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Stem orientation

The Molitorisz Hayroll winds grass or alfalfa hay into a cigar-like roll which is cut into short lengths, taking advantage of stem orientation to achieve density (l) The roll is similar to the microstructure of a cellulose molecule. But we found it impossible to make in the field with stiff brittle straw. [Pg.183]

Fig. 11. Perpendicular crystalline stem orientation with respect to cylinders... Fig. 11. Perpendicular crystalline stem orientation with respect to cylinders...
Fig. 2.8. Tilted extended chain crystal, (a) Tilted stems lead to a decrease of the grafting density of the tails. The angle at is defined between the stem orientation and the normal of the interface between the crystaline and the amorphous phase, (b) Tilting of stems increases the free energy by creating excess surface... Fig. 2.8. Tilted extended chain crystal, (a) Tilted stems lead to a decrease of the grafting density of the tails. The angle at is defined between the stem orientation and the normal of the interface between the crystaline and the amorphous phase, (b) Tilting of stems increases the free energy by creating excess surface...
In terms of recraitment strategies should more emphasis be put on the options within or emanating from an engineering degree And what of interdisciplinarity - is this solely within STEM or should it extend to the humanities and social sciences At the moment there seems to be a disconnect in this respect between the narrower (STEM-oriented) perceptions of the students and the broader understanding of interdiciplinarity conveyed by leaders in engineering education. [Pg.264]

The treatment of transverse shear stress effects in plates made of isotropic materials stems from the classical papers by Reissner [6-26] and Mindlin [6-27. Extension of Reissner s theory to plates made of orthotropic materials is due to Girkmann and Beer [6-28], Ambartsumyan [6-29] treated symmetrically laminated plates with orthotropic laminae having their principal material directions aligned with the plate axes. Whitney [6-30] extended Ambartsumyan s analysis to symmetrically laminated plates with orthotropic laminae of arbitrary orientation. [Pg.350]

Theories of the oxidation of tantalum in the presence of suboxide have been developed by Stringer. By means of single-crystal studies he has been able to show that a rate anisotropy stems from the orientation of the suboxide which is precipitated in the form of thin plates. Their influence on the oxidation rate is least when they lie parallel to the metal interface, since the stresses set up by their oxidation to the pentoxide are most easily accommodated. By contrast, when the plates are at 45° to the surface, complex stresses are established which create characteristic chevron markings and cracks in the oxide. The cracks in this case follow lines of pores generated by oxidation of the plates. This behaviour is also found with niobium, but surprisingly, these pores are not formed when Ta-Nb alloys are oxidised, and the rate anisotropy disappears. However, the rate remains linear it seems that this is another case in which molecular oxygen travels by sub-microscopic routes. [Pg.285]

Note that the scalar product is formally the same as in the nonrela-tivistic case it is, however, now required to be invariant under all orthochronous inhomogeneous Lorentz transformations. The requirement of invariance under orthochronous inhomogeneous Lorentz transformations stems of course from the homogeneity and isotropy of space-time, send corresponds to the assertion that all origins and orientation of the four-dimensional space time manifold are fully equivalent for the description of physical phenomena. [Pg.497]

There has been considerable interest in the structure and properties of poly(tetra-methylene terephthalate) 4GT, stemming from the observation that when the oriented polymer is stretched, the crystalline regions are transformed from one structure to a new one30,3l). It appears from the X-ray diffraction data that in the structure... [Pg.110]

If a spinning electron behaved like a spinning ball, the axis of spin could point in any direction. The electron would behave like a bar magnet that could have any orientation relative to the applied magnetic field. In that case, a broad band of silver atoms should appear at the detector, because the field would push the silver atoms by different amounts according to the orientation of the spin. Indeed, that is exactly what Stem and Gerlach observed when they first carried out the experiment. [Pg.155]

This is very different from the case with single bonds, which are freely rotating aU of the time. But a double bond is the result of overlapping p orbitals, and double bonds cannot freely rotate at room temperature (if you had trouble with this concept when you first learned it, you should review the bonding structure of a double bond in your textbook or notes). So there are two ways to arrange the atoms in space cis and trans. If you compare which atoms are connected to each other in each of the two possibilities, yon will notice that all of the atoms are connected in the same order. The difference is how they are connected in 3D space. This is why they are called stereoisomers (this type of isomerism stems from a difference of orientation in space— stereo ). [Pg.94]

The physical meaning of the g (ion) potential depends on the accepted model of an ionic double layer. The proposed models correspond to the Gouy-Chapman diffuse layer, with or without allowance for the Stem modification and/or the penetration of small counter-ions above the plane of the ionic heads of the adsorbed large ions. " The experimental data obtained for the adsorption of dodecyl trimethylammonium bromide and sodium dodecyl sulfate strongly support the Haydon and Taylor mode According to this model, there is a considerable space between the ionic heads and the surface boundary between, for instance, water and heptane. The presence in this space of small inorganic ions forms an additional diffuse layer that partly compensates for the diffuse layer potential between the ionic heads and the bulk solution. Thus, the Eq. (31) may be considered as a linear combination of two linear functions, one of which [A% - g (dip)] crosses the zero point of the coordinates (A% and 1/A are equal to zero), and the other has an intercept on the potential axis. This, of course, implies that the orientation of the apparent dipole moments of the long-chain ions is independent of A. [Pg.41]


See other pages where Stem orientation is mentioned: [Pg.153]    [Pg.147]    [Pg.96]    [Pg.1129]    [Pg.1132]    [Pg.116]    [Pg.20]    [Pg.23]    [Pg.38]    [Pg.246]    [Pg.748]    [Pg.749]    [Pg.312]    [Pg.20]    [Pg.18]    [Pg.153]    [Pg.147]    [Pg.96]    [Pg.1129]    [Pg.1132]    [Pg.116]    [Pg.20]    [Pg.23]    [Pg.38]    [Pg.246]    [Pg.748]    [Pg.749]    [Pg.312]    [Pg.20]    [Pg.18]    [Pg.426]    [Pg.256]    [Pg.536]    [Pg.255]    [Pg.953]    [Pg.317]    [Pg.495]    [Pg.388]    [Pg.482]    [Pg.1282]    [Pg.140]    [Pg.73]    [Pg.191]    [Pg.155]    [Pg.154]    [Pg.291]    [Pg.499]    [Pg.550]    [Pg.99]    [Pg.832]    [Pg.182]    [Pg.195]    [Pg.27]   
See also in sourсe #XX -- [ Pg.17 , Pg.143 , Pg.144 , Pg.152 , Pg.219 , Pg.220 , Pg.221 , Pg.222 , Pg.223 , Pg.224 , Pg.225 , Pg.228 , Pg.229 , Pg.238 ]




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Stem leaf, orientation

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