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Kepler frequency

Figure 11. The gravitational mass (in units of the solar mass M ) versus the normalized central energy density (eo = 156 MeV fm-3) (left panel) and versus the equatorial radius (right panel). The thin lines represent static equilibrium configurations, whereas the thick fines display configurations rotating at their respective Kepler frequencies. Several different stellar matter compositions are considered (see text for details). Figure 11. The gravitational mass (in units of the solar mass M ) versus the normalized central energy density (eo = 156 MeV fm-3) (left panel) and versus the equatorial radius (right panel). The thin lines represent static equilibrium configurations, whereas the thick fines display configurations rotating at their respective Kepler frequencies. Several different stellar matter compositions are considered (see text for details).
The analytical computation of critical ionization fields starts with an analysis of the widths of resonances in the classical phase space. Resonances occur whenever the ratio of the external driving frequency u and the unperturbed Kepler frequency Cl of the Rydberg electron is rational, i.e. [Pg.192]

Kepler Space Telescope a NASA-built optical space telescope that monitors 170000 stars continuously for four years to search for transiting exoplanets. The goal of the Kepler mission is to determine the frequency of Earth-sized planets around other stars. [Pg.355]

Both definitions are natural since wq turns out to be the ratio of the microwave frequency w and the Kepler firequency H of the Rydberg electron, and Sq is the ratio of the microwave field strength and the field strength experienced by an electron in the noth Bohr orbit of the hydrogen atom. Motivated by the above discussion we have redrawn the results obtained by Bayfield and Koch (1974) and present them in Fig. 7.2 as an ionization signal (in arbitrary units) versus the scaled field strength defined in (7.1.3). For no in (7.1.3) we chose no = 66, the centroid of the band of Rydberg states present in the atomic beam. [Pg.184]

While pattern formation, epitomized by beautiful snowflakes, was first liberated from theology by Kepler in 1611, it is only relatively recently some progress has been made in its scientific investigation [4]. Pattern formation refers to spatial structures, usually characterized by a band of wavelengths, that replace a uniform state above a critical distance from equilibrium. Patterns are nonequilibrium structures resulting from several dissipative processes characterized by diffusion constants. They are quantified by their wavevector, q, and their frequency, co. [Pg.483]

Traub WA (2011) Terrestrial, habitable-zone exoplanet frequency from Kepler. Astrophys J 745 20... [Pg.165]

Kepler s principal contribution is summarized in his laws of planetary motion. Originally derived semiempir-ically, by solving for the detailed motion of the planets (especially Mars) Ifom Tycho s observations, these laws embody the basic properties of two-body orbits. The first law is that the planetary orbits describe conic sections of various eccentricities and semimajor axes. Closed, that is to say periodic, orbits are circles or ellipses. Aperiodic orbits are parabolas or hyperbolas. The second law states that a planet will sweep out equal areas of arc in equal times. This is also a statement, as was later demonstrated by Newton and his successors, of the conservation of angular momentum. The third law, which is the main dynamical result, is also called the Harmonic Law. It states that the orbital period of a planet, P, is related to its distance from the central body (in the specific case of the solar system as a whole, the sun), a, by a. In more general form, speaking ahistorically, this can be stated as G M -h Af2) = a S2, where G is the gravitational constant, 2 = 2n/P is the orbital frequency, and M and M2 are the masses of the two bodies. Kepler s specific form of the law holds when the period is measured in years and the distance is scaled to the semimajor axis of the earth s orbit, the astronomical unit (AU). [Pg.17]

Fig. 7.16 An artist conception of water maser emission in the accretion disk of the accretion disk and radio jet around the black hole in the heart of the Seyfert galaxy NGC 4258. This accretion disk material lies within a few tenths of a parsec from a supermassive black hole. The disk is warped, rotating differentially according to Kepler s laws. The inset at the bottom of the graphic is a radio spectrum (intensity as a function of frequency or velocity) of the water maser emission. The white glints on the disk surface show the locations of regions where maser emission has been detected. Image courtesy of NRAO/AUl and Artist John Kagaya (Hoshi No Techou)... Fig. 7.16 An artist conception of water maser emission in the accretion disk of the accretion disk and radio jet around the black hole in the heart of the Seyfert galaxy NGC 4258. This accretion disk material lies within a few tenths of a parsec from a supermassive black hole. The disk is warped, rotating differentially according to Kepler s laws. The inset at the bottom of the graphic is a radio spectrum (intensity as a function of frequency or velocity) of the water maser emission. The white glints on the disk surface show the locations of regions where maser emission has been detected. Image courtesy of NRAO/AUl and Artist John Kagaya (Hoshi No Techou)...

See other pages where Kepler frequency is mentioned: [Pg.131]    [Pg.182]    [Pg.196]    [Pg.289]    [Pg.131]    [Pg.182]    [Pg.196]    [Pg.289]    [Pg.333]    [Pg.393]    [Pg.184]    [Pg.200]    [Pg.57]    [Pg.52]    [Pg.507]    [Pg.217]    [Pg.263]   
See also in sourсe #XX -- [ Pg.182 , Pg.184 , Pg.192 , Pg.196 , Pg.289 ]




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