1
Generally, thermal anomalies are described as those regions where are colder or warmer than the surroundings. If the center TB (TB cent ) is higher than the surrounding TB (TB surr ), these regions should be identified as hot spots. Otherwise, the regions with lower center TB should be identified as cold spots. It is necessary to give a subjective threshold value to define the cold spots or hot spots. In this paper, 3 K is defined as a rational threshold value. The 37GHz nighttime image is used to built the catalogue of them. Firstly, we use the microwave image to produce a contour map (Fig.6). On the contour map with interval of 0.5K, the thermal anomalies are shown as multi-ring patches. The TB value of the outermost ring was treated and extracted as surrounding TB (TB surr ), the TB within the centre ring was treated as center TB (TB cent ). ∆TB=TB surr -TB cent , stands for the abnormal degree of the thermal anomalies. We identified 266 thermal anomalies. Among them, 244 are cold spots, 22 are hot spots in the nighttime microwave map. CATALOGUE OF LUNAR THERMAL ANOMALIES Y. C. Zheng, K. L. Chan, K. T, Tsang, and Y.C. Zhu 1 National Astronomical Observatories, Chinese Academy of Sciences, Beijing, China; Email: [email protected] 2 Center For Space Science Research, The Hong Kong University of Science and Technology, Hong Kong; 3 Space Science Institute, Macau University of Science and Technology, Macao; 4 United International College, Beijing Normal University-Hong Kong Baptist University, Zhuhai, China. The scene on the night-time lunar surface is still poorly understood until today, making it an curious and attractive topic for the astronomers and the general public. Without heat preservation by atmosphere like as on the Earth, the lunar surface cools rapidly during lunar night or lunar eclipse. However, the heating and cooling rate of the lunar surface is not uniform. Many ground-based observations in microwave (MW) and infrared (IR) band have revealed that some areas on the Moon cool much slowly or rapidly than the surroundings, which resulted as hot spots or cold spots on the Moon. In the observation from the Earth or lunar orbit, the lunar surface during eclipse or lunar night are dotted by hundreds of thermal anomalies (Shorthill and Saari, 1965). These thermal anomalies were explained as topographic effects (Ronca, 1970), rock abundances (Mendell and Low, 1974), internal heating (Saari, 1969) or other factors. Such thermal are also found on Io (Goguen et al., 1988). New observation data from recent lunar missions give us a chance to renew our understandings of thermal anomalies. The orbital MW and IR observation data sets are much benefit to this research. The orbital MW observations were carried by China’s Chang’E-1 (CE-1) and Chang’E-2 (CE-2) missions in 2007 and 2010, respectively. The infrared observation was carried by LRO Diviner radiometer. We have discovered many cold spots on the nighttime lunar surface in CE-1’s observation. However, most of them are shown as hot spots in the IR observation. In this paper, we present the complete catalogue of lunar thermal anomalies discovered from the recent CE-2 observation. The thermal anomalies are jointly confirmed by the CE-1’s and CE-2’s MW data. We integrated the Diviner’s nighttime surface temperature, the composition data and the image data in the Geographic Information System (GIS) software. We classify the thermal anomalies into five types, Ray crater, Crater with bright wall, Crater with rough floor, Shadowed topography and others. INTRODUCTION E. Catalogue of Thermal Anomalies A. CE-2 Lunar Orbiter and its Microwave Radiometer The MRM operated in four microwave frequency channels: 3.0, 7.8, 19.35 and 37.0 GHz (with wavelengths 10.0, 3.84, 1.55, and 0.81 cm, respectively). All four channels are estimated to have a sensitivity of 0.5 K in brightness temperature. Benefited from the lower altitude (about 100 km), the spatial resolution has been improved by four factors than CE-1. The resolution on the lunar surface are in the range 17.5 km for 3.0 GHz channel and 25 km for 7.8, 19.35 and 37.0 GHz channels. Fig.1. Configuration of CE-2’s microwave radiometer Correspondence author: Dr. Y.C ZHENG. A20, Datun Rd. Chaoyang, Beijing 100012, National Astronomical Observatories, Chinese Academy of Sciences, China. Email: [email protected]. Department of Mathematics, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong. Tel: (852) 2358 7426. Email: [email protected]. B. Brightness Temperature data fitting Acknowledgements: This work is supported by the NSFC program (40904051), CAS program (XDA040 71900), and Hong Kong Scholar Program. Acknowledgements and Correspondence C. Microwave Images of the Moon CE-2 is the second lunar mission of China’s Lunar Exploration Program. It was launched in 1st, Oct, 2010, after three years of CE-1’s launch in 24th, Oct, 2007. MRMs are the common scientific instruments aboard CE-1 and CE-2, which made the first two passive microwave remote sensing of the Moon. The science goal of CE-2’s MRM is to measure the TB of the Moon, and from which to retrieve the physical properties of lunar regolith. Brightness temperature of the Moon is characterized by latitudinal variation and diurnal variation. To get the large-scale trends caused by lunar latitude and local time, we constructed a numerical model by expanding the TB data within latitude N/S 60° in spherical harmonics to the 4th degree, which is sampled as TB model . With this fitting model, we can (1) get the TB variation features of the four channel and compare their differences; (2) normalize the TB data measured in different local time to a certain time. The normalized TB data have the same solar conditions. The latitude effects of the TB data can also be removed. Fig.2. a-d: the 4 th order spherical harmonics fitting models (TB model ) fitted by CE-2 TB data within latitude N/S 60° at 3.0, 7.8, 19.35, 37.0 Ghz channel, respectively. (d) (b) (c) (a) CE-2 MRM measured the lunar surface at different solar condition, i.e. different local time. Using the spherical harmonics fitting models of TB data in section B, the measured TB data were normalized into the same local time. The normalized TB data were loaded into the GIS to get the microwave images of the Moon (Fig.3, 4). D. Surface material units revealed by the microwave images We removed the latitude effects using spherical harmonic fitting model from the microwave images shown in section C. These images without latitude effects, which has the same solar conditions, could reveal clearly the surface materials unit than ever (Fig. 5). In Fig.5d: 1) the red regions own relative strong daytime microwave radiation. They are corresponding well with the high titanium lava material in the maria and the material in SPA basin. 2) The green regions own relative strong nighttime microwave radiation. They are corresponding well with the low titanium materials in the maria. There are heat released slowly in lunar night. The heat might correlated with the high content of radioactive element. 3) The blue regions are those own great diurnal difference between the daytime and nighttime microwave radiation. They are corresponding well with the young rayed craters. Fig.6. Identification of microwave thermal anomalies on the Moon. Total 266 thermal anomalies are identified from the contour map of 37GHz TB. All lunar thermal anomalies Between N60° to S60° are shown Fig.7. The distribution density of anomalies in the highland are higher than those in the maria. The maria are covered by the homogeneous basaltic material with similar thermal properties. In addition, the maria are characterized by their smooth topography an low density of craters which lead to relative uniform thermal performance in the maria. In order to understand the factors to produce thermal anomalies on the Moon, we combined the different data sets to study the correlation between the visible image, microwave TB and infrared observation. The data sets include the CE-2’s and LRO WAC’s visible image, 37GHz daytime and nighttime TB data, and the Diviner nighttime infrared data which is corresponding the surface temperature well. According to the corresponding topographic features, the 266 thermal anomalies in our catalogue, including cold spots and hot spots, could be classified as five types (Table 1and Fig. 8). -20 -15 -10 -5 0 5 -20 -10 0 10 20 30 40 37GHz nighttime TB difference (TB 37Ncenter - TB 37Nsurr ) (K) Infrared nighttime temperature difference (T Ncenter - T Nsurr ) (K) Ray Crater Crater with Bright Wall Crater with Rough Floor Shadowed topography Other Crater IR hot spots and MW cold spots IR cold spots and MW cold spots IR hot spots and MW hot spots ΔTB Ray crater Crater with bright wall Crater with rough floor Shadowe d topograph y others IR night Hot spot Hot spot Hot spot Cold spot Cold/hot spot MW night Cold spot Cold spot Cold spot Cold spot Cold/hot spot MW night Cold/hot spot Cold spot Hot spot Cold spot Cold/hot spot Total 103 22 21 71 49 Fig.3. Daytime microwave TB images (normalized to lunar noon). a-d: 3.0, 7.8, 19.35, 37GHz. (a) (b) (c) (d) (a) (b) (c) (d) (a) (b) (c) (d) (a) (b) (c) (d) Fig.5. The surface material units revealed by the 37GHz microwave images. (a) the normalized noon image, (b) the normalized midnight image, (c) the diurnal difference image between the noon and the midnight microwave radiation, (d) the false color image combined by Red (Fig.5a), Green (Fig.5b), Blue (Fig.5c). Fig.7. The distribution of lunar thermal anomalies in the range of N60° to S60°. The base maps of a-d are DOM of CE-1, combination color map, nighttime TB image of 37Ghz and the average nighttime temperature image of Diviner, respectively. The characteristics of thermal anomalies in the MW and IR observations, and their corresponding topographic features are summarized in Table 1. Four types of topographic features, ray crater, crater with bright wall, crater with rough floor, and shadowed topography, present as cold spots in the nighttime microwave map. However, they show different characters in the daytime microwave map and the nighttime infrared map. These characters give us clues to reveal the underlying physical mechanism of thermal anomalies. Table 1. Classification and the performance of thermal anomalies in the MW and IR observation Fig. 8. The performance of thermal anomalies in nighttime microwave map and infrared maps. X axis: the 37GHz nighttime ∆TB. Y axis: the infrared temperature difference between the center and surrounding. The negative values means cold spots. The positive value means hot spots. Fig.4. Nighttime microwave TB images (normalized to lunar midnight). a-d: 3.0, 7.8, 19.35, 37GHz. Reference Goguen, J.D., Sinton, W.M., Matson, D.L., Howell, R.R., Dyck, H.M., Johnson, T.V., Brown, R.H., Veeder, G.J., Lane, A.L., Nelson, R.M., Mc Laren, R.A., 1988. Io hot spots: Infrared photometry of satellite occultations. Icarus 76, 465-484. Mendell, W.W., Low, F.J., 1974. Preliminary Results of the Apollo 17 Infrared Scanning Radiometer. Moon 9, 97-103. Ronca, L.B., 1970. The relationship between lunar hot spots and the geomorphic index. The Moon 2, 202-210. Saari, J.M., 1969. Lunar thermal anomalies and internal heating. Astrophysics and Space Science 4, 275-284. Shorthill, R., Saari, J., 1965. Nonuniform cooling of the eclipsed Moon: a listing of thirty prominent anomalies. Science 150, 210-212.

CATALOGUE OF LUNAR THERMAL ANOMALIES

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Generally, thermal anomalies are described as those regions where are colder or warmer than the surroundings. If the center TB (TBcent) is higher than the surrounding TB (TBsurr), these regions should be identified as hot spots. Otherwise, the regions with lower center TB should be identified as cold spots. It is necessary to give a subjective threshold value to define the cold spots or hot spots. In this paper, 3 K is defined as a rational threshold value. The 37GHz nighttime image is used to built the catalogue of them. Firstly, we use the microwave image to produce a contour map (Fig.6). On the contour map with interval of 0.5K, the thermal anomalies are shown as multi-ring patches. The TB value of the outermost ring was treated and extracted as surrounding TB (TBsurr), the TB within the centre ring was treated as center TB (TBcent). ∆TB=TBsurr-TBcent, stands for the abnormal degree of the thermal anomalies. We identified 266 thermal anomalies. Among them, 244 are cold spots, 22 are hot spots in the nighttime microwave map.

CATALOGUE OF LUNAR THERMAL ANOMALIES

Y. C. Zheng, K. L. Chan, K. T, Tsang, and Y.C. Zhu

1 National Astronomical Observatories, Chinese Academy of Sciences, Beijing, China; Email: [email protected] 2 Center For Space Science Research, The Hong Kong University of Science and Technology, Hong Kong;

3 Space Science Institute, Macau University of Science and Technology, Macao; 4 United International College, Beijing Normal University-Hong Kong Baptist University, Zhuhai, China.

The scene on the night-time lunar surface is still poorly understood until today, making it an curious and attractive topic for the astronomers and the general public. Without heat preservation by atmosphere like as on the Earth, the lunar surface cools rapidly during lunar night or lunar eclipse. However, the heating and cooling rate of the lunar surface is not uniform. Many ground-based observations in microwave (MW) and infrared (IR) band have revealed that some areas on the Moon cool much slowly or rapidly than the surroundings, which resulted as hot spots or cold spots on the Moon. In the observation from the Earth or lunar orbit, the lunar surface during eclipse or lunar night are dotted by hundreds of thermal anomalies (Shorthill and Saari, 1965). These thermal anomalies were explained as topographic effects (Ronca, 1970), rock abundances (Mendell and Low, 1974), internal heating (Saari, 1969) or other factors. Such thermal are also found on Io (Goguen et al., 1988).

New observation data from recent lunar missions give us a chance to renew our understandings of thermal anomalies. The orbital MW and IR observation data sets are much benefit to this research. The orbital MW observations were carried by China’s Chang’E-1 (CE-1) and Chang’E-2 (CE-2) missions in 2007 and 2010, respectively. The infrared observation was carried by LRO Diviner radiometer. We have discovered many cold spots on the nighttime lunar surface in CE-1’s observation. However, most of them are shown as hot spots in the IR observation.

In this paper, we present the complete catalogue of lunar thermal anomalies discovered from the recent CE-2 observation. The thermal anomalies are jointly confirmed by the CE-1’s and CE-2’s MW data. We integrated the Diviner’s nighttime surface temperature, the composition data and the image data in the Geographic Information System (GIS) software. We classify the thermal anomalies into five types, Ray crater, Crater with bright wall, Crater with rough floor, Shadowed topography and others.

INTRODUCTION E. Catalogue of Thermal Anomalies

A. CE-2 Lunar Orbiter and its Microwave Radiometer

The MRM operated in four microwave frequency channels: 3.0, 7.8, 19.35 and 37.0 GHz (with wavelengths 10.0, 3.84, 1.55, and 0.81 cm, respectively). All four channels are estimated to have a sensitivity of 0.5 K in brightness temperature. Benefited from the lower altitude (about 100 km), the spatial resolution has been improved by four factors than CE-1. The resolution on the lunar surface are in the range 17.5 km for 3.0 GHz channel and 25 km for 7.8, 19.35 and 37.0 GHz channels. Fig.1. Configuration of CE-2’s microwave radiometer

Correspondence author: Dr. Y.C ZHENG. A20, Datun Rd. Chaoyang, Beijing 100012, National Astronomical Observatories, Chinese Academy of Sciences, China. Email: [email protected]. Department of Mathematics, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong. Tel: (852) 2358 7426. Email: [email protected].

B. Brightness Temperature data fitting

Acknowledgements: This work is supported by the NSFC program (40904051), CAS program (XDA040 71900), and Hong Kong Scholar Program.

Acknowledgements and Correspondence

C. Microwave Images of the Moon

CE-2 is the second lunar mission of China’s Lunar Exploration Program. It was launched in 1st, Oct, 2010, after three years of CE-1’s launch in 24th, Oct, 2007. MRMs are the common scientific instruments aboard CE-1 and CE-2, which made the first two passive microwave remote sensing of the Moon. The science goal of CE-2’s MRM is to measure the TB of the Moon, and from which to retrieve the physical properties of lunar regolith.

Brightness temperature of the Moon is characterized by latitudinal variation and diurnal variation. To get the large-scale trends caused by lunar latitude and local time, we constructed a numerical model by expanding the TB data within latitude N/S 60° in spherical harmonics to the 4th degree, which is sampled as TBmodel. With this fitting model, we can (1) get the TB variation features of the four channel and compare their differences; (2) normalize the TB data measured in different local time to a certain time. The normalized TB data have the same solar conditions. The latitude effects of the TB data can also be removed.

Fig.2. a-d: the 4th order spherical harmonics fitting models (TBmodel) fitted by CE-2 TB data within latitude N/S 60° at 3.0, 7.8, 19.35, 37.0 Ghz channel, respectively.

(d)

(b)

(c)

(a)

CE-2 MRM measured the lunar surface at different solar condition, i.e. different local time. Using the spherical harmonics fitting models of TB data in section B, the measured TB data were normalized into the same local time. The normalized TB data were loaded into the GIS to get the microwave images of the Moon (Fig.3, 4).

D. Surface material units revealed by the microwave images

We removed the latitude effects using spherical harmonic fitting model from the microwave images shown in section C. These images without latitude effects, which has the same solar conditions, could reveal clearly the surface materials unit than ever (Fig. 5).

In Fig.5d: 1) the red regions own relative strong daytime microwave radiation. They are

corresponding well with the high titanium lava material in the maria and the material in SPA basin.

2) The green regions own relative strong nighttime microwave radiation. They are corresponding well with the low titanium materials in the maria. There are heat released slowly in lunar night. The heat might correlated with the high content of radioactive element.

3) The blue regions are those own great diurnal difference between the daytime and nighttime microwave radiation. They are corresponding well with the young rayed craters.

Fig.6. Identification of microwave thermal anomalies on the Moon. Total 266 thermal anomalies are identified from the contour map of 37GHz TB.

All lunar thermal anomalies Between N60° to S60° are shown Fig.7. The distribution density of anomalies in the highland are higher than those in the maria. The maria are covered by the homogeneous basaltic material with similar thermal properties. In addition, the maria are characterized by their smooth topography an low density of craters which lead to relative uniform thermal performance in the maria. In order to understand the factors to produce thermal anomalies on the Moon, we combined the different data sets to study the correlation between the visible image, microwave TB and infrared observation. The data sets include the CE-2’s and LRO WAC’s visible image, 37GHz daytime and nighttime TB data, and the Diviner nighttime infrared data which is corresponding the surface temperature well. According to the corresponding topographic features, the 266 thermal anomalies in our catalogue, including cold spots and hot spots, could be classified as five types (Table 1and Fig. 8).

-20 -15 -10 -5 0 5-20

-10

0

10

20

30

40

37GHz nighttime TB difference(TB37Ncenter - TB37Nsurr ) (K)

Infra

red

nigh

ttim

e te

mpe

ratu

re d

iffer

ence

(TN

cent

er -

T Nsu

rr) (

K)

Ray CraterCrater with Bright WallCrater with Rough FloorShadowed topographyOther Crater

IR hot spots and MW cold spots

IR cold spots and MW cold spots

IR hot spots andMW hot spots

ΔTB Ray crater Crater with bright wall

Crater with rough floor

Shadowed topography

others

IRnight Hot spot Hot spot Hot spot Cold spot Cold/hot spot

MWnight Cold spot Cold spot Cold spot

Cold spot Cold/hot spot

MWnight Cold/hot spot

Cold spot Hot spot Cold spot Cold/hot spot

Total 103 22 21 71 49

Fig.3. Daytime microwave TB images (normalized to lunar noon). a-d: 3.0, 7.8, 19.35, 37GHz.

(a) (b)

(c) (d)

(a) (b)

(c) (d)

(a) (b)

(c) (d)

(a) (b)

(c) (d)

Fig.5. The surface material units revealed by the 37GHz microwave images. (a) the normalized noon image, (b) the normalized midnight image, (c) the diurnal difference image between the noon and the midnight microwave radiation, (d) the false color image combined by Red (Fig.5a), Green (Fig.5b), Blue (Fig.5c).

Fig.7. The distribution of lunar thermal anomalies in the range of N60° to S60°. The base maps of a-d are DOM of CE-1, combination color map, nighttime TB image of 37Ghz and the average nighttime temperature image of Diviner, respectively.

The characteristics of thermal anomalies in the MW and IR observations, and their corresponding topographic features are summarized in Table 1. Four types of topographic features, ray crater, crater with bright wall, crater with rough floor, and shadowed topography, present as cold spots in the nighttime microwave map. However, they show different characters in the daytime microwave map and the nighttime infrared map. These characters give us clues to reveal the underlying physical mechanism of thermal anomalies.

Table 1. Classification and the performance of thermal anomalies in the MW and IR observation

Fig. 8. The performance of thermal anomalies in nighttime microwave map and infrared maps. X axis: the 37GHz nighttime ∆TB. Y axis: the infrared temperature difference between the center and surrounding. The negative values means cold spots. The positive value means hot spots.

Fig.4. Nighttime microwave TB images (normalized to lunar midnight). a-d: 3.0, 7.8, 19.35, 37GHz.

Reference Goguen, J.D., Sinton, W.M., Matson, D.L., Howell, R.R., Dyck, H.M., Johnson, T.V., Brown, R.H., Veeder, G.J., Lane, A.L., Nelson, R.M., Mc Laren, R.A., 1988. Io hot spots: Infrared photometry of satellite occultations. Icarus 76, 465-484. Mendell, W.W., Low, F.J., 1974. Preliminary Results of the Apollo 17 Infrared Scanning Radiometer. Moon 9, 97-103. Ronca, L.B., 1970. The relationship between lunar hot spots and the geomorphic index. The Moon 2, 202-210. Saari, J.M., 1969. Lunar thermal anomalies and internal heating. Astrophysics and Space Science 4, 275-284. Shorthill, R., Saari, J., 1965. Nonuniform cooling of the eclipsed Moon: a listing of thirty prominent anomalies. Science 150, 210-212.