geomagnetic studies (22-33 millihertz) fileHigh-latitude geomagnetic studies (22-33 millihertz) A....

2
High-latitude geomagnetic studies (22-33 millihertz) A. WOLFE*, L.J. LANZEROTTL, C.G. MACLENNAN, and L.V. MEDFORD AT&T Bell Laboratories Murray Hill, New Jersey 07974 Geomagnetic field measurements were initiated at Iqaluit (formerly Frobisher Bay) in the Northwest Territories of Can- ada during July 1985 (Wolfe et al. 1986). This site was selected because it was calculated to be in the conjugate area to the Amundsen-Scott South Pole Station where extensive geomag- netic research has been conducted. The principal scientific ob- jectives are to study the conjugacy of high-latitude magnetic fluctuations observed at Iqaluit and South Pole (L13). In this report, we extend the previous report of Wolfe et al. (1987) and comment upon the conjugacy of the stations for magnetic field fluctuations in the Pc3 (22-33 millihertz) hydromagnetic regime and upon the penetration of hydromagnetic energy deeper into the magnetosphere on the local dayside. Figure 1 shows the antarctic continent mapped in geomag- netic coordinates to the Northern Hemisphere (courtesy of M. Rycroft and R. Greenwald). The locations of Iqaluit (IQ), South Pole (SP), and Green Hill (GH), Rhode Island (a Bell Labora- 1' IL GH - ANTARCTIC CONTINENT GH GREEN HILL IQ IQALUIT (FROBISHER BAY) SP SOUTH POLE tories station at lower latitude near L3), are indicated. Three- axis fluxgate magnetometer measurements were recorded at intervals of 1 second (South Pole), 5 seconds (Iqaluit), and 10 seconds (Green Hill). Local time is nearly equivalent to uni- versal time minus 3.5, 4, and 5 hours at South Pole, Iqaluit, and Green Hill, respectively. Field measurements were made in the geomagnetic north-south (H), east-west (D), and vertical (Z) directions at all three ground sites. Noise levels in all in- struments were 0.2 nanoteslas. Digitization increments were 0.06 nanoteslas provided by 10-bit analog-to-digital converters. Hourly power spectral energy densities were calculated for the H-component fluctuations at the three ground stations for simultaneous data collected from 17 July to 3 August 1985 during 1100-2000 universal time, hours which are geomagnetic local daytime at all three stations. These spectra were inte- grated over several frequency bandwidths within the Pc 3-5 range. The resulting spectral powers (magnetic energies) were compared at the three stations. Figure 2 shows boxplots of the log power ratios South Pole/Iqaluit (upper panel) and Green JULY 17—AUG 3 9 1985 11 12 13 14 15 16 17 18 19 20 1 0 —1 I —2 E^] E^] —3 A. —4 2 I 0 —1 —2 —3 0 I- 4-4 . U 4, in 0 . 2 2 at GH/IQ 2 1 11 12 13 14 15 16 17 18 19 20 UT(h) Figure 1. Locations of Iqaluit (10), South Pole (SP), and Green Hill (GH) in geomagnetic coordinates. The antarctic continent has been mapped to the Northern Hemisphere. * Also affiliated with City University of New York, Brooklyn, New York 11201. Figure 2. Boxplots of the log power (magnetic energy) ratio for the conjugate stations South Pole/Iqaluit (SP/IQ) (upper panel) and Green Hill/Iqaluit (GH/IQ) (lower panel) during local daytime hours. The medians near zero (upper panel) show that comparable powers are generally observed at South Pole and Iqaluit. Log power ratios evident between -3 and -2 (bottom panel) correspond to wave decay lengths between 3 and 4 earth radii (Re). (UT denotes universal time.) 210 ANTARCTIC JOURNAL

Transcript of geomagnetic studies (22-33 millihertz) fileHigh-latitude geomagnetic studies (22-33 millihertz) A....

High-latitudegeomagnetic studies (22-33 millihertz)

A. WOLFE*, L.J. LANZEROTTL,C.G. MACLENNAN, and L.V. MEDFORD

AT&T Bell LaboratoriesMurray Hill, New Jersey 07974

Geomagnetic field measurements were initiated at Iqaluit(formerly Frobisher Bay) in the Northwest Territories of Can-ada during July 1985 (Wolfe et al. 1986). This site was selectedbecause it was calculated to be in the conjugate area to theAmundsen-Scott South Pole Station where extensive geomag-netic research has been conducted. The principal scientific ob-jectives are to study the conjugacy of high-latitude magneticfluctuations observed at Iqaluit and South Pole (L13). In thisreport, we extend the previous report of Wolfe et al. (1987)and comment upon the conjugacy of the stations for magneticfield fluctuations in the Pc3 (22-33 millihertz) hydromagneticregime and upon the penetration of hydromagnetic energydeeper into the magnetosphere on the local dayside.

Figure 1 shows the antarctic continent mapped in geomag-netic coordinates to the Northern Hemisphere (courtesy of M.Rycroft and R. Greenwald). The locations of Iqaluit (IQ), SouthPole (SP), and Green Hill (GH), Rhode Island (a Bell Labora-

1'ILGH

- ANTARCTIC CONTINENTGH GREEN HILLIQ IQALUIT (FROBISHER BAY)SP SOUTH POLE

tories station at lower latitude near L3), are indicated. Three-axis fluxgate magnetometer measurements were recorded atintervals of 1 second (South Pole), 5 seconds (Iqaluit), and 10seconds (Green Hill). Local time is nearly equivalent to uni-versal time minus 3.5, 4, and 5 hours at South Pole, Iqaluit,and Green Hill, respectively. Field measurements were madein the geomagnetic north-south (H), east-west (D), and vertical(Z) directions at all three ground sites. Noise levels in all in-struments were 0.2 nanoteslas. Digitization increments were0.06 nanoteslas provided by 10-bit analog-to-digital converters.

Hourly power spectral energy densities were calculated forthe H-component fluctuations at the three ground stations forsimultaneous data collected from 17 July to 3 August 1985during 1100-2000 universal time, hours which are geomagneticlocal daytime at all three stations. These spectra were inte-grated over several frequency bandwidths within the Pc 3-5range. The resulting spectral powers (magnetic energies) werecompared at the three stations. Figure 2 shows boxplots of thelog power ratios South Pole/Iqaluit (upper panel) and Green

JULY 17—AUG 3 9 1985

11 12 13 14 15 16 17 18 19 20

1

0

—1 I

—2E^] E^]

—3 A.—4

2

I

0

—1

—2

—30I-4-4. U

4,in

0.2

2

atGH/IQ21

11 12 13 14 15 16 17 18 19 20

UT(h)

Figure 1. Locations of Iqaluit (10), South Pole (SP), and Green Hill(GH) in geomagnetic coordinates. The antarctic continent has beenmapped to the Northern Hemisphere.

* Also affiliated with City University of New York, Brooklyn, New York11201.

Figure 2. Boxplots of the log power (magnetic energy) ratio for theconjugate stations South Pole/Iqaluit (SP/IQ) (upper panel) and GreenHill/Iqaluit (GH/IQ) (lower panel) during local daytime hours. Themedians near zero (upper panel) show that comparable powers aregenerally observed at South Pole and Iqaluit. Log power ratiosevident between -3 and -2 (bottom panel) correspond to wavedecay lengths between 3 and 4 earth radii (Re). (UT denotesuniversal time.)

210 ANTARCTIC JOURNAL

Hill/Iqaluit (bottom panel) calculated for the 30- to 45-secondperiod band within the Pc 3 range. Each boxplot shows themedian (line through the boxes), quartiles (upper and lowerboxes around each median), and full extent of data values usedfor each universal time hour. A concentration of these mediansnear zero (upper panel) suggests that comparable powers gen-erally are observed at South Pole and Iqaluit during local day-time, although a one order of magnitude difference in powersis also seen (i.e., 1400 universal time).

One new result in this study is evident in the bottom panelof figure 2. Medians are found to be from —3 to —2 for thelog power ratio of Green Hill results to those at Iqaluit. In otherwords, wave amplitudes (square root of power) at the lowerlatitude station Green Hill are only 10 to 30 times smaller thanwave amplitudes observed at the higher latitude station Iqaluit.These wave amplitude ratios correspond to decay lengths 8 =10 RE! I ln(0.033) 3 R E to as long as 10 RE! ln(0.1) 4RE. Such a high penetration of hydromagnetic energy deepinto the magnetosphere has not been quantitatively under-stood previously. That is, no theoretical calculations have shownsuch long decay lengths. More observational research as well

as theoretical calculations of magnetopause surface wave at-tenuation into the magnetosphere are being pursued. Detailsof this work are contained in a paper in preparation (Wolfe etal. in preparation).

The Division of Polar Programs, U.S. National Science Foun-dation, provided logistics support for the South Pole mea-surements and partial support under grant DPP 86-18074 toNew York City Technical College. We would like to thank C.Lessard for assistance with station maintenance at Iqaluit.

References

Wolfe, A., L.J. Lanzerotti, C.G. Maclennan, and L.V. Medford. 1986.Geomagnetic studies near the magnetospheric cusps. Antarctic Jour-nal of the U.S., 21(5) 277.

Wolfe, A., L.J. Lanzerotti, C.G. Maclennan, and L.V. Medford. 1987.Relationships of high-latitude geomagnetic variations to interpla-netary plasma conditions. Antarctic Journal of the U.S., 22(5), 277-278.

Wolfe, A., C. Uberoi, L.J. Lanzerotti, C.T. Russell, C.G. Maclennanand L.V. Medford. In preparation. Penetration of hydromagneticenergy deep into the magnetosphere.

Ionospheric signatures ofcusp-latitude Pc 3 pulsations

M.J. ENGEBRETSON

Department of PhysicsAugsburg College

Minneapolis, Minnesota 55454

L.J. CAHILL, JR.

School of Physics and AstronomyUniversity of Minnesota

Minneapolis, Minnesota 55455

R.L. ARNOLDY

Institute for the Study of the Earth, Oceans, and SpaceUniversity of New Hampshire

Durham, New Hampshire 03824

It has been well established that many of the disturbancesin the Earth's magnetosphere, such as auroral substorms, area response to variations in the solar wind that continuallysweeps from the Sun past the Earth and other planets. Studiesover the past several years, most recently reviewed by Odera(1986) and Arnoldy et al. (1988), have shown that Pc 3 pul-sations, a class of ultra-low-frequency waves in the Earth'smagnetic field with periods between 15 and 40 seconds, arealso directly related to activity in the solar wind just "up-stream" of the Earth.

We present in this report new observations from South PoleStation, Antarctica, which during certain hours every day is

located under the nominal position of the magnetospheric cleft/cusp region. There has been ample evidence that plasmas frominterplanetary space can penetrate to ionospheric altitudes inthe cusp region (Heikkila and Winningham, 1971). Two earlierpapers based on South Pole data (Engebretson et al. 1986, inpress) noted that large-amplitude, narrowband Pc 3 magneticpulsations occurred at South Pole Station near local magneticnoon when the interplanetary magnetic field was aligned nearthe Earth-Sun direction (low interplanetary magnetic field coneangle). We have now found evidence of these pulsations indata from other South Pole instruments as well.

Observations. Our study compared representative signals frommany of the upper atmospheric monitoring instruments in-stalled at South Pole Station (- 74 degrees geomagnetic lati-tude, near the nominal cusp/cleft position) and McMurdo Station(- 79 degrees geomagnetic latitude):• the University of New Hampshire/University of Minnesota

search coil magnetometers (Taylor et al. 1975),• the University of Maryland riometers,• Boston College photometers, and• Stanford University very-low-frequency radio receivers.

Figure 1 shows stacked waveform plots for a 1-hour period27 April 1986 from several instruments at South Pole Station.From top to bottom are signals from wave magnetometersoriented east-west and north-south, respectively (XBB and YBB),30-megahertz riometer (RI03), 427.8-nanometer wavelengthphotometer (PH02), and 0.5-1.0 kilohertz and 1.0-2.0 kilo-hertz very-low-frequency receivers (VLF1 and VLF2) at SouthPole Station. Wave packets with Pc 3 pulsations are clearlyevident in the top two (magnetic field) panels, for examplebetween 1320 and 1330 universal time, and similar large am-plitude waves are evident in the very-low-frequency signalsshown in the bottom panels. The photometer, sensitive toauroral light generated in the upper ionosphere (including thatcaused by electrons below 1-kiloelectronvolt energy), showsvariations similar to those of the XBB magnetic field sensor

1988 REVIEW 211