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Packed Position

In a real population, the dynamics are complicated by territorial disputes between predators. A pride of lions may establish and defend a territory against other lions by driving away intruders. A "repulsion" term that keeps members of different packs apart can be included in a CA simulation by allowing cells that contain lions to interact over large neighborhoods. However, if the two-dimensional simulation "wraps around" on itself, the region that a pack of lions controls may become mirrored, so that what appear to be intruders encroaching into one side of the territory are, in fact, members of the same pack positioned at the other side of the territory that have been... [Pg.193]

Figure 3.4. Construction of the basic close-packed unit (two packing layers for any close-packed structure), P, a packing atom O, an octahedral site T, a tetrahedral site A, B, and C are the three relative packing positions in projection. Figure 3.4. Construction of the basic close-packed unit (two packing layers for any close-packed structure), P, a packing atom O, an octahedral site T, a tetrahedral site A, B, and C are the three relative packing positions in projection.
Figure 9.18. A close-packed layer of the structure of Ga3Pt5 is shown (squares are for Pt and circles for Ga). Packing positions in the other two close-packed layers are shown as solid dots labeled B and C. Figure 9.18. A close-packed layer of the structure of Ga3Pt5 is shown (squares are for Pt and circles for Ga). Packing positions in the other two close-packed layers are shown as solid dots labeled B and C.
Figure 10.43. The unit cell of chlorite, Mg5Al(AlSi3lOio)(OH)8, is extended along c to show the TOT O TOT packing. Packing positions of oxygen layers are shown. Oxygen atoms of OH- ions are lighter in color and not bonded to Si. Figure 10.43. The unit cell of chlorite, Mg5Al(AlSi3lOio)(OH)8, is extended along c to show the TOT O TOT packing. Packing positions of oxygen layers are shown. Oxygen atoms of OH- ions are lighter in color and not bonded to Si.
Figure 12.5 shows a projection of three close-packed positions, A, B, and C. The octahedra are shown for P OcPg/ but the pattern for the projection pattern is the same for P PcPg or Pa PcTb (the T sites between Pa and Pg are Tg and T. ) Three cells are shown with A positions (dark balls) at comers and edges. The simplest cell is shown in two equivalent orientations. The other cell has A positions at comers with B and C positions in the edges. This plot is very helpful in assigning positions of atoms in a cell. Unless there is distortion, it should be possible to account for the position of each atom in each layer. For structures in the system, CrystalMaker makes it possible to... [Pg.304]

Layered silicates reveal two types of filled close-packed layers of oxide ions. Those bonded to Al3+ or Mg2+ ions in octahedral sites are the usual close-packed layers, oxide ions form a network of hexagons with an oxide ion at the centers. The oxide layers forming the bases of tetrahedra have oxide ions which form smaller hexagons without oxide ions at the centers. This is also the pattern found for layers 2/3 filled, but those oxide layers in silicates are filled. For many of the layered silicates the repeating units, based on packing positions, requires stacking as many as three unit cells. [Pg.353]

Bartlett and co-workers (65) have pointed out the relationship of this structure to that of rutile. The MF4 stoichiometry is achieved by an ordered removal of half the metal atoms from the MF2 structure. Each fluorine atom is then either two- (for bridging atoms) or one-coordinate (for terminal atoms), rather than three-coordinate as in the rutile structure. In the rutile arrangement the anions are moved from hexagonal, close-packed positions to have a symmetric arrangement of three metal atom neighbors, with planar coordination. The tetra-... [Pg.99]

The text of the frozen uncoated-paper research book was dried in the next experimental run with this oven. Eight 45-sec bursts of energy were required to remove the water from this lightly wetted 244.5-g text. The amount of water absorbed by this text during the simulated flood was small since it was in the tightly packed position (1). Its dry weight... [Pg.138]

Rutherford suggested that this nucleus at the center of the atom was composed of densely packed positively charged particles. Soon after, Henry Moseley, before his early death at Gallipoli in World War I, supplied experimental evidence for these particles, the protons. The other particles in the nucleus, the neutrons, proved a bit harder to pin down because they have no charge. But James Chadwick, taking Rutherford s advice, finally confirmed their existence in 1932. Chadwick measured the rebound of certain radiation from nitrogen and helium and found it corresponded to a neutral particle with about the same mass as a proton. ... [Pg.47]

The question of what happens when a bunch of particles comes together was asked by Newton, who found the process diffieult. Yet if aU particles adhere strongly as described above, they should leap into contact, then deform and squash closer to each other as a result of molecular adhesion. It is a paradox that particles which adhere sttongly do not do this. Instead they form weak, loose treelike structures because each particle sticks where it touches, as shown in Fig. 9.19(a). This instant adhesion therefore prevents good compaction, which can only be achieved if the particles do not adhere strongly but can wander around to find dense close-packing positions. Fig. 9.19(b). [Pg.197]

Prepare a spun Sephadex G-50 column. Block the end of a 1-mL disposable syringe with glass wool. Pill with Sephadex G-50 nntil all the excess fluid drains out and the beads are packed. Position the colnmn in a disposable 15-mL plastic conical centrifuge tube, and centrifuge at 4,000g for 3 min. Equilibrate this column with 100pL MITE by spinning as before. Do this five times. [Pg.88]

The flexibility of the SMP composite material is important for folding the structure into the spacecraft for transfer to space the folding temperature is highly dependent on both the resin and fibre properties. Once the structure is packed into its folded position, it is constrained in that position until cooled to approximately 15°C, or lower below Tg at which point the SMP composite structure will remain locked or frozen in the packed position umestrained until it is again heated above the Tg. When the SMP structure is heated, internal strain energy will cause it to return to its initial cured shape. The speed and the accuracy of the shape return are a function of the shape memory recovery force of the composite. [Pg.731]

The very large ionic conductivity of silver iodide crystal is explained by its structure. The crystal is cubic, with the four iodide ions in the unit cell in the close-packed positions 00 0, (Figure 2-7). The... [Pg.355]


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