Pub Date : 2024-03-01DOI: 10.1016/j.pss.2024.105866
Barton Paul Levenson
A climate model is developed for Earth climate history simulations or snapshots of possible conditions on Earthlike exoplanets. It includes estimates for shortwave and longwave optical thickness based on data from Venus, Earth, and Mars; expressions for atmospheric shortwave absorption and surface convective heat loss; climate feedbacks due to water vapor, ice-albedo, clouds, and lapse rate; and a new model for planetary and surface albedo which takes account of surface cover, Rayleigh scattering, and differing wavelength fractions due to primary spectral class. While somewhat complex, it is still orders of magnitude faster than full-spectrum methods or radiative-convective convergence. The model can be modified for use with tidally locked planets, and is here applied to Proxima Centauri b as an example.
开发了一个气候模型,用于模拟地球气候历史或类似地球的系外行星的可能状况。它包括基于金星、地球和火星数据的短波和长波光学厚度估算;大气短波吸收和地表对流热损失的表达式;水蒸气、冰-反照率、云和失效率引起的气候反馈;以及一个新的行星和地表反照率模型,该模型考虑了地表覆盖、瑞利散射和主光谱类别引起的不同波长分数。虽然有些复杂,但它仍然比全光谱方法或辐射对流收敛快几个数量级。该模型可以进行修改以用于潮汐锁定行星,在此以比邻半人马座 b 为例进行说明。
{"title":"A comprehensive semigray climate model","authors":"Barton Paul Levenson","doi":"10.1016/j.pss.2024.105866","DOIUrl":"10.1016/j.pss.2024.105866","url":null,"abstract":"<div><p>A climate model is developed for Earth climate history simulations or snapshots of possible conditions on Earthlike exoplanets. It includes estimates for shortwave and longwave optical thickness based on data from Venus, Earth, and Mars; expressions for atmospheric shortwave absorption and surface convective heat loss; climate feedbacks due to water vapor, ice-albedo, clouds, and lapse rate; and a new model for planetary and surface albedo which takes account of surface cover, Rayleigh scattering, and differing wavelength fractions due to primary spectral class. While somewhat complex, it is still orders of magnitude faster than full-spectrum methods or radiative-convective convergence. The model can be modified for use with tidally locked planets, and is here applied to Proxima Centauri b as an example.</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"243 ","pages":"Article 105866"},"PeriodicalIF":2.4,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140043911","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-01DOI: 10.1016/j.pss.2024.105864
Nand Jee Kanu , Eva Gupta , Girish C. Verma
With the mission's completion, India became only the fourth nation in history to successfully perform a soft landing on the Moon and the first nation to land a spacecraft close to the lunar south pole. The purpose of the article is to present a comprehensive review of the Chandrayaan-3 mission (a sequel operation to Chandrayaan-2) to demonstrate complete capabilities in secure lunar landing and exploration on the Moon's surface. It is equipped with a Vikram lander and Pragyan rover. An in-depth review is carried out to discuss the findings of the Chandrayaan-3 mission. The goals of Chandrayaan-3's mission are: (a) to show a safe and soft landing on the surface of the Moon; (b) to showcase roving lunar rover technology; and (c) to carry out in-situ scientific research. The goals are achieved through the lander payloads, which include the Langmuir Probe (LP), Chandra's Surface Thermophysical Experiment (ChaSTE), Instrument for Lunar Seismic Activity (ILSA), and Chandra's Surface Thermophysical Experiment (ChaSTE) to measure thermal conductivity and temperature. For lunar laser-ranging investigations, the space agency NASA has provided a passive Laser Retroreflector Array. The Alpha Particle X-ray Spectrometer (APXS) and the Laser Induced Breakdown Spectroscope (LIBS) are rover payloads that were used to determine the elemental composition close to the landing site. The mission goals are highly accomplished with the successful hop experiment of Vikram on the Chandrayaan-3 mission! As ordered, it raised itself to a height of around 40 cm, turned on its engines, and then made a safe landing between 30 and 40 cm away. To put an end to the controversy, the study finishes with highlights on (a) the significant area of the southernmost polar region of the Moon with latitudes ranging from 60 to 90°S and (b) Shiv Shakti point (coordinates 69.373°S 32.319°E).
{"title":"An insight into India's Moon mission – Chandrayan-3: The first nation to land on the southernmost polar region of the Moon","authors":"Nand Jee Kanu , Eva Gupta , Girish C. Verma","doi":"10.1016/j.pss.2024.105864","DOIUrl":"10.1016/j.pss.2024.105864","url":null,"abstract":"<div><p>With the mission's completion, India became only the fourth nation in history to successfully perform a soft landing on the Moon and the first nation to land a spacecraft close to the lunar south pole. The purpose of the article is to present a comprehensive review of the Chandrayaan-3 mission (a sequel operation to Chandrayaan-2) to demonstrate complete capabilities in secure lunar landing and exploration on the Moon's surface. It is equipped with a Vikram lander and Pragyan rover. An in-depth review is carried out to discuss the findings of the Chandrayaan-3 mission. The goals of Chandrayaan-3's mission are: (a) to show a safe and soft landing on the surface of the Moon; (b) to showcase roving lunar rover technology; and (c) to carry out in-situ scientific research. The goals are achieved through the lander payloads, which include the Langmuir Probe (LP), Chandra's Surface Thermophysical Experiment (ChaSTE), Instrument for Lunar Seismic Activity (ILSA), and Chandra's Surface Thermophysical Experiment (ChaSTE) to measure thermal conductivity and temperature. For lunar laser-ranging investigations, the space agency NASA has provided a passive Laser Retroreflector Array. The Alpha Particle X-ray Spectrometer (APXS) and the Laser Induced Breakdown Spectroscope (LIBS) are rover payloads that were used to determine the elemental composition close to the landing site. The mission goals are highly accomplished with the successful hop experiment of Vikram on the Chandrayaan-3 mission! As ordered, it raised itself to a height of around 40 cm, turned on its engines, and then made a safe landing between 30 and 40 cm away. To put an end to the controversy, the study finishes with highlights on (a) the significant area of the southernmost polar region of the Moon with latitudes ranging from 60 to 90°S and (b) Shiv Shakti point (coordinates 69.373°S 32.319°E).</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"242 ","pages":"Article 105864"},"PeriodicalIF":2.4,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140010343","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-06DOI: 10.1016/j.pss.2024.105853
Anthony B. Davis , Kevin H. Baines , Brian M. Sutin , James A. Cutts , Leonard I. Dorsky , Paul K. Byrne
We use a customized radiative transfer model to show that sharp (10 m resolution) images of the Venus surface can be achieved at night in spectral windows free of CO absorption found between 1.0 and using a camera at 47 km altitude, just below the planet’s optically thick clouds. This is in spite of the Rayleigh scattering by the dense but still semi-transparent lower atmosphere, and the potential for underlying hazes beneath the clouds. The thermal radiation transmitted directly to the camera forms images of spatially varying surface emissivity and/or temperature at the native sensor resolution, platform stability permitting and under reasonable seeing conditions. Near-isotropic Rayleigh scattering dominates in the window. Combined with near-Lambertian reflections off the base of the cloud layer, the diffuse light field builds up a background radiance from surface emission averaged spatially out to several 10s of km, i.e., beyond the camera’s field-of-view. At the longer wavelengths (1.1 and windows), the sub-cloud atmosphere itself partially absorbs (hence less direct light), and therefore weakly emits (hence more background light), but the rapidly decreasing Rayleigh scattering compensates and contrast is maintained. In all cases, we demonstrate that the directly-transmitted surface-leaving radiance from the native sensor resolution element (10 m) is a significant fraction of the total radiance, and thus can be detected above the background light. Extending down to the 0.85 and spectral windows, there is less direct and more background due to the enhanced Rayleigh scattering, but the resulting reduction in contrast can be mitigated by co-adding the 10 m pixels. This technological advance will open a new era in Venusian geology by enabling discrimination between different surface materials at fine scales. Moreover, potentially active volcanism on our sister planet may be revealed by surface spots that are much hotter than their surroundings.
{"title":"Feasibility of high-spatial-resolution nighttime near-IR imaging of Venus’ surface from a platform just below the clouds: A radiative transfer study accounting for the potential of haze","authors":"Anthony B. Davis , Kevin H. Baines , Brian M. Sutin , James A. Cutts , Leonard I. Dorsky , Paul K. Byrne","doi":"10.1016/j.pss.2024.105853","DOIUrl":"https://doi.org/10.1016/j.pss.2024.105853","url":null,"abstract":"<div><p>We use a customized radiative transfer model to show that sharp (<span><math><mo>∼</mo></math></span>10 m resolution) images of the Venus surface can be achieved at night in spectral windows free of CO<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> absorption found between 1.0 and <span><math><mrow><mn>1</mn><mo>.</mo><mn>2</mn><mspace></mspace><mi>μ</mi><mi>m</mi></mrow></math></span> using a camera at 47 km altitude, just below the planet’s optically thick clouds. This is in spite of the Rayleigh scattering by the dense but still semi-transparent lower atmosphere, and the potential for underlying hazes beneath the clouds. The thermal radiation transmitted directly to the camera forms images of spatially varying surface emissivity and/or temperature at the native sensor resolution, platform stability permitting and under reasonable seeing conditions. Near-isotropic Rayleigh scattering dominates in the <span><math><mrow><mn>1</mn><mo>.</mo><mn>0</mn><mspace></mspace><mi>μ</mi><mi>m</mi></mrow></math></span> window. Combined with near-Lambertian reflections off the base of the cloud layer, the diffuse light field builds up a background radiance from surface emission averaged spatially out to several 10s of km, i.e., beyond the camera’s field-of-view. At the longer wavelengths (1.1 and <span><math><mrow><mn>1</mn><mo>.</mo><mn>18</mn><mspace></mspace><mi>μ</mi><mi>m</mi></mrow></math></span> windows), the sub-cloud atmosphere itself partially absorbs (hence less direct light), and therefore weakly emits (hence more background light), but the rapidly decreasing Rayleigh scattering compensates and contrast is maintained. In all cases, we demonstrate that the directly-transmitted surface-leaving radiance from the native sensor resolution element (<span><math><mo>∼</mo></math></span>10 m) is a significant fraction of the total radiance, and thus can be detected above the background light. Extending down to the 0.85 and <span><math><mrow><mn>0</mn><mo>.</mo><mn>90</mn><mspace></mspace><mi>μ</mi><mi>m</mi></mrow></math></span> spectral windows, there is less direct and more background due to the enhanced Rayleigh scattering, but the resulting reduction in contrast can be mitigated by co-adding the <span><math><mo>∼</mo></math></span>10 m pixels. This technological advance will open a new era in Venusian geology by enabling discrimination between different surface materials at fine scales. Moreover, potentially active volcanism on our sister planet may be revealed by surface spots that are much hotter than their surroundings.</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"242 ","pages":"Article 105853"},"PeriodicalIF":2.4,"publicationDate":"2024-02-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139726307","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The surface of Mars preserves a variety of structural and geomorphic features such as wrinkle ridges, graben, lobate scarps, impact basins, paleochannels etc., which owe their origin to endogenic processes of deformation as well as meteorite impacts. Graben, which form in extensional stress regimes, are one of the most common structural features identified on these planetary bodies. Many graben are observed in the Margaritifer Terra, a Noachian (4.1 Ga to 3.7 Ga) highland terrain in the southern hemisphere of Mars; but a detailed structural study of these graben have not been carried out so far. The diverse geomorphology of these graben such as their orientation, planform and disposition make the region interesting for structural geological studies. With an aim to unveil the causes behind the formation of these graben, detailed morphometric analyses, estimation of maximum displacement of the faults, and extension across them (ranging between ∼0.3 and ∼0.8 km), as well as age estimation (minimum ∼1 Ga to maximum ∼3.8 Ga) and correlation with the stratigraphic units are carried out on eleven prominent graben in the Margaritifer Terra. The graben belong to two age clusters: 1) late Noachian–early Hesperian and 2) Amazonian. The age-depth correlation, proximity to chaos and floor-fractured craters, absence of any dominant geographic trend and presence of circular graben together indicate that the graben were formed due to dike emplacement in the area in two distinct phases separated by about 2 Ga. Older graben were formed above dike tops at greater depth (>50 km below the surface) while dikes below the younger graben reached shallower levels (∼4 km below the surface) below the surface. The intrusive activities are local to the Margaritifer Terra region and were possibly not caused by Tharsis and Valles Marineris related deformation.
火星表面保留了各种结构和地貌特征,如皱脊,地堑,叶状疤痕,撞击盆地,古河道等,这些特征的形成源于内源变形过程和陨石撞击。在伸展应力机制中形成的地堑是这些行星体上最常见的结构特征之一。在火星南半球的诺亚纪(4.1 Ga 到 3.7 Ga)高原地形 Margaritifer Terra 中观察到许多地堑,但迄今为止尚未对这些地堑进行详细的结构研究。这些地堑的不同地貌,如走向、平面形态和布局,使该地区成为结构地质研究的热点。为了揭示这些地堑形成的原因,我们对 Margaritifer Terra 地区的 11 条主要地堑进行了详细的形态计量分析、断层最大位移估算、断层延伸(0.3 至 0.8 千米)、年龄估算(最小 1 Ga 至最大 3.8 Ga)以及与地层单元的相关性研究。这些地堑属于两个时代群:1)晚新元古代-早黑斯佩尔元古代;2)亚马逊元古代。年龄-深度的相关性、与混沌陨石坑和地面断裂陨石坑的邻近性、没有任何主要的地理趋势以及圆形地堑的存在共同表明,这些地堑是由于该地区的堤坝堆积而形成的,分为两个不同的阶段,相距约 2 Ga。年代较早的地堑形成于地表以下较深的堤顶之上(距地表 50 公里),而年代较晚的地堑之下的堤顶则位于地表以下较浅的位置(距地表 4 公里)。这些侵入活动是 Margaritifer Terra 地区的局部活动,可能不是由与 Tharsis 和 Valles Marineris 有关的变形引起的。
{"title":"Structural study of graben within the Margaritifer Terra region of Mars","authors":"Supratik Basu, Ashmita Dasgupta, Abhik Kundu, Dipayan Dasgupta","doi":"10.1016/j.pss.2024.105840","DOIUrl":"10.1016/j.pss.2024.105840","url":null,"abstract":"<div><p><span><span>The surface of Mars preserves a variety of structural and geomorphic features such as wrinkle ridges, graben, lobate scarps, impact basins, </span>paleochannels etc., which owe their origin to endogenic processes of deformation as well as </span>meteorite impacts<span><span>. Graben, which form in extensional stress regimes, are one of the most common structural features identified on these planetary bodies<span>. Many graben are observed in the Margaritifer Terra, a Noachian (4.1 Ga to 3.7 Ga) highland terrain in the southern hemisphere of Mars; but a detailed structural study of these graben have not been carried out so far. The diverse </span></span>geomorphology<span><span> of these graben such as their orientation, planform and disposition make the region interesting for structural geological studies. With an aim to unveil the causes behind the formation of these graben, detailed morphometric analyses, estimation of maximum displacement of the faults, and extension across them (ranging between ∼0.3 and ∼0.8 km), as well as age estimation (minimum ∼1 Ga to maximum ∼3.8 Ga) and correlation with the stratigraphic units are carried out on eleven prominent graben in the Margaritifer Terra. The graben belong to two age clusters: 1) late Noachian–early Hesperian and 2) Amazonian. The age-depth correlation, proximity to chaos and floor-fractured craters, absence of any dominant geographic trend and presence of circular graben together indicate that the graben were formed due to </span>dike emplacement in the area in two distinct phases separated by about 2 Ga. Older graben were formed above dike tops at greater depth (>50 km below the surface) while dikes below the younger graben reached shallower levels (∼4 km below the surface) below the surface. The intrusive activities are local to the Margaritifer Terra region and were possibly not caused by Tharsis and Valles Marineris related deformation.</span></span></p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105840"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139579523","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.pss.2024.105850
S. Alan Stern , Silvia Protopapa , Matthew Freeman , Joel Wm. Parker , Mark Tapley , Darryl Z. Seligman , Caden Andersson
The first discoveries of Interstellar Objects (ISOs), i.e., small bodies moving through our Solar System on high-speed hyperbolic orbits, occurred in 2017 and 2019, decades after ISOs were first predicted. The scientific value of ISOs is high, as they represent samples, most likely planetesimals, from other solar systems. A significant increase in the rate of ISO discoveries is expected in the late 2020s and in the 2030s owing to the advent of several new observing capabilities enabling more routine ISO detections. Here we investigate how a space mission to reconnoiter an ISO can be designed, including discussions of the scientific objectives and payload for such a mission, its unique mission design aspects, and some preliminary spacecraft and payload considerations, all in support of possible proposals to conduct such a mission in the 2030s.
{"title":"A study of an interstellar object explorer (IOE) mission","authors":"S. Alan Stern , Silvia Protopapa , Matthew Freeman , Joel Wm. Parker , Mark Tapley , Darryl Z. Seligman , Caden Andersson","doi":"10.1016/j.pss.2024.105850","DOIUrl":"https://doi.org/10.1016/j.pss.2024.105850","url":null,"abstract":"<div><p>The first discoveries of Interstellar Objects (ISOs), i.e., small bodies moving through our Solar System on high-speed hyperbolic orbits, occurred in 2017 and 2019, decades after ISOs were first predicted. The scientific value of ISOs is high, as they represent samples, most likely planetesimals, from other solar systems. A significant increase in the rate of ISO discoveries is expected in the late 2020s and in the 2030s owing to the advent of several new observing capabilities enabling more routine ISO detections. Here we investigate how a space mission to reconnoiter an ISO can be designed, including discussions of the scientific objectives and payload for such a mission, its unique mission design aspects, and some preliminary spacecraft and payload considerations, all in support of possible proposals to conduct such a mission in the 2030s.</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105850"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139726967","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.pss.2024.105841
Scott L. Murchie , Frank P. Seelos , Bethany L. Ehlmann , John D. Boldt , Lawrence E. Brown , Jacob M. Greenberg , Karl A. Hibbitts , W. Jeffrey Lees , David M. Linko , Joseph J. Linden , Graham P. Murphy , Jorge I. Núñez , Katherine L. Rorschach , Calley L. Tinsman , Frank Winterling
Here we describe the design, prototyping, testing, and simulations that were conducted to demonstrate the technology for a concept of the next generation landed planetary spectral imager, the Europa Lander Stereo Spectral Imaging Experiment (ELSSIE). The concept was developed originally for a Europa Lander mission, but the design is applicable, with simplifications, to any ocean world of the outer solar system or to non-icy bodies, including Enceladus, the Moon, Mars, or the surface of Ceres. ELSSIE's design consists of two subassemblies. A Sensor melds a high-resolution, 20-filter, 0.4–3.65 μm, adjustable-focus multispectral stereo imager with a 0.8–3.6 μm point spectrometer, sharing a radiation-shielded single Teledyne H2RG 2048 × 2048 pixel focal plane array (FPA). Each camera includes two 6-position filter wheels with 5 filters and a blank position, providing 10 bandpasses for each of the 2 stereo eyes, and uses 700 × 700 pixels of the FPA. The point spectrometer uses a 6 ×350 pixel strip of the FPA. The Sensor provides stereo and imaging/spectroscopic measurements of reflected light from visible to medium wave-infrared (MWIR) wavelengths to characterize surface morphology, search for pyroclastic plumes, search for organics, identify salts and possible biominerals, characterize crystalline vs. amorphous ice and ice grain sizes, and map the distributions of key phases. In addition to addressing important geologic questions, these measurements support selection of a site for in situ sampling and analysis. A Data Processing Unit (DPU) performs mitigation of radiation that penetrates the shielding using sets of same-filter image frames or spectra of a single spot by removing image spatial pixels with radiation hits, and coadding the remainder for the same spatial pixel, improving signal-to-noise ratio (SNR). The DPU also performs onboard calibration of imager and spectrometer data, co-registration of multispectral images, and calculation of spectral index (“summary parameter”) images for efficient use of lander downlink. Co-registered multispectral image sets and spectra are retained onboard and can be downlinked upon query.
{"title":"ELSSIE: A compact stereo spectral imager for planetary surface morphology and composition","authors":"Scott L. Murchie , Frank P. Seelos , Bethany L. Ehlmann , John D. Boldt , Lawrence E. Brown , Jacob M. Greenberg , Karl A. Hibbitts , W. Jeffrey Lees , David M. Linko , Joseph J. Linden , Graham P. Murphy , Jorge I. Núñez , Katherine L. Rorschach , Calley L. Tinsman , Frank Winterling","doi":"10.1016/j.pss.2024.105841","DOIUrl":"10.1016/j.pss.2024.105841","url":null,"abstract":"<div><p><span>Here we describe the design, prototyping, testing, and simulations that were conducted to demonstrate the technology for a concept of the next generation landed planetary spectral imager, the Europa </span>Lander<span> Stereo Spectral Imaging Experiment (ELSSIE). The concept was developed originally for a Europa Lander mission, but the design is applicable, with simplifications, to any ocean world of the outer solar system or to non-icy bodies, including Enceladus, the Moon<span><span><span><span>, Mars, or the surface of Ceres. ELSSIE's design consists of two subassemblies<span>. A Sensor melds a high-resolution, 20-filter, 0.4–3.65 μm, adjustable-focus multispectral stereo imager with a 0.8–3.6 μm point spectrometer, sharing a radiation-shielded single Teledyne H2RG 2048 × 2048 pixel focal plane array (FPA). Each camera includes two 6-position filter wheels with 5 filters and a blank position, providing 10 bandpasses for each of the 2 stereo eyes, and uses 700 × 700 pixels of the FPA. The point spectrometer uses a 6 ×350 pixel strip of the FPA. The Sensor provides stereo and imaging/spectroscopic measurements of reflected light from visible to medium wave-infrared (MWIR) wavelengths to characterize surface morphology, search for pyroclastic plumes, search for organics, identify salts and possible </span></span>biominerals<span>, characterize crystalline vs. amorphous ice and ice grain sizes, and map the distributions of key phases. In addition to addressing important geologic questions, these measurements support selection of a site for in situ sampling and analysis. A </span></span>Data Processing<span> Unit (DPU) performs mitigation of radiation that penetrates the shielding using sets of same-filter image frames or spectra of a single spot by removing image spatial pixels with radiation hits, and coadding the remainder for the same spatial pixel, improving signal-to-noise ratio (SNR). The DPU also performs onboard calibration of imager and spectrometer data, co-registration of multispectral images, and calculation of </span></span>spectral index (“summary parameter”) images for efficient use of lander downlink. Co-registered multispectral image sets and spectra are retained onboard and can be downlinked upon query.</span></span></p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105841"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139556162","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.pss.2024.105839
A.T. Basilevsky , Yuan Li
Our study is based on a photogeological analysis of the hill-shade images produced from the LOLA digital terrain models and on a stereometric analysis of LROC NAC images. Our results demonstrate that surface morphology of the permanently shadowed floor of crater Shoemaker is nearly identical to that of the regularly illuminated mare surface at the Lunokhod-2 working area and the surface of the highland plain of the Apollo-16 landing site, being dominated by populations of craters smaller than 1 km in diameters. Craters on the Shoemaker floor have approximately the same depth-to-diameter ratios as those within the Lunokhod-2 and Apollo-16 areas. The observed surface morphology of the Shoemaker floor is the result of meteorite bombardment like in other areas of the Moon. Within the permanently shadowed surface areas we detected no morphological peculiarities that could result from the absence of the diurnal temperature variations that excludes the temperature-related creep component of the downslope material movement. This probably means that in the areas with regular solar illumination, the role of the downslope movement of debris by thermally induced creep mechanisms is secondary compared to shaking by close and distant meteorite impacts and locally by moonquakes.
{"title":"Surface morphology inside the PSR area of lunar polar crater Shoemaker in comparison with that of the sunlit areas","authors":"A.T. Basilevsky , Yuan Li","doi":"10.1016/j.pss.2024.105839","DOIUrl":"10.1016/j.pss.2024.105839","url":null,"abstract":"<div><p><span>Our study is based on a photogeological analysis of the hill-shade images produced from the LOLA<span><span> digital terrain models and on a stereometric analysis of LROC NAC images. Our results demonstrate that surface morphology of the permanently shadowed floor of crater Shoemaker is nearly identical to that of the regularly illuminated mare surface at the Lunokhod-2 working area and the surface of the highland plain of the Apollo-16 landing site, being dominated by populations of craters smaller than 1 km in diameters. Craters on the Shoemaker floor have approximately the same depth-to-diameter ratios as those within the Lunokhod-2 and Apollo-16 areas. The observed surface morphology of the Shoemaker floor is the result of meteorite bombardment like in other areas of the </span>Moon. Within the permanently shadowed surface areas we detected no morphological peculiarities that could result from the absence of the diurnal temperature variations that excludes the temperature-related creep component of the downslope material movement. This probably means that in the areas with regular solar illumination, the role of the downslope movement of debris by thermally induced creep mechanisms is secondary compared to shaking by close and distant </span></span>meteorite impacts<span> and locally by moonquakes.</span></p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105839"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139501038","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.pss.2024.105842
L. Trompet , Y. Geunes , T. Ooms , A. Mahieux , V. Wilquet , S. Chamberlain , S. Robert , I.R. Thomas , S. Erard , B. Cecconi , P. Le Sidaner , A.C. Vandaele
{"title":"Addendum to “Description, accessibility and usage of SOIR/Venus Express atmospheric profiles of Venus distributed in VESPA (Virtual European Solar and Planetary Access)”","authors":"L. Trompet , Y. Geunes , T. Ooms , A. Mahieux , V. Wilquet , S. Chamberlain , S. Robert , I.R. Thomas , S. Erard , B. Cecconi , P. Le Sidaner , A.C. Vandaele","doi":"10.1016/j.pss.2024.105842","DOIUrl":"https://doi.org/10.1016/j.pss.2024.105842","url":null,"abstract":"","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105842"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139653684","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.pss.2024.105838
I.G. Brykina, L.A. Egorova
The mass distribution of fragments is an important characteristic that often needs to be defined for forward modelling the interaction of disrupted meteoroids and asteroids with the atmosphere, and which can be inferred to some extent by the distribution of meteorites that fell to the ground. In previous studies, we derived a formula for the mass distribution of fragments of a disrupted body assuming a power law for the distribution in a differential form, and applied this formula to describe the results of many impact experiments modelling fragmentation of asteroids in outer space. The formula represents the cumulative number of fragments as a function of the fragment mass normalized to the total mass, the mass fraction of the largest fragment and the power index, which is the only free parameter adjusted to best fit the analytical distribution to the empirical one. Here, we use the proposed formula to describe the mass distributions of recovered meteorites that fell to the ground after the passage and disruption of thirteen extraterrestrial objects in the atmosphere, as well as the mass distributions of fragments of meteorite samples disrupted in impact experiments. A comparison is made between the distributions of unevaporated fragments of bodies disrupted in the atmosphere and the distributions obtained after the disruption of bodies in experiments. Some regularities in meteorite distributions and the influence of the incompleteness of the available collection of meteorites on their mass distribution are discussed.
{"title":"Describing the fragment mass distribution in meteorite showers","authors":"I.G. Brykina, L.A. Egorova","doi":"10.1016/j.pss.2024.105838","DOIUrl":"10.1016/j.pss.2024.105838","url":null,"abstract":"<div><p>The mass distribution of fragments is an important characteristic that often needs to be defined for forward modelling the interaction of disrupted meteoroids and asteroids with the atmosphere, and which can be inferred to some extent by the distribution of meteorites that fell to the ground. In previous studies, we derived a formula for the mass distribution of fragments of a disrupted body assuming a power law for the distribution in a differential form, and applied this formula to describe the results of many impact experiments modelling fragmentation of asteroids in outer space. The formula represents the cumulative number of fragments as a function of the fragment mass normalized to the total mass, the mass fraction of the largest fragment and the power index, which is the only free parameter adjusted to best fit the analytical distribution to the empirical one. Here, we use the proposed formula to describe the mass distributions of recovered meteorites that fell to the ground after the passage and disruption of thirteen extraterrestrial objects in the atmosphere, as well as the mass distributions of fragments of meteorite samples disrupted in impact experiments. A comparison is made between the distributions of unevaporated fragments of bodies disrupted in the atmosphere and the distributions obtained after the disruption of bodies in experiments. Some regularities in meteorite distributions and the influence of the incompleteness of the available collection of meteorites on their mass distribution are discussed.</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"241 ","pages":"Article 105838"},"PeriodicalIF":2.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139507541","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-01DOI: 10.1016/j.pss.2023.105834
N.V. Erkaev
The magnetized supersonic solar wind, when flowing around planets, forms a magnetic barrier near the streamlined surface. The main feature of the magnetic barrier is that the magnetic pressure prevails over the plasma pressure. The Hall-MHD model is used to simulate the magnetic barrier in the case of solar wind flow around the atmosphere of Venus. The obtained numerical results are compared with an analytical approximation of the magnetic barrier thickness, which expresses the dependence of the magnetic barrier on solar wind parameters. Particular attention is paid to the physical reasons for the asymmetry of the magnetic barrier caused by the Hall effects, which are mainly concentrated in the boundary layer near the ionopause, where the electric current has a maximum strength. An additional source of asymmetry is also considered, which acts in the same direction and is associated with the influence of the normal component of the electric field on the specific behavior of new atmospheric ions. It is shown that solar wind protons are loaded by new atmospheric ions mainly in the hemisphere. In the case of more intense loading, the boundary of the magnetic barrier and the shock wave are located farther from the ionopause.
{"title":"About the magnetic barrier of Venus","authors":"N.V. Erkaev","doi":"10.1016/j.pss.2023.105834","DOIUrl":"10.1016/j.pss.2023.105834","url":null,"abstract":"<div><p><span>The magnetized supersonic<span> solar wind, when flowing around planets, forms a magnetic barrier near the streamlined surface. The main feature of the magnetic barrier is that the magnetic pressure prevails over the plasma pressure<span>. The Hall-MHD model is used to simulate the magnetic barrier in the case of solar wind flow around the atmosphere of Venus. The obtained numerical results are compared with an analytical approximation of the magnetic barrier thickness, which expresses the dependence of the magnetic barrier on solar wind parameters. Particular attention is paid to the physical reasons for the asymmetry of the magnetic barrier caused by the Hall effects<span>, which are mainly concentrated in the boundary layer near the ionopause, where the electric current has a maximum strength. An additional source of asymmetry is also considered, which acts in the same direction and is associated with the influence of the normal component of the electric field on the specific behavior of new atmospheric ions. It is shown that solar wind protons are loaded by new atmospheric ions mainly in the </span></span></span></span><span><math><msub><mrow><mi>E</mi></mrow><mrow><mo>+</mo></mrow></msub></math></span> hemisphere. In the case of more intense loading, the boundary of the magnetic barrier and the shock wave are located farther from the ionopause.</p></div>","PeriodicalId":20054,"journal":{"name":"Planetary and Space Science","volume":"240 ","pages":"Article 105834"},"PeriodicalIF":2.4,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139063718","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}