Wave Coupling Between the Lower Atmosphere and Thermosphere: Solar Cycle Influences 1 Jeffrey M. Forbes 1, Sean L. Bruinsma 2, Maura E. Hagan 3, and Xiaoli.

Slides:



Advertisements
Similar presentations
Introduction to the Ionosphere
Advertisements

1 Ionospheres of the Terrestrial Planets Stan Solomon High Altitude Observatory National Center for Atmospheric Research
Ionosphere Climate Studied by F3 / COSMIC Constellation C. H. Liu Academia Sinica In Collaboration with Tulasi Ram, C.H. Lin and S.Y. Su.
The primary mechanism through which energy and momentum are transferred from the lower atmosphere to the upper atmosphere and ionosphere is through the.
The role of the mean flow and gravity wave forcing in the observed seasonal variability of the migrating diurnal tide. David A. Ortland NorthWest Research.
The Effects of El Niño-Southern Oscillation on Lightning Variability over the United States McArthur “Mack” Jones Jr. 1, Jeffrey M. Forbes 1, Ronald L.
Comparative Dynamics and Aeronomy of the Atmospheres of Earth and Mars Jeffrey M. Forbes Department of Aerospace Engineering Sciences University of Colorado,
Results of an analysis of diurnal and semi-diurnal tides using GPS radio occultation data, done in collaboration with Janet Zeng and Bill Kuo at NCAR.
Upper atmospheric density profiles from the Mars Odyssey Accelerometer: Report on data processing, archiving plans, and scientific analysis Paul Withers.
EQUATORIAL WAVES part 2: Vertical Propagation & the QBO.
Asymmetry Reversal in Solar Acoustic Modes Dali Georgobiani (1), Robert F. Stein (1), Aake Nordlund (2) 1. Physics & Astronomy Department, Michigan State.
Deuterated Methane and Ethane in the Atmosphere of Jupiter Christopher D. Parkinson 1,2, Anthony Y.-T. Lee 1, Yuk L. Yung 1, and David Crisp 2 1 Division.
MGS Accelerometer-derived profiles of Upper Atmospheric Pressures and Temperatures: Similarities, Differences, and Winds Withers, Bougher, and Keating.
Periodic Modulations in Thermospheric Composition by Solar Wind High Speed Streams G. Crowley, A. Reynolds, J. P. Thayer, J. Lei, L.J. Paxton, A.B. Christensen,
Theoretical Simulations of the Martian Ionosphere and Comparisons to Observations (How do thermospheric tides and variations in solar flux affect ionospheric.
The Impact of Composition on the Thermosphere Mass Density during Geomagnetic Activity Jeffrey P. Thayer, Xianjing Lui, Jiuhou Lei, Marcin Pilinski and.
NATS 101 Lecture 2 Vertical Structure of the Atmosphere.
Exosphere Temperature Variability at Earth, Mars and Venus
*K. Ikeda (CCSR, Univ. of Tokyo) M. Yamamoto (RIAM, Kyushu Univ.)
Using GPS data to study the tropical tropopause Bill Randel National Center for Atmospheric Research Boulder, Colorado “You can observe a lot by just watching”
IPPW-9, Toulouse 2012A. Sánchez Hernández, UPC D YNAMICAL STUDY OF THE AEROBRAKING TECHNIQUE IN THE ATMOSPHERE OF M ARS Alberto Sánchez Hernández ETSEIAT.
J. M. Forbes, E. K. Sutton, R. S. Nerem Department of Aerospace Engineering Sciences, University of Colorado, Boulder, Colorado, USA Sean Bruinsma, CNES.
Effect of data gaps: Comparison of different spectral analysis methods Effect of data gaps: Comparison of different spectral analysis methods Catalin Negrea.
Jeff Forbes (CU), Xiaoli Zhang (CU), Sean Bruinsma (CNES), Jens Oberheide (Clemson U), Jason Leonard (CU) 1 Coupling to the Lower Atmosphere, an Observation-Based.
Vertical Wavenumber Spectrum of Gravity Waves at the Northern High Latitude Region in the Martian Atmosphere Hiroki Ando.
Abstract: A simple representative model of the ionosphere of Mars is fit to the complete set of electron density profiles from the Mars Global Surveyor.
Coupling Between the Lower Atmosphere and Thermosphere as Revealed in GOCE and Swarm Accelerometer Measurements Jeffrey M. Forbes, Xiaoli Zhang and Jesse.
Neutral Winds in the Upper Atmosphere Qian Wu National Center for Atmospheric Research.
Scott M. Bailey, LWS Workshop March 24, 2004 The Observed Response of the Lower Thermosphere to Solar Energetic Inputs Scott M. Bailey, Erica M. Rodgers,
MESOSPHERE COUPLING THE ROLE OF WAVES AND TIDES. Spectra show that waves & tides of large amplitude dominate the MLT region A typical power spectrum of.
An assessment of the NRLMSISE-00 density thermosphere description in presence of space weather events C. Lathuillère and M. Menvielle The data and the.
Kelvin Waves as Observed by the SABER Instrument on the TIMED Spacecraft Jeffrey M. Forbes, Xiaoli Zhang, Saburo Miyahara, Scott E. Palo, James Russell,
1 Atmospheric Tides: Linking Deep Tropical Convection to Ionosphere-Thermosphere Variability Briefly discuss migrating vs. non-migrating tides. Demonstrate.
EGU General Assembly 2007 Vienna, Austria, 15 – 20 April Oscillation of Venus’ Upper Atmosphere* Jeffrey M. Forbes Department of Aerospace Engineering.
CEDAR 2007 Student Workshop, June Dynamics of the Thermosphere Jeffrey M. Forbes, University of Colorado
NCAR Advanced Study Program (ASP) Seminar, February 13, Solar Semidiurnal Tide in the Atmosphere Jeff Forbes Department of Aerospace Engineering.
Aerosol distribution and physical properties in the Titan atmosphere D. E. Shemansky 1, X. Zhang 2, M-C. Liang 3, and Y. L. Yung 2 1 SET/PSSD, California,
1 Observations of tides and temperatures in the martian atmosphere by Mars Express SPICAM stellar occultations Paul Withers 1, Jean-Loup Bertaux 2, Franck.
Mattias Mohr, Johan Arnqvist, Hans Bergström Uppsala University (Sweden) Simulating wind and turbulence profiles in and above a forest canopy using the.
Focus Area VIII: Satellite Drag in the Re-Entry Region: Tidal and Longitude Variations in Density Jeff Forbes (CU) and Jens Oberheide (Univ. of Wuppertal)
COSMIC Ionospheric measurements Jiuhou Lei NCAR ASP/HAO Research review, Boulder, March 8, 2007.
Space-based studies of low-latitude ionospheric forcing originating in the lower atmosphere Thomas J. Immel, Scott L. England Space Sciences Laboratory,
Effects of January 2010 stratospheric sudden warming in the low-latitude ionosphere L. Goncharenko, A. Coster, W. Rideout, MIT Haystack Observatory, USA.
5 th GOCE user workshop Aeronomy / Novel applications(1/18) The contribution of GOCE densities to the semi-empirical thermosphere model DTM (Drag Temperature.
Project presentation - Significant parameters for satellite communication.
Impact of midnight thermosphere dynamics on the equatorial ionospheric vertical drifts Tzu-Wei Fang 1,2 R. Akmaev 2, R. Stoneback 3, T. Fuller-Rowell 1,2,
When Lower Atmosphere Waves Invade the Upper Atmosphere
Variations of hydrogen in the thermosphere: nature and causes
Using the Mars climate Database for aerobraking ( km)
End of Semester Groupmeeting
Sensitivity of Orbit Predictions to Density Variability
The Atmosphere.
Atmosphere-Ionosphere Wave Coupling as Revealed in Swarm Plasma Densities and Drifts Jeffrey M. Forbes Department of Aerospace Engineering Sciences, University.
Static Stability in the Global UTLS Observations of Long-term Mean Structure and Variability using GPS Radio Occultation Data Kevin M. Grise David W.
D. E. Shemansky† , J. A. Kammer ‡ , X. Zhang ‡ & Y. L. Yung‡
Mars Climate Sounder observations of wave structure in the North polar middle atmosphere of Mars during the summer season Paulina Wolkenberg1 and John.
Thermosphere-Ionosphere Issues for DASI - I:
The ionosphere is much more structured and variable than ever predicted. Solar Driven Model Since 2000, we have seen more, very clear evidence that the.
Why Should We Care About the Stratosphere?
Study of the sporadic E (Es) layer by GPS radio occultation (RO)
Ionospheric Effect on the GNSS Radio Occultation Climate Data Record
Charles Lin1, Jia-Ting Lin1, Loren Chang2, Yang-Yi Sun2
Section 3: Ocean Movements
Coronal Loop Oscillations observed by TRACE
Tidal Signatures in the Extended Canadian Middle Atmosphere Model
Variation of Protonated Ions and H2 as observed by MAVEN NGIMS
Lower thermosphere factor in formation
The Mars Pathfinder Atmospheric Structure Investigation/Meteorology (ASI/MET) Experiment by J. T. Schofield, J. R. Barnes, D. Crisp, R. M. Haberle, S.
Department of Physics and Astronomy, University of Louisville, KY, USA
NASA’s Global-scale Observations of the Limb and Disk (GOLD) Mission: Unprecedented Imaging of the Boundary Between Earth and Space Richard Eastes GOLD.
Presentation transcript:

Wave Coupling Between the Lower Atmosphere and Thermosphere: Solar Cycle Influences 1 Jeffrey M. Forbes 1, Sean L. Bruinsma 2, Maura E. Hagan 3, and Xiaoli Zhang 1 1 Department of Aerospace Engineering Sciences, University of Colorado Boulder, Colorado, USA 2 Department of Terrestrial and Planetary Geodesy, CNES, Toulouse, France 3 National Center for Atmospheric Research, Boulder, Colorado, USA

Longer vertical wavelength waves more easily penetrate into the thermosphere (2,2) (2,3) (2,4) F 10.7 = 110 Normalized to 1 2 Exponential growth of a vertically-propagating tide ceases (peak occurs) when the time scale for molecular dissipation is of order the wave period: GSWM Simulations, No Winds

* is the ratio of the scale height for increase in dissipation (density) to the vertical scale of the wave: The decrease in amplitude above the peak increases with F 10.7 = 60 F 10.7 = 170      (2,2) Waves often affect the upper thermosphere more during solar minimum 3 GSWM Simulations, No Winds Large means large reflection (Yanowitch, 1967; Lindzen, 1968; 1970)

DE3 = Eastward-Propagating Diurnal Tide with Zonal Wavenumber = 3 SE2 = Eastward-Propagating Semidiurnal Tide with Zonal Wavenumber = 2 Appears as wave-4 longitude structure in a LST = constant reference frame. DE2 = Eastward-Propagating Diurnal Tide with Zonal Wavenumber = 2 SE1 = Eastward-Propagating Semidiurnal Tide with Zonal Wavenumber = 1 Appears as wave-3 longitude structure in a LST = constant reference frame. Reminder! 4

Eastward-Propagating Diurnal Tide with Zonal Wavenumber = 3 (DE3) F 10.7 = 60 F 10.7 = 170 Factor of 4-5 difference in relative density amplitude at 400 km 5

DE3 Texo DE3 density

DE3, similar to (2,4) DE2, similar to (2,3) 7 DE2 Penetrates Into the Thermosphere Much More Efficiently Than DE3

8 Not obvious 180-deg phase differences between day and night, which would occur if the structures were predominantly associated with diurnal tides 1-Week-Mean CHAMP Densities Imply Strong Influence of Semidiurnal Tides Wave-3 character suggests DE2 and SE1 Wave-4 character suggests DE3 and SE2 ( ) Not obvious symmetry about the equator, which would be consistent with DE3; more antisymmetric behavior (SE2)

CONCLUSIONS Long vertical wavelength waves experience exponential growth to a higher altitude in the thermosphere than waves with shorter vertical wavelengths Waves of a given wavelength achieve higher peak amplitudes (and at a higher altitude) during SSMAX than SSMIN However, the profile shape above the peak varies with solar cycle, such that (for a wave of a given wavelength) higher amplitudes are achieved in the upper thermosphere (ca. > 300 km) during solar minimum Solar cycle effects at, e.g., 400 km are much more pronounced for density as opposed to temperature, since the former reflects a height-integrated response to the former. The behavior of the DE3 tide derived from CHAMP measurements is consistent with the above Density observations during 2008 suggest the strong presence of SE2 and SE1 in addition to DE3 and DE2 9