Commit 286e37cd4b383be870f91055e2fb20a7ddc7f0c6
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Fix in Solar Orbiter MAG & RPW descriptions
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Instrument/CDPP-AMDA/Solar_Orbiter/MAG.xml
... | ... | @@ -7,15 +7,15 @@ |
7 | 7 | <ResourceName>MAG</ResourceName> |
8 | 8 | <AlternateName>Magnetometer</AlternateName> |
9 | 9 | <ReleaseDate>2018-10-27T18:45:12Z</ReleaseDate> |
10 | - <Description>The magnetometer is a unique instrument on Solar Orbiter in that it provides essential | |
11 | -information about both the largest scale structures in space around the Sun, as well as the | |
12 | -smallest scale kinetic processes in the plasma. Indeed, the magnetic field plays a central role in | |
13 | -plasma dynamics since charged particles generally travel along the magnetic field, making it | |
14 | -the route from the Sun into space. The accurate measurement of the local magnetic field is | |
15 | -therefore central to the scientific success of Solar Orbiter. Magnetometer data are expected to | |
16 | -lead to significant advances in our understanding of how the Sun’s magnetic field links into | |
17 | -space and evolves over the solar cycle; how particles are accelerated and propagate around the | |
18 | -solar system, including to the Earth; and how the corona and solar wind are heated and | |
10 | + <Description>The magnetometer is a unique instrument on Solar Orbiter in that it provides essential | |
11 | +information about both the largest scale structures in space around the Sun, as well as the | |
12 | +smallest scale kinetic processes in the plasma. Indeed, the magnetic field plays a central role in | |
13 | +plasma dynamics since charged particles generally travel along the magnetic field, making it | |
14 | +the route from the Sun into space. The accurate measurement of the local magnetic field is | |
15 | +therefore central to the scientific success of Solar Orbiter. Magnetometer data are expected to | |
16 | +lead to significant advances in our understanding of how the Sun’s magnetic field links into | |
17 | +space and evolves over the solar cycle; how particles are accelerated and propagate around the | |
18 | +solar system, including to the Earth; and how the corona and solar wind are heated and | |
19 | 19 | accelerated, among many others. |
20 | 20 | |
21 | 21 | The MAG team science objectives include: |
... | ... | @@ -32,13 +32,13 @@ The MAG team science objectives include: |
32 | 32 | * What is the structure of plasma turbulence and how does it evolve? |
33 | 33 | * How do large and small scale structures modulate particle fluxes? |
34 | 34 | |
35 | -In order to achieve these objectives, the magnetometer will measure the magnetic field | |
36 | -continuously with sufficient cadence and precision to quantify fluid-scale phenomena | |
37 | -throughout the mission and, in burst mode, with sufficient cadence and precision to study ion | |
35 | +In order to achieve these objectives, the magnetometer will measure the magnetic field | |
36 | +continuously with sufficient cadence and precision to quantify fluid-scale phenomena | |
37 | +throughout the mission and, in burst mode, with sufficient cadence and precision to study ion | |
38 | 38 | kinetic phenomena. |
39 | 39 | |
40 | -Low latency data are generated at a very low cadence compared to normal magnetometer data | |
41 | -and are intended for rapid, broad characterisation of solar wind conditions at the spacecraft | |
40 | +Low latency data are generated at a very low cadence compared to normal magnetometer data | |
41 | +and are intended for rapid, broad characterisation of solar wind conditions at the spacecraft | |
42 | 42 | location.</Description> |
43 | 43 | <Acknowledgement></Acknowledgement> |
44 | 44 | <Contact> |
... | ... |
Instrument/CDPP-AMDA/Solar_Orbiter/RPW.xml
... | ... | @@ -7,59 +7,46 @@ |
7 | 7 | <ResourceName>RPW</ResourceName> |
8 | 8 | <AlternateName>Plasma Wave Investigation</AlternateName> |
9 | 9 | <ReleaseDate>2017-11-27T21:10:13Z</ReleaseDate> |
10 | - <Description>RPW will make key measurements in support of the first three, out of four top-level scientific questions, | |
10 | + <Description>RPW will make key measurements in support of the first three, out of four top-level scientific questions, | |
11 | 11 | which drive Solar Orbiter overall science objectives: |
12 | 12 | * How and where do the solar wind plasma and magnetic field originate in the corona? |
13 | 13 | * How do solar transients drive heliospheric variability? |
14 | 14 | * How do solar eruptions produce energetic particle radiation that fills the heliosphere? |
15 | 15 | * How does the solar dynamo work and drive connections between the Sun and the heliosphere? |
16 | 16 | |
17 | -Here is the summary of the specific RPW Science Objectives. | |
18 | -* Solar and Interplanetary Radio Burst: | |
19 | - - What is the role of shocks and flares in accelerating particles near the Sun? | |
20 | - - How is the Sun connected magnetically to the interplanetary medium? | |
21 | - - What are the sources and the global dynamics of eruptive events? | |
22 | - - What is the role of ambient medium conditions on particle acceleration and propagation? | |
23 | - - How do variations and structure in the solar wind affect low frequency radio wave propagation? | |
24 | -* Electron density and temperature measurements with the Quasi-Thermal Noise spectroscopy: | |
25 | - - Precise measurement of both the electron density and temperature, with accuracies respectively of | |
26 | - a few % and around 10 %, at perihelion. | |
27 | - - Study the non-thermal character of the electron distributions at perihelion. | |
28 | -* Radio emission processes from electron beams: Langmuir waves and electromagnetic mode conversion: | |
29 | - - Measurements for the first time in the Solar Wind of both the electric and magnetic field waveforms | |
30 | - at high time resolution (up to 500 kSs). | |
31 | - - Study of the mode conversion from Langmuir to electromagnetic waves. | |
32 | - - Study of the energy balance between electron beams, Langmuir waves and e.m. radio waves at | |
33 | - several radial distances | |
34 | -* Solar wind microphysics and turbulence: | |
35 | - - Measure of the waves associated with the plasma instabilities that are generated by temperature | |
36 | - anisotropies in the solar wind. | |
37 | - - First DC/LF electric field measurements in the inner heliosphere and over a large radial distance | |
38 | - in the solar. | |
39 | -* Shocks, Reconnection, Current Sheets, and Magnetic Holes: | |
40 | - - Identification and study of the reconnection process in current sheets with thickness down to the ion | |
41 | - scales and smaller. | |
42 | - - Determination of the interplanetary shock structure down to the spatial and temporal scales comparable | |
43 | - and smaller than the typical ion scales. | |
44 | - - Determination of different particle energisation mechanisms within shocks and reconnection regions. | |
45 | - - Distinguish different radio burst generation mechanisms. Interplanetary Dust | |
46 | - - Determination, in combination with the EPD instrument, the spatial distribution, mass and dynamics | |
47 | - of dust particles in the near-Sun heliosphere, in and out of the ecliptic. | |
17 | +Here is the summary of the specific RPW Science Objectives: | |
18 | +* Solar and Interplanetary Radio Burst: | |
19 | +- What is the role of shocks and flares in accelerating particles near the Sun? | |
20 | +- How is the Sun connected magnetically to the interplanetary medium? | |
21 | +- What are the sources and the global dynamics of eruptive events? | |
22 | +- What is the role of ambient medium conditions on particle acceleration and propagation? | |
23 | +- How do variations and structure in the solar wind affect low frequency radio wave propagation? | |
24 | +* Electron density and temperature measurements with the Quasi-Thermal Noise spectroscopy: | |
25 | +- Precise measurement of both the electron density and temperature, with accuracies respectively of a few % and around 10 %, at perihelion. | |
26 | +- Study the non-thermal character of the electron distributions at perihelion. | |
27 | +* Radio emission processes from electron beams: Langmuir waves and electromagnetic mode conversion: | |
28 | +- Measurements for the first time in the Solar Wind of both the electric and magnetic field waveforms at high time resolution (up to 500 kSs). | |
29 | +- Study of the mode conversion from Langmuir to electromagnetic waves. | |
30 | +- Study of the energy balance between electron beams, Langmuir waves and e.m. radio waves at several radial distances | |
31 | +* Solar wind microphysics and turbulence: | |
32 | +- Measure of the waves associated with the plasma instabilities that are generated by temperature anisotropies in the solar wind. | |
33 | +- First DC/LF electric field measurements in the inner heliosphere and over a large radial distance in the solar. | |
34 | +* Shocks, Reconnection, Current Sheets, and Magnetic Holes: | |
35 | +- Identification and study of the reconnection process in current sheets with thickness down to the ion scales and smaller. | |
36 | +- Determination of the interplanetary shock structure down to the spatial and temporal scales comparable and smaller than the typical ion scales. | |
37 | +- Determination of different particle energisation mechanisms within shocks and reconnection regions. | |
38 | +- Distinguish different radio burst generation mechanisms. Interplanetary Dust | |
39 | +- Determination, in combination with the EPD instrument, the spatial distribution, mass and dynamics of dust particles in the near-Sun heliosphere, in and out of the ecliptic. | |
48 | 40 | |
49 | -To cover its specific Science Objectives, RPW will measure magnetic and electric fields at high time | |
50 | -resolution using a number of sensors, to determine the characteristics of electromagnetic and electrostatic | |
51 | -waves in the solar wind. More precisely, RPW will: | |
52 | -* Make the first-ever high accuracy, high-sensitivity and low noise measurements of electric fields | |
53 | - at low frequencies (below ~1 kHz) in the inner Heliosphere. | |
54 | -* Measure the magnetic and electric fields of the solar wind turbulence with high sensitivity and | |
55 | - dynamic range along the spacecraft trajectory. | |
56 | -* Store high-resolution data from scientifically interesting regions such as in-situ shock crossings, | |
57 | - in-situ Type III events and others. | |
58 | -* Measure the satellite potential with high temporal resolution permitting to estimate the density | |
59 | - fluctuations in the solar wind and allowing higher accuracy particle instrument measurements. | |
41 | +To cover its specific Science Objectives, RPW will measure magnetic and electric fields at high time | |
42 | +resolution using a number of sensors, to determine the characteristics of electromagnetic and electrostatic | |
43 | +waves in the solar wind. More precisely, RPW will: | |
44 | +* Make the first-ever high accuracy, high-sensitivity and low noise measurements of electric fields at low frequencies (below ~1 kHz) in the inner Heliosphere. | |
45 | +* Measure the magnetic and electric fields of the solar wind turbulence with high sensitivity and dynamic range along the spacecraft trajectory. | |
46 | +* Store high-resolution data from scientifically interesting regions such as in-situ shock crossings, in-situ Type III events and others. | |
47 | +* Measure the satellite potential with high temporal resolution permitting to estimate the density fluctuations in the solar wind and allowing higher accuracy particle instrument measurements. | |
60 | 48 | * Measure the quasi thermal noise and Langmuir waves around the local plasma frequency |
61 | -* Measure for the first type the high frequency magnetic counterpart of Langmuir waves associated | |
62 | - with in-situ Type III bursts | |
49 | +* Measure for the first type the high frequency magnetic counterpart of Langmuir waves associated with in-situ Type III bursts | |
63 | 50 | * Observe the solar and interplanetary radio burst |
64 | 51 | * Observe the radio counterpart of dust particle impacts |
65 | 52 | * Detect on-board in-situ shock crossings and store the corresponding data |
... | ... |