Subionospheric VLF Propagation Modelling During Solar Flare

16
Akel, A. F. ;Raulin,J. -P [1] CRAAM, Centro de Radio astronomia e Astrofísica Mackenzie, Universidade Presbiteriana Mackenzie Subionospheric VLF Propagation Modelling During Solar Flare São Paulo, 03 de Outubro de 2014

Transcript of Subionospheric VLF Propagation Modelling During Solar Flare

Page 1: Subionospheric VLF Propagation Modelling During Solar Flare

Akel, A. F. ;Raulin,J. -P

[1] CRAAM, Centro de Radio astronomia e Astrofísica

Mackenzie, Universidade Presbiteriana Mackenzie

Subionospheric VLF Propagation Modelling During Solar Flare

São Paulo, 03 de Outubro de 2014

Page 2: Subionospheric VLF Propagation Modelling During Solar Flare

Outline � Overview � Quiescente VLF simulations � Estimate of ionospheric parameters � Results � Conclusions

Page 3: Subionospheric VLF Propagation Modelling During Solar Flare

D layer

E layer

For VLF waves , frequencies between 3 – 30 kHz, the ionospheric D region (day) and the Earth’s surface are good electrical conductors and reflecting media.

ωων

ω rp iiN Ω−=−= 11

22 rΩ Conductivity parameter (Wait & Spies, 1964)

)( '

~ Hzr e −Ω β Conductivity gradient β [km-1] (sharpness)

Reference height H′ [km]

Page 4: Subionospheric VLF Propagation Modelling During Solar Flare

Propagation Model LWPC(Long-Wavelength Propagation Capability) �  Geographic position of Transmitter and Receiver �  Frequency and power of Transmitter �  Date �  Ionospheric conductivity profile

Day 𝜒< 90↑𝑜  𝛽=0.3  𝑘𝑚↑−1  ℎ↑′ =74  𝑘𝑚

Noite 𝜒> 99↑𝑜  𝛽=0.5  𝑘𝑚↑−1  ℎ↑′ =87  𝑘𝑚

(Exponential Wait model)

Page 5: Subionospheric VLF Propagation Modelling During Solar Flare

Quiescente VLF simulations To calculate the diurnal variation of signal, we use polynomial functions dependent on the zenith angle for beta and h’ described by McRae and Thomson (2000). We use this polynomial to develop new functions most appropriate geometry of the path.

Page 6: Subionospheric VLF Propagation Modelling During Solar Flare
Page 7: Subionospheric VLF Propagation Modelling During Solar Flare

Solar transients Increases of incoming X-ray fluxes during flares and increasing particle precipitations during geomagnetic storms produce ionization excesses and change of the electrical properties of the lower ionosphere D region. Then changing: β [km-1] H′ [km]. Excesses of ionization can be monitored using the phase of long distance VLF propagating waves

+ 3.7 dB

+ 93º

Page 8: Subionospheric VLF Propagation Modelling During Solar Flare

How to estimate the variation of parameters during solar flare ?

∆∅= 93.↑𝑜     →∆ℎ′−5.9   ±0.1  𝑘𝑚

Using the relationship propuse by Muraoka, Murato e Sato (1977)

∆∅=360 𝑑/𝜆↓𝑜  (1/2𝑅 + 𝜆↓𝑜↑ /16ℎ↓𝑜  )Δℎ′

∆𝜷  ?????

Page 9: Subionospheric VLF Propagation Modelling During Solar Flare

Extraction of Ionospheric parameters

In left hand panel contour plot of amplitude vs. Δℎ ’ and ∆𝛽   and the right-hand panel contour plot of phase amplitude vs. Δℎ ’

and ∆𝛽.

Page 10: Subionospheric VLF Propagation Modelling During Solar Flare
Page 11: Subionospheric VLF Propagation Modelling During Solar Flare

Results

Page 12: Subionospheric VLF Propagation Modelling During Solar Flare

Results

Page 13: Subionospheric VLF Propagation Modelling During Solar Flare

Results

Page 14: Subionospheric VLF Propagation Modelling During Solar Flare

Conclusions Using the simple model for lower ionosphere was possible fitted the VLF amplitude and phase. This work The quiescent model we calculated the parameters for solar flare. The height reference variation estimated was -6.6 km (decrese) and the sharpnessa as 0.1 km-1 (increase). This variations was responsable by increase of electron density in 20 times, at “diunal altitude” (70 km). The next step is find the parameters for other Solar flares allowing evaluate the general effects the increase os ionization by diferentes levels of solar X-ray flux.

Page 15: Subionospheric VLF Propagation Modelling During Solar Flare

Acknowledgments

Page 16: Subionospheric VLF Propagation Modelling During Solar Flare

Obrigado pela atenção

Obrigado pela atenção