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Dave Paige / Francis Nimmo

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ESS 250: MARS Dave Paige / Francis Nimmo Lecture Outline Mars Mission Basics Getting to Mars The Deep Space Network Getting Into Orbit Orbits Landing Cartography ... – PowerPoint PPT presentation

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Title: Dave Paige / Francis Nimmo


1
ESS 250 MARS
  • Dave Paige / Francis Nimmo

2
Lecture Outline
  • Mars Mission Basics
  • Getting to Mars
  • The Deep Space Network
  • Getting Into Orbit
  • Orbits
  • Landing
  • Cartography
  • Selected Instrument Techniques
  • Visible Imaging
  • Near IR Spectroscopy
  • Thermal IR Radiometry and Spectroscopy
  • Laser Altimetry
  • Particle and High Energy Photon Spectroscopy
  • RADAR
  • Organics and Life Detection
  • Sample Return

3
Getting to Mars
Lowest Energy Hohman Transfer Orbit
Pork Chop Plot
  • Mars launch opportunities occur every 26
    months
  • Type I trajectories require less than 180 deg
    transfer, 180 lt Type II lt 360, etc.
  • 8 months for Type 1 Transfer, 4 months using
    nuclear propulsion.
  • Launch vehicle requirements are determined by
    C3, the excess energy per unit mass (km/s)2
    required after reaching Earth escape velocity
    required to make the transfer

4
Deep Space Network (DSN)
  • NASAs Pioneer Deep Space Network provides
    radio communications via three principal stations
    at Goldstone, CA, near Madrid, Spain, and near
    Canberra, Australia
  • Each station has 70m and 34m antennas that can
    monitor multiple Mars spacecraft simultaneously
  • Data rates are a function of power, sensitivity,
    noise, encoding efficiency, and the directivity
    of antennas etc.
  • Landers can communicate to orbiters using UHF
    (Ultra High Frequency) 65 cm wavelength signals
    which are then relayed by the orbiters to the DSN

Band Wavelength Frequency Name Origin Uses
L 23 cm 1.3 GHz Long Long wavelength RADAR and low data rate
S 10 cm 3 GHz Short Low data Rate
X 3 cm 10 GHz X marks the spot for weapons targeting High data rate direct to earth communications
K, Ka and Ku 1.5 cm 20 GHz Kurt (German for short) K band has highest data rate, but significant water absorption, Ka (higher) and Ku (lower) frequency reduces effects of water, but still cant be used in bad weather
5
Getting Into Orbit
  • Mars Orbit Insertion (MOI) can be accomplished
  • Purely Propulsively - safest, larger rockets,
    more fuel)
  • Aerobrake Assisted (using the atmosphere to help
    slow down) - more risky, smaller rockets, less
    fuel
  • Aerocapture (using the atmosphere to do all the
    slowing down) - requires a first pass at 25 km
    altitude look out for Olympus Mons!, requires
    no fuel, but good heat shield and nerves of
    steel..
  • Aerobraking can be used to gradually circularize
    orbits, at the cost of time and some risk

6
Orbits
  • Orbits can be tailored to meet specific mission
    needs (mapping, communications, planetary
    protection etc.)
  • Orbits with periapses less than 200 km above
    the surface interact with the atmosphere and is
    not stable

Orbit Type Characteristics Pros/Cons Examples
Sun Synchronous Mapping 300 km circular, near polar, 1.52 hour period, with precession rate that matches Mars orbital period to give observations close to two times per day Pros Excellent global coverage at consistent and close range, consistent illumination Cons No nadir coverage within 2 degrees of poles, very high energy, incomplete hourly coverage, long eclipse durations MGS, Odyssey
Elliptical 250 km at periapsis and up to 40,000 km at apoapsis, periods from 8 to 24 hours Pros Low energy, stable, potential for improved time of day coverage, potential for unique science opportunities at periapsis Cons Instruments spend most of their time far from planet, with inconsistent surface resolution Viking (24 hour equatorial and high inclination) Mars Express (8 hour high inclination)
Synchronous Circular, Equatorial, period matched to planetary rotation rate (aerostationary) Pros Continuous visibility of fixed surface location, excellent for communications with the surface Cons Cant see other sides of planet, very far from planet (30,000 km) Future communications orbiters
7
Landing
  • At the top of the atmosphere Vtop Vinf
    Vesc, where Vinf is the vehicles approach
    velocity at infinite distance (not including the
    gravitational effects from Mars itself), and Vesc
    is the Martian escape velocity (5 km/sec).
  • Direct from Earth trajectories have Vinf that
    are greater than Vinf from orbit
  • The energy required to slow the vehicle from
    Vtop to 0 goes as the square of Vtop
  • The atmosphere of Mars is an aid to landing as
    it provides aerodynamic resistance
  • The atmosphere of Mars hinders landing due to
    unpredictable density variations and winds

Mars Pathfinder Accelerometer Data
  • Most of the energy is taken out by the aeroshell
    heat shield high in the atmosphere
  • Three types of terminal descent and landing
    systems. Rockets and landing legs, Airbags and
    Penetrators (no airbags or legs)
  • Score so far, Earth Vs. Mars Rockets and Legs
    (2 to 1), Airbags (4 to 2), Penetrators (0 to 2)
  • Landing failures can be caused by malfunction of
    landing system and by landing hazards/design
    weaknesses

8
Cartography - Latitude
  • Mapping surface features to coordinate systems,
    and keeping track of conventions can be tricky.
  • The northern hemispheric peoples won the battle
    over which hemisphere should be positive latitude
    years many years ago
  • Because of Mars oblate shape, there are two
    ways to measure latitude

Aerographic Latitude (f)
Aerocentric Latitude (f)
  • Aerographic latitude is favored by imaging teams
    because the local zenith angle is perpendicular
    to the surface (this makes measuring your
    latitude easier if you ever need to take your
    bearings using a sextant while on a boat at
    sea..)
  • Aerocentic latitude is favored by gravity and
    topography teams, and most modern, right-minded
    people, because spacecraft orbit the center of
    mass (this makes measuring your latitude easier
    when using modern spacecraft technology using the
    fewest assumptions)

9
Cartography - Longitude
  • Mapping longitude requires a reference
    longitude, and a sense of direction
  • The British established the Earths reference
    longitude at Greenwich
  • The International Astronomical Union (IAU) has
    established Mars zero longitude based on the
    position of the small crater Airy, or the Airy-0
    frame
  • The Mars reference longitude has been updated
    through time as the position of Airy has been
    better determined in Mars inertial frame
  • Early telescopic observers used a West-positive
    longitude system for Mars so that longitude would
    increase as they observed through the night
  • The convention has held on in some of the more
    backward circles (that include telescopic
    astronomers and Mars geologists that are
    unfamiliar with the most basic principles of
    algebra and geometry)
  • Most right minded and right-handed individuals
    prefer the East-positive longitude system because
    of the obvious and natural benefits of using a
    mathematically-sound, right-handed coordinate
    system.
  • Unbelievably, the different experiment groups on
    the MGS mission have archived their data using
    different conventions for both latitude and
    longitude, which makes comparison of datasets
    difficult for the uninitiated!
  • At least we dont use Martian Minutes and
    Martian Seconds when specifying fractional
    longitudes.

10
Map Projections
  • Mars is basically spherical, but its difficult
    to print out a sphere.
  • Desired qualities of a map projection
  • Equal Area preserves size relationships
    between large and small features
  • Conformal preserves the shapes of features,
    maps great circles as straight lines

Common Mars Map Projections
Mercator (conformal, non equal area)
Robinson (nonconformal, non equal area)
Stereographic (conformal, non equal area)
Sinusoidal (non-conformal, equal area)
11
Visible Imaging
  • Imaging is a key component of most Mars missions
  • The images can be used in fairly unprocessed
    forms for seeing whats there
  • Quantitative work with images requires multiple
    levels of processing
  • Level 1
  • Raw, unprocessed unmerged spacecraft data
    acquired from different ground stations
  • Level 0
  • Compressed, raw, unprocessed whole images
  • Level 1
  • Decompressed images merged with associated
    spacecraft and instrument geometry and timing
    data
  • Level 2Beautified, and geometrically corrected
    individual images with associated timing and
    solar geometry data
  • Level 3 Photometrically calibrated individual
    images with Level 2 geometry
  • Level 4
  • Higher-order image products, often employing
    multiple images to create color images, mosaics,
    stereo images, movies, maps, spectra etc.
  • Note The definitions of these various levels
    vary from experiment to experiment

12
Near IR Spectroscopy (Minerals)
  • Near IR spectroscopy can provide considerable
    information about the presence of various
    minerals
  • Caveats
  • Mixtures of minerals and/or minerals in low
    abundance can cause problems for whole rock or
    whole region spectra
  • Dust on top of rocks obscures rock signals
  • Atmospheric H20 and CO2 gas absorption can
    hinder orbital measurements

Laboratory reflectance spectra of (a) pure
igneous minerals, (b) iron oxides/hydroxides, (c)
anhydrous carbonates, (d) sulfates, (e) clays and
(f) nitrates
13
Near IR Spectroscopy (Volatiles)
  • CO2 gas and water vapor in the Martian
    Atmosphere absorbs strongly at 1.37, 2.0, and 2.7
    microns.
  • Water ice and CO2 ice have distinct absorption
    features, whose shapes are sensitive to grain
    size

Mars Express Omega Spectrometer Results Water Ice
(left), CO2 Ice (middle), Visible (right)
14
Thermal IR Radiometry and Spectroscopy
  • Objects at Martian temperatures emit radiation
    at infrared wavelengths (peak at 15-20 microns)
  • Emission can be measured from orbit, or from
    surface
  • Resulting spectra are determined by
  • Blackbody function for surface temperature
  • Absorption, emission by atmospheric gas and
    aerosols
  • Emissivity of the surface as a function of
    wavelength
  • Measurements can be made by
  • Spectrometers (resolved spectral features)
  • Radiometers (unresolved spectral features in
    spectral bands)

15
Atmospheric Properties from Thermal IR
Observations
The radiative effects of atmospheric temperature,
dust, water vapor etc. discussed in the last
lecture can be exploited to retrieve these
atmospheric properties from infrared spectra
MGS TES Multi-Year Atmospheric Retrieval Results
16
Surface Properties from Thermal IR Observations
  • IR observations can be used to infer the thermal
    state of the surface and near-subsurface, as well
    as aspects of the bulk thermal properties of
    materials
  • Key parameters
  • Surface Albedo As
  • Controls surface solar heating
  • Thermal Inertia I ( k ? c )1/2
  • Controls heat flux
  • Controls amplitude of temperature variations
  • Significant regional variations due to soil
    particle size, rock and ice abundance
  • Thermal inertia and Albedo determine daily
    average and annual average temperature
  • Thermal Skin Depth D ( ( k P ) / ( ? ? c ) )
    1/2
  • Controls penetration of diurnal and seasonal
    temperature waves
  • Annual skin depth is 26 times diurnal skin depth
  • For low thermal inertia soil, D (diurnal) 6.6
    mm, D (seasonal) 17 cm
  • For solid ice, D (diurnal) 25 cm, D (seasonal)
    6.5 meters

17
Surface Properties from Thermal IR Observations
For most geologic materials in the Martian
environment, the ?c product varies by less than
a factor of 2, whereas the thermal conductivity
varies by factors of 100, primarily due to the
effects gain size variations and atmospheric gas.
Implication Significant spatial variability in
thermal behavior good for remote sensing!
18
Martian Daily Surface Temperature Variations
A 0.2, I 50 (Low Thermal Inertia) A 0.2, I
250 (Mars Average) A 0.2, I 1000 (High
Thermal Inertia) A 0.5, I 250 (High Albedo)
  • The effects of albedo and thermal inertia can
    generally be separated
  • Albedo affects daily average temperature
  • Thermal inertia controls amplitude of daily
    temperature variation, with second-order effect
    on daily average temperature (low I soils have
    colder average temperatures)
  • Albedo and thermal inertia can be uniquely
    determined from two surface temperature
    measurements (day and night)
  • Thermal inertia can be guessed from a single
    pre-dawn surface temperature measurement, and an
    estimate of surface albedo

19
Global Albedo and Thermal Inertia
  • Albedo variations caused by distribution of
    bright surface dust relative to darker sand and
    rocks
  • High albedo regions generally correlated with
    low thermal inertia more bright fine-grained
    particles
  • Large low thermal inertia regions centered on
    Tharsis, Arabia, Elysium and South Polar regions

20
Temperature Variations With Depth
Surface D 5 mm D 20 mm D 37 mm D 67 mm
  • Surface temperature measurements can be fit with
    the results of models to infer
  • Annual Average Temperature
  • The presence of high thermal inertia material
    close to the surface
  • Mixtures of high and low thermal inertia
    material in the instrument field of view (rock
    abundance)

21
Annual Average Temperature and Rock Abundance Maps
The annual average temperature is equal to the
temperature at great depth (excluding the effects
of planetary heat flow)
Mid-Latitude Rock Abundance Map from Viking IRTM
Radiometer Data
22
Effects of Slopes on Annual Average Temperatures
Topographic slopes magnitudes and orientations
can affect insolation, and annual average
temperatures
0 K
Latitude
Latitude
Northward Slope (deg)
Eastward Slope (deg)
23
Thermal Emission Spectroscopy
  • lt10 variations in the infrared emissivity
    result in thermal emission spectra
  • Energies of IR photons similar to lattice
    vibration energies for many minerals
  • Thermal IR spectroscopy generally superior to
    Near IR spectroscopy for mineralogy
  • Identifying minerals on Mars is complicated by
  • Atmospheric gas and aerosols
  • Particle size effects (example spectra are for
    homogeneous slabs)
  • Mixing within spectrometer field of view
  • Rocks and minerals identified thus far from TES
    orbital spectra
  • Basalt
  • Andesite
  • Hematite
  • Carbonate

24
Laser Altimetry
  • MGS MOLA laser altimeter provides range to
    surface and clouds
  • MOLA spot size is 130 m, along track shot
    spacing is 330 m
  • Topographic profiles require MOLA data plus
    detailed spacecraft ephemeris based on radio
    tracking
  • Topographic maps require gridding of profiles
    from multiple orbits. MOLA gridded topographic
    maps available with resolutions as high as 1/128
    degree (500 m)
  • By measuring returned pulse width and inter-shot
    variability, MOLA data can be used to estimate
    surface roughness

25
MOLA Map Products
  • MOLA map products provide excellent quantitative
    information regarding elevations, slopes etc
  • MOLA maps can also be displayed as shaded relief
    maps, providing detailed morphology etc.
  • Using MOLA data as basemaps for dataset analyses
    instead of images has several advantages
  • Consistent resolution, lighting angles
  • No atmospheric, camera or mosaic artifacts (but
    no color or albedo info either..)
  • Extremely accurate feature locations in
    planetocentric coordinates
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