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Weight density

Properties unfilled Fow-density Medium-density High-density weight high-density copolymer... [Pg.1049]

The physics and modeling of turbulent flows are affected by combustion through the production of density variations, buoyancy effects, dilation due to heat release, molecular transport, and instabiUty (1,2,3,5,8). Consequently, the conservation equations need to be modified to take these effects into account. This modification is achieved by the use of statistical quantities in the conservation equations. For example, because of the variations and fluctuations in the density that occur in turbulent combustion flows, density weighted mean values, or Favre mean values, are used for velocity components, mass fractions, enthalpy, and temperature. The turbulent diffusion flame can also be treated in terms of a probabiUty distribution function (pdf), the shape of which is assumed to be known a priori (1). [Pg.520]

Usually a good deal of experimentation is needed before a substance can be considered to be pure. Even then, much more work and study are needed before one can decide with confidence that a given pure substance is an element or a compound. Consider the substance water. Water is probably the most familiar substance in our environment and all of us recognize it easily. We are familiar with its appearance and feel, its density (weight per unit volume), the way in... [Pg.28]

The SPRITE signal equation is identical to Eq. (3.4.1) and it is possible to acquire density weighted images in the same manner as an SPI experiment. The TR in a SPRITE experiment is only a few milliseconds, which is similar to the Tj of a concrete specimen. Therefore to remove this influence from the image, a can be... [Pg.288]

The density weighted images and their absolute quantification demonstrated through concrete drying experiments are very powerful tools for material science. [Pg.293]

The SPI and SPRITE class of measurements for imaging short MR signal lifetimes are quantitative and have signal equations that are readily understood. The centric SPRITE methods are much faster and feature signal equations that are easier to interpret. This feature makes these measurements more readily density weighted and better suited to imaging quadrupolar nuclei. [Pg.302]

The measurement applications of density weighted drying profiles, water ingress, water phase transitions, crack detection, chlorine, sodium and lithium imaging applied to cement-based materials can be easily translated to other porous media. Density weighted MRI will no doubt prove to be a powerful tool in material science research. [Pg.302]

Listed Alphabetically) Conformation Structure Type Density Weight... [Pg.43]

The near-absence of DLAs with log N/n > 13.2, corresponding to an obscuration of the order of one magnitude in the rest-frame UV, supports the existence of some obscuration and implies some biases in the H I column density distribution and perhaps in the column-density-weighted metallicity, but these cannot be very large (Akerman et at. 2005). The type of object that can be missed is one not shown in the figure a system at a redshift of 0.52 towards the BL Lac object4 AO 0235 +164, with an H I log column density of about 21.7, Z (0.7 0.3) Z and about 1/2 to 1 magnitude of extinction in the visible (Junkkarinen et at. 2004). [Pg.387]

Fig. 12.14. Metallicity evolution in DLAs. Curves show predicted mean metallic-ity in the interstellar gas relative to solar predicted by chemical evolution models of Pei, Fall and Hauser (1999), Pei and Fall (1995), Malaney and Chaboyer (1996) and Somerville, Primack and Faber (2001) respectively. Data points giving column-density weighted metallicities based on zinc only (filled circles) or other elements (open circles) are plotted in the upper panel taking upper limits as detections and in the lower panel taking upper limits as zeros. Horizontal error bars show the redshift bins adopted. After Kulkarni et al. (2005). Fig. 12.14. Metallicity evolution in DLAs. Curves show predicted mean metallic-ity in the interstellar gas relative to solar predicted by chemical evolution models of Pei, Fall and Hauser (1999), Pei and Fall (1995), Malaney and Chaboyer (1996) and Somerville, Primack and Faber (2001) respectively. Data points giving column-density weighted metallicities based on zinc only (filled circles) or other elements (open circles) are plotted in the upper panel taking upper limits as detections and in the lower panel taking upper limits as zeros. Horizontal error bars show the redshift bins adopted. After Kulkarni et al. (2005).
Vd, Wd, MH, SWNT, PCP, and AC mean volume density, weight density,metalhydrides, single walled carbon-nanotubes, pressurized carbon polymer, and activated carbon, respectively. [Pg.9]

For variable-density flows, the transport equation for the density-weighted PDF is used as the starting point. The resulting PDF codes use the particle mass as an intrinsic random variable. The particle density and specific volume can be computed based on the particle properties. [Pg.349]

Fig. 5. Standard fast spin-echo imaging of the pelvis and the lower leg. Typical contrasts between musculature and other tissues are demonstrated. Bl = bladder, Fe = femur. Gluteus = gluteus muscle. Original recording parameters matrix 192 x 256, slice thickness 6 mm, a-c field of view (fov) = 380 mm, d-f fov = 180 mm. (a) and (d) Proton density weighting TR = 5000 ms, TE = 12 ms. (b) and (e) Ti-weighting TR = 500 ms, TE = 12 ms. (c) and (f) 7 2-weighting TR = 5000 ms, TE = 100 ms. Fig. 5. Standard fast spin-echo imaging of the pelvis and the lower leg. Typical contrasts between musculature and other tissues are demonstrated. Bl = bladder, Fe = femur. Gluteus = gluteus muscle. Original recording parameters matrix 192 x 256, slice thickness 6 mm, a-c field of view (fov) = 380 mm, d-f fov = 180 mm. (a) and (d) Proton density weighting TR = 5000 ms, TE = 12 ms. (b) and (e) Ti-weighting TR = 500 ms, TE = 12 ms. (c) and (f) 7 2-weighting TR = 5000 ms, TE = 100 ms.
Compared to lipids in the subcutaneous fat layer and in the bone marrow (TiR O.S s), musculature shows a clearly slower longitudinal relaxation (Ti 1.0 s). For this reason, musculature has lost more signal intensity than fat in Ty weighted images, when compared with proton density weighting (Fig. 5a... [Pg.12]

The calculations show that the central contribution to the EFG, due to the valence electrons, is shielded rather than antishielded, but the effect is less pronounced. The shielding factor R is the density-weighted average of y(r), <7( ) "3>core,vaience/core,valence, where the average is to be taken separately over the core and valence shells, depending on the shell in which polarization is induced. [Pg.226]

Figure 2 shows a multiple-echo, intensity-weighted cyclohexane MRM image of a 300 pm cross-sectional slice of a 4 mm diameter coke bean. The density-weighted H images are collected with an unprocessed image resolution of 24 pm pixel"1. Since the coke is packed in wet gypsum, the area outside the coke shows very little cyclohexane intensity and appears black. Several feature arise from this image which complement the SEM images in Figure 1. Firstly, a dark band at the perimeter of the coke corresponds to the exterior shell depicted in deal in Figure lc. This dark feature reflects the absence of cyclohexane and thus indicates the... Figure 2 shows a multiple-echo, intensity-weighted cyclohexane MRM image of a 300 pm cross-sectional slice of a 4 mm diameter coke bean. The density-weighted H images are collected with an unprocessed image resolution of 24 pm pixel"1. Since the coke is packed in wet gypsum, the area outside the coke shows very little cyclohexane intensity and appears black. Several feature arise from this image which complement the SEM images in Figure 1. Firstly, a dark band at the perimeter of the coke corresponds to the exterior shell depicted in deal in Figure lc. This dark feature reflects the absence of cyclohexane and thus indicates the...
The distillation may be carried out in a current of steam and is then continued until no oily drops are condensed with the water the volume of the oil separating above the water in a graduated cylinder is then measured (volume of oil) x (its density) - = weight of oil. [Pg.300]

Vapor Density—Weight of a volume of pure (no air present) vapor compared to the weight of an equal volume of dry air at the same temperature and pressure. A vapor density of less than one describes a vapor which is lighter than air, while a value greater than one describes a vapor that is heavier than air [2.1]. [Pg.46]


See other pages where Weight density is mentioned: [Pg.143]    [Pg.433]    [Pg.6]    [Pg.288]    [Pg.289]    [Pg.289]    [Pg.290]    [Pg.293]    [Pg.294]    [Pg.314]    [Pg.412]    [Pg.67]    [Pg.11]    [Pg.147]    [Pg.158]    [Pg.19]    [Pg.9]    [Pg.10]    [Pg.109]    [Pg.110]    [Pg.110]    [Pg.643]    [Pg.315]    [Pg.535]    [Pg.377]    [Pg.199]    [Pg.509]    [Pg.513]    [Pg.169]    [Pg.909]   
See also in sourсe #XX -- [ Pg.19 ]

See also in sourсe #XX -- [ Pg.20 ]




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Bimodal distribution, high density polyethylene molecular weight

Bulk density weight

Density high molecular weight

Density matrix energy weighted

Density measurement weight

Density weighting function

Density, melt index, and molecular weight

Density-weighted vapor velocity

Franck-Condon weighted density

Franck-Condon weighted density of states

Franck-Condon weighted density of states FCWD)

Franck-Condon weighted density states

High-density polyethylene molecular weight

High-density polyethylene molecular weight distribution

High-density polyethylene, molecular weight averages with

Material Densities and. Atomic Weights

Modified weighted density approximations

Molar weight, determination density

Molecular weight and charge density

Molecular weight density function

Molecular weight low-density polyethylene

Molecular weight medium-density polyethylene

Molecular weight suppression polymer density

Probability density volume-weighted

Proton Density Weighted MRI

Relativistic Weighted Density Approximation

Tarazona weighted density

Tarazona weighted density approximation

Ultra high density molecular weight

Ultra high density molecular weight polyethylene

Ultrahigh molecular weight high-density

Understanding mass, weight, volume and density

Velocity superficial density-weighted

Weight Fraction Solubles and Crosslink Density

Weight basis probability density function

Weight from Gas Density (the Dumas Bulb Method)

Weighted density

Weighted density

Weighted density approximation

Weighted density approximation scheme

Weighted density functional

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