1/14 2 nd , URSI Atlantic Radio Science Meeting Gran Canaria, Spain - - PowerPoint PPT Presentation

1 14 2 nd ursi atlantic radio science meeting gran
SMART_READER_LITE
LIVE PREVIEW

1/14 2 nd , URSI Atlantic Radio Science Meeting Gran Canaria, Spain - - PowerPoint PPT Presentation

1/14 2 nd , URSI Atlantic Radio Science Meeting Gran Canaria, Spain 28 May 1 June 2018 Dario Sabbagh (1),(2) , Carlo Scotto (2) , Alessandro Ippolito (2) , Vittorio Sgrigna (1) (1) Universit degli Studi Roma Tre, Dipartimento di Matematica e


slide-1
SLIDE 1

Dario Sabbagh(1),(2), Carlo Scotto(2), Alessandro Ippolito (2), Vittorio Sgrigna(1)

(1) Università degli Studi Roma Tre, Dipartimento di Matematica e Fisica, Via della Vasca Navale 84, I-00146 Roma, Italy (2) Istituto Nazionale di Geofisica e Vulcanologia, Via di Vigna Murata 605, I-00143 Roma, Italy

2nd, URSI Atlantic Radio Science Meeting Gran Canaria, Spain 28 May – 1 June 2018 1/14 dario.sabbagh@ingv.it

slide-2
SLIDE 2

Outline

✓ The Regional Assimilative Three-dimensional Ionospheric Model (RATIM)* 2/14 ✓ Vertical HF radio-sounding data ingestion ✓ Oblique HF radio-sounding data ingestion (new) ✓ Preliminary results over the Japanese-South Korean region

Sabbagh, D., Scotto, C., Sgrigna, V., 2016. A regional adaptive and assimilative three-dimensional ionospheric model.

  • Adv. Space Res. 57 (5), 1241-1257, doi:10.1016/j.asr.2015.12.038.

*

slide-3
SLIDE 3

The adaptive N(h) model

1) NmF2 2) hmF2 3) NmF1 4) B0 5) B1 6) D1 7) NmE 8) hmE 9) hvE 10) dhvE 11) dNvE 12) ymE F region E region 3/14 ✓ Adaptive Ionospheric Profiler (AIP)* applied by Autoscala ✓ 12 free parameters

Scotto, C., 2009. Electron density profile calculation technique for Autoscala ionogram analysis. Adv. Space Res. 44, 756-766. *

slide-4
SLIDE 4

Climatological 3D model

4/14 1) NmF2 2) hmF2 3) NmF1 4) B0 5) B1 6) D1 7) NmE 8) hmE 9) hvE 10) dhvE 11) dNvE 12) ymE foF2 (IRI) → Jones et al. (1962, 1969) Bradley and Dudeney (1973) foF1 (IRI) → DuCharme et al. (1971, 1973) Scotto (2009) B1=3 c dependent variation foE (IRI) → Davies (1990) hmE=110 km (IRI) Mahajan et al. (1997) ymE=15 km (t,j,l) dependence: 3D description of a monthly median ionosphere at specified

  • time
  • region
slide-5
SLIDE 5

Vertical plasma frequency profiles ingestion

✓ Climatological parameter Pibase(j,l) Pi(j,l) = Pibase(j,l) + Pi variation Pi Actual value ✓ Parameters varied ✓ RMSD minimization σ𝑗=1

𝑂tot 𝑔 p[ionos] ℎ 𝑗

− 𝑔

p[model] ℎ 𝑗 2

𝑂tot 5/14

  • 𝑔
  • F2
  • ℎmF2
  • 𝜀ℎvE
  • Δ𝑔
  • F2
  • ΔℎmF2
  • Δ𝜀ℎvE

𝜀ℎvE 𝑔

  • F2

ℎmF2

slide-6
SLIDE 6
  • March 27, 2015, 12:45 UT
  • from Rome (41.8° N, 12.5° E)

and Gibilmanna (40.6° N, 18.0° E) data

Products

✓ 𝑔

p at fixed altitude

6/14 ✓ 𝑔

  • F2

✓ 𝑔

  • F1

height=180 km height=110 km height=300 km

slide-7
SLIDE 7

7/14 ✓ 𝑔

p cross-sectional maps

✓ 𝑔

p(ℎ) profiles and corresponding simulated ionograms

slide-8
SLIDE 8

MUF from oblique radio-soundings

image recognition technique: determination of the MUF through the maximum contrast method 8/14 Maximum Usable Frequency (MUF) p’(MUF) 𝑞′ = 𝑑∆𝑢 𝑔 Oblique Ionogram Automatic Scaling Algorithm (OIASA)*

[1] Ippolito, A., Scotto, C., Francis, M., Settimi, A., Cesaroni, C., 2015. Automatic interpretation of oblique ionograms, Adv. Space Res., 55, 1624–1629. [2] Ippolito, A., Scotto, C., Sabbagh, D., Sgrigna, V., Maher, P., 2016. A procedure for the reliability improvement of the oblique ionograms automatic scaling

  • algorithm. Radio Sci. 51, doi:10.1002/2015RS005919.
slide-9
SLIDE 9

9/14

Eikonal based ray-tracing technique

𝑒 𝑒𝑡 𝑜 𝑡 𝑒Ԧ 𝑠(𝑡) 𝑒𝑡 = ∇𝑜 𝑡 ✓ phase refraction index ✓ differential ray equation 𝑜 Ԧ 𝑠 = 1 − 𝑔

p Ԧ

𝑠 𝑔

2 Τ 1 2

neglecting:

  • Earth’s Magnetic Field
  • collisions

skip distance simulation associated to fixed frequencies simulation of the ground range between the end points of an

  • blique radio-sounding from

the corresponding MUF skip distance ≡ ground range D, when f = MUF

slide-10
SLIDE 10

10/14

RATIM MUF ingestion procedure

  • ∆𝐸 < ∆𝐸t
  • 𝑆𝑁𝑇𝐸 < 𝑆𝑁𝑇𝐸current min

∆𝐸 = |𝐸[real] − 𝐸 MUF | ✓ simplified ionosphere between the transmitter and the receiver same parabolic vertical profile:

  • 𝑂max = 𝑂mF2[midpoint]
  • thickness ∝ 𝐶0[midpoint]

modelled by RATIM further adapting condition ✓ Combined 𝑔

p(ℎ) and MUF ingestion procedure

  • 𝑔

p(ℎ) ingestion

𝑆𝑁𝑇𝐸 minimization testing a number of combination of ∆𝑔

  • F2, ∆ℎmF2, ∆𝜀ℎvE values
  • MUF ingestion

for each iteration: where

  • ℎmax = ℎmF2[midpoint]
slide-11
SLIDE 11

11/14

Data set

✓ Japanese-South Korean region Jeju (33.4° N, 126.3° E), South Korea Icheon (37.1° N, 127.5° E), South Korea Kokubunji (35.7° N, 139.5° E), Japan Icheon (37.1° N, 127.5° E), South Korea 140 cases ↔ measurements K I J 1079 km October 5, 2016 November 3, 2016 November 19, 2016 every 30 min. vertical ionograms recorded at

  • blique ionograms recorded between
slide-12
SLIDE 12

12/14 good degree of adaptability (~0.1 MHz) poor-quality data rejection ability better adaptability for low ∆𝐸t

Preliminary results

  • Tab. 1
  • Tab. 2

✓ all available input data ✓ only validated input data

slide-13
SLIDE 13

Conclusions

13/14 ✓ Improvement of the RATIM ionosonde data assimilation capability, including oblique radio-sounding data (MUF) ✓ Introduction of ionospheric radio-propagation modelling capabilities ✓ Preliminary results in agreement with previous results

  • adaptability (better for low ∆𝐸t)
  • incorrect input data rejection ability (better)
  • promising for automatically retrieving N from oblique ionograms

✓ Too long computational times for the data ingestion ✓ Different parts of the system not yet automatically interconnected need to faster algorithms, and automatic procedures for the real-time application

slide-14
SLIDE 14

Thank you for your attention

  • Dr. Jun-Cheol Mun,

Korean Space Weather Center (KSWC), Jeju, Korea. Acknowledgments:

  • Dr. Terence Bullett and Dr. Justin Mabie,

National Oceanic and Atmospheric Administration (NOAA), Boulder, Colorado.

  • Dr. Takuay Tsugawa,

National Institute of Information and Communications Technology (NICT), Kokobunji, Japan. 14/14

slide-15
SLIDE 15

foF2 [MHz] hmF2 [km] dhvE (night) [km] dhvE (day) [km] min

  • 4.0
  • 150

10

  • 7.5

max 4.0 150 105 40.0 step 0.1 15 5 2.5 # values 81 21 20 20 # combinations 34020 34020 B0

[n] = (-1)n+1 ∙ n ∙ 0.05% ∙ B0[base]

B0 = B0

[N]

n = 0, … N (until the algorithm is able to link the profile consistently with the Reinisch and Huang formulation)