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The identification of the fluctuation effects related to the turbulence and “permanent” layers in the atmosphere of Venus from radio occultation data V.N.Gubenko.

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Presentation on theme: "The identification of the fluctuation effects related to the turbulence and “permanent” layers in the atmosphere of Venus from radio occultation data V.N.Gubenko."— Presentation transcript:

1 The identification of the fluctuation effects related to the turbulence and “permanent” layers in the atmosphere of Venus from radio occultation data V.N.Gubenko and V.E.Andreev Institute of Radio Engineering and Electronics, Russian Academy of Sciences The scintillations observed in radio waves propagating through the atmosphere of Venus represent an important tool for measuring small-scale irregularities in the atmosphere of this planet. The outstanding feature is the upper region of enhanced scintillations located in the vicinity of 60 km. This upper region was present in the Mariner 5 and 10, Venera 9 and Pioneer Venus occultations. Therefore, it appears to be planetwide. It is assumed now, that the enhanced scintillations are due to the random turbulence in the upper region which is caused by trapped small-scale gravity waves. If the scintillations observed in the different occultations are correlated, then these scintillations may be attributed to the “permanent” layers. The goal of this report is the presentation and cross-correlation analysis related to the amplitude fluctuations of radio waves of the 32cm band in seven sessions of radio occultations of the Venusian atmosphere. The experiments were carried out in the period from October 16 to October 31, 1983, in seven adjacent northern regions with latitudes more than 83° onboard Venera 15 and 16 spacecrafts.

2 Experimental dependences of the field strength on the minimal altitude of the ray in the 24 th and 30 th sessions of radio occultation. The curves in this figure represent typical variations of the normalized amplitude E(h) of the signal versus the altitude h of the ray above the surface of Venus. The smoothed curves in this figure represent the mean variations of the field strength E 0 (h) in the range of altitudes from 58 to 90 km. They were obtained by fitting quadratic altitude functions.

3 Altitude dependences of the normalized fluctuations of the amplitude in the interval 61.5–65.0 km observed in the sounding of two polar regions of the atmosphere (N24 (85.3N, 308.9W) – 23.10.1983; N30 (86.5N, 310.4W) – 25.10.1983). Altitude series have been detrended to show the high correlation between the fluctuations in different occultation sessions more clearly.

4 Table 1 N sessions N24 (85.3N, 308.9W) 23.10.1983 N28 (87.0N, 301.2W) 24.10.1983 N30 (86.5N, 310.4) 25.10.1983 N42 (85.5N, 179.7W) 31.10.1983 N2410.690.60 N280.6910.480.61 N300.600.4810.37 N420.600.610.371 The coefficients of cross-correlation b χ of the amplitude fluctuations in the different sessions of radio measurements in the altitude interval 61.5 – 65.0 km. The coefficient of cross-correlation b χ is: where χ(h) = ln(E(h)/E 0 (h)) ≈ ∆E(h)/E 0 (h) and χ 1 (h), χ 2 (h) are the altitude realizations χ(h) in the different sessions.

5 The averaged time series (solid, irregular curve) of 32 cm band signal amplitudes in the upper region of enhanced scintillations (layered cluster) of the Venus polar atmosphere. The ensemble averages were determined by using three realizations obtained in the 24th, 28th and 30th sessions of radio occultation (October 23, 24 and 25, 1983). The sine function (smooth curve shown superimposed) 0.3*sin(t*43/180) was fitted to measured dependence, and it is represented for comparison. The cross-correlation coefficient for the experimental and model dependences is equal to bχ ≈ 0.8. The scale size in the Venus atmosphere which is correspondent to the time period of the sine function is about 1 km.

6 Observed log-amplitude power spectra for the 24 th, 28 th and 30 th sessions of radio occultation. The total variances σ 2 for each sessions are represented (σ 2 <<1 – weak scintillation theory is applicable). Example for comparison: the Pioneer Venus radio occultation measurements at S-band (13 cm) of the same Venus region (latitude 86.6N, 1978) show that σ 2 13 = 0.044. The layers were not discovered and the total variance σ 2 13 was associated with turbulence alone. Taking into account wavelength dependence σ 2 ~ λ -7/6, which takes place for well-developed turbulence, the total variance in our case (if the layers are absent and λ = 32cm) must be equal to σ 2 32 ≈ 0.018. Indeed, the measured variances by us are much more than predicted ones, that point out on possible layering in the observed region.

7 The averaged log-amplitude power spectrum. The ensemble averages were determined by using three log-amplitude power spectra obtained in the 24 th, 28 th and 30 th sessions of radio occultation (October 23, 24 and 25, 1983). A dotted line with a slope of -4.0 is depicted for comparison.

8 The power spectra of regular part (layers) and random part (turbulence) of log-amplitude scintillations for session N24 (85.3N, 308.9W, 23.10.1983). The power spectrum of random part was obtained by using results of the cross-correlation analysis of data in sessions N24, N28 and N30.

9 Summary and conclusions Inner layering of the upper layer of the Venusian clouds is observed in the northern polar atmosphere. The vertical structure of the small-scale irregularities was identical in three regions at altitudes of 61.5 – 65.0 km sounded on October 23, 24, and 25, 1983. The characteristic “lifetime” of the small-scale structures, during which they remain essentially unchanged and do not disintegrate under the effect 9of different unfavorable factors (atmosphere circulation, turbulence, etc.), exceeds the time interval between the measurements equal to 49 h. In some cases (October 23, 24 and 25), the regular layers observed against the constant background of random turbulence in the upper cloud layer may be distinctly identified by their prevailing contribution (existence of the significant cross-correlation) to the formation of amplitude fluctuations in radio occultation measurements. We believe that the formation of the small-scale layered structures in the polar atmosphere may be associated with phase transitions in the aerosol medium of the upper cloud layer of Venus. From the diagram of the phase state of the sulfuric acid – water system it follows that the temperature of the phase transition from the liquid to solid state for tetrahydrate of sulfuric acid is very close to the temperature T=245–246K that is characteristic for the isothermal atmosphere in the northern polar region at altitudes of 61-68 km.


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