ASTR 400/700: Stellar Astrophysics Stephen Kane Stellar Pulsation Chapter 14.1, 14.2 Stellar Models: The complete set of differential equations describing the interiors of stars is therefore: Equation of Continuity: Hydrostatic Equilibrium: Energy Generation: Temperature Gradient: dM ( r ) = 4π r 2 ρ dr dP − G M ( r ) ρ = dr r2 dL = 4π r 2 ρ ε dr − 3 κ ρ Lr dT = 3 2 dr 4 ac T 4 π r rad − 1 GM ( r ) dT = 2 dr C r ad P If a star is neither expanding nor contracting, we may assume that throughout the star there is a balance between pressure and 1. 2. 3. 4. temperature density luminosity gravity RR Lyrae variables in the globular cluster M3 (one night’s observation) http://www.astro.princeton.edu/~jhartman/M3_movies.html Observations of Pulsating Variables • • First noticed in 1595 by David Fabricius. Mira would be 2nd magnitude at its brightest…then would “vanish”… Believed to be due to dark splotches on rotating star… Delta-Cephei John Goodricke discovered in 1784 that the brightness of Delta-Cephei was variable with a period of about 5 days!!!! Prototype of the classical cepheid variable star magnitude varies from 3.4 to 4.3, luminosity changes by factor of 100(∆m/5) = 100(0.9/5) = 2.3 Period-Luminosity Relation Stars of the “Classical Cepheid Variable” type in the Small Magellanic Cloud were observed…and found to have a strong correlation between Period and apparent magnitude… • Henrietta Swan Leavitt discovered and classified ~2400 classical cepheid variable stars • Periods 1-50 days • She plotted luminosity vs. period for a set of cepheids from the Small Magellanic Cloud and found the Period-Luminosity relation Henrietta Swan Leavitt (1868-1921) • Ability to measure Distances !!!!! Period-Luminosity Relation Notice that there is scatter… Calibration of Cepheids The nearest Cepheid is Polaris (~200 pc), too far for trigonometric parallax. d (pc) = 1/p (in arcsec) In 1913, Ejnar Hertzsprung of Denmark used least squares mean parallax to determine the average magnitude M = -2.3 for a Cepheid with Π = 6.6 days. d (pc) = 4.16/slope (in arcsec/yr) (4.16 AU/yr is the Sun’s motion) Calibration of Cepheids • Relation between average V band absolute magnitude and Period Cepheid Calibration-Infrared • Improved calibration at infrared wavelengths that suffer less from extinction • Adding a color term gives further improvement How to Find the Distance to a Pulsating Star • • • • Find the star’s apparent magnitude m (just by looking) Measure the star’s period (bright-dim-bright) Use the Period-Luminosity relation to find the stars absolute magnitude M Calculate the star’s distance (in parsecs) using d (pc) = 10(m-M+5)/5 Pulsation Hypothesis for Brightness Variation • Shapley proposed that the observed variation in brightness and temperature caused by radial pulsations of single stars. • Rhythmically “breathing” in and out! • R varies-->causes Luminosity and temperature to vary • Sir Arthur Eddington provided theoretical framework that could explain the variations in Brightness, temperature, radius and surface velocity • Delta-Cephei: supergiant star. Radius varies by 5%-10% (~1 solar radius). F5(hottest)-G2(coolest) • Star is brightest when its surface is expanding outward most rapidly, after it has passed through its minimum radius…phase lag Delta-Cephei The Instability Strip • Majority of pulsating stars lie in the instability strip on the H-R diagram • As stars evolve along these tracks they begin to pulsate as they enter the instability strip and cease oscillations once they leave it. ∆T ~ 600 – 1100 K Classes of Pulsating Stars Type Range of Periods Population Type Type of Oscillation Long-Period Variables 100 – 700 days I, II R Classical Cepheids 1 – 50 days I R W Virginis stars 2 – 45 days II R RR Lyrae stars 1.5 – 24 hours II R d Scuti stars 1 – 8 hours I R, NR b Cephei stars 3 – 7 hours I R, NR DAV stars 100 – 1000 s I NR The Physics of Stellar Pulsation • The radial oscillations of a pulsating star are the result of sound waves resonating in the stars interior • Pulsation period can be roughly estimated from how long it takes a sound wave to cross the star’s diameter Standing sound waves in an organ pipe. Radial modes for a pulsating star
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