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Surface brightness

Fig. 5.3. Schematic view offerees encountered when the tip touches the sample surface. Bright circles symbolize tip atoms, dark circles symbolize sample atoms. Fig. 5.3. Schematic view offerees encountered when the tip touches the sample surface. Bright circles symbolize tip atoms, dark circles symbolize sample atoms.
Figure 5.8 Images observed during the adsorption of 02 on the CO-saturated RuO2(110) surface. Bright dots are CO-cus molecules along the <001 > direction dark sites in (a) are vacancies. The circle shows the development of a vacancy with time at an oxygen pressure of 2 x 10 8 Torr at room temperature. (Reproduced from Ref. 28). Figure 5.8 Images observed during the adsorption of 02 on the CO-saturated RuO2(110) surface. Bright dots are CO-cus molecules along the <001 > direction dark sites in (a) are vacancies. The circle shows the development of a vacancy with time at an oxygen pressure of 2 x 10 8 Torr at room temperature. (Reproduced from Ref. 28).
Scl is a close companion of the Milky Way, at a distance of 72 5 kpc [7], with a low total (dynamical) mass, (1.4 0.6) x 107Mq [8], and modest luminosity, My = —10.7 0.5, and central surface brightness, Soy = 23.5 0.5 mag/arcsec2 [9] with no HI gas [10]. CMD analysis, including the oldest Main Sequence turnoffs, has determined that this galaxy is predominantly old and that the entire star formation history can have lasted only a few Gyr [11]. [Pg.214]

Fig. 3.46. Radial trend of Mg2 index in the elliptical galaxy NGC 4881, after Thomsen and Baum (1987). 1 arcsec = 500 pc, the surface brightness in the adjoining continuum decreases from 17th to 26th magnitude per square arcsec over the range of the diagram in accordance with de Vaucouleurs law I a e r/a)V4 and a and b refer to observations taken on separate dates. Courtesy Bjarne Thomsen. Fig. 3.46. Radial trend of Mg2 index in the elliptical galaxy NGC 4881, after Thomsen and Baum (1987). 1 arcsec = 500 pc, the surface brightness in the adjoining continuum decreases from 17th to 26th magnitude per square arcsec over the range of the diagram in accordance with de Vaucouleurs law I a e r/a)V4 and a and b refer to observations taken on separate dates. Courtesy Bjarne Thomsen.
Parameters of dynamically hot galaxies , i.e. various classes of ellipticals and the bulges of spirals, generally lie close to a Fundamental Plane in the 3-dimensional space of central velocity dispersion, effective surface brightness and effective radius or equivalent parameter combinations (Fig. 11.10). This is explained by a combination of three factors the Virial Theorem, some approximation to... [Pg.356]

Check the cleanliness of cleanroom surfaces bright light or ultraviolet light for sampling location guiding. [Pg.1031]

Figure 1 shows the polarization vectors at K superposed on the surface brightness map and Figure 2 shows the radial distribution of the polarized intensity. The infrared envelope is roughly circular symmetric with radial extent greater than 1 arcmin ( 0.09 pc), comparable to the size of the molecular gas... [Pg.181]

Figure Surface brightness and polarization map of IRC+10216 in the K band, with the beam size of 20" and 12", respectively. Filled and open circles in the middle of the polarization vectors indicate positions of polarimetry made in 1987 January and February, respectively. Figure Surface brightness and polarization map of IRC+10216 in the K band, with the beam size of 20" and 12", respectively. Filled and open circles in the middle of the polarization vectors indicate positions of polarimetry made in 1987 January and February, respectively.
Almost a quarter of a century before the photometric attempts we have just mentioned were carried out, Greenstein (1940) had called attention to the fact that in the spectrum of the 137.94-day period binary u Sagittarii (B2 by the high excitation lines early A by the metallic lines fainter companion smaller and of larger surface brightness) H is very weak and He is strong. [Pg.199]

On the other hand, an ingenious proposal by Mullan (1975) apparently rescues the Lucy model. The Mullan proposal populates the primary component photosphere with starspots. These reduce the average surface brightness, thereby reduce the light loss at transit eclipse, and produce W-type light curves. This proposal has been received favorably by many specialists in the binary star field. [Pg.214]

We begin with an introduction to a simple model first proposed by Cavaliere and Fusco-Femiano (1976). This model assumes that the gas and galaxies are in equilibrium within the same gravitational potential. Through a measure of the X-ray surface brightness, the model relates the gas temperature to the cluster velocity dispersion, measured from the galaxies. [Pg.33]

The X-ray surface brightness is found by integrating the square of the gas density along the line of sight ... [Pg.34]

Thus, by measuring the gas temperature T, and the slope of the gas density distribution (or that of the surface brightness distribution), the radial distribution of the total gravitating mass can be found. [Pg.35]

Figure 2.7. The X-ray observables surface brightness profile and projected gas temperature and their simple derivatives, deprojected temperature, gas density, and gas pressure for the regular galaxy A478 (Sun et al. 2003). (top left) Surface brightness (0.5 - 5 keV) distribution, (upper right) electron density, (lower left) gas temperature, (lower right) gas pressure. Only statistical uncertainties are shown (1 a random errors). In the temperature profile, the data points with small circles are projected temperatures, while the data points with large filled circles are deprojected (three dimensional) values. Figure 2.7. The X-ray observables surface brightness profile and projected gas temperature and their simple derivatives, deprojected temperature, gas density, and gas pressure for the regular galaxy A478 (Sun et al. 2003). (top left) Surface brightness (0.5 - 5 keV) distribution, (upper right) electron density, (lower left) gas temperature, (lower right) gas pressure. Only statistical uncertainties are shown (1 a random errors). In the temperature profile, the data points with small circles are projected temperatures, while the data points with large filled circles are deprojected (three dimensional) values.
Figure 2.10 The flat-fielded Chandra image in the energy band 0.5-2.5 keV with a King model subtracted to remove the large scale radial surface brightness gradient. Many faint features are seen including 1) the prominent eastern and southwestern arms and their bifurcation (El, E2 and SI, S2 identify the extensions of the eastern and southwestern arms), 2) the 14 kpc (3 ) ring, 3) the 17 kpc (3.75 ) arc, and 4) the faint southern 37 kpc (8 ) arc. Figure 2.10 The flat-fielded Chandra image in the energy band 0.5-2.5 keV with a King model subtracted to remove the large scale radial surface brightness gradient. Many faint features are seen including 1) the prominent eastern and southwestern arms and their bifurcation (El, E2 and SI, S2 identify the extensions of the eastern and southwestern arms), 2) the 14 kpc (3 ) ring, 3) the 17 kpc (3.75 ) arc, and 4) the faint southern 37 kpc (8 ) arc.
A second partial ring is seen to the west at a radius of 17 kpc (3.75 ) extending over 60° in azimuth (see Fig. 2.10b). To form this surface brightness enhancement, a disturbance traveling at the sound speed would have originated... [Pg.40]

Unfortunately, observations seem to be in mild disagreement with this predicted profile merr. A low CDM concentration is observed in low surface brightness dwarf galaxies where the rotation curve is well measured. The predicted dark matter cusp is not usually seen the typical profile has a soft core, although the interpretation is compounded by issues of disk inclination, of the HI distribution which is usually used to measure the rotation curve, and of the possible mismatch between baryon and CDM potential well depths. [Pg.268]

Radiation intensities are referred to the radiation of a black body. In the radio frequency range it is convenient to express line intensities in equivalent line brightness temperatures, since the surface brightness Bv of a black body... [Pg.36]

Qualitative abundance ratios of HjO /CO have been derived from surface brightnesses of ionized gas tails by a comparison of red sensitive to blue sensitive plates for 13 comets by Miller . The comets could be grouped into three classes, one containing 5 comets with relatively high HjO brightness, one containing 4 comets with moderate H O brightness and a third class with 4 comets which had a very weak red tail. However, there was no noticeable dependence on the comets orbital parameters or heliocentric distances. [Pg.92]

Figure 5 shows an STM image of a stoichiometric (1x1) surface. Bright and dark rows run along the [001] direction. The distance between the rows is... [Pg.452]


See other pages where Surface brightness is mentioned: [Pg.292]    [Pg.275]    [Pg.195]    [Pg.213]    [Pg.2]    [Pg.84]    [Pg.85]    [Pg.112]    [Pg.243]    [Pg.357]    [Pg.358]    [Pg.358]    [Pg.366]    [Pg.373]    [Pg.386]    [Pg.214]    [Pg.217]    [Pg.311]    [Pg.30]    [Pg.32]    [Pg.34]    [Pg.36]    [Pg.83]    [Pg.229]    [Pg.295]    [Pg.316]    [Pg.138]    [Pg.203]    [Pg.235]   
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