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Hubbles Constant

The age of the Universe is the inverse of the Hubble constant. The system of units must first be rationalised to convert all of the light-years into kilometres and then years, so that ... [Pg.34]

Hubble constant The numerical constant, H, that relates the red shift of a galaxy to its... [Pg.311]

M. Schwarzschild, A. Sandage and others pioneer theory of stellar evolution without extensive mixing and apply it to HR diagrams of globular clusters getting ages of several Gyr, comparable to the new inverse Hubble constant. [Pg.402]

Hubble s crucial observation was that, in every direction one looks, the farther away a galaxy is, the more the light from that galaxy is red-shifted. If the red shift is a Doppler shift, this implies that the farther away the galaxy is, the faster it is moving away from us. The most reasonable explanation for this observation is that the universe is uniformly expanding everywhere. The current best estimate for the Hubble Constant, which describes the rate of expansion, is 70.8 km s-1 megaparsec-1, with an uncertainty of 5.6%. [Pg.57]

J. P. Vigier, G. Le Denmat, M. Moles, and J. L. Nieto, Possible local variable of the Hubble constant in VanDenBergh s calibration of Sc-type galaxies, Nature, 257, 773 (1975). [Pg.190]

Again, Fuli [41] established a relation between nonzero photon mass and the Hubble constant H. Using that relation, one obtains... [Pg.600]

Now measuring the conductivity in vacuo, one can obtain an estimate of Hubble constant. This gives rise to a new possibility to test cosmological models in laboratory experiments. [Pg.600]

Figure 9.21. Cloud of points from a Monte Carlo Markov chain sampling of the likelihood of models fit to the WMAP plus other CMB datasets. The size of the points indicates how consistent the model is with the HST Key Project on the Distance Scale value for the Hubble constant. The contours show the likelihood computed for 230 Type la supernovae (Tonry et al., 2003). Figure 9.21. Cloud of points from a Monte Carlo Markov chain sampling of the likelihood of models fit to the WMAP plus other CMB datasets. The size of the points indicates how consistent the model is with the HST Key Project on the Distance Scale value for the Hubble constant. The contours show the likelihood computed for 230 Type la supernovae (Tonry et al., 2003).
Because the matter density VLmh2 was fairly well constrained by the amplitudes, the positions of a point in Figure 9.21 served to define a value of the Hubble constant. The size of the points in Figure 9.21 indicates how well this derived Hubble constant agrees with the H0 = 72 8 from the HST Key Project (Freedman et al., 2001). Shown as contours are the Ax2 = 1, 4, 9 contours from my fits to 230 SNe la (Tonry et al., 2003). Clearly the CMB data, the HST data, and the SNe data are all consistent at a three-way crossing that is very close to the flat Universe line. Assuming the Universe actually is flat, the age of the Universe is very well determined 13.7 0.2 Gyr. [Pg.170]

For completeness, we present here the equations governing the evolution of an FRW Universe. First, we define the expansion rate as the value of a/a, where the overdot is a time derivative the value of the expansion rate today is the Hubble Constant,... [Pg.177]

The data are consistent with other cosmological observations, including the Hubble constant, Ho = 71 JJ [ km/s/Mpc, and the baryon density, QBh2 = 0.0224 0.0009. [Pg.191]

The simplest method is to assume that all supernovae are identical. This is, of course, not true (see previous paper) but it turns out that the subclass of the Type la supernovae is indeed rather homogeneous. The first to plot a Hubble diagram of Type la Supernovae was Kowal Kowal 1968. There are essentially three quantities that can be derived from such a Hubble diagram in the nearby universe the slope of the expansion line, the scatter around the expansion line and the value of the local Hubble constant from the intercept at zero redshift (e.g. Tammann Leibundgut 1990 Leibundgut. Pinto 1992). The slope gives an indication of the local expansion and for a linear expansion in an isotropic universe it has a fixed value. The scatter around the expansion line provides a measure of the accuracy of the standard candle and the measurement errors. The intercept of the line, finally, together with an estimate of the... [Pg.208]

Recently, Mario Hamuy has realised that the expansion velocity and the luminosity during the plateau phase correlate and that Type II SNe may be quite good distance indicators Hamuy. Pinto. 2002. The distance accuracy achieved this way can be better than 20%. These determinations are based on the physical understanding of the plateau phase of SNe II and are linked to physics of the supernova atmosphere. This means that they are independent of the distance ladder, which is needed, e.g., for the SNe la. Typical values for the Hubble constant from SNe II are in the range of 65 to 75 km s-1 Mpc-1 Hamuy 2003. [Pg.210]

Re Entries [8]-[ll], Refs. [2], [8], [10], and [11]) As per Entries [8]—[11], results for the Hubble constant have improved with time, asymptotically converging onto those provided by Ref. [11]. The results for the Hubble constant as per Ref. [8] are in essential agreement with Entry [9]. The history of values of the Hubble constant also is briefly discussed in Entry [9] and Ref. [10]. Reference [10] surveys the history of values of the Hubble constant determined via work done through 2012. Reference [10] was for sale at the 27th Texas Symposium on Relativistic Astrophysics, held at the Fairmont Hotel in Dallas, Texas, December 8-13, 2013. [Pg.225]

In order to compare numbers across the decades, it is essential to allow for changes in the best estimate of the cosmic distance scale or the Hubble constant (H). In most cases, the L that you deduce for a galaxy (etc.) from its brightness will be proportional to the square of its distance, d, or to H 2, and the mass you calculate, from some form of M = V2R/G, will be proportional to d or H 1. Thus M/L scales as d 1 or H, and a velocity dispersion for a cluster of galaxies plus its angular size on the sky that led to M/L = 1000 for H = 500 km/sec/Mpc now, with H - 70 km/sec/Mpc, corresponds to M/L = 140. When Schwarzschild produced his table, the community was just incorporating the first of the large drops in H, from about 500 to 250 km/sec/Mpc. [Pg.184]


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