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Acoustic-gravity wave Acoustic-gravity wave monitoring monitoring for global atmospheric for global atmospheric studies studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover, Germany 1- CEA / DIF/ DASE, Arpajon, France Infrasound Technology Workshop Bermudas - 2008

Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

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Page 1: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Acoustic-gravity wave monitoringAcoustic-gravity wave monitoringfor global atmospheric studiesfor global atmospheric studies

Elisabeth Blanc1 Alexis Le Pichon1

Lars Ceranna2 Thomas Farges1

2- BGR / B3.11, Hannover, Germany

1- CEA / DIF/ DASE, Arpajon, France

Infrasound Technology Workshop Bermudas - 2008

Page 2: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

OutlineOutline

• Properties of acoustic and gravity waves

• Possibility of gravity wave observations with the IMS stations

• Four years of gravity wave observations in Antarctica

• Effect of wave activity on the infrasound bulletins in polar regions

• Mid latitude gravity waves related to thunderstorm activity

• Possible global atmospheric studies

Page 3: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Acoustic and gravity wavesAcoustic and gravity waves

Acoustic waves: - Frequency higher than the acoustic cut off frequency- Propagation at the sound velocity in the acoustic wave channels of the atmosphere

Gravity waves: - Frequencies lower than the Brunt-Väisälä frequency periods ~ 5 min to hours- Group velocity < sound velocity – group velocity perpendicular to phase velocity- Observed in the different layers of the atmosphere from ground up to the ionosphere - Propagating vertically and horizontally, transporting momentum from their source to their sink

Page 4: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

• Gravity wave at low ad middle latitudes produce a forcing of the stratosphere

• This induces long-lived changes in the stratospheric circulation, leading to fluctuations in the strength of the polar vortex

• These fluctuations move down to the lower stratosphere in high latitude regions with possible effects on the troposphere (Baldwin et al., 2003)

Holton, (1995)

Gravity waves are part of this global system and influence energy exchanges between warm low latitude regions and polar regions

Gravity wave activity and global dynamics

Page 5: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Infrasound observations

Microbarometer MB2000Bandwidth : 0 – 1 kHz (measure absolute pressure)

sensitivity : 2 mPa

Dynamic : 137 dB

Frequency bandwidth of the microbarometer

The sensors are adapted to infrasound measurements.As the filter slope ( MB2000) decrease slowly, gravity wave are also observed with the networkAs the amplitude of gravity waves is very large, this filtering prevent saturation in measurements without suppressing the gravity wave response

Example of spectrum showing gravity wave activity

Page 6: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Example of Gravity Wave event

Gravity wave period : 1 mn to 1 dayWave amplitude at period : ~1 hour : 0.3 Pa Real wave amplitude : 9 Pa or 90 µbar (correction of the filter effect)

January 26th, 2005 - IS27 station

Page 7: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

From West

4 years of gravity wave in Antarctica4 years of gravity wave in Antarctica

Automatic processing for wave periods 8 min to 2h30Seasonal effect (largest amplitudes during Austral winter)

9 Pa (after correction)

Page 8: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Gravity waves velocity

Surface winds

Comparison with surface windsComparison with surface winds

Page 9: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

I27DE

Origin of the Antarctica gravity waves Origin of the Antarctica gravity waves

Comparison of 3 month of GW observations by satellite published by Wu et al., 2006 and microbarometers (June-August 2003)

Page 10: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

- Infrasound bulletins in Antarctica station I27DE and Alaska station I53US (microbaroms)- Strong infrasound amplitude in winter, fluctuations from gravity waves more frequent in Northern hemisphere

Monitoring of the infrasound channel in Arctic and AntarcticaMonitoring of the infrasound channel in Arctic and Antarctica

Seasonal azimuth changes produced by stratospheric winds

2006 anomaly

Page 11: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Ceranna et al., 2007, 2008

Anomaly in the acoustic wave channel in Antarctica Anomaly in the acoustic wave channel in Antarctica during the Austral winter 2006during the Austral winter 2006

Example of observation of large scale event (during one season)

Page 12: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Farges et al, 2005

- Propagation in the acoustic wave channel, frequency dispersion - Signal duration relate to sprite size- Produced by heating T/T ~ 1% at altitude 30 km (Pasko and Snively, 2008)

Acoustic gravity waves from thunderstorms

infrasound from sprites

Mobile infrasound station in France European project CAL (Coupling of Atmospheric Layers)

Page 13: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

01/09/2005

Gravity waves from thunderstormsGravity waves from thunderstorms

5m/s

Page 14: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Thunderstorm of September 1st, 2005

31/08/2005Thunderstorm of September 1st, 2005Gravity waves from thunderstormsGravity waves from thunderstorms

31/08/2005

Page 15: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

02/09/2005Thunderstorm of September 1st, 2005Gravity waves from thunderstormsGravity waves from thunderstorms

02/09/2005

Page 16: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Comparison between infrasound Comparison between infrasound from lightning and gravity waves from lightning and gravity waves

Gravity waves

Infrasound

• Infrasound are followed during all the thunderstorm evolution from SW to NE• At the contrary, gravity waves are observed only in the SW direction, were thunderstorm activity persists in the thunderstorm tail• No observation of gravity waves from distant thunderstorms

Page 17: Acoustic-gravity wave monitoring for global atmospheric studies Elisabeth Blanc 1 Alexis Le Pichon 1 Lars Ceranna 2 Thomas Farges 1 2- BGR / B3.11, Hannover,

Conclusion- The infrasound network is a powerful tool for the global monitoring of the acoustic and gravity waves of the atmosphere

- The acoustic channel monitoring, performed by permanent measurement of infrasound from ocean swell, provide imaging of planetary wave activity, different in the Northern and Southern hemispheres

- Monitoring of gravity waves in polar regions could be used to study the sudden stratospheric warming events (2006 Antarctica anomaly)

- Monitoring of gravity waves in tropical regions could provide the evolution of gravity waves from thunderstorms in tropical regions where measurements are rare. These sources affect the global circulation of the stratosphere

- Infrasound monitoring provides then an image of the atmospheric waves which can significantly contribute to a better knowledge of the dynamics of the atmosphere.