Stellar Continua How do we measure stellar continua

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Stellar Continua • • How do we measure stellar continua? How precisely can we

Stellar Continua • • How do we measure stellar continua? How precisely can we measure them? What are the units? What can we learn from the continuum? – – Temperature Luminosity Metallicity Presence of binary companions • Bolometric corrections

Measuring Stellar Flux Distributions • Low resolution spectroscopy (R~600 or 50 -100 Å) •

Measuring Stellar Flux Distributions • Low resolution spectroscopy (R~600 or 50 -100 Å) • Wide spectral coverage • Access to fainter stars (why? ) • Use a large (but not too large) entrance aperture (why? ) • Correct for sky brightness and telluric extinction

Measuring Stellar Flux Distributions • Four steps – Select a standard star (Vega) –

Measuring Stellar Flux Distributions • Four steps – Select a standard star (Vega) – Measure the shape of standard star’s energy distribution (relative Fn vs. l) – Measure the standard star’s absolute flux at (at least) one wavelength – Correct for line absorption

Primary Photometric Standards • Vega (A 0 V) • For absolute flux, compare to

Primary Photometric Standards • Vega (A 0 V) • For absolute flux, compare to standard laboratory sources, usually black bodies • Flux measured in ergs cm-2 s-1 A-1 at the top of the Earth’s atmosphere • Often plotted as – – Fl vs. A Fn vs. wavenumber (cm-1 = 1/l in cm) Log Fl + constant vs. A Log Fn + constant vs. wavenumber

Stellar SEDs

Stellar SEDs

Calculating Fl from V • Best estimate for Fl at V=0 at 5556Å is

Calculating Fl from V • Best estimate for Fl at V=0 at 5556Å is Fl = 3. 36 x 10 -9 erg s-1 cm-2 Å-1 Fl = 996 photon s-1 cm-2 Å-1 Fl = 3. 56 x 10 -12 W m-2 Å-1 • We can convert V magnitude to Fl: Log Fl = -0. 400 V – 8. 449 (erg s-1 cm-2 Å-1) Log Fn = -0. 400 V – 19. 436 (erg s-1 cm-2 Å-1) • To correct from 5556 to 5480 Å: Log [Fl (5556)/Fl(5480)]=-0. 006– 0. 018(B-V)

What about the Sun? • Absolute flux uncertain by about 2% • Mv (~4.

What about the Sun? • Absolute flux uncertain by about 2% • Mv (~4. 82) uncertain by about 0. 02 mags • B-V even more uncertain • values range from 0. 619 to 0. 686

Practice Problems • Assuming an atmosphere + telescope + spectrograph+ detector efficiency of 10%,

Practice Problems • Assuming an atmosphere + telescope + spectrograph+ detector efficiency of 10%, how many photons would be detected per Angstrom at 5480 A using a 1. 2 -m telescope to observe a star with V=12 (and B-V=1. 6) for one hour? • Using the CTIO 4 -m telescope, an astronomer obtained 100 photons per A at 5480 A in a one hour exposure. Again assuming an overall efficiency of 10%, what was the magnitude of the star if B-V=0?

Bound Free Continua • Lyman – far UV • Balmer – UV • Paschen

Bound Free Continua • Lyman – far UV • Balmer – UV • Paschen – optical • Brackett – IR • Pfund – more IR

Interpreting Stellar Flux Distributions I. The Paschen Continuum • The Paschen continuum slope (B-V)

Interpreting Stellar Flux Distributions I. The Paschen Continuum • The Paschen continuum slope (B-V) is a good temperature indicator • Varies smoothly with changing temperature • Slope is negative (blue is brighter) for hot stars and positive (visual is brighter) for cooler stars • B-V works as a temperature indicator from 3500 K to 9000 K (but depends on metallicity) • For hotter stars, neutral H and H- opacities diminish, continuum slope dominated by Planck function, and the Rayleigh-Jeans approximation gives little temperature discrimination

The Paschen Continuum vs. Temperature 50, 000 K 4000 K

The Paschen Continuum vs. Temperature 50, 000 K 4000 K

Interpreting Stellar Flux Distributions II – The Balmer Jump • The Balmer Jump is

Interpreting Stellar Flux Distributions II – The Balmer Jump • The Balmer Jump is a measure of the change in the continuum height at 3647 A due to hydrogen bound-free absorption • Measured using U-B photometry • Sensitive to temperature BUT ALSO • Sensitive to pressure or luminosity (at lower gravity, the Balmer jump is bigger – recall that kbf depends on ionization, and hence on Pe) • Works for 5000 < Teff < 10, 000 (where Hbf opacity is significant)

Flux Distributions at T=8000 Log g = 4. 5 Log g = 1. 5

Flux Distributions at T=8000 Log g = 4. 5 Log g = 1. 5

Bolometric Flux • Bolometric flux (Fbol) is the integral of Fn over all wavelengths

Bolometric Flux • Bolometric flux (Fbol) is the integral of Fn over all wavelengths • Fbol is measured in erg cm-2 s-1 at the Earth • Luminosity includes the surface area (where R is the distance from the source at which Fbol is measured): • L is measured in units of erg s-1, R is distance, r is radius

Bolometric Corrections • Can’t always measure Fbol • Compute bolometric corrections (BC) to correct

Bolometric Corrections • Can’t always measure Fbol • Compute bolometric corrections (BC) to correct measured flux (usually in the V band) to the total flux • BC is usually defined in magnitude units: BC = m. V – mbol = Mv - Mbol

Bolometric Corrections from AQ

Bolometric Corrections from AQ

Class Problem • A binary system is comprised of an F 0 V star

Class Problem • A binary system is comprised of an F 0 V star (B-V=0. 30) and a G 3 IV star (B-V=0. 72) of equal apparent V magnitude. – Which star has the larger bolometric flux? – What is the difference between the stars in Mbol?