The 2009–2010 fade of Jupiter’s South Equatorial Belt: Vertical cloud structure models and zonal winds from visible imaging
► We present observations of the 2009 fade of Jupiter’s South Equatorial Belt. ► We model the vertical cloud structure changes using HST imaging. ► We measure the unchanged zonal wind profile using high-quality IOPW observations. ► The propagation moves upwards and reaches the highest in June 2010....
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Published in | Icarus (New York, N.Y. 1962) Vol. 217; no. 1; pp. 256 - 271 |
---|---|
Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Amsterdam
Elsevier Inc
2012
Elsevier |
Subjects | |
Online Access | Get full text |
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Abstract | ► We present observations of the 2009 fade of Jupiter’s South Equatorial Belt. ► We model the vertical cloud structure changes using HST imaging. ► We measure the unchanged zonal wind profile using high-quality IOPW observations. ► The propagation moves upwards and reaches the highest in June 2010. ► Density of clouds at ∼1
bar and particle blue reflectivity increases.
The South Equatorial Belt (SEB) of Jupiter is known to alternate its appearance at visible wavelengths from a classical belt-like band most of the time to a short-lived zone-like aspect which is called a “fade” of the belt, hereafter SEBF. The albedo change of the SEB is due to a change in the structure and properties of the clouds and upper hazes. Recent works based on infrared observations of the last SEBF have shown that the aerosol density below 1
bar increased in parallel with the reflectivity change. However, the nature of the change in the upper clouds and hazes that produces the visible reflectivity change and whether or not this reflectivity change is accompanied by a change in the winds at the upper cloud level remained unknown. In this paper we focus in the near ultraviolet to near infrared reflected sunlight (255–953
nm) to address these two issues. We characterize the vertical cloud structure above the ammonia condensation level from Hubble Space Telescope images, and the zonal wind velocities from long-term high-quality images coming from the International Outer Planet Watch database, both during the SEB and SEBF phases. We show that reflectivity changes do not happen simultaneously in this wavelength range, but they start earlier in the most deep-sensing filters and end in 2010 with just minor changes in those sensing the highest particle layers. Our models require a substantial increase of the optical thickness of the cloud deck at 1.0
±
0.4
bar from
τ
cloud
=
6
±
2 in July 2009 (SEB phase) to semiinfinite at visual wavelengths in 2010 (SEBF). Upper tropospheric particles (∼240–1400
mbar) are also required to become substantially reflectant and their single scattering albedo in the blue changes from
ϖ
0
=
0.905
±
0.005 in November 2009 to
ϖ
0
=
0.95
±
0.01 in June 2010. No significant changes were found in the cloud top heights or in the particle density of the tropospheric haze. The disturbance travels from the levels below ∼3
bar to a level about 400
±
100
mbar. We derive an upward velocity of 0.15
±
0.05
cm/s, in agreement with a diffusive process in Jupiter’s upper troposphere requiring a mean eddy coefficient
K
∼
8
×
10
5
cm
2
s
−1. On the other hand, cloud tracking on the IOPW imaging showed no significant changes in the zonal wind profile between the SEB and SEBF stages. As in other visually huge changes in Jupiter’s cloud morphology and structure, the wind profile remains robust, possibly indicating a deeply rooted dynamical regime. |
---|---|
AbstractList | The South Equatorial Belt (SEB) of Jupiter is known to alternate its appearance at visible wavelengths from a classical belt-like band most of the time to a short-lived zone-like aspect which is called a "fade" of the belt, hereafter SEBF. The albedo change of the SEB is due to a change in the structure and properties of the clouds and upper hazes. Recent works based on infrared observations of the last SEBF have shown that the aerosol density below 1bar increased in parallel with the reflectivity change. However, the nature of the change in the upper clouds and hazes that produces the visible reflectivity change and whether or not this reflectivity change is accompanied by a change in the winds at the upper cloud level remained unknown. In this paper we focus in the near ultraviolet to near infrared reflected sunlight (255-953nm) to address these two issues. We characterize the vertical cloud structure above the ammonia condensation level from Hubble Space Telescope images, and the zonal wind velocities from long-term high-quality images coming from the International Outer Planet Watch database, both during the SEB and SEBF phases. We show that reflectivity changes do not happen simultaneously in this wavelength range, but they start earlier in the most deep-sensing filters and end in 2010 with just minor changes in those sensing the highest particle layers. Our models require a substantial increase of the optical thickness of the cloud deck at 1.0+/-0.4bar from tau cloud=6+/-2 in July 2009 (SEB phase) to semiinfinite at visual wavelengths in 2010 (SEBF). Upper tropospheric particles (a arrow right 4240-1400mbar) are also required to become substantially reflectant and their single scattering albedo in the blue changes from [piv]|>0=0.905+/-0.005 in November 2009 to [piv]0=0.95+/-0.01 in June 2010. No significant changes were found in the cloud top heights or in the particle density of the tropospheric haze. The disturbance travels from the levels below a arrow right 43bar to a level about 400+/-100mbar. We derive an upward velocity of 0.15+/-0.05cm/s, in agreement with a diffusive process in Jupiter's upper troposphere requiring a mean eddy coefficient Ka arrow right 48105cm2s-1. On the other hand, cloud tracking on the IOPW imaging showed no significant changes in the zonal wind profile between the SEB and SEBF stages. As in other visually huge changes in Jupiter's cloud morphology and structure, the wind profile remains robust, possibly indicating a deeply rooted dynamical regime. ► We present observations of the 2009 fade of Jupiter’s South Equatorial Belt. ► We model the vertical cloud structure changes using HST imaging. ► We measure the unchanged zonal wind profile using high-quality IOPW observations. ► The propagation moves upwards and reaches the highest in June 2010. ► Density of clouds at ∼1 bar and particle blue reflectivity increases. The South Equatorial Belt (SEB) of Jupiter is known to alternate its appearance at visible wavelengths from a classical belt-like band most of the time to a short-lived zone-like aspect which is called a “fade” of the belt, hereafter SEBF. The albedo change of the SEB is due to a change in the structure and properties of the clouds and upper hazes. Recent works based on infrared observations of the last SEBF have shown that the aerosol density below 1 bar increased in parallel with the reflectivity change. However, the nature of the change in the upper clouds and hazes that produces the visible reflectivity change and whether or not this reflectivity change is accompanied by a change in the winds at the upper cloud level remained unknown. In this paper we focus in the near ultraviolet to near infrared reflected sunlight (255–953 nm) to address these two issues. We characterize the vertical cloud structure above the ammonia condensation level from Hubble Space Telescope images, and the zonal wind velocities from long-term high-quality images coming from the International Outer Planet Watch database, both during the SEB and SEBF phases. We show that reflectivity changes do not happen simultaneously in this wavelength range, but they start earlier in the most deep-sensing filters and end in 2010 with just minor changes in those sensing the highest particle layers. Our models require a substantial increase of the optical thickness of the cloud deck at 1.0 ± 0.4 bar from τ cloud = 6 ± 2 in July 2009 (SEB phase) to semiinfinite at visual wavelengths in 2010 (SEBF). Upper tropospheric particles (∼240–1400 mbar) are also required to become substantially reflectant and their single scattering albedo in the blue changes from ϖ 0 = 0.905 ± 0.005 in November 2009 to ϖ 0 = 0.95 ± 0.01 in June 2010. No significant changes were found in the cloud top heights or in the particle density of the tropospheric haze. The disturbance travels from the levels below ∼3 bar to a level about 400 ± 100 mbar. We derive an upward velocity of 0.15 ± 0.05 cm/s, in agreement with a diffusive process in Jupiter’s upper troposphere requiring a mean eddy coefficient K ∼ 8 × 10 5 cm 2 s −1. On the other hand, cloud tracking on the IOPW imaging showed no significant changes in the zonal wind profile between the SEB and SEBF stages. As in other visually huge changes in Jupiter’s cloud morphology and structure, the wind profile remains robust, possibly indicating a deeply rooted dynamical regime. |
Author | Sanz-Requena, J.F. Sánchez-Lavega, A. Barrado-Izagirre, N. Rojas, J.F. Pérez-Hoyos, S. |
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Keywords | Atmospheres, Dynamics Jupiter, Atmosphere Radiative transfer Wind field Atmospheres Zonal wind Haze Infrared observation Vapor condensation Jupiter planet Reflectivity Ammonia Jupiter Albedo Dynamics Morphology Atmosphere Disturbances Outer planet Aerosols Sunlight Models Optical thickness Solar system |
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Snippet | ► We present observations of the 2009 fade of Jupiter’s South Equatorial Belt. ► We model the vertical cloud structure changes using HST imaging. ► We measure... The South Equatorial Belt (SEB) of Jupiter is known to alternate its appearance at visible wavelengths from a classical belt-like band most of the time to a... |
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SubjectTerms | Astronomy Atmospheres, Dynamics Earth, ocean, space Exact sciences and technology Jupiter, Atmosphere Radiative transfer Solar system |
Title | The 2009–2010 fade of Jupiter’s South Equatorial Belt: Vertical cloud structure models and zonal winds from visible imaging |
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