meridional winds and temperatures - uni-leipzig.de · 2013. 7. 10. · meridional circulation in...

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Middle and Upper Atmosphere Research at LIM Middle Atmosphere The middle atmosphere includes the atmospheric region above the tropopause up to the lower thermosphere (10-100 km). The middle atmosphere, mainly through wave coupling, acts as a sensor of lower atmosphere variability. Research at Leipzig mainly aims into two directions: VHF radar wind and temperature measurements at 80-100 km Numerical modeling of the middle and upper atmosphere and its variability due to natural and anthropogenic forcing printed at Rechenzentrum Leipzig poster available on http://www.uni-leipzig.de/~jacobi/docs/WG.pdf Thermosphere/Ionosphere The thermosphere / ionosphere region is mainly forced by solar variability, but also reacts on the variability of lower regions. Research focuses on solar variability, and long-term changes of the thermosphere and ionosphere system. EUV measurements on board ISS, and ionization from measured EUV spectra Planetary waves in ionospheric electron density Lower E-region variability Collm Observatory At Collm, since the 1950 remote sensing instruments are operated especially for the investigation of the upper and middle atmosphere, which form the basis for the middle and upper atmosphere research: - VHF meteor radar - LF receiver - GPS receiver At Collm, also seismic measurements are run by the Institute of Geophysics and Geology of the University of Leipzig. Information and contact: http://www.uni-leipzig.de/~jacobi/collm [email protected] Vertical Coupling Middle and upper atmosphere dynamics is, besides solar forcing, also determined by forcing from below. We look for forcing mechanisms that couple the lower and the upper atmosphere, as well as the neutral and ionized part. Fakultät für Physik und Geowissenschaften Figures show transmitting antenna (right), and transmitter and receiver units (above) of the meteor radar. Left: EUV-TEC index, defined as normalized primary ionization calculated from TIMED SEE solar EUV spectra. Also shown is global total electron content (TEC) and F10.7 solar proxy. The figure below shows energy absorbed by different species. 1985 1990 1995 2000 2005 85 86 87 88 89 90 91 92 93 94 95 96 Year Collm 21-1 UT mean LF nighttime reflection height (km) Right: The equatorial lower ionosphere shows a wave 4 signature (colors), owing to neutral atmosphere dynamcis (contours). The figure shows GPS sporadic E occurrence rates together with satellite temperature anomalies. Figures on the left show zonal (upper panel) and meridional (lower panel) prevailing winds at midlatitudes according to measurements. The zonal mean flow is characterized by mesospheric westerlies in winter and easterlies in summer, and a wind reversal in the lower thermosphere. This reversal is forced by breaking gravity waves that also lead to an equatorward meridional circulation in summer. Figures on the right show mean temperatures and zonal winds according to numerical model results. In the lower panels differences between solar maximum and minimum conditions are shown. Results refer to Northern Hemisphere winter conditions. Left: The figure shows solar EUV fluxes as measured with the SolACES spectrometer on board ISS (see figures below). Left: Long-term measurements of LF reflection heights in the lower ionosphere. The time series show a decadal change due to the 11-year solar cycle. -2 -1 0 1 2 0 3 6 9 12 15 Zonal wind at 90 km (m/s) NAO index r = 0.52 Left: The figure shows mesopause region zonal winds vs. NAO indices. The correlation shows that there is a coupling throughout the winter atmosphere via the strength of the polar vortex. Right: Modulation of gravity waves by planetary wave (yellow lines) shows the same seasonal cycle as planetary wave-type os- cillations (upper line) in the ionosphere do. This shows that the signature of planetary waves in the ionosphere is probably due to modulation of gravity waves. Left: Sporadic E layers in the lower ionosphere (colors) show a semidiurnal signature, which is owing to wind shear variability (contours) in the neutral atmosphere. The figure shows GPS measurements together with Collm radar wind data. The symbols denote the phases of the semidiurnal signature. -180° -150° -120° -90° -60° -30° 30° 60° 90° 120° 150° 180° Longitude 85 90 95 100 105 110 115 120 Height (km) 4/1000 8/1000 12/1000 16/1000 20/1000 Collm Observatory, about 50 km east of Leipzig, was founded in 1932 by Ludwig Weickmann, the former Director of the Geophysical Institute. SolACES 30 60 90 120 150 180 210 240 270 300 330 360 doy 82 84 86 88 90 92 94 96 height (km) -35 m/s -25 m/s -15 m/s -5 m/s 5 m/s 15 m/s 25 m/s 35 m/s 30 60 90 120 150 180 210 240 270 300 330 360 doy 82 84 86 88 90 92 94 96 height (km) -15 m/s -10 m/s -5 m/s 0 m/s 5 m/s 10 m/s 0 3 6 9 12 15 18 21 24 Time (LT) 85 90 95 100 105 110 115 120 Height (km) 10 20 30 40 50 1/1000 2008 2009 2010 2011 2012 1.5x10 -3 2.0x10 -3 2.5x10 -3 3.0x10 -3 16-58 nm flux (Wm -2 ) Year 60 70 80 90 100 110 120 130 140 150 160 170 F10.7 (sfu)

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Page 1: Meridional winds and temperatures - uni-leipzig.de · 2013. 7. 10. · meridional circulation in summer. Figures on the right show mean temperatures and zonal winds according to numerical

Middle and Upper Atmosphere

Research at LIM

Middle Atmosphere

The middle atmosphere includes the atmospheric region above the

tropopause up to the lower thermosphere (10-100 km). The middle

atmosphere, mainly through wave coupling, acts as a sensor of

lower atmosphere variability. Research at Leipzig mainly aims into

two directions:

VHF radar wind and temperature measurements at 80-100 km

Numerical modeling of the middle and upper atmosphere and its

variability due to natural and anthropogenic forcing

printed at Rechenzentrum Leipzig poster available on http://www.uni-leipzig.de/~jacobi/docs/WG.pdf

Thermosphere/Ionosphere

The thermosphere / ionosphere region is mainly forced by solar

variability, but also reacts on the variability of lower regions.

Research focuses on solar variability, and long-term changes of the

thermosphere and ionosphere system.

EUV measurements on board ISS, and ionization from measured

EUV spectra

Planetary waves in ionospheric electron density

Lower E-region variability

Collm Observatory

At Collm, since the 1950 remote sensing instruments are operated

especially for the investigation of the upper and middle atmosphere,

which form the basis for the middle and upper atmosphere

research:

- VHF meteor radar

- LF receiver

- GPS receiver

At Collm, also seismic measurements are run by the Institute of

Geophysics and Geology of the University of Leipzig.

Information and contact: http://www.uni-leipzig.de/~jacobi/collm

[email protected]

Vertical Coupling

Middle and upper atmosphere dynamics is, besides solar forcing,

also determined by forcing from below. We look for forcing

mechanisms that couple the lower and the upper atmosphere, as

well as the neutral and ionized part.

Fakultät für Physik und Geowissenschaften

Figures show transmitting antenna

(right), and transmitter and receiver

units (above) of the meteor radar.

Left: EUV-TEC index, defined as normalized

primary ionization calculated from TIMED

SEE solar EUV spectra. Also shown is global

total electron content (TEC) and F10.7 solar

proxy. The figure below shows energy

absorbed by different species.

1985 1990 1995 2000 200585

86

87

88

89

90

91

92

93

94

95

96

Year

Collm 21-1 UT mean

LF

nig

httim

e r

efle

ctio

n h

eig

ht (k

m)

Right: The equatorial lower ionosphere shows

a wave 4 signature (colors), owing to neutral

atmosphere dynamcis (contours). The figure

shows GPS sporadic E occurrence rates

together with satellite temperature anomalies.

Figures on the left show zonal (upper panel)

and meridional (lower panel) prevailing winds

at midlatitudes according to measurements.

The zonal mean flow is characterized by

mesospheric westerlies in winter and

easterlies in summer, and a wind reversal in

the lower thermosphere.

This reversal is forced by breaking gravity

waves that also lead to an equatorward

meridional circulation in summer.

Figures on the right show mean temperatures

and zonal winds according to numerical model

results.

In the lower panels differences between solar

maximum and minimum conditions are shown.

Results refer to Northern Hemisphere winter

conditions.

Left: The figure shows solar EUV fluxes as

measured with the SolACES spectrometer

on board ISS (see figures below).

Left: Long-term measurements of LF reflection heights

in the lower ionosphere. The time series show a

decadal change due to the 11-year solar cycle.

-2 -1 0 1 20

3

6

9

12

15

Zo

na

l w

ind

at 9

0 k

m (

m/s

)

NAO index

r = 0.52

Left: The figure shows mesopause region zonal

winds vs. NAO indices. The correlation shows

that there is a coupling throughout the winter

atmosphere via the strength of the polar vortex.

Right: Modulation of gravity waves by

planetary wave (yellow lines) shows the same

seasonal cycle as planetary wave-type os-

cillations (upper line) in the ionosphere do.

This shows that the signature of planetary

waves in the ionosphere is probably due to

modulation of gravity waves.

Left: Sporadic E layers in the lower ionosphere

(colors) show a semidiurnal signature, which is

owing to wind shear variability (contours) in the

neutral atmosphere. The figure shows GPS

measurements together with Collm radar wind

data. The symbols denote the phases of the

semidiurnal signature.

-180° -150° -120° -90° -60° -30° 0° 30° 60° 90° 120° 150° 180°

Longitude

85

90

95

100

105

110

115

120

He

igh

t (k

m)

4/1000

8/1000

12/1000

16/1000

20/1000

Collm Observatory, about 50 km east of

Leipzig, was founded in 1932 by Ludwig

Weickmann, the former Director of the

Geophysical Institute.

SolACES

30 60 90 120 150 180 210 240 270 300 330 360

doy

82

84

86

88

90

92

94

96

heig

ht (k

m)

-35 m/s

-25 m/s

-15 m/s

-5 m/s

5 m/s

15 m/s

25 m/s

35 m/s

30 60 90 120 150 180 210 240 270 300 330 360

doy

82

84

86

88

90

92

94

96

heig

ht (k

m)

-15 m/s

-10 m/s

-5 m/s

0 m/s

5 m/s

10 m/s

0 3 6 9 12 15 18 21 24

Time (LT)

85

90

95

100

105

110

115

120

Heig

ht (k

m)

10

20

30

40

50

1/1000

2008 2009 2010 2011 2012

1.5x10-3

2.0x10-3

2.5x10-3

3.0x10-3

16

-58

nm

flu

x (

Wm

-2)

Year

60

70

80

90

100

110

120

130

140

150

160

170

F1

0.7

(sfu

)