OBSERVING THE IONOSPHERE- THERMOSPHERE-MESOPHERE … · 2019. 11. 21. · Michael Mendillo...

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International School of Space Science (ISSI) The Polar Upper Atmosphere: From Science to Operational Issues, LAquila, Italy, 16-21 Sep. 2018 OBSERVING THE IONOSPHERE- THERMOSPHERE-MESOPHERE SYSTEMby Michael Mendillo Professor of Astronomy Boston University [[email protected]]

Transcript of OBSERVING THE IONOSPHERE- THERMOSPHERE-MESOPHERE … · 2019. 11. 21. · Michael Mendillo...

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International School of Space Science (ISSI)

The Polar Upper Atmosphere: From Science to

Operational Issues, L’Aquila, Italy, 16-21 Sep. 2018

“OBSERVING THE IONOSPHERE-

THERMOSPHERE-MESOPHERE

SYSTEM”

by

Michael Mendillo

Professor of Astronomy

Boston University

[[email protected]]

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MAKING THE IONOSPHERE --- OBSERVING THE IONOSPHERE-THERMOSPHERE-MESOPHERE SYSTEM Mendillo/L’Aquila/2018 2

Observing the Ionosphere

• Satellites

• Sounding Rockets

• Ground-based Radio

• Ground-based Optical

In-situ

Remote Sensing

In-situ

“Active Experiments”

Radars

Trans-ionosphere (SAT Ground; SAT SAT)

Passive (Reception)

Active (Probing)

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MAKING THE IONOSPHERE --- OBSERVING THE IONOSPHERE-THERMOSPHERE-MESOPHERE SYSTEM Mendillo/L’Aquila/20183

NASA’s Space-based Observatories

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Ground-based Ionospheric Measurements – Radio

Plasma frequencies Layer peak densities

[fp (Hz)]2 = 80.5 Ne (m-3)

(from Prölss, ’04)

•Reflection of radiowaves (fHF ~ 3-30 MHz)

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Example of Ionogram

Network of ionosondes

Lowell Digisonde International: www.digisonde.com

INGV: www.eswua.ingv.it/ingv/i_ita.php

(from Hargreaves,’92)

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* Trans-Ionospheric Radiowaves (fVHF ~ 30-300 Mhz)

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Index of refraction (phase):

End result: wave is slowed down by plasma Group Delay

2 2

2

2 21 ; if 1 then

p pn

(Ne in m-3

and f in Hz)

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The effect is cumulative

By measuring total group delay STEC

Equivalent Vertical (for small spatial gradients) TEC

TEC =STEC cos

eN ( ) SLANT TECs ds

From GIM/JPL (http://iono.jpl.nasa.gov/gim.html)

Other sources: MIT Madrigal Database (http://cedar.openmadrigal.org/)

RING: (http://ring.gm.ingv.it/)

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• Back-scattering of Radiowaves

- Incoherent scatter Radars (ISRs)

The transmitted signal returns with a “spread in frequency”ISR spectrum

(Adapted from

Hunsucker, ’91)

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Total power Ne

Physical parameters at each height: Peak/center spectrum Te /Ti

width of spectrum Ti /mi

Data base at MADRIGAL site

(http://madrigal.haystack.mit.edu/madrigal/)

Kwajalein

Poker Flat

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Ionospheric Effects on Technological Systems

Example #1 : GPS signal Amplitude and Phase Scintillations

impact radio communications

Cause: small-scale ionospheric irregularities Ne/<Ne> along raypath

cause diffraction patterns (scale sizes from cm to 10’s km)

Effect: “Loss of Lock” for signal by receiver. Inability to use

GPS reliably for continuous position determinations

(from Beach and Kintner, RS’99)

amplitude

phase

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Example # 2 : Group Delay and Ranging Errors

- In vacuum, R = c x t (Range = speed of light x time)

- For trans-ionospheric radio path , v < c. So R’ = v x t

R = R- R’ “Ranging Error”. R thus depends on Ne along path

TEC (and )

R = 0.403 TEC/f2

where TEC is in TECU (1016 el m-2 ),

f is in GHz, and ΔR is in meters.

TEC can vary between ~ 2 to

200 TECU depending on LT,

LAT, season and solar cycle

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Solutions:

(a) TEC everywhere in real time from GPS receiver networks

(b) TEC from models data assimilation models

Positive Phase

Major concern: TEC during storms

with strong spatial gradients in TEC Negative Phase

“ How far down is the runway?”… “Look out the window !”

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Superdarn

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Optical Aeronomy

(Ground-based & Space-based)

LIDAR

(Light detection and Ranging)

Structures & dynamics in

Mesosphere

Fabry-Perot-Interferometer

(FPI)

Neutral Winds &

Temperatures

Spectrograph

(Brightness vs. Wavelength)

Identifies Species

All-Sky-Imager

(ASI)

Broad spatial patterns of

structures & dynamics

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SU

N

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Where do the Photons come from?

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Contribution of Professor Syun-Ichi Akasofu (1960s)

All-Sky-Imager at single site Global Pattern of Auroral Storms

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Movie

Auroral Oval

Auroral Polar Caps

Images of Aurora

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What does an ASI look like?MAKING THE IONOSPHERE --- OBSERVING THE IONOSPHERE-THERMOSPHERE-MESOPHERE SYSTEM Mendillo/L’Aquila/2018

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Horizon of ASIAGO in different spectral bands

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Red = 6300 Å at 300 km Green = 5577 Å at 100 km ZA = Zenith Angle

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ASIAGO location at Cima Ekar

Location in Juy

1.8m Copernicus

telescope

S767-92 cm Schmidt

telescope

N

E

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Housing

The BU camera is lodged in a small container,

which has been equipped with temperature

and humidity controls, and safety devices.

Two telescopes can be sited inside the

container. The glassy domes are permanently

open. Only occasional maintenance

operations are required by the Observatory

technical staff.

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Example: Formation of SAR Arcs

heat fluxcorotation

Coulomb

collisons

heat fluxheat flux

heat flux

westward

drifting ring

current ions

SAR Arcs

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Sub-Auroral Inner Magnetosphere ScienceSAR Arc from space

SAR Arc from Millstone Hill

[Craven et al., 1980]

A SAR Arc of Visible Brightness

[Foster et al., 1994]

[Baumgardner et al., 2007]

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“Normal” SAR ArcMAKING THE IONOSPHERE --- OBSERVING THE IONOSPHERE-THERMOSPHERE-MESOPHERE SYSTEM Mendillo/L’Aquila/2018

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Networks of All-Sky-Imagers

(ASIs)

for ITM System Science

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3. Sub-auroral Ionosphere (latitudes below auroral ovals). Stable auroral red (SAR) arcs (magnetic activity effects that transfer magnetospheric ring current energy into the I-T system)

1. Equatorial and low latitude Ionosphere (from magnetic equator to the crests of the Appleton Anomaly). ESF and MSTIDs, effects on trans-ionospheric radio signals using GPS and optical diagnosis.

2. Mid latitude Ionosphere (poleward from Anomaly crests to ~ 40 mag lat). Nighttime

MSTIDs, E and F region coupling.

4. Mesospheric Dynamics (above mountains, coastal & oceanic sites)

MAKING THE IONOSPHERE --- OBSERVING THE IONOSPHERE-THERMOSPHERE-MESOPHERE SYSTEM Mendillo/L’Aquila/2018

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MLT Gravity Waves and M-T Dynamical Coupling Processes

Mt. John Observatory, New Zealand 4 March 2009

Secondary thermospheric GW’s in 630.0 nm emission generated

from breaking GW’s in the MLT (Smith et al., 2013 JGR).

•Strong SE-ward waves 9:00-12:30UT Two simul. wave sets

•Weaker NW-ward waves 9:00-10:30UT prop. in opp. dirs.

Clear example of dynamical coupling between mesosphere

and thermosphere.

McDonald Observatory, Texas 14 November 1999

Large mesospheric bore disturbance in the 557.7 nm

emission. Naked–eye visibility (Smith et al., 2003 JGR).

Indicated presence of stable temperature inversion layer

near 90 km altitude spanning over 1100 km.

Mesospheric BoresSecondary GW’s in

Thermosphere

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6300 Å

Images

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6300 Å

Images

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7774 Å

Images

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Summary --- Conjugate Site ASIs

• First network of All-Sky-Imagers poised to

contribute to studies of upper atmosphere

phenomena linked by common electro-dynamical

mechanisms along same geomagnetic field lines

• Upcoming NASA missions (ICON and GOLD) will

focus attention on N-S hemisphere effect with high

resolution provided by ASI networks

• Opportunities for international collaborations.

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All BU imaging data available on website.

Collaborations Welcome!

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Global ITM system Requires Global (Space-based & Ground-based) Observing Networks

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