Radiative Transfer Flashcards

(31 cards)

1
Q

What is Jy?

A

Janksy
It is a unit of spectral flux density, designed for the low energies of radio astronomy.
1Jy = 10^-26 W m^-2 Hz^-1

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2
Q

What is the integral for Energy?

A

dE = Iν dA dt dΩ dν
E: energy
Iv: intensity at a specific frequency
A: area
t: time
Ω: solid angle
ν: frequency

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3
Q

What is the integral for intensity?

A

dI = Iν dν
I: intensity
Iv: intensity at a specific frequency
ν: frequency

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4
Q

What is the integral for flux?

A

dF = Iν dΩ dν
F: flux
Iv: intensity at a specific frequency
Ω: solid angle
ν: frequency

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5
Q

What is the integral for luminosity?

A

dL = Iν dA dΩ dν
L: luminosity
Iv: intensity at a specific frequency
A: area
Ω: solid angle
ν: frequency

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6
Q

What is av?

A

Absorption coefficeint
m^-1

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7
Q

what is jv?

A

Emmission coeffficeint
W m^-3 Hz^-1 sterad^-1

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8
Q

What is τv?

A

Optical depth

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9
Q

What do different values of τv mean?

A

τ ≥ 1 optically thick (opaque)
τ &laquo_space;1 optically thin (transparent)

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10
Q

What is the general radiative transfer equation?

A

Iν = I0 exp(-τv) +Sv(1-exp(-τv))

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11
Q

What is Sv?

A

Source function
= jv / av

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12
Q

What happens to the radiative transfer equation if the medium is optically thin?

A

τv &laquo_space;1
exp(-τv) ≈ 1 - τ

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13
Q

What happens to the radiative transfer equation if the source is emmits thermally?

A

Sv = jv / av = B(v,T)
B(v,t): Plank’s black body function.

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14
Q

What happens to Plank’s black body function at low frequencies?

A

(exp(-hv/kT) -1) ≈ hv/kT

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15
Q

What is the equation for dust’s optical depth?

A

τv = kv NH μ mp
τv: optical depth
NH: column density of H atoms
μ: mean molecular weight
mp: mass of proton

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16
Q

What happens to the radiative transfer equation if there is no background source?

17
Q

What happens to the radiative transfer equation if the medium is optically thick?

A

exp(-τv) ≈ 0

18
Q

What is the Lynman Series?

A

Hydrogen lines.
N=1 upwards
UV

19
Q

What is the Balmer Series?

A

Hydrogen lines.
N=2 upwards
Visable
Halpha is N=2 and N=3

20
Q

What is the Paschen Series?

A

Hydrogen lines.
N=3 upwards
IR

21
Q

Where is Bremstrahlung Radiation found?

A

Local group: HII regions (cm and microwave)
Extragalactic: galaxy clusters (X-rays)

22
Q

Where is Synchrotron Radiation found?

A

Local group: SN remnants (radio, IR, visible, x-ray), Diffuse ionised gas (radio).
Extragalactic: Galaxy jets (radio, X-ray)

23
Q

What is Bremstrahlung Radiation?

A

Radiation which is emitted when an electron is accelerated by nuclei, through the Coulomb force.

24
Q

What is the E field in Bremstrahlung?

A

E = (q |a| sinθ ) / (4 π ε₀ r c^2)
E: E field strength
q: charge
a: acceleration of charge
θ: angle between the direction of movement and the observer.
r: distance from charge

25
How are E and B related for Bremsstrahlung radiation?
B = |E| / c
26
How is Larmor's formula derived?
B = |E| / c S = E B / μ0 dP = |S| dA
27
In the emission coefficeint equation what are Z^2 e^6, n ne, exp(-hv/kT) ?
Z^2 e^6: that power output is proportional to attraction in the Coulomb force. n ne: emission is proportional to the density of nuclei and electrons. exp(-hv/kT): Comes from the Maxwellian velocity distribution of electrons.
28
What is gff (v,T)?
Gautt factor. gff ∝ v (usually) gff ≈ 1 (Radio)
29
What is synchrotron radiation?
Radiation is emitted by the acceleration of electrons by a strong magnetic field. Does not obey the plank function
30
What is different between the Larmor's formula for synchrotron and bremsstrahlung radiations?
Synchrotron has to factor in relativity, and Bremstrahlung doesn't. P ∝ γ^4
31