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Initial Measurements of Mesospheric Gravity Waves
over McMurdo, Antarctica
Introduction
The ANtarctic Gravity Wave Instrument Network (ANGWIN) is an NSF sponsored
international program designed to develop and utilize a network of gravity wave
observatories using existing and new instrumentation operated at several established
research stations around the continent. The primary goal is to better understand and
quantify large-scale gravity wave climatology and their effects on the upper
atmosphere over Antarctica. ANGWIN currently comprises research measurements
from five nations (U.S., U.K., Australia, Japan, and Brazil) at seven international stations
(see map). Utah State University’s Atmospheric Imaging Lab operates all-sky infrared
and CCD imagers and an Advanced Mesospheric Temperature Mapper (AMTM) imager
at several research stations (Davis, Halley, Rothera, McMurdo, and South Pole). In this
poster we present new measurements of short-period mesospheric gravity waves
imaged from McMurdo Station (77°S, 166°E) on Ross Island. This camera has operated
alongside the University of Colorado Fe Lidar during the past two winter seasons
(March-September 2012, 2013). Here we present image results from the first year.
The OH airglow emissions extend from approximately 0.4-4 µm. The infrared emissions
as shown in blue in the above figure are much stronger in the infrared region (>1 µm)
are used by InGaAs cameras and enable high-quality short-exposure (a few seconds)
imaging of gravity waves under auroral observing conditions. For example the infrared
OH (3,1) band at 1.55 µm is ~70 times brighter than the OH (6,2) band which is a
prominent component of submicron OH emission used for CCD measurements.
Another major advantage of IR OH imaging is that the scattered moonlight spectrum is
much weaker in the IR as shown in the right-hand figure.
Data Reduction Method
Raw images (a) were calibrated using the IR star field. The stars were then removed (b)
and an average image known as a flat-field was created of the entire night and
subtracted from the data images (c). The images were then unwarped and mapped
onto a 350 x 320 km geographic grid as shown in figure (d).
Jonathan R. Pugmire, Mike J. Taylor, Yucheng Zhao, P.-Dominique Pautet
Center for Atmospheric and Space Sciences, Utah State University
All-sky image data were recorded every 10 s with a XX s exposure at McMurdo Station
enabling detailed measurements of individual gravity wave events in the infrared OH
emission layer (~87 km). During the 2012 observing period (March-September, nighttime
hours) at McMurdo over 300 short period (<1 hr) gravity wave events were observed. Gravity
waves were analyzed using well developed Fourier analysis techniques to determine direction
of propagation, horizontal wavelength, and observed horizontal phase speed. The gravity
wave characteristics observed at McMurdo (blue) are contrasted with 3 years of wave
measurements (1100+ wave events) from other sites around the continent: Rothera station
(67° S) in red, and Halley Station (76° S) in green.
IR Imaging
10 20 30 40 50 60 70
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20
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60
80
NumberofEvents
Observed Wavelength (km)
0 10 20 30 40 50 60 70 80 90 100
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NumberofEvents
Observed Phase Speed (m/s)
10 20 30 40 50 60 70
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NumberofEvents
Horizantal Wavelength (km)
0 10 20 30 40 50 60 70 80 90100
0
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NumberofEvents
Observed Phase Speed (m/s)
Halley Station (76° S)
Rothera Station (67° S)
McMurdo Station (77° S)
Polar Plots Showing Distribution of Wave Headings: 2002-2004
Note the strong and consistent westward wave motions
observed each year from Rothera.
Polar Plots Showing Distribution of Wave Headings: 2000, 05-06
Note the strong and consistent ~poleward wave motions
observed each year from Halley [Nielsen et al, 2009 ].
Month by Month Variability In Wave Propagation Headings 2012
A clear change from NW focused propagation during the fall expanding to more isotropic motions during the
winter and later becoming anisotropic with dominant SW motion in the spring can be seen at McMurdo
Station during the 2012 observation season. The strong spring and fall asymmetries both with westward
components of motion strongly suggests localized sources.
Acknowledgements This research was supported by NSF grant ANT-1045356.
References
Nielsen, K. (2006), Climatology and Case Studies of Mesospheric Gravity Waves Observed At High Latitudes, Ph.D. Dissertation,
Utah State University.
Nielsen, K., Taylor, M.J., Hibbins R.E., and Jarvis, M.J. (June 2009), Climatology of short-period mesospheric gravity waves over
Halley, Antarctica (76 S, 27 W), Journal of Atmospheric and Solar-Terrestrial Physics, Vol. 71.
Nielsen, K., Taylor, M. J., Hibbins, R. E., Jarvis, M. J., & Russell, J. M. (2012). On the nature of short‐period mesospheric gravity
wave propagation over Halley, Antarctica. Journal of Geophysical Research: Atmospheres (1984–2012),117(D5).
Taylor, M.J., W.R. Pendleton, Jr, S. Clark, H. Takahashi, D. Gobbi, and R.A. Goldberg (1997). Image measurements of short-period
gravity waves at equatorial latitudes, J. Geophys. Res., 102, 26,283-26,299.
Digital (CCD) imaging systems are regularly used to study
gravity wave properties in the Mesosphere and Lower
Thermosphere (MLT) region (~80-100 km) using well-defined
nighttime airglow emission layers (e.g. Taylor, et al., 1997).
However, moonlight and other sources of light pollution (e.g.
aurora, street lights, etc.) can significantly limit the use of CCD
imagers which are sensitive to light in the visible and near-
infrared spectral range (< 1 µm). Therefore we use new
dfddfdfd
0
5
10
15
0
30
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Aug-Sept
10 20 30 40 50 60
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Horizontal Wavelength (km)
0 10 20 30 40 50 60 70 80 90 100
0
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Observed Phase Speed
Direction of Propagation
Observed Wavelength
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Optical site at Arrival Heights,
McMurdo Station
Sketch illustrating different wave anisotropy
from McMurdo, Halley and Rothera.
South Pole
Halley
Rothera
McMurdo
Polar Plot Showing Distribution
of Wave Headings: 2012
Wave motion is prominent in three
directions, from the Antarctic continent
(polar vortex), from the Ross Sea, and
from the Weddell Sea (which is the
dominant direction observed at Halley).
Distributions of Observed Horizontal Wavelengths
At McMurdo, during the 2012 season the average horizontal wavelength is 22 km with a range of ±10.5 km
(blue). At Rothera, 2006 the average was measured to be 27.6 (range ± 12.3) km (red). At Halley, 2005 the
average was measured to be 27.8 (range ± 10.3) km (green). McMurdo shows a stronger tendency for waves
of shorter wavelength.
Distributions of Wave Parameters
At McMurdo, during the 2012 season the average measured phase speed is 53.3 m/s with a range of ±24.0
m/s (blue). At Rothera the average was 31.7 m/s with a range of ±19.3 m/s (red). At Halley, the average was
observed to be 45.5 m/s with a range of ±18.6 m/s (green).
Summary and Future Work
We have analyzed one year of data to date from McMurdo Station, Antarctica. The results are
the following:
 A large number (300+) of short-period gravity waves observed over McMurdo, Antarctica
enabling the climatology to be investigated.
 Similar magnitude horizontal wave characteristics (wavelength, phase speed) observed
annually at each site although McMurdo does exhibit a large spread of phase speeds.
 The sources of the wave events observed from McMurdo are probably associated with
strong weather systems outside Antarctica (over the Weddell and Ross Seas), with
another source perhaps being the polar vortex.
 Dominant poleward wave propagation observed at Halley Station with strong year to year
consistency. The source of the waves may be similar to those observed at McMurdo, from
convection in the South Atlantic. Evidence for a rotation of the direction of propagation
during the winter season [Nielsen, et al., 2009, 2012].
 Dominant westward wave propagation observed at Rothera Station with strong intra-
annual consistency and no variation during the winter season shows signatures of
mountain waves being created off of the Antarctic Peninsula.
Wavelength (nm)
All-sky InGaAs camera
infrared imaging systems to help mitigate these problems and to enable more detailed
studies at high latitudes. As part of ANGWIN program all-sky observations of the OH
emission (~87 km) were made from McMurdo using an infrared (0.9-1.7 µm) cooled
InGaAs camera.
Map showing ANGWIN sites. McMurdo is highlighted in bold blue. The comparison
sites of Rothera and Halley are highlighted in red and green respectively.
 New measurements have recently been
initiated from the South Pole Station and in
combination with other ANGWIN sites will be
used to investigate pan-Antarctic anisotropy and
wave parameters.
 Ongoing analysis of McMurdo data from 2013
and soon to be available 2014 data will further
clarify the asymmetries in the wave propagation
at this key site for understanding the
climatology of gravity waves observed at
McMurdo.
Moon Spectrum: Note that the intensity of scattered
moonlight is much weaker in the IR region.

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CEDAR2014-McMurdo

  • 1. Initial Measurements of Mesospheric Gravity Waves over McMurdo, Antarctica Introduction The ANtarctic Gravity Wave Instrument Network (ANGWIN) is an NSF sponsored international program designed to develop and utilize a network of gravity wave observatories using existing and new instrumentation operated at several established research stations around the continent. The primary goal is to better understand and quantify large-scale gravity wave climatology and their effects on the upper atmosphere over Antarctica. ANGWIN currently comprises research measurements from five nations (U.S., U.K., Australia, Japan, and Brazil) at seven international stations (see map). Utah State University’s Atmospheric Imaging Lab operates all-sky infrared and CCD imagers and an Advanced Mesospheric Temperature Mapper (AMTM) imager at several research stations (Davis, Halley, Rothera, McMurdo, and South Pole). In this poster we present new measurements of short-period mesospheric gravity waves imaged from McMurdo Station (77°S, 166°E) on Ross Island. This camera has operated alongside the University of Colorado Fe Lidar during the past two winter seasons (March-September 2012, 2013). Here we present image results from the first year. The OH airglow emissions extend from approximately 0.4-4 µm. The infrared emissions as shown in blue in the above figure are much stronger in the infrared region (>1 µm) are used by InGaAs cameras and enable high-quality short-exposure (a few seconds) imaging of gravity waves under auroral observing conditions. For example the infrared OH (3,1) band at 1.55 µm is ~70 times brighter than the OH (6,2) band which is a prominent component of submicron OH emission used for CCD measurements. Another major advantage of IR OH imaging is that the scattered moonlight spectrum is much weaker in the IR as shown in the right-hand figure. Data Reduction Method Raw images (a) were calibrated using the IR star field. The stars were then removed (b) and an average image known as a flat-field was created of the entire night and subtracted from the data images (c). The images were then unwarped and mapped onto a 350 x 320 km geographic grid as shown in figure (d). Jonathan R. Pugmire, Mike J. Taylor, Yucheng Zhao, P.-Dominique Pautet Center for Atmospheric and Space Sciences, Utah State University All-sky image data were recorded every 10 s with a XX s exposure at McMurdo Station enabling detailed measurements of individual gravity wave events in the infrared OH emission layer (~87 km). During the 2012 observing period (March-September, nighttime hours) at McMurdo over 300 short period (<1 hr) gravity wave events were observed. Gravity waves were analyzed using well developed Fourier analysis techniques to determine direction of propagation, horizontal wavelength, and observed horizontal phase speed. The gravity wave characteristics observed at McMurdo (blue) are contrasted with 3 years of wave measurements (1100+ wave events) from other sites around the continent: Rothera station (67° S) in red, and Halley Station (76° S) in green. IR Imaging 10 20 30 40 50 60 70 0 20 40 60 80 NumberofEvents Observed Wavelength (km) 0 10 20 30 40 50 60 70 80 90 100 0 15 30 45 60 75 NumberofEvents Observed Phase Speed (m/s) 10 20 30 40 50 60 70 0 20 40 60 80 NumberofEvents Horizantal Wavelength (km) 0 10 20 30 40 50 60 70 80 90100 0 15 30 45 60 75 NumberofEvents Observed Phase Speed (m/s) Halley Station (76° S) Rothera Station (67° S) McMurdo Station (77° S) Polar Plots Showing Distribution of Wave Headings: 2002-2004 Note the strong and consistent westward wave motions observed each year from Rothera. Polar Plots Showing Distribution of Wave Headings: 2000, 05-06 Note the strong and consistent ~poleward wave motions observed each year from Halley [Nielsen et al, 2009 ]. Month by Month Variability In Wave Propagation Headings 2012 A clear change from NW focused propagation during the fall expanding to more isotropic motions during the winter and later becoming anisotropic with dominant SW motion in the spring can be seen at McMurdo Station during the 2012 observation season. The strong spring and fall asymmetries both with westward components of motion strongly suggests localized sources. Acknowledgements This research was supported by NSF grant ANT-1045356. References Nielsen, K. (2006), Climatology and Case Studies of Mesospheric Gravity Waves Observed At High Latitudes, Ph.D. Dissertation, Utah State University. Nielsen, K., Taylor, M.J., Hibbins R.E., and Jarvis, M.J. (June 2009), Climatology of short-period mesospheric gravity waves over Halley, Antarctica (76 S, 27 W), Journal of Atmospheric and Solar-Terrestrial Physics, Vol. 71. Nielsen, K., Taylor, M. J., Hibbins, R. E., Jarvis, M. J., & Russell, J. M. (2012). On the nature of short‐period mesospheric gravity wave propagation over Halley, Antarctica. Journal of Geophysical Research: Atmospheres (1984–2012),117(D5). Taylor, M.J., W.R. Pendleton, Jr, S. Clark, H. Takahashi, D. Gobbi, and R.A. Goldberg (1997). Image measurements of short-period gravity waves at equatorial latitudes, J. Geophys. Res., 102, 26,283-26,299. Digital (CCD) imaging systems are regularly used to study gravity wave properties in the Mesosphere and Lower Thermosphere (MLT) region (~80-100 km) using well-defined nighttime airglow emission layers (e.g. Taylor, et al., 1997). However, moonlight and other sources of light pollution (e.g. aurora, street lights, etc.) can significantly limit the use of CCD imagers which are sensitive to light in the visible and near- infrared spectral range (< 1 µm). Therefore we use new dfddfdfd 0 5 10 15 0 30 60 90 120 150 180 210 240 270 300 330 0 5 10 15 March-May 0 5 10 15 0 30 60 90 120 150 180 210 240 270 300 330 0 5 10 15 June-July 0 5 10 15 20 25 30 0 30 60 90 120 150 180 210 240 270 300 330 0 5 10 15 20 25 30 Aug-Sept 10 20 30 40 50 60 0 20 40 60 80 NumberofEvents Horizontal Wavelength (km) 0 10 20 30 40 50 60 70 80 90 100 0 5 10 15 NumberofEvents Observed Phase Speed (m/s) Observed Phase Speed Direction of Propagation Observed Wavelength 0 10 20 30 40 0 30 60 90 120 150 180 210 240 270 300 330 0 10 20 30 40 Optical site at Arrival Heights, McMurdo Station Sketch illustrating different wave anisotropy from McMurdo, Halley and Rothera. South Pole Halley Rothera McMurdo Polar Plot Showing Distribution of Wave Headings: 2012 Wave motion is prominent in three directions, from the Antarctic continent (polar vortex), from the Ross Sea, and from the Weddell Sea (which is the dominant direction observed at Halley). Distributions of Observed Horizontal Wavelengths At McMurdo, during the 2012 season the average horizontal wavelength is 22 km with a range of ±10.5 km (blue). At Rothera, 2006 the average was measured to be 27.6 (range ± 12.3) km (red). At Halley, 2005 the average was measured to be 27.8 (range ± 10.3) km (green). McMurdo shows a stronger tendency for waves of shorter wavelength. Distributions of Wave Parameters At McMurdo, during the 2012 season the average measured phase speed is 53.3 m/s with a range of ±24.0 m/s (blue). At Rothera the average was 31.7 m/s with a range of ±19.3 m/s (red). At Halley, the average was observed to be 45.5 m/s with a range of ±18.6 m/s (green). Summary and Future Work We have analyzed one year of data to date from McMurdo Station, Antarctica. The results are the following:  A large number (300+) of short-period gravity waves observed over McMurdo, Antarctica enabling the climatology to be investigated.  Similar magnitude horizontal wave characteristics (wavelength, phase speed) observed annually at each site although McMurdo does exhibit a large spread of phase speeds.  The sources of the wave events observed from McMurdo are probably associated with strong weather systems outside Antarctica (over the Weddell and Ross Seas), with another source perhaps being the polar vortex.  Dominant poleward wave propagation observed at Halley Station with strong year to year consistency. The source of the waves may be similar to those observed at McMurdo, from convection in the South Atlantic. Evidence for a rotation of the direction of propagation during the winter season [Nielsen, et al., 2009, 2012].  Dominant westward wave propagation observed at Rothera Station with strong intra- annual consistency and no variation during the winter season shows signatures of mountain waves being created off of the Antarctic Peninsula. Wavelength (nm) All-sky InGaAs camera infrared imaging systems to help mitigate these problems and to enable more detailed studies at high latitudes. As part of ANGWIN program all-sky observations of the OH emission (~87 km) were made from McMurdo using an infrared (0.9-1.7 µm) cooled InGaAs camera. Map showing ANGWIN sites. McMurdo is highlighted in bold blue. The comparison sites of Rothera and Halley are highlighted in red and green respectively.  New measurements have recently been initiated from the South Pole Station and in combination with other ANGWIN sites will be used to investigate pan-Antarctic anisotropy and wave parameters.  Ongoing analysis of McMurdo data from 2013 and soon to be available 2014 data will further clarify the asymmetries in the wave propagation at this key site for understanding the climatology of gravity waves observed at McMurdo. Moon Spectrum: Note that the intensity of scattered moonlight is much weaker in the IR region.