Asteroid Themophysical Modeling Assuming Ellipsoid Shapes Eric - - PowerPoint PPT Presentation

asteroid themophysical modeling assuming ellipsoid shapes
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Asteroid Themophysical Modeling Assuming Ellipsoid Shapes Eric - - PowerPoint PPT Presentation

Asteroid Themophysical Modeling Assuming Ellipsoid Shapes Eric MacLennan & Joshua Emery Thermal Models for Planetary Science III Budapest, Hungary February 20 th , 2019 Outline Ellipsoid Shape TPM Method Traditional Approach


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Asteroid Themophysical Modeling Assuming Ellipsoid Shapes

Eric MacLennan & Joshua Emery

Thermal Models for Planetary Science III Budapest, Hungary February 20th, 2019

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Outline

Ellipsoid Shape TPM Method

  • ‘Traditional’ Approach
  • Description & Application
  • Validation Testing

Implementation & Analysis

  • Thermal Inertia of objects observed by WISE
  • Thermal Conductivity/Grain Size Modeling
  • Asteroid Population Grain Size Analysis
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SLIDE 3

‘Traditional’ TPM

Bennu

(from Emery et al., 2014)

  • 1. calculate surface energy

budget across shape model

  • 2. numerically solve the 1-D

heat diffusion equation for each shape facet (top)

  • 3. calculate the emitted flux

from surface temperatures

  • 4. integrate over entire

surface to calculate emitted flux value for desired wavelength(s)

  • 5. adjust TPM parameters to

find best-fit to the data

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Ellipsoid TPM

sphere ellipsoid

  • 1. calculate surface energy budget across

sphere

  • 2. numerically solve the 1-D heat

diffusion equation for each facet

  • 3. transform surface temperatures to

prolate (b = c) ellipsoid

  • 4. calculate the emitted flux from surface

temperatures

  • 5. integrate over entire surface to

calculate emitted flux value for desired wavelength(s)

  • 6. extract lightcurve mean and amplitude
  • 7. adjust TPM parameters and spin axis

to find best-fit to *multi-epoch* data

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SLIDE 5

Multi-epoch Data

  • pre-/post-opposition data guarantee
  • bservations of morning & afternoon
  • sense of spin determines morning/

afternoon temperate asymmetry

  • thermal inertia affects the flux change

as a function of phase angle

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𝛥 = 40 (SI) 𝛥 = 200 (SI) 𝛥 = 40 (SI) 𝛥 = 200 (SI)

Af Afternoon Mo Morni ning ng

100 142 185 227 270

Temperature (K)

𝛥 = 40 𝛥 = 200 𝛥 = 2000

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Validation using Synthetic Dataset

convex asteroid shape model from DAMIT surface temperatures pre-select TPM parameters, Deff, Γ, etc. calculate multi-epoch emitted flux fit ellipsoid models to flux dataset search for parameter combination that minimizes chi-square

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SLIDE 7

Validation Results

  • The best-fit diameter

closely follows the expected (model) diameter, within 10%

b

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SLIDE 8

Validation Results

  • The best-fit thermal

parameter closely follows the synthetic (model) thermal parameter, Θ

d

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SLIDE 9

TPM Results on WISE Data

Inverse relationship between thermal inertia and asteroid size Analysis:

  • 1. Use thermal inertia in a

thermal conductivity model to estimate the grain size

  • 2. Run multivariate model
  • n grain size data
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Model effective thermal conductivity: keff = a + bT3

keff = kgas + ksolid + krad

Thermal Conductivity Model

Observed effective thermal conductivity:

keff

eff =

= 𝛥2C C

C = ρcϕ, heat capacity ρ, grain density c, volumetric heat capacity ϕ, porosity

  • a & b from G&B (2013)
  • use spectral classification to infer the

grain density and heat capacity

  • assume several values of porosity to

account for uncertainty

Gundlach & Blum (2013)

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SLIDE 11

Grain Size Estimation

thermal conductivity model

ρ, c & other material properties

run 1 million times dϕ= log2(2rg)

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Grain Size Results & Model Fit

Used multivariate linear model to fit a linear function to grain size (dependent variable) and both independent variables (diameter and rotation period)

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Compositional Differences

grain sizes of S-types are slightly below average grain sizes of P-types are below average, E- types slightly above average M-types exhibit 4 x greater regolith grain size

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Thank You!

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Compositional Properties

E pV > 0.42 M 0.12 < pV < 0.42 P pV < 0.12

  • Link spectral groups with meteorite analog
  • Use meteorite ρ, c in conductivity model

ρ ≈ 3500 kg m-3 c ≈ 650 J kg-3K-1 ksolid ≈ 4 Wm-1K-1 ρ ≈ 2700 kg m-3 c ≈ 650 J kg-3 K-1 ksolid ≈ 0.6 Wm-1K-1 ρ ≈ 7500 kg m-3 c ≈ 400 J kg-3 K-1 ksolid ≈ 25 Wm-1K-1

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impact generation & ejection of regolith impact gardening of existing regolith M-t

  • types –

– diff comp mposition

  • r me

mechanical property?

estimated weathering timescale is 750 kyr – 1.5 My, which is longer than lifetime of a 1 km asteroid (200 kyr)

(Basilevsky et al., 2013; Holsapple et al, 2002)

above trend is consistent with modeling prediction

  • f fast sunrises = greater thermal stress

(Molaro & Byrne, 2012)

Regolith Generation & Loss