Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space...

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Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA) www.astraspace.net TIMEGCM: Thermosphere-Ionosphere- Mesosphere-Electrodynamics-General Circulation Model ASPEN: A dvanced SP ace EN vironment Model

Transcript of Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space...

Page 1: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Modeling the Upper Atmosphere and Ionosphere with TIMEGCM

Geoff Crowley

Atmospheric & Space Technology Research Associates (ASTRA)

www.astraspace.net

TIMEGCM: Thermosphere-Ionosphere-Mesosphere-Electrodynamics-General Circulation Model

ASPEN: Advanced SPace ENvironment Model

Page 2: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:
Page 3: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

ASPEN-TIMEGCM

Page 4: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Simulating Mars and EarthSimulating Mars and Earth

Temperatures, Chemistry & Winds

Page 5: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Think I’ll develop another GCM this afternoon

So it’s Easy …….. Right?

Page 6: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Simplified Physics of Upper AtmosphereSimplified Physics of Upper Atmosphere

Composition

Temperature Winds

E-fields

Electron Density

Diffusion Coeffs

Boundary Conds

Chemistry

Joule Heating Particle Heating

Solar EUV Chemical HeatingTides

Gravity Waves

Solar EUV

Page 7: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Important Inputs to the Thermosphere – Ionosphere System

Solar EUV Input

Coupled Thermosphere –Ionosphere-Electrodynamics

Tides and Gravity Waves

High Latitude Inputs

E-fields Particles

Neutral density Composition Temperature Wind Electron densityDynamo E-fields

OUTPUT

Page 8: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Neutral Temperature 12 UT

MODEL - %DIFFERENCE (Storm – Quiet)

MODEL - QUIET - 12UT

MODEL - STORM - 12UT

Page 9: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Meridional Wind 12 UT

MODEL - %DIFFERENCE (Storm – Quiet)

MODEL - QUIET - 12UT

MODEL - STORM - 12UT

Page 10: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

180 magnetometers

3 DMSP satellites

X SuperDARNs

Data Inputs:

Most Realistic High Latitude Inputs

Page 11: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

325 (11/21) 324 (11/20) 323 (11/19) 322 (11/18)

325 (11/21) 324 (11/20) 323 (11/19) 322 (11/18)

325 (11/21) 324 (11/20) 323 (11/19) 322 (11/18)325 (11/21) 324 (11/20) 323 (11/19) 322 (11/18)

325 (11/21) 324 (11/20) 323 (11/19) 322 (11/18)

TIMEGCM+AMIE

Time runs right to left

Page 12: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Vertical Coordinate System

If Zp is the pressure level (usually ranging from –17 to +5), and Po is the base

pressure

P = Po exp (-Zp) (ASPEN has 88 pressure levels; 30 to 600 km)

Density is

= Po exp (-Zp) Mbar / (Kb T), 

where Kb is the Boltzman constant (gas constant / Avogadro number). Units

depend on the choice of Po and Kb. If Kb = 1.38e-16 erg/K then density is in

g/cm3.

Horizontal Coordinates

-87.5S (5) +87.5N latitude ; -180E (5) +180E longitude (72*36 grid points)

Page 13: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

The leap-frog method is employed with vertical thermal conductivity treated implicitly to second order accuracy. This leads to a tridiagonal scheme requiring boundary conditions at the top and bottom of the domain as implied by the differential equation. Advection is treated implicitly to fourth order in the horizontal, second order in the vertical

Energy equation

ppp

e

p

i

po

s

c

Q

Hc

RTTV

c

aT

c

aT

sK

H

1

scp

ge

t

T+

ω−∇⋅−−−⎟

⎠⎞

⎜⎝⎛ ε+

∂∂

∂∂

=∂∂ −

Molecular conduction radiation advection adiab. heating

Many terms

Page 14: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Heating Terms

QEUV EUV (1-1050 Å) (EUVEFF= 5%)

QSRC O2 -Schumann-Runge continuum (1300 -1750 Å)

QSRB O2 -Schumann-Runge bands (1750-2000 Å)

QO3 O3- Lyman a (1215.67 Å)

O3- Hartley, Huggins and Chappuis (203-850 nm)

QO2 O2- Lyman a (1215.67 Å)

O2 Herzberg (2000-2420 Å)

QNC Exothermic neutral-neutral chemistry

(NOX, HOX, OX, CH4, O(1D) quench, CLX)

Atomic O recombination

Heating from O(1D) quenching

QIC Exothermic ion-neutral chemistry

QA Non-Maxwellian auroral electrons (AUREFF= 5%)

QP Photoelectrons (X-rays, EUV, and Night) (EFF=5%)

QEI Collisions between e-, ions and neutrals

QDH 4th order diffusion heating

QGW Gravity Waves

QM Viscous Dissipation

QJ Joule heating

QT Total Heating

Cooling Terms

O(3P) 63 m O(3P) fine structure

NO 5.3 m Nitric Oxide

CO2 15 m Carbon Dioxide

O3 9.6 m Ozone

Km Molecular Conduction

DIFKT Eddy Diffusion Cooling

Dynamical terms

Adiabatic cooling

Horizontal Advection

Vertical Advection

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NEUTRAL GAS HEATING

Page 16: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

50

103

90

Neutral Temperature

120

150

275 km

Figure 2. Diurnal global mean deg K/day

a) b)

Global Mean Heating and Cooling Terms (Solar Min.)

Heating (K/day) Cooling (K/day)Heating (K/day) Cooling (K/day)

150

90

Page 17: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Effect of Season On Heating (SMAX)

SMAX SMAX

Equinox Solstice

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Page 20: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Continuity equation

{ } ( ){ } RSdz

dV

dz

dezK

dz

deL

T

T

m

m

dz

de

dt

d zz125.0

0

N

1z

2

−+Ψ

ω−Ψ∇•−Ψ

+Ψα⎟⎠⎞

⎜⎝⎛τ−=

Ψ −−−

molecular diffusion eddy diffusion Horiz. advection

Vert. adv.

Production

Recombination

The leap-frog method is employed leading to a tridiagonal scheme requiring boundary conditions at the top and bottom of the domain.

Page 21: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Nitrogen Chemistry (Simplified for This Talk)

Each species equation includes horizontal and vertical advection, photo-chemical production and loss, and vertical molecular and eddy diffusion.

Page 22: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:
Page 23: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Neutral Species

The model includes 15 separate neutral species, not counting some excited states which are also tracked.

O, N2, O2, CO2, CO, O3, H, H2, H2O, HO2,

N, NO, NO2, Ar, and He.

Ionized Species

The model includes 6 ion species

O+, N+, O2+, N2

+, NO+, and H+

with ionization primarily from solar EUV and x-rays, together with auroral particles.

Page 24: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Momentum equations

Zonal velocity

Meridional velocity

The Leap frog method is employed with vertical molecular viscosity treated implicitly to second order accuracy. Since the zonal and meridional momentum equations are coupled through Coriolis and off-diagonal ion drag terms, the system reduces to a diagonal block matrix scheme, where (2 x 2) matrices and two component vectors are used at each level. Boundary conditions for the zonal (u) and meridional ( v) wind components are needed at the top and bottom of the model.

GWU + F + u + + t

cosr

g u vu RAYK* ) tan

r

u + (f +

s

u

H

) K+ K(

s

P

eg =

t

uxIxxIxyxxuxy

EM

o

s

λνλλ∂∂

φ−∇⋅−−λ−νλ−φ

∂∂

∂∂

∂∂ rr

GWV+ F + + u z

r

g v RAYK* u) tan

r

u + (f

s

H

)K + K(

s

P

eg =

tIyyIyxxxxy

EM

o

s

φν νλλ−φ∂

∂−ν∇⋅−ν−λ−λ−φ−

∂ν∂

∂∂

∂ν∂ rr

Viscosity (Molecular and Eddy)

Coriolis

gravity wave drag

Pressure gradientsRayleigh friction

ion drag momentum advection

Page 25: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Momentum Forcing Terms

(u,v) = neutral velocity (cm/s)

(ui, vi) = ion velocity (cm/s)

Pressure gradients

f = 2 sin(colatitude) (s-1) part of Coriolis forcing

Molecular viscosity = Km (g/cm/s)

Eddy viscosity (vertical) = DIFKV (g/cm/s)

Momentum advection

GWU, GWV = gravity wave drag

RAYK = Rayleigh friction

λij = ion drag tensor (must have units of s-1)

Page 26: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Balance of Forces

Page 27: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

a) b)

c) d)

Electron Density

NUMERICAL EXPERIMENTS

Electric Potential

Page 28: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Conjugate Enhancements

Page 29: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

MODEL COUPLING #1 MODEL COUPLING #1 ASPEN-IDA3D-AMIE (AIA)ASPEN-IDA3D-AMIE (AIA)

Self-consistently coupled - each output feeding the input of the other.

Each algorithm has strengths that address the weaknesses of others.

Coupled together, a more accurate specification of ionosphere and thermospheric state variables is obtained.

Output: complete, data-driven specification (and prediction) of ionospheric and thermospheric state variables. Particularly:– High latitude conductances– High latitude field aligned currents

(FAI)– High latitude potentials– High latitude Joule heating– Global Electron density, neutral winds,

neutral composition etc.

AMIE

TIMEGCM

IDA4D

Ne

Background Ne

Ne

, Q, E

TIMEGCM-IDA3D-AMIE interaction

FAC

Page 30: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

GUVI Raw GUVI Binned

ASPEN IDA3D/ASPENAMIE

50

0

H

EFFECT OF ADDING IDA4D ELECTRON DENSITY TO TGCM NEUTRALS

Page 31: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

Conductance Affects Field Aligned Conductance Affects Field Aligned Currents from AMIECurrents from AMIE

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TIMEGCM

RCM (inner magnetosphere)

SAMI3 (ionos-plasmasphere)

MODEL COUPLING #2 MODEL COUPLING #2 Extension to Plasmasphere/Inner Magnetos.Extension to Plasmasphere/Inner Magnetos.

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TIMEGCM

RCM (inner magnetosphere)

SAMI3 (ionos-plasmasphere)

MODEL COUPLING #3 MODEL COUPLING #3 Addition of Hydrogen GeocoronaAddition of Hydrogen Geocorona

Hydrogen Geocorona

(2-4 RE)

Page 34: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

TIMEGCM

RCM (inner magnetosphere)

SAMI3 (ionos-plasmasphere)

MODEL COUPLING #4 MODEL COUPLING #4 Coupling to Lower Atmosphere??Coupling to Lower Atmosphere??

Hydrogen Geocorona

(2-4 RE)NOGAPS

http://uap-www.nrl.navy.mil/dynamics/html/nogaps.html

NCEP

Page 35: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

How to Think About About Upper Atmosphere GCMs

• They are numerical laboratories• Can do controlled (numerical) experiments• They approximate reality• Good “first stop” for atmospheric predictions • Useful framework for understanding a system• Useful framework for data analysis, and can be studied for mechanisms• Useful place to test ideas (what if …..)• Necessary first step to space-weather forecasting

Page 36: Modeling the Upper Atmosphere and Ionosphere with TIMEGCM Geoff Crowley Atmospheric & Space Technology Research Associates (ASTRA)  TIMEGCM:

SummaryThermosphere-Ionosphere-Mesosphere-

Electrodynamics-General Circulation Model

30-600 km Fully coupled thermodynamics, chemistry Inputs - tidal, solar, high latitude Outputs

• Neutral: Temp, Wind, Density, Composition• Ionosphere: Electron density, ions (dynamo E-field)

Extensively Validated Various model coupling studies

Provides useful background fields and test-bed e.g. gravity wave propagation