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From temporal spectra to stellar interiors (and back). J ørgen Christensen-Dalsgaard Institut for Fysik og Astronomi, Aarhus Universitet Dansk AsteroSeismologisk Center. Overview. Pulsating stars in the HR diagram. Excitation mechanisms. Heat engine ( k mechanism, etc)
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From temporal spectra to stellar interiors (and back) Jørgen Christensen-Dalsgaard Institut for Fysik og Astronomi, Aarhus Universitet Dansk AsteroSeismologisk Center
Excitation mechanisms • Heat engine (k mechanism, etc) • Critical layer in the star is heated at compression • Mode is intrinsically unstable and grows exponentially • ???Amplitude limitation mechanism, mode selection ??? • Stochastic excitation • Mode is intrinsically damped • Excitation through stochastic driving by convection (compare church bell in sandstorm) • Resulting amplitudes from balance between forcing and damping
Observational differences 1/(Observing time) 1/(Lifetime) Heat engine mode Stochastically excited mode
Separated equations Separation of time as exp(- i t)
However, from hydrostatic equilibrium and Poisson’s equation p and g can be determined from r Hence adiabatic oscillations are fully characterized by or, equivalently Frequency dependence on stellar structure Frequencies depend on dynamical quantities:
Characteristic frequencies Acoustic frequency Buoyancy frequency:
In reality increased inertia owing to horizontal motion Internal gravity waves
Boundary conditions At centre At surface Equations and boundary conditions determine frequencies wnl
Cowling approximation High radial order Approximated equations
Model of present Sun Mode trapping Eigenfunction oscillates as function of r when
Large frequency separation: Asymptotics of low-degree p modes
Frequency separations: Small frequency separations
Structure of evolving star with convective core 2.2 M¯ (Scaling with tdyn to ZAMS)