a short review the basic equation of transfer for radiation passing through gas: the change in...

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A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d = I - j / = I - S • Assumptions LTE… (all physical processes in balance) S = B Flux constant with depth Plane parallel atmosphere

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Page 1: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

A short review• The basic equation of transfer for

radiation passing through gas: the change in specific intensity I is equal to:

-dI /d = I - j/ = I - S

• Assumptions– LTE… (all physical processes in balance)

S= B

– Flux constant with depth– Plane parallel atmosphere

Page 2: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Black Body Radiation• walls heated• emit and reabsorb

radiation• interior of

chamber in thermodynamic equilibrium

• leakage in or out of the whole is small

• Stellar photospheres approximate blackbodies• Most photons are reabsorbed near where they are emitted• Higher in the atmosphere, a star departs from a black body

Page 3: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

See: http://homepages.wmich.edu/~korista/phys325.html

Page 4: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

See: http://www.jb.man.ac.uk/distance/life/sample/stars/index.html

Page 5: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

See: http://astro1.panet.utoledo.edu/~ndm/4810.html

Page 6: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Black Bodies - Observations

• spectrum continuous, isotropic, unpolarized• continuum intensity depends on frequency

and temperature• observed relation:

• From this observational result can be derived Wien’s law (peak intensity) and the Stefan-Boltzman law (luminosity)

• Also Rayleigh-Jeans approx. and Wien approx. of flux above and below BB peak

T

fI

3

Page 7: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Wien’s Law – Peak Intensity

Iis maxat max = 0.29/T ( in cm)

or’max = 0.51/T (where ’max is the wavelength at which I is max)

Thought Problem: Calculate the wavelengths at which I and I are maximum in the Sun. Think about why these are different.

Page 8: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Luminosity – Stefan Boltzman Law

• F = T4 or L = 4 R2 T4

• Class Problem: What is the approximate absolute magnitude of a DA white dwarf with an effective temperature of 12,000, remembering that its radius is about the same as that of the Earth?– what is the simplest approach?

Page 9: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Deriving the Planck Function• Several methods (2 level atom,

atomic oscillators, thermodynamics)• Use 2-level atom: Einstein

Coefficients– Spontaneous emission proportional to

Nn x Einstein probability coefficient

j = NuAulh

– Induced (stimulated) emission proportional to intensity

= NlBluh – NuBulh

Page 10: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Steps to the Planck Function

• Energy level populations given by the Boltzman equation:

• Include spontaneous and stimulated emission

• Solve for I, substitute Nu/Nl

• Note that

IBNIBNAN lululuulu

kTh

l

n

l

u eg

g

N

N /

u

lluul g

gBB ulul B

c

hA

2

32

Page 11: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Planck’s Law

• Rayleigh-Jeans Approximation (at long wavelength, h/kT is small, ex=x+1)

• Wien Approximation – (at short wavelength, h/kT is large)

1

12)(

/5

2

kThce

hcTB

1

12)(

/2

3

kThec

hTB

kThec

hI /

2

32

22

2

22 kt

ckTI

Page 12: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Class Problem

• The flux of M3’s IV-101 at the K-band is approximately 4.53 x 105 photons s–1 m–2 m-1. What would you expect the flux to be at 18 m? The star has a temperature of 4250K.

Page 13: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Using Planck’s Law

Computational form:

For cgs units with wavelength in Angstroms

1

1019.1)(

/1044.1

527

8

Txe

xTB

Page 14: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Class Problems

• You are studying a binary star comprised of an B8V star at Teff = 12,000 K and a K2III giant at Teff = 4500 K. The two stars are of nearly equal V magnitude. What is the ratio of their fluxes at 2 microns?

• In an eclipsing binary system, comprised of a B5V star at Teff = 16,000K and an F0III star at Teff = 7000K, the two stars are known to have nearly equal diameters. How deep will the primary and secondary eclipses be at 1.6 microns?

Page 15: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Class Problems

• Calculate the radius of an M dwarf having a luminosity L=10-2LSun and an effective temperature Teff=3,200 K. What is the approximate density of this M dwarf?

 • Calculate the effective temperature of a proto-

stellar object with a luminosity 50 times greater than the Sun and a diameter of 3” at a distance of 200 pc.

Page 16: A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =

Class Problems

• You want to detect the faint star of an unresolved binary system comprising a B5V star and an M0V companion. What wavelength regime would you choose to try to detect the M0V star? What is the ratio of the flux from the B star to the flux from the M star at that wavelength?

• You want to detect the faint star of an an unresolved binary system comprising a K0III giant and a DA white dwarf with a temperature of 12,000 K (and MV=10.7). What wavelength regime would you choose to try to detect the white dwarf? What is the ratio of the flux from the white dwarf to the flux from the K giant at that wavelength?