VLF Research in India and setup of AWESOME Receivers

Slides:



Advertisements
Similar presentations
Chapter 3 – Radio Phenomena
Advertisements

HOW DOES MY SIGNAL GET FROM HERE TO THERE? By Forest Cummings, W5LQU And Dave Russell, W2DMR.
BELGRADE DATABASES - ionospheric observations and detections astro- and geophysical phenomena by radio signals Aleksandra Nina Institute of Physics, Belgrade.
1 FIREBIRD Science Overview Marcello Ruffolo Nathan Hyatt Jordan Maxwell 2 August 2013FIREBIRD Science.
Using a DPS as a Coherent Scatter HF Radar Lindsay Magnus Lee-Anne McKinnell Hermanus Magnetic Observatory Hermanus, South Africa.
Which describes a variation of wave frequency ω(t) in a geometric-optic approximation [4]. Here n(ω) is the refractive index of the medium, is the vector.
Statistical Analysis of Electrostatic Turbulences over Seismic Regions T. Onishi and J.J. Berthelier Centre d'Etude des Environnements Terrestre et Planétaires.
ALTITUDE PROFILES OF ELECTRON DENSITY DURING LEP EVENTS FROM VLF MONITORING OF THE LOWER IONOSPHERE Desanka Šulić 1 and Vladimir Srećković 2 1 Institute.
Theoretical study of the diurnal behavior of VLF signal and comparison with VLF campaign data Sujay Pal [1], Sudipta Sasmal[2], and Sandip K. Chakrabarti[1,2]
Subionospheric VLF propagation
Features of Tweeks observed in Indian Low Latitudes Rajesh Singh, B. Veenadhari, A.K. Maurya, P. Pant 1, A.K. Singh 2 Indian Institute of Geomagnetism.
B. Veenadhari, Rajesh Singh, Sushil Kumar and Ajeet Maurya
Terrestrial gamma-ray flashes Prepared by Morris Cohen Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME Network.
VLF measurements of lightning induced electron precipitations and their effects on the D-region electron density profile D. Šulić, and V. D. Šulić 1, and.
Theoretical Study & Modelling of the Intensity Distribution of VLF Signals Tamal Basak [1], Sujay Pal [1], S K Chakrabarti [1,2] 1] S N Bose National Centre.
ELF/VLF waves as Earthquake precursor – A case study (May 12, 2008 Wenchuan, China earthquake) Rajesh Singh, A.K. Maurya, B. Veenadhari, P. Pant 1, A.K.
The DEMETER satellite: Payload, Operations and Data
22 July, 2009 Total Solar Eclipse: Effect on D-region Ionosphere Dynamics as Studied from AWESOME VLF Observations Rajesh Singh B. Veenadhari, A.K. Maurya.
1 Sferics and Tweeks Prepared by Ryan Said and Morris Cohen Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME.
VLF sub-ionospheric signals and Earthquake precursor signatures? Results from the studies of some recent Earthquakes Ajeet K Maurya, Rajesh Singh, B. Veenadhari.
1 Sounds of VLF Prepared by Morris Cohen and Nader Moussa Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME Network.
Solar Activity and VLF Prepared by Sheila Bijoor and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME.
Characteristics of VLF Tweeks Nedra Tounsi & Hassen Ghalila Laboratoire de Spectroscopie Atomique Moléculaire et Applications 1 In this spectrogram recorded.
Whistlers, Magnetospheric Reflections, and Ducts Prepared by Dan Golden, Denys Piddyachiy, and Naoshin Haque Stanford University, Stanford, CA IHY Workshop.
PARS Workshop on Novel Methods of Excitation of ULF/ELF/VLF to Improve Efficiency and Availability" November 3 - 6, 2002 Sponsored by Air Force Research.
Geospace Variability through the Solar Cycle John Foster MIT Haystack Observatory.
Workshop on Earthquakes: Ground- based and Space Observations 1 1 Space Research Institute, Austrian Academy of Science, Graz, Austria 2 Institute of Physics,
Solar wind-magnetosphere- atmosphere coupling: effects of magnetic storms and substorms in atmospheric electric field variations Kleimenova N., Kozyreva.
General Licensing Class G3A – G3C Radio Wave Propagation Your organization and dates here.
Space Weather Major sources of space weather ● Solar wind – a stream of plasma consisting of high energy charged particles released from the upper atmosphere.
Y. Bouderba, S. Naitamor, O. Boumia Research Center on Astronomy, Astrophysics and Geophysics. CRAAG (Algeria). 1 International School of Space Science,
RADAR Detection of Extensive Air Showers Nils Scharf III. Physikalisches Institut A Bad Honnef Nils Scharf III. Physikalisches Institut A Bad.
Ionospheric-magnetospheric VLF Wave Propagation: RPI/IMAGE-HAARP Correlative Study RPI/IMAGE-HAARP Correlative Study V. Paznukhov, B. Reinisch, G. Sales,
Importance Of Very Low Frequency Radio Signal Data Registered By VLF-receiver System A. Nina, V. Čadež and V. Srećković Institute of Physics, Belgrade,
Effects of ionospheric small- scale structures on GNSS G. WAUTELET Royal Meteorological Institute of Belgium Ionospheric Radio Systems & Techniques (IRST)
Remote Radio Sounding Science For JIMO J. L. Green, B. W. Reinisch, P. Song, S. F. Fung, R. F. Benson, W. W. L. Taylor, J. F. Cooper, L. Garcia, D. Gallagher,
Workshop on Coupling of Thunderstorms and Lightning Discharges to Near-Earth Space June 2008, University of Corsica, Corte in Corsica, France (weekends.
Stanford VLF Remote Sensing Science, Engineering, Educational outreach Morris Cohen Along with Phil Scherrer, Deborah Scherrer, Umran Inan, Ray Mitchell,
A tool to maximize the scientific output of PWI target physics: Intelligent Signal Detector Module J. Lichtenberger (1), P. Steinbach (2) and L. Bodnár.
© TAFE MECAT 2008 Chapter 6(b) Where & how we take measurements.
Electromagnetic and plasma disturbances caused by impact to the ionosphere Valery M. Sorokin Pushkov Institute of Terrestrial Magnetism, Ionosphere and.
NATIONAL INSTITUTE FOR SPACE RESEARCH – INPE/MCT SOUTHERN REGIONAL SPACE RESEARCH CENTER – CRS/CIE/INPE - MCT SOUTHERN SPACE OBSERVATORY– SSO/CRS/CIE/INPE.
On the Role of Electric Field Changes when Calculating Thunderstorm Currents Yu.V. Shlugaev, V.V. Klimenko, E.A. Mareev Institute of Applied Physics RAS,
1 On remote sensing of TLEs by ELF/VLF wave measurements on board a satellite F. Lefeuvre 1, R. Marshall 2, J.L. Pinçon 1, U.S. Inan 2, D. Lagoutte 1,
Whistler Waves and Related Magnetospheric Phenomena
Proposed project on lightning-induced electron precipitation (LEP) Lightning produces VLF waves that propagate globally in the Earth- ionosphere waveguide.
Operational and Scientific Results Obtained from AWESOME Receivers in India: Setup under IHY/UNBSSI Program Rajesh Singh, B. Veenadhari, A.K. Maurya, P.
Extremely-Low-Frequency Whistler-Like Waves Observed at South Pole Station Drastically lower frequency ELF events are found between Hz, as opposed.
Transient response of the ionosphere to X-ray solar flares Jaroslav Chum (1), Jaroslav Urbář (1), Jann-Yenq Liu (2) (1) Institute of Atmospheric Physics,
Stanford VLF Remote Sensing Science, Engineering, Educational outreach Morris Cohen Along with Phil Scherrer, Deborah Scherrer, Umran Inan, Ray Mitchell,
Simulation of Terrestrial Gamma Ray and Neutron Flashes (Small variations of thundercloud dipole moment) L.P. Babich, Е.N. Donskoĭ, A.Y. Kudryavtsev, M.L.
NATIONAL INSTITUTE FOR SPACE RESEARCH – INPE/MCT SOUTHERN REGIONAL SPACE RESEARCH CENTER – CRS/CCR/INPE – MCT FEDERAL UNIVERSITY OF SANTA MARIA - UFSM.
Planetary waves in the equatorial mesosphere and ionosphere measurements Lourivaldo Mota Lima (UEPB) Luciana R. Araújo, Maxwelton F. Silva (UEPB) H. Takahashi,
DETECTING WHISTLERS WITH A VLF ANTENNA LOCATED IN HUMAIN (BELGIUM) S. Ranvier (1), F. Darrouzet (1), H. Lamy (1), J. De Keyser (1) ‏, J. Lichtenberger.
Lee-Anne McKinnell and Mpho Tshisaphungo
The D-region Ionospheric Perturbations Caused by Solar Flares:
Space weather phenomena in the ionosphere and their effect on GNSS
Chapter 8 Antennas Propagation Dave Piersall, N6ORB.
Connecting Earth to Space: NASA Heliophysics Provides Data on how Space Weather Impacts Earth’s Environment Using NASA Van Allen Probes mission data, researchers.
CEDAR Frontiers: Daytime Optical Aeronomy Duggirala Pallamraju and Supriya Chakrabarti Center for Space Physics, Boston University &
Recent progress of WDC for Geophysics, Beijing
Atmospheric and ionospheric parameter variations inferred from sub-ionospheric seismo-electromagnetic VLF/LF observations K. Schwingenschuh1, H. U. Eichelberger1,
IONOSPHERIC PERTURBATIONS INDUCED BY SOLAR X-RAY FLARES
Ionosphere, Magnetosphere and Thermosphere Anthea Coster
R. Bucˇık , K. Kudela and S. N. Kuznetsov
Introduction to Atmospheric Science at Arecibo Observatory
Charles Lin1, Jia-Ting Lin1, Loren Chang2, Yang-Yi Sun2
Climate change in the D-region
Course: Topics in Discharge Phenomena
General Licensing Class
Presentation transcript:

VLF Research in India and setup of AWESOME Receivers B. Veenadhari, Rajesh Singh, P. Vohat and A. Maurya Indian Institute of Geomagnetism, Navi Mumbai, India P. Pant, ARIES, Nainital, Uttrakhand, India A.K. Singh, Physics Department, Banaras Hindu University, Varanasi, India ADVANCING VLF SCIENCE THROUGH THE GLOBAL AWESOME NETWORK, 30-May to 01-Jun 2009, Tunis, Tunisia

Outline of talk Introduction The earlier VLF research work in India, high lights and limitations The motivation of set up of new AWESOME installation and IHY UNBSS initiation Importance of VLF stations, other supported data from multi instrument observatories Initial observations and results of using present VLF AWESOME receivers at India Future plans

Whistlers and VLF emissions: Main whistler mode waves include: Lightning whistlers, Triggered emissions, Hiss, Chorus, etc. Generated either by lightning strikes or by wave-particle interaction in the magnetosphere Whistler Spectrum Whistlers Generated by Lightning Propagate along geomagnetic field line Dispersed By analyzing dispersion curve of the VLF whistler waves, plenty of information about the magnetospheric medium can be obtained viz.: Electron density Total electron content in a flux tube Electric field

How Important are VLF signals in Indian Low latitude region? India is a very interesting location for several reasons like: - conjugate region of the India lies in Indian Ocean less lightning activity expected Also the height of the magnetic field lines (~ 800 km max.) connecting conjugate regions lies in the ionosphere Probable absorption of signals Indian Conjugate Region Not enough VLF activity expected

Even though very interesting records of whistlers/VLF waves at Indian Low latitude locations has been observed like: Whistlers VLF emissions like – continuous and pulsing hiss Periodic emissions Hiss triggered emissions Whistler triggered emissions Hissler, etc . VLF emissions like whistlers is also a class of natural radio phenomena, whose origin is in magnetospheric sources or in man made sources such as VLF transmitters. Generation mechanism of VLF emissions are poorly understood, and they remain the focus of intense research activity.

Importance of source location of VLF signals in low latitude Because of curvature of magnetic field line at low latitude, it is difficult to get down coming whistler mode (WM) wave inside the WM transmission cone As a result, quiet a bit of activity seen at low latitudes may have exited at an ionospheric exit point at some what higher latitudes and then propagated in the Earth-ionosphere waveguide to the observation point Furthermore at low latitude we expect WM waves exciting ionosphere both in the North and South to reach the observation location

VLF Research in India - Status Soon after the usage of whistlers and VLF waves was gaining importance in 1950’s at mid and high latitudes, for the study of ionosphere/magnetosphere VLF research activity In 1963’s at B.H.U., Varanasi First Whistler recording at station Gulmarg (1965-72) (24o N) (Somayajulu et al., 1965) Subsequent stations setup at: Nainital (1970-75) (20o N) Varanasi (1975..) (14o N) (Singh et al., Nature, 1977) Also at: Agra (1980’s), Srinagar (1980’s) and Bhopal (1990’s) These studies have emphasized occurrence & importance of Whistlers/VLF phenomena in low latitude region - Synoptic mode for couple of months every year - Study of naturally occurring phenomena

Some examples of observation Fig. Spectrogram of Hissler (Ref: Singh et al., GRL, 2004) Fig. Spectrogram of Pulsing Hiss

Important observations Different whistlers like short, diffused, multifalsh, multipath, twin synchronized etc Emissions like hiss, pulsing hiss, risers, triggered, periodic, quasi periodic etc were observed at low latitudes of Indian sector (Somayajulu et al., 1972, Singh R P., 1993) Also rare phenomena of hisslers also reported (Singh et al., 2004) Propagation mechanisms are well discussed and good number of review papers published. Used analog Experimental set up consists of T type antenna, pre and main amplifier, magnetic cassette tape recorder. Analyzed on advanced VLF data analysis system (AVDAS) at BHU, varanasi Later used loop antenna was better to avoid back ground noise. Fig. Synchronized Whistler Fig. Low dispersion short Whistler

Main limitations The T type antenna records Ez components of the waves and vertical antennas are heavily masked by local noises compared to loop antenna. All sites used analog systems and single channel Ez measurements which limits the scientific application and interpretation of data. Not possible for direction finding which is essentially considered at mid and high latitude Further traditional system used forbade the use of VLF transmitter signal as there was no facility to monitor those signals. Because of these limitations, probing of D region ionospheric have not been given due attention at low latitudes. The solar flare effects and magnetic storms studies on D region ionosphere have not been possible because of non availability of Narrow band data.

With the association of IHY UNBSS program, a collaboration between Stanford University and Indian Institute of Geomagnetism has made during 2007 Three AWESOME VLF receivers were installed and monitoring natural and sub-ionospheric VLF signals continuously. This will help us in better understanding of VLF wave phenomena in low latitude region The AWESOME receivers are deployed at Dr KS Krishnan Geophysical Research Laboratory, IIG, Allahabad (16.490N), also (in collaboration with) ARIES, Nainital (20.290 N) B.H.U., Varanasi (14.910N)

Experimental Setup: Crossed loop antenna – VLF Receiver installed AWESOME VLF Receiver – Stanford University Narrowband + Broadband VLF data Amplitude and Phase of Transmitter signal Capable of collecting Saves entire VLF signal spectrum Crossed loop antenna – 10 x 10 meter Frequency response – 300 Hz to 47.5 kHz Sampling – 100 kHz 10-microsecond time resolution

Direction Finding (DF) Study by AWESOME Locating the source of observed VLF signals in India was always a problem, because of the absence of Direction Finding measurements. The VLF receiver used was very simple – T-type antenna, pre- and main- amplifiers and a magnetic cassette tape recorder Direction Finding (DF) Study by AWESOME Three Channel - AWESOME can measure X- component (North-South) Y- component (East-West) Ez – Vertical E-field (interested to install at one site at least) Ez measurement is useful for studying near ionospheric exit signal and also to remove 180 degree ambiguity

Under IHY/UNBSSI program Nainital Lat.20.48N Long.153.34E May, 2007 Allahabad Lat.16.49N Long.155.34E March, 2007 Varanasi Lat. 15.41N Long. 156.37E October, 2007 Under IHY/UNBSSI program

VLF receivers sites

Importance of VLF sites Allahabd (16.490N) – multi parameter observatory Digital flux gate magnetometer Digital CADI Ionosonde Air glow optical experiments VHF Scintillation receivers, TEC measurements Search coil magnetometer for ULF observations Nainital (20.290 N) : A high altitude observatory with lower Atmospheric observations, Solar observations are monitored regularly and best location for sprites observations in future Varanasi (14.910N) : The most active group in VLF research in India and very good VLF events were observed in past. Also, Scintillation and TEC measurement experiments are going on.

Matlab codes are developed for data analysis Monitor natural and sub-ionospheric VLF signals continuously with AWESOME receivers. Matlab codes are developed for data analysis VTX NWC JJI 3SA ICV HWU FTA2 DHQ GBR Allahabad Nainital VNS Port Blair, Andaman multi parameter Observatory essential for EQ studies

Data Storage : 250 GB pocket external hard disks are used to store the data at sites and final data is stored in server at IIG head quarters (Mumbai). Objectives: Understand the generation and propagation mechanism of naturally occurring VLF waves in low latitude region. To investigate long-term trends of magnetospheric parameters such as electron density, total electron content in a flux tube and electric fields during quiet and active solar periods. Correlation between VLF wave activity and geomagnetic activity. Remote sensing of the lower ionosphere, lightning and thunderstorms. VLF waves as precursors to Earthquakes.

Sudden Ionospheric Disturbance Electromagnetic effects Solar Flare Detection Cosmic Gamma Rays Chorus Emissions Lightning Whistler waves LEP Events, hurricane studies Early/fast Events Mesospheric lightning discharges Sprites, elves, blue jets, TGFs Sudden Ionospheric Disturbance

Examples of some spectrograms Varanasi Allahabad

Studies in Progress Dynamic spectra of First Whistler recorded at Allahabad on 17 June, 2008 Dynamic spectrograms of tweeks observed simultaneously at Allahabad and at Nainital on 13 June, 2007

Earth quake precursor study for China EQ on 12 May, 2008 Dynamic spectrum of chorus between 0.75 and 3.2 kHz recorded at Allahabad on 12 August 2007 Earth quake precursor study for China EQ on 12 May, 2008 The JJI signals which are received at Indian sites are analyzed during pre and post EQ period

Objectives of Solar Eclipse campaign period: (19 – 25 July, 2009) Study of ionospheric D-region variability i.e. electron density, ionospheric reflection height, etc. Effect of Solar Eclipse on Marine VLF communication by monitoring VLF transmitter signals operated by several countries globally. Special emphasis on VTX – Indian and NWC – Australian transmitters. Since solar eclipse creates nighttime conditions during daytime, an attempt will also be made to record naturally occurring magnetospheric VLF emissions. Such eclipse time emissions will provide opportunity to study the complex VLF emissions generation and propagation mechanism involved in low latitude region.

Location of VLF stations VTX NWC JJI 3SA ICV HWU FTA2 DHQ GBR Allahabad Nainital VNS Location of VLF stations Allahabad (16.040N), Nainital (20.290) and Varanasi (14.910 N) (In Geomagnetic Latitude) Indian VLF Transmitter Australian VLF Transmitter

Future plans Solar Eclipse Time, Lower Ionosphere/Magnetosphere studies using ELF/VLF (30 Hz-30 kHz) waves (19 – 25 July, 2009). Total solar eclipse provides a rare opportunity to study the Electro-Dynamic processes in the D-region of the ionosphere and magnetosphere. As solar cycle 24 is in progress, expecting intense solar flares and geomagnetic storms, best use the supporting data from other multi instruments for campaign periods. Coupling of D, E and F region studies during quiet and disturbed periods. Interested in collaborative studies with other AWESOME VLF community for some event studies or campaign plans.

Thank You for your kind Attention! Allahabad - Site Thank You for your kind Attention!

VLF Presentation at Libya History of VLF studies in India : Earlier work, some Whistlers, tweeks and emission examples, importance of Indian stations Present AWESOME installation and importance of Narrowband data (first study) and reason of choosing ALD, BHU, NAI. VF project initiated during 2007 which low solar activity period, good time to study quite time D region night time electron density variations. Allahabad station, the multi instruments observatory which is useful to supplement other data of gravity waves, pulsation data and Ionosonde to study F and D region coupling (??) Maintaining the VLF stations and storage system of huge VLF data. Developing Matlab codes for various VLF studies Narrowband data especially NWC etc which receive at Indian stations cover the seismological areas like Aandamon, Sumatra and China: pre signatures of Earthquake and any anomalies, new IIG observatory functioning at Andamon. Significance of IIG magnetic data for SFE events and these effects can be seen in Narrowband data, expected good solar flares during high solar activity period. Geomagnetic storms Some typical VLF events noticed during 2007 and 2008 (Details by Dr. Rajesh) Future plan, mention solar eclipse campaign during July 2009

electron precipitation (LEP) Sprites, Elves, Blue jets, etc VTX NWC JJI 3SA ICV HWU FTA2 DHQ GBR Allahabad Nainital VNS Lightning discharges Whistlers ELF/VLF emissions Lightning induced electron precipitation (LEP) Sprites, Elves, Blue jets, etc Solar flares Geomagnetic storms Earthquake precursors etc.

Sources of ELF / VLF waves ELF/VLF waves has various Natural and Artificial origin : Natural sources of ELF/VLF waves: Includes Lightning discharge from thunder storms , volcanic eruptions , dust storm and tornadoes, etc Man Made Sources of ELF and VLF Radio Waves: HF heating Fixed frequency VLF transmitters Nuclear explosions However, on a global basis, by far the most significant source of wave at ELF/VLF is that generated by lightning discharges from thunderstorms. Global Lightning Flash rate ~ 50-100 sec-1 km-2

Introduction: The Earth’s magnetosphere is capable of sustaining wide variety of wave phenomena. These waves are important partly because they influence the behavior of the magnetosphere and partly because they can be used as an experimental tool to investigate the upper atmosphere.   One of the most widely studied wave mode is the whistler mode waves. The aim is to use this as a diagnostic tool for the study of Earths magnetosphere. Whistler mode radiation consists of electromagnetic waves whose upper frequency cutoff is either the local electron plasma frequency (fp) or gyrofrequency (fg), which ever is less (Stix, 1992).

VLF remote sensing of the lower ionosphere: Solar flares Giant cosmic -ray flares Lightning induced electron precipitation (LEP) Effects of lightning discharge Sprites, elves, blue jets, TGFs Source: Neubert T., Science, vol 300, 2003

Subionospheric VLF observations allow the measurement of the D-region of the lower ionosphere, normally not accessible with other instruments. The ambient nighttime electron densities in D-region are typically  1 to 10 el/cc Even the most powerful VHF or HF radar cannot measure the D-region at nighttime - >1000 el/cc for useful echoes Precipitating electrons with >100 keV energy penetrate to altitudes < 85 km, creating secondary ionization therein. The additional ionization produced is typically < 100 el/cc. The reflection height of the VLF waves propagating in the earth ionosphere wave guide is  85 km at night. Amplitude/phase of the VLF signal is highly sensitive to conductivity. VLF radio remote sensing is the technique suited for detection of disturbances in D-region. Subionospheric VLF signals are also helpful in the study of VLF waves as a precursor to earthquakes.

Table 1. The details of ground geomagnetic stations in India. Station/Code Geographic Latitude Longitude Geomagnetic Dip. Latitude Tirunelvelli (TIR) 8.7 N 77.8 E 0.17 S 149.97 E 0.96 Trivandrum (TRD) 8.48 76.95 0.31 S 149.1 0.73 Ettaiyapuram (ETT) 9.17 78.0 0.28 N 150.2 1.54 Kodaikanal (KOD) 10.23 77.47 1.39 N 149.78 2.86 Pondicherry(PON) 11.92 79.92 152.33 4.82 Hyderabad(HYD) 17.42 78.55 8.45 151.5 11.62 Visakhapatnam(VSK) 17.68 83.32 8.34 156.09 11.77 Alibag (ABG) 18.62 72.87 10.17 146.15 13.31 Nagpur(NGP) 21.15 79.08 12.12 152.32 16.20 Ujjain(UJJ) 23.18 75.78 14.43 149.39 18.83 Silchar(SIL) 24.93 92.82 15.02 165.6 20.62 Jaipur (JAI) 26.92 75.80 18.15 149.80 23.48 Sabhawala (SAB) 30.37 77.80 21.41 152.02 27.78 Hanle(HAN) 32.76 78.95 23.69 153.32 30.81

Geomagnetic variations on consecutive days at three magnetic observatories reflecting the solar conditions 10 April 2001 : X2.3 Solar flare (sfe) at 05:25 UT modified the ionospheric current and affected the magnetic field within a few minutes. 11 April : Pre-noon Quiet day condition prevails showing a steady geomagnetic field. 11-12 April : Effect on the ground magnetic variation following the flare and earth directed Halo CME on 10 April, which impacted the earth’s magnetosphere almost 34 hours after the solar burst.