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The identification of the fluctuation effects related to the turbulence and permanent layers in the

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radio occultation data. V.N.Gubenko and V.E.Andreev ... in different occultation sessions more clearly. ... 28th and 30th sessions of radio occultation. ... – PowerPoint PPT presentation

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Title: The identification of the fluctuation effects related to the turbulence and permanent layers in the


1
The identification of the fluctuation effects
related to the turbulence and permanent layers
in the atmosphere of Venus fromradio occultation
dataV.N.Gubenko and V.E.AndreevInstitute 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 24th and
30th 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 E0(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
61.565.0 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
The coefficients of cross-correlation b? 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? is
where ?(h) ln(E(h)/E0(h)) ?E(h)/E0(h) and
?1(h), ?2(h) are the altitude realizations ?(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) 0.3sin(t43/180) was fitted
to measured dependence, and it is represented for
comparison. The cross-correlation coefficient for
the experimental and model dependences is equal
to b? 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 24th, 28th
and 30th sessions of radio occultation. The
total variances s2 for each sessions are
represented (s2ltlt1 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 s213 0.044. The layers
were not discovered and the total variance s213
was associated with turbulence alone. Taking into
account wavelength dependence s2 ?-7/6, which
takes place for well-developed turbulence, the
total variance in our case (if the layers are
absent and ? 32cm) must be equal to s232
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 24th,
28th and 30th 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 T245246K that is characteristic
for the isothermal atmosphere in the northern
polar region at altitudes of 61-68 km.
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