radio & Space Physics Vol. 29, February 2000, pp. 22-29 Co-ordinated observations of VHF scintillations in India during February-March 1993 Sushi I Kumar'. A K Gwa 1 1 , P V S Rama Rao 2 , P T Jaychandran 2 , D S V V D Prasad 2 , R P Sing)l 3 , UP Singh 3 , A Dasgupta 4 . K Ba su 4 , R Sethuraman 5 , B M Pathan 6 , DR K Rao 6 , S Banola 6 , P S Kesava Rao 7 , Appala Naidu 7 , T R Tyagi x. P N Yijaykumar 8 , H Chandra 9 , G D Vyas 9 , Birb al Singh 10 , P awan Chauhan 10 , K N ly er 11 , K N Pathak 11 , C S Shal gao nkar 12 , B M Vyas 13 & R G Rastogi 14 1 Department of Ph ys ics, Barkatull ah Univ ers ity , Bhopal 462 026 ' Department of Ph ys ics , Andhra Univers it y, Waltair 530 003 1 Department of Physics. Ban aras Hindu University, Varanasi 221 005 4 ln stitut e of Radio Physics & Elect roni cs, Calcutta University, 92 Acharya Prafull a Chandra Road, Calcutta 700 009 1 Dep;trtme nt pf Ph ys ics, Hindu sthan Co ll ege of Engineering, Padur, Di st Chingleput 603 I 03 , (via) Kelambakkam, Tamil Nadu "Indi an Institute of Geomagneti sm, Colaba, Munibai 400 005 7 Dcpartment of Phys ic s, JNTU Co ll ege of Engineering, Anantpur 515 022 ' Radio Scie nce Divi sion, National Physical Laboratory, New Delhi II 0 0 12 '' Ph ysical Research Laboratory, Ahmedabad 380 009 '"Department of Physics. RBS College, Agra 283 105 11 Department of Ph ysics, Sa ur as htra Un ive rsit y, Rajk ot 360 005 12 Department of Ph ys ics, Shivaji University, Kolh apur 416 004 11 Departme nt of Ph ys ics, M L Sukhadia University , Udaipur 14 1 NSA Senior Scientist, Department of Physics, Gujarat University, Ahmedabad 380 009 Received 8 July 1999; revised received I No vember 1999 The VHF sc intillation obse rv ations made at a chain of stati ons in India during February-M arch 1993 under AICPITS (third campa ign). using th e 244 MHz radio beacon from FLEETSAT, and analysed joi ntly by all participating investigators at ;l works hop held at Raj kot are described. The occurrence features of sci ntill ati ons during th e th ird campaign were si milar to tho se observed during the lirst campaign of March-April 199 1. The maxi mum occu rr ence was, however, red uced to some ex tent due to th e lower so lar ac tivit y. The latitudinal variations showed an increased occurrence in th e region of about 17- 1 xo l at itude. The data duri ng th e ni ght of 19-20 Feb. 1993 when an extensive 'Ion isa tion Hol e Campaign' was undertaken showed sc intillations marked by earlier onset and longer duration at stations Walt air a nd Nuzvid than at th e stat ions close to th e magn e ti c equator. Howeve r, based on th e average variations during February-Ma rch 199 3 the onset at Tiruchendur, Anantpur and Wa lt air was at nearly the same time. The vertical ri se velocity of the plasma depletions, es timated from th e time delays in the onse t of sci ntillations at latitudes away from th e dip eq uato r, was found to range from 40 m/s to 420 m/ s in the altitude reg ion 300- 1 .'1 50 km . I Introduction Monitorin g of satellite radio beaco ns provide s a simple method to study the ionospheric irregular ities. The flu ctuati ons in the signal strength, c haracterized by some form of scintillation index are related to the fluctuations in electron densit y. Th e amplitude fluctuations can also be u sed to derive the temporal spectra of the electron density fluctua ti ons in the ionosphere and ca n be co nverted into spatial spectra if the veloc it y of the irregulariti es is kn ow n. R adio be acons on-b oa rd orbiting or geo-stationary sate llit es have been used extens ively to study the temporal and spatial vanat10ns of scintillation index , power spectral features and the velocity of the irregularities (in case of s paced rece iver reco rdings). Globally there are two regions of strong scintillation s-o ne centred at the magnetic equator with a width of 20° and another at hi gh latitudes (Aaro ns 1 and refe renc es ther ein). India provide s a unique location for studying scintillaions at low latitud es covering a reg io n ri ght from the magne ti c equator to beyo nd the F-region ionization anoma ly crest reg ion. Detailed studies on

Transcript of Co-ordinated observations of VHF scintillations in...

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Indian Journal of Radio & Space Physics Vol. 29, February 2000, pp. 22-29

Co-ordinated observations of VHF scintillations in India during February-March 1993

Sushi I Kumar ' . A K Gwa11, P V S Rama Rao2

, P T Jaychandran2, D S V V D Prasad2

, R P Sing)l3, UP Singh3

,

A Dasgupta4. K Basu4

, R Sethuraman5, B M Pathan6

, DR K Rao6, S Banola6

, P S Kesava Rao7, Appal a Naidu7

,

T R Tyagi x. P N Yijaykumar8, H Chandra9

, G D Vyas9, Birbal Singh 10

, Pawan Chauhan 10, K N lyer 11

,

K N Pathak 11, C S Shalgaonkar 12

, B M Vyas 13 & R G Rastogi 14

1 Department of Ph ysics, Barkatullah University, Bhopal 462 026

' Department of Ph ysics , Andhra University, Waltair 530 003 1Department of Physics. Banaras Hindu University, Varanasi 221 005 4 lnstitute of Radio Physics & Electronics, Calcutta University, 92 Acharya Prafull a Chandra Road, Calcutta 700 009 1Dep;trtment pf Physics, Hindusthan College of Engineering, Padur, Dist Chingleput 603 I 03 , (via) Kelambakkam, Tamil Nadu

"Indi an Institute of Geomagneti sm, Colaba, Munibai 400 005 7Dcpartment of Physics, JNTU Co llege of Engineering, Anantpur 515 022

' Radio Science Divi sion , National Physical Laboratory, New Delhi II 0 0 12

'' Ph ysica l Research Laboratory, Ahmedabad 380 009

'"Department of Physics. RBS College, Agra 283 105 11 Department of Ph ysics, Sauras htra University, Rajkot 360 005 12Department of Ph ys ics, Shivaji University, Kolhapur 416 004 11Department of Ph ysics, M L Sukhadia University, Udaipur 141NSA Senior Scientist, Department of Physics, Gujarat University, Ahmedabad 380 009

Received 8 July 1999; revised received I No vember 1999

The VHF sc intillation observations made at a chain of stati ons in India during February-M arch 1993 under AICPITS (third campaign). using the 244 MHz radio beacon from FLEETSAT, and analysed joi ntly by all participating investigators at ;l works hop held at Raj kot are described. The occurrence features of scintill ati ons during the th ird campaign were si milar to those observed during the lirst campaign of March-April 199 1. The maxi mum occu rrence was, however, reduced to some ex tent due to the lower so lar activit y. The latitudinal variations showed an increased occurrence in the region of about 17-1 xo lat itude. The data duri ng the night of 19-20 Feb. 1993 when an extensive ' Ion isation Hole Campaign' was undertaken showed sc intillations marked by earlier onset and longer duration at stations Waltair and Nuzvid than at the stat ions close to the magneti c equator. However, based on the average variations during February-March 1993 the onset at Tiruchendur, Anantpur and Wa lt air was at nearly the same time. The vertical ri se velocity of the plasma depletions, estimated from the time delays in the onset of sci ntill ations at latitudes away from the dip equator, was found to range from 40 m/s to 420 m/s in the altitude region 300- 1.'1 50 km.

I Introduction Monitoring of sate llite radio beacons provides a

simpl e method to study the ionospheric irregularities . The flu ctuati ons in the s ignal strength , characterized by some form of sc intillati on index are re lated to the fluctuations in e lect ron density. The amplitude fluctuati o ns ca n a lso be used to derive the temporal spec tra of the e lec tron density fluctuations in the ionosphere and can be converted into spatial spectra if the ve loc ity of the irregu la rities is known. Radio beacons on-board orbiting or geo-stationary sate llites

have been used extensively to study the temporal and spatial vanat10ns of sc intillation index , power spectral features and the velocity of the irregularities (in case of spaced receiver recordings). Globally there are two regions of strong sc intillations-one centred at the magnetic equator with a width of 20° and another at high latitudes (Aarons 1 and references therein) .

India provides a unique location for studying sc intillaions at low latitudes covering a region right from the magnetic equator to beyond the F-region ionization anomaly crest region . Detailed studies on

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SUSHIL KUMAR et al.: VHF SCINTILLATIONS IN INDIA DURING FEB.-MAR. I 993 23

scintillations m the equatorial region were made during the A TS-6 phase II from Thumba2

and Ootacamund '·6 from the multi-frequency measure ments . Sc intillation studies covering a chain of stations in India were attempted during the total so lar ec li pse event of February 1980 by Somayajulu et o/7 However, an extensive study on scinti ll ations at equatoria l and low latitudes in India was possible when a network of nearl y 20 stations was establi shed under the All Indi a Co-ordinated Programme of Ionospheric and Thermospheric Studie·s (A ICPJTS). The obse rvati ons were made at 244 MHz using the

radi o beacon on-board FLEETSAT (73°E). The sc intillati on data were recorded using identical systems at most of the locations, consisting of a simple 11-e le ment Yagi-Uda antenna, VHF receiver and sing le channe l chart recorder which were es tablished with the help from the Indian Institute of Geomagnetism, Colaba, Bombay. However, there were a fe w locati ons with data recorded in digital form also. As part of the co-ordinated studies, campa1 gns were conducted which were followed by j oint data anal ys is workshops. The first of such campaigns was conducted during March-April 199 1 and the sa lient features of the scintillations at low latitudes in the Indi an longitude region during the campaign have been described by Chandra et al8

. The scintillations were general ly found to occur in a continuous patc h or in patches of longer duratism near the magnetic equator, wh ile away from the equator there is a systematic de lay in its onset (they occur in smaller patches with a smaller duration) . The half widths of the equatorial belt of scintill ations, as determined from the latitudinal variations, were found

to be about I so before midni ght and 6° in the post midni ght peri od.

In the present paper, the results obtained from the third ' sate llite sc intillation network' campaign, conducted during Fe bruary-March 1993, have been reported . The peri od covered the ' Ionisation Hole Campai gn ' , unde rtaken by the Physical Research Labpratory, Ahmedabad, to study the equatorial spread-F. The ' Ioni sati on Hole Campaign ' involved the launc hing of two RH-560 rockets on 19 Feb. 1993. The first o f the rockets re leased active chemica ls at four a ltitudes for measuring the electric fi e lds and neutral winds. Thi s was fo ll owed by another roc ket in strumented with plasma probes and

') mass spectrometers . A number of complementary ground-based radio and optical experiments were also

conducted during the rocket campaign . The scinti llation data collected at the AICPITS network of stations during the campaign of February-March 1993 were jointly analysed by the participating investigators at the workshop held at Rajkot, Gujarat, during April 1993.

2 Observations and data analysis The locations of the stations operated during the

campaign are shown in Fig. I . The geographic co­ordinates of the stations along with the dip angle at the sub-ionospheric point of the satellite-to-rece iver path (at 400 km) are also provided in the Table I . The chain covers the region from dip equator to about dip angle of 44°N. The sub-ionospheric points corresponding to an altitude of 400 km cover from

dip equator to about 40°N. The two new stations included in this campaign are Nuzvid and Udaipur. Data recorded on charts have been used in the present study . On examination of the chart recording the fo ll owing information were compi led: (i) start time and end time of each patch of scintillat ions and

. '" 35or~-~~,H--... ---f-----4--+-- 3S' I I ,.. -~

r---~ --~ -5d'N- --­) \.

30° r--t---r-"t---+~'~·-+--r---,30° /

...__I eDHL (_ (\ ,·'

\~--- AGRe 4 rJ'N-::_ -..J-:::- -~ 2~ ~ v~. ~

~ ,- .,AH~~ UJJ ._1 / ~ ~ • • • B~P C~Al.el. '-'\ :)

20o lRJKJ'l·----..-r-30°N-- ~- rl A' r-r~-+-~~-~~~G~--~L--t--12U

I 5o tir..__~·_..B~YJ.!!'~~·\~P-· -w;:;-.-----4-~---N~:--_-_--t---fl !l ' ANT'" .wos,.. ----r---- ---- -lvN-t-

1\ ANM•

1 oo rr---t·---\-'--7"'1---+----t--11 0° 1----(..&' --r!- ----

LONGITUDE

Fig. !-Map of Indi a showing the localions of the stations recording the 244 MH z radio beacon from FLEETSAT for sci ntillation studi es during the AICPITS

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24 INDIAN J RADIO & SPACE PHYS, FEBRUARY 2000

Tahle !- Locations of the scinti llation recording stations in India during the campaign of February-March I 993

Name of Geog. !at Geog. long. Dip angle Dip angle at sub-stat ion deg deg deg ionospheric point

deg

Trivandrum* 8.4 76.9 0.6 -0.6

Tiruchendur 8.5 78.2 0.7 -0.5

Annamalai nagar* 11.4 79.4 7.6 6.0

Madras 13 .1 80.3 I 1.6 9.5

Anantpur 14.7 77.6 15.7 13.4

Goa* 15.2 74.0 17.2 14.9

Kolhapur 16.7 74.2 20.6 18. 1

uzvid 16.8 80.8 19.9 18.0

Waltair 17.7 83.3 21.9 19.3

Bombay 19.0 73.0 25.7 22.9

Nagpur* 21.1 79 .1 29.5 26.6 .

Rajkot 22.3 70.8 32.6 29.6

Calcu lla 22.6 88.4 3 1.9 28 .7

Ahmedabad 23.0 72.4 33 .8 30.7

Ujp1n 23 .2 75 .8 33.9 30.8

Bhopal 23 .2 77 .6 33 .8 30.7

Udaipur 24.0 73 .7 35.3 32.3

Yaranas i* 25.3 83.0 37.3 34.0

Agra 27.2 78.1 41.1 37.7

Delhi 28.8 77.2 43.7 40.72

*Stations operated during A1CPITS but data not available for the present study.

(ii ) ~very quarter-hourly (± 7.5 minutes) presence of c intillati ons.

3 Results The mean nocturnal vanat10ns of the percentage

occurrence of sc int illations at 14 of the total stations during the period February-March 1993 are shown in Fig. 2. The stations Tiruchendur, Madras and Anantpur situated in the magnetic equatorial zone show onset around 1900 hr 1ST (77 .5° EMT) with peak occurrence of about 40 %. It must be noted that the occurrence rates are higher at Madras and Anantpur, s ituated a few degrees away from the magnetic equator, than at Tiruchendur, situated at the magnetic equator. The stations Kolhapur, Nuzvid, Waltair and Bombay, situated in the zone intermed iate to equatorial and the anomaly crest zones, are characterized by onset around 2000 hrs IST and sc intill ati ons last ing till sunrise with maximum occurrence of about 30 % (occurrence are little higher at Nuzvid) . The stat ions si tuated in the anomaly crest zone (Rajkot , Calcutta, Ahmedabad, Ujjain and Bhopal) show onset of scinti llations at around 2000

hrs IST and lasting till 0600 hrs 1ST with maximum occurrence of 20 %. In the zone beyond the anomaly crest (Agra and Delhi), the onset time is around 2100 hrs 1ST with peak occurrence of only lO%. The onset times are not different from those reported for the campaign period of March 1991 . However, the maximum occurrence were slightly higher for the campaign of March 1991 with values of 50%, 40%, 30% and 20% for the four zones. T he decrease in the maximum occurrence rates of scintillations is due to the lower sunspot activity during 1993.

The latitudinal vanat10ns of the percentage occurrence of scintillations for different local times plotted against the geographic latitude are shown in Fig. 3. The local time groupings are the post-sunset ( 1900-2100 hrs 1ST), pre-midnight (2200-0000 hrs IST), post-mjdnight (0 I 00-0300 hrs 1ST) and pre­sunrise (0400-0600 hrs 1ST). The occurrence does not seem to be maximum at the magnetic equator, but at few degrees away . In the first campaign, the maximum occurrence of scintillations was observed at the magnetic equator. However, one has to consider the fact that during the present campaign there is no

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SUSHIL KUMAR et al.: VHF SCINTILLATIONS IN INDIA DURING FEB.-MAR. 1993 25

data ava il able from Tri vandrum and Annamalainagar. Another po int of interest is that there is an increase in

the occurrence around 17-1 8° latitude . This feature was a lso observed in campaign of March-April 1991 .

The sc intillati on data recorded at a ll the stations of the chain during the night of 19-20 Feb . 1993 have been plotted in Fig. 4 to show the duration of sc intillati ons as a functi on of the dip angle. The

w (.)

z w 0::: ~ :J (.) (.)

0

u.i C>

~ z w u 0::: UJ 0...

40

30 20

10

T iruchendur Raj kot

0~~----------~------~~~~~--------~~~~~--~

40

30 20

10 o~L---------------~--~~----------~~~~

40 30 20

10

0~~------------------~~--~~~---~----~"'~~~~~~

40 Kolhapur Ujjain

30 20

10

0~~--~-----------=--~~-L~----------~~~ 40

30 20

10

0~~------------------------~~~~----------------~~~ 40

30 20

10

Waltair Agrci

o~~-------------------------~~~~--------------------4 40

30 20

10 0~~~---.---.---.--~~~r-~~~~~-=~""~~~~""~~

1& 20 22 00 02 04 06 18 20 22 00 02 04 06

TIME, hrs I ST

Fig. 2- Nocturnal varia tions of the percentage occurrence of cint ill ations at 14 locations averaged over the campaign period February-March 1993

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26 INDIAN J RADIO & SPACE PHYS, FEBRUARY 2000

.30 (04-06hrs)

20

10 I

0 w (01-03hrs) u 30 z w 0::

20 0:: => u u 10 0

w C) 0 ct ( 22-00 hrs ) .... z 40 w u 0:: w 30 11.

20

10

0 ( 19-21 hrs )

30

20

10

14 16 18 20 22 24 26 28

GEOGRAPHIC LAT., deg.

Fig. 3-Vari ati on with geographi <.: latitude of the mean percentage occ urrence of s<.: in till atiu ns at di fferent local times for the period Feh ru ary- March I <J'J3

45 ,-----------------------------~

40

35

Ol 30 ., "0

w 25 _J

t? ~ 20 0..

0 15

10

5

18

19 FEBRUARY, 1993

_......;;..;-;;_ _'-____ _

21 00

TIME, hrs LT

OJ 06

Fi g. 4- T imc duration o f sci nti ll atio ns during the ni ght of 19-20 Feh . I 'J'J3 at the chai n o f statio ns pl otted on a grid o f local time a nd dip angle

observations cover the region right from the magnetic equator to dip of 40°. The local time correction has been made in the figure. The onset is earliest at Waltair (dip 19.3°N) and Nuzvid (dip I8°N), which is about an hour before the onset at Tiruchendur, located at the dip equator. The duration of scintillations is also longest at these two stations. There is a systematic decrease in the duration of scintillations for the stations located in the anomaly crest region and beyond. Progressive delay in the onset time is seen, but more striking is the earlier decay of scintillations at these stations .

The variation of the onset time of scintillations with latitude is studied from the average nocturnal variations of the percentage occurrence of scintillations during the campaign period of February­March 1993 based on quarter-hourly values and shown in Fig. 5. The onset time is corrected for the local time differences. It is clearly seen that the scintillations first appear near the magnetic equator (at 1840 hrs 1ST at T iruchendur, at 1900 hrs 1ST at Madras with dip of I 0°N) and the onset time increases with the dip angle. There is a delay of about an hour fo r stations close to the ionization anomaly crest and about two hours for Delhi , the northernmost station. Assuming that scintillations first appear at magnetic equa~or and that the onset at latitudes away frorn the dip equator is related to the vertical ri se of the depleted regions of pl asma density through the geomagnetic fie ld lines, the vertical rise veloci ties of the pl asma depletions have been estimated by some

21~ .------------------------------. (a) February-March 1993 •

20~

~ "~ ~ •

I! 18~ • &.

~ 21~ i= (b)

19 February 1993

20~

19~

18~4-----r----r----~--~----,---~

-1 0 0 10 20 ~ 40 50

DIP ANGLE, deg

Fig. 5-Vari ations of the onset times o f sci ntill ations wi th dip angle: [(a) average tor February-March 1993 and (b) fo r the night o f 19-20 Feb. 1993)

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SUSHIL KUMAR et al. : VHF SCINTILLATIONS IN INDIA DURING FEB.-MAR. I 993 27

workers to.tt _ If we assume that F-region altitudes

associated with irregularities causing scintillations are around 300 km, the altitudes of the depleted plasma over the. dip equator, connected to the 300 km at other latitudes through magnetic field lines, can be obtained . The vertical velocity of the plasma depletions has been estimated from time delays between the onset of scintillations at locations centred at 0 , I 0, 20, 30 and 40° dip angles. The altitudes at dip equator corresponding to the field lines at 300 km at the locations of I 0, 20, 30 and 40° dip are about 365, 550, 850, and 1350 km, respectively. Thus, one can compute ' vertical rise velocity at different altitudes of F-region . For the time delays observed from the monthly mean onset times, the velocities come out to be 40, 420, 330 and 140 rrvs for the altitude regions 300-365 , 365-550, 550-850 and 850-1350 km, respectively . Thus, the high vertical velocity is noticed between the altitude regions of 365-550 and 550-850 km.

The variation with latitude of the onset time of scintillations on the night of 19-20 February is also shown in Fig. 5 . During this night the onset is earliest at dip angles 18-20°. Chandra et al.t 2 have reported a case of ni ghttime F-region scintillations extending into daytime during II Nov. 1991. The event was characterized by onset earlier at Bombay than at Trivandrum. Also the scintillations disappeared first at Trivandrum rather than at Bombay. The event, however, followed a magnetic storm with sudden commencement on I 0 Nov. 1991. The period of 19 February is not cl ass ified as a geomagnetic disturbed day; however, there was a sudden commencement on

17 February and the period after 20 February had high Kp values . The time delays in the onset of

scintillations from region of 20° dip angle and beyond during the night of 19 Feb. 1993 give vertical velocity of 400 rnls between 550 and 850 km and I 00 m/s between 850 and 1350 km. These are close to the values estimated from the mean time delays for February-March 1993.

The locations of the stations Bhopal and Ujjain in the anomaly crest zone with same latitude but different longitudes have been utilized to determine east-west velocity of the scintillation patches derived from the time de lay in the onset of scint illation patches at the two stations . Figure 6 shows a plot of the eastward ve locity during the night of 19-20 Feb. 1993 . The velocity decreases from more than 200 rnls at around 2000 hrs IST to about I 00 rnls at around

250 19 February, 1993

~ • ~ 200

~ ~ • ...l

~ 150 • ~ ~ 100 • Cll • < Ill

50

2000 2100 2200 2300 0000 0100

TIME, hr.iiST

Fi g. 6- Time vari ati on of the eastward velocity of the patches of scintillations during the night of 19-20 Feb. 1993 derived from the time delay in the onset time of scintillations at Bhopal and Ujjain located at the same latitude but at different longitudes

midnight. This is consistent with the velocity obtained from the recording of scinti llations of SIRIO and FLEETS AT signals simultaneously over Bombay 13

.

4 Discussion The irregularities associated with equatorial

spread-F (ESF) cover a wide range of scale sizes from several hundreds of kilometres to few centimetres. It is well accepted that the onset of ESF is due to the generation of intermediate scale size irregularities in the bottom side of F-region by the generalized Rayleigh-Taylor instability that includes the electric field and neutral windst 4,t5 . The depleted regions of plasma rise rapidly and align along the geomagnetic field lines. The sharp gradients at the walls of plasma depletions result in smaller scale irregularities that give rise to scintillation of radio waves, plumes on backscatter radar maps. and spread-F on ionograms 16

-21

. The plasma depletions have large spatial extent along N-S and the rapid rise of these results in the onset of scintillations at latitudes away from the dip equator. The plasma depletions (bubbles) are known to have large vertical velocities . At colli sion-dominated low-altitude region (-below 350 km) the rise velocity is related to the degree of depletion . Measured bubble velocities show a saturation value of around 200 rnls for the collision­dominated region2 1

. At higher altitudes the ri se velocity is related to the size of the bubble and should reach a maximum value between 200 and 700 rnls above 550 km for bubble radii between 16 and 200

ry' km (Ref. 22) . Tsunoda et aL.-- have reported bubble

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28 INDIAN J RADIO & SPACE PHYS, FEBRUARY 2000

ri se ve l9c ity ranging between 50 and 350 rnls . Dabas and Redd/ 1 made sc intill ation observations at four stati ons in Indi a during hi gh solar activity period (covering geographic locations from dip equator to up

to 30°N). The time de lays in the onset of sc intill ations were fo und to be consistent with the bubbl e ri se ve loc ity of 50-350 rnls. Aggson et a /.24

repon ed two events of pl asma bubbles up-drifting with ve loci ties of about 2 krnls from satellite measurements of eastward e lec tric fi eld within the bubble. The locati on of the two events mapped to altitudes of about 600 and 800 km at dip equator. Rocket-borne in situ DC electric fie ld measurements have been made up to 950 km during equatorial spread-F (Ref. 25). Outs ide the regions of plasma depleti ons, elec tric fie ld was fo und to be primarily ve rtica l. . However, ins ide the depletions vertical e lec tri c fi e lds were found to be comparable to zonal e lectric fie lds. The zonal e lectric field was found to be en hanced in the depleted regions with maximum around 550 km. T he pl asma depleti ons were found to rise with speeds of up to I 00 rnls. Recently , Sekar et a/.26 have reported upward ve loci ty up to 200 rnis in the cent ral regions of the plume structures from the observa ti ons made by us ing Indi an MST radar.

The bubble ri se ve loc ity of about 300-400 rnls in the a ltitude region 365-850 km and a less ve loc ity at lower and higher altitudes estimated from the time de lays in the onset of sc intillations at a chain of stations in India are consistent with the satellite-borne in situ measurements of e lectric fi eld . The values are in agreement with those determined from the chain of sc intill ati ons receivers and radar. Sekar et a/.15 had shown earlier, fro m non-linear s imulation studies, the upward ve loc iti es of few hundreds of metres per second under favo urable vertical winds. The sc intill ati on data at the closely spaced meridional chai n of stat ions offer a simple method to detect the bubbl e ri se ve loc ity on a day-to-day bas is.

5 Summary The sc intill ati on data at the chain of stations that

operated during the third campaign of February­March 1993 revea l that

(i) The max imum occurrence of sc intillations in the equ atorial, intermedi ate, anomaly crest region and beyond the anomaly crest region has dec reased by about I 0 % from the maximum va lues observed during the campaign of March-

April 1991 . Thi s is due to the decrease in solar activity .

(ii) The latitudinal variations of the occurrence of s cintillations during different hours show that there is an increase in the occurrence rates

around latitude of 17-18°. Thi s was al so seen in the plots from the earlier campaign.

(iii ) The data during the night of 19-20 Feb. 1993, when an ex tensive ' Ionisation Hole Campaign ' was conducted, show earlier onset of sc intillations and longer duration at Waltair and Nuzvid compared to the magnetic equator. However, based on the month ly mean variations during February 1993, the onset appeared first in the equatori al region .

(iv) Eastward ve loc ity of the patches of scintillations has been determined from the time delay in the onset time of sc intillations at Ujjain and Bhopal (same latitude but different longitudes) during the night of 19-20 Feb. 1993. The eastward ve loc ity decreases from about 200 rnls at the time of onset to less than I 00 rnls around midnight.

(v) The delays in the mean onset time with latitude for the period Feb. uary-March 1993, after local time correcti on, are used to determine the vertical ve locity of plasma depletions for different altitude regions. The velocity ranges from less than I 00 rnls at altitudes be low 365 km to more than 400 rnls at a ltitudes of 365-850 km. These are consistent with the electric fi eld measurements wi thin the depletions by sate llite measurements and with the ve loc ities reported from radar observations.

Acknowledgements The cha in of sc intillation stations operated under

the All India Co-ordinated Programme of Ionospheric and Thermospheric Studies (AICPITS) with funding from the Department of Sc ience and Technology (DST). The data were analysed j o intly at the third data analys is workshop he ld at Raj kot during April 1993 with funding from DST. Thanks are a lso due to the heads of vari ous university centres and institutes for providing fac ilities.

References I Aarons J, Proc IEEE (USA), 70 ( 1982) 360. 2 Moonhy K, Reddy C R & Mu rth y B V K, J Atmos & Terr

Phys(UK), 4 1 ( 1979) 123 . 3 Rastogi R G, Des hpande M R, Vats H 0, Davies K, Grubb R

N & Jones J E, Pramana (India), 8 ( 1977) I.

Page 8: Co-ordinated observations of VHF scintillations in …nopr.niscair.res.in/bitstream/123456789/25901/1/IJRSP 29...Indian Journal of Radio & Space Physics Vol. 29, February 2000, pp.

SUSHIL KUMAR et al.: VHF SCINTILLATIONS IN INDIA .DURING FEB.-MAR. 1993 29

4 Chandra H, Vat s H 0 , Deshpande M R, Rastogi R G, Sethia G, Sastry 1 H & Murth y B S, Ann Geophys (France), 35 ( 1979) 145 .

5 Ras togi R G, Chandra H & Deshpande M R, Indian 1 Radio & Space Ph1·s. I I ( 1982) 240.

6 Rastogi R G, Kuparkar P V, Chandra H & Deshpande M R, 1 A1nws & Terr Phvs (UK), 52 ( 1990) 69.

7 Sumayaju lu Y V, Garg S C, Dabas R S, Lakha Singh, Tyagi T R, Lokanadham B. Ramakrishna S & Navaneeth G N, Radio Sci (USA ), 19 ( 1984) 707.

8 Chandra H, Vyas G D. Rao D R K, Pathan B M, lype A, Ram Sckran B. Naidu A, Sadique S M, Salgaonkar C S, Tyagi T R, Vij ayk umar P N, Lakha Singh, lyer K N, Pathak K N, Gwal A K. Sushi! Kumar. Singh R P, Singh U P, Birbal Singh. Jain V K. Navaneeth G N, Koparkar P V, Rama Rao P V S. Jayachandran P T, Sriram P, Santa Rao N Y S, Das Gupta A, Basu K & Rastogi R G, Indian 1 Radio & Space Ph1·s. 22 ( 1993) 69.

9 Sridharan R. Chandra H, Das S R, Sekar R, Sinha H S S, Pall am Raj u D, Narayanan R, Shikha Raizada, Misra R N, Raghava Rao R, Rao P B. Ramarao P V S, Somayaju1u V V, Babu V V & Danilov A D. 1 Almos & Terr Phys (UK), 59 ( 1997) 205 1.

I 0 Somayaj ulu V V. Garg S C, Dabas R S, Singh L, Tyagi T R, Lokanad ham B, Ramakri shna S & Navneeth G, Radio Sci (USA). 19 ( 1984)707.

II Dabas R S & Reddy B M. Radio Sci (USA), 21 (1986) 453. 12 Chandra H, Vyas G D, Path an B M & Rao DR K, 1 Atmos &

Terr Phv.1 (UK), 57 (1995) 1273.

13 Koparkar P V & Rastogi R G, 1 Atmos & Terr Phys (UK), 47 (1985) 907.

14 Ossakow S L, 1 Atmos & Terr Phys (UK), 43 (1981) 437. 15 Sekar R, Suhasini R & Raghava Rao R, 1 Geophys Res

(USA), 99 (1994) 2205. 16 McClure 1 P, Hanson W B & Hoffman 1 H, 1 Geophys Res

(USA). 82 (1977) 2650. 17 Basu S, McClure J P, Basu Su, Hanson W B & Aarons J, 1

Geophys Res (USA), 85 ( 1980) 5119. 18 Kelley M C and McClure J P, 1 Atmos & Terr Phys (UK), 43

(1981) 427. 19 Tsunoda R T, 1 Atmos & Terr Phys (UK), 42 (1980) 743. 20 Weber E J, Brinton H C. Buchan J & Moore J G, 1 Geophys

Res (USA), 87 (1982) 503. 21 Hanson W B & Bamgboye D K, 1 Geophys Res (USA), 89

( 1984) 8997. 22 Ott E, 1 Geophys Res (USA), 83 ( 1978) 2066. 23 Tsunoda R T, Livingston R C, McClure J P & Hanson W B,

1 Geophys Res (USA), 87 ( 1982) 9 171. 24 Jahn 1M, LaBelle J & Plaff R F, Geophys Res Lett (USA), 24

(1997) 1695. 25 Aggson T L, Burke W J, Maynard N C, Hanson W B,

Anderson P C, Slavin J A, Hoegy W R & Saba J L, 1 Geopliys Res (USA), 97 ( 1992) 8581.

26 Sekar R, Kherani E A, Vi swanathan K S, Patra A K, Rao P B, Devasia C V, Subba Rao K S V, Tiwari D & Ramchandran N, "Preliminary results on equatorial spread-F irregularities by VHF and HF radars", Private Communication, 1999.