Dispersal of the Protoplanetary Disk Flashcards

towards the main sequence, lifetime of the dusty disk, dust removal mechanisms. radiation pressure, poyting-robertson effect

1
Q

What happens as stars move towards the main sequence?

A
  • major accretion and outflows have ended

- remnant (debris) disk around the young star

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2
Q

What happens as a star evolves?

A
  • inner region of the disk disappears first
  • disk loses dust and becomes fainter overtime
  • cool, black body hence a weaker emitter
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3
Q

Lifetime of the Dusty Disk

A
  • using measurements of infra-red ‘excess’, it can be deduced that disks disappear after 10-100 million years
  • as the disk is only around for ~10 million years, planets must form on this timescale
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4
Q

Momentum of a Photon

A

p = E/c

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5
Q

List two dust removal mechanisms

A
  • radiation pressure

- Poynting-Robertson effect

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6
Q

Dust Removal - Radiation Pressure

Force on a Dust Particle from Radiation

A

Fr = (flux of radiation / c) * projected area of a dust particle
Fr = Qoptπa²L*/4πr²c
-where Qopt is the extinction at optical wavelength, ~1 and a is the dust grain radius

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7
Q

Dust Removal - Radiation Pressure

Force on a Dust Particle due to Gravity

A

Fg = GMm/r² = 4/3 πa³ρGM/r²

-where ρ is the bulk density of the dust grain material

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8
Q

Dust Removal - Radiation Pressure

Blow-Out

A

-consider the balance of radiation and gravitational force on a dust grain
-if Fr>Fg, the grain will be blown out
-this process doesn’t depend on r at all:
a = 0.3 L(L☉)/M(M☉) μm
-dust particles ≤1μm will be blown out of a solar-like system, this is a very fast process, ~10^4yr

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9
Q

What are the issues with radiation pressure for explaining dust removal?

A
  • the equation has no dependence on radius, it affects particles at all radii equally so cannot explain inside-out clearing
  • the process is much faster than observed disk lifetimes of 10-100Myr
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10
Q

Dust Removal - Poyting-Robertson Effect

Relativistic Effects

A

-for a particle with Fr<

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11
Q

Dust Removal - Poyting-Robertson Effect

Rate of Change of Angular Momentum

A
-there is a tangential radiation pressure on the grain:
p = v/c pphot = vE/c²
-angular momentum:
L = mwr² = mvr
-rate of change of angular momentum:
dL/dt ∝ L/r²
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12
Q

Dust Removal - Poynting-Robertson Effect

Description

A
  • the dust grain due to the relativistic effect is experiencing a small retarding force so is loosing angular momentum
  • we are ultimately interested in how long it takes for the dust grain to spiral into the centre of the star
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13
Q

Dust Removal - Poynting-Robertson Effect

Time

A
t = 1/2 R² 2mc²/L*a²
= 1400 (a/μm)(R/AU)²/(L*/L☉) yr
-time is proportional:
t ∝ aR²/L*
-Poynting-Robertson effect clears the disk from the inside out and the smallest grains first
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14
Q

What are the problems with the Poytning-Robertson effect?

A
  • it is inconsistent with some observations
  • micron wavelength emission comes from micron-sized grains, too large, too cold grains otherwise
  • fits imply disk sizes of the order of ~100au
  • while few images actually show disks ~100au and smaller
  • this implies that dust grains lost to the star are somehow replenished
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15
Q

How are dust grains replenished?

A
  • best explanation is colliding asteroid, planetesimals etc. breaking down into smaller material
  • there is evidence for this in the solar system (E.g. craters in th moon)
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