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Model of a Water

Recently, we have also prepared nanosized polymersomes through self-assembly of star-shaped PEG-b-PLLA block copolymers (eight-arm PEG-b-PLLA) using a film hydration technique [233]. The polymersomes can encapsulate FITC-labeled Dex, as model of a water-soluble macromolecular (bug, into the hydrophilic interior space. The eight-arm PEG-b-PLLA polymersomes showed relatively high stability compared to that of polymersomes of linear PEG-b-PLLA copolymers with the equal volume fraction. Furthermore, we have developed a novel type of polymersome of amphiphilic polyrotaxane (PRX) composed of PLLA-b-PEG-b-PLLA triblock copolymer and a-cyclodextrin (a-CD) [234]. These polymersomes possess unique structures the surface is covered by PRX structures with multiple a-CDs threaded onto the PEG chain. Since the a-CDs are not covalently bound to the PEG chain, they can slide and rotate along the PEG chain, which forms the outer shell of the polymersomes [235,236]. Thus, the polymersomes could be a novel functional biomedical nanomaterial having a dynamic surface. [Pg.88]

The chemical formula for a water molecule is H20. Using the atomic model kit, construct a model of a water molecule. Use toothpicks to hold the atoms together. Have your teacher check your model to see if it is correct. [Pg.5]

Scientists use models to represent molecules. The models are made from small balls with the balls representing atoms. These models allow scientists to understand more about molecules. Models of a water molecule, a carbon dioxide molecule, an oxygen molecule, and a methane molecule are shown below. You can make similiar models with marshmallows or gumdrops held together by toothpicks. Each marshmallow or gumdrop can represent one atom. [Pg.3]

Fig. 22 A and B. Electron-domain models of a water molecule sharing with a metal cation (solid circle) (A) one and (B) two electron pairs... Fig. 22 A and B. Electron-domain models of a water molecule sharing with a metal cation (solid circle) (A) one and (B) two electron pairs...
Figure 1,4. Model of a water molecule. The curved lines represent borders at which van der Waals attractions are counterbalanced by repulsive forces (after Hillel, 1980, with permission). Figure 1,4. Model of a water molecule. The curved lines represent borders at which van der Waals attractions are counterbalanced by repulsive forces (after Hillel, 1980, with permission).
Figure 1. Scheme of the arrangement of the cations LT, K, and Cs" at Sji sites (hatched circles) and Sm sites (filled circles). The other prolection of that part of the lattice of the KX zeolite containing a six-membered oxygen ring as well as a model of a water molecule are also shown on the same scale... [Pg.191]

Fig. 13. Modeling of a water-repellent silicone resin network on quartz (arbitrary assembly), viewed from the front (a) and from the side (b). Hie three-dimensional network is built up of two-dimensional monolayers (methyl derivative) for optical reasons (this leads to seemingly unsaturated oxygen atoms, which form the oxygen bridges in the three-dimensional case). A simplified silicone resin network on quartz could be composed of covalently bound polysiloxane chains, incompletely crosslinked polysiloxane, and embedded silsesquioxanes or homosilsesquioxanes (cages and ladders), going from the bottom (quartz) to the top [28, 42, 75, 78, 79]. The network has been optimized from graphical aspects. Total height approx. SO A. Fig. 13. Modeling of a water-repellent silicone resin network on quartz (arbitrary assembly), viewed from the front (a) and from the side (b). Hie three-dimensional network is built up of two-dimensional monolayers (methyl derivative) for optical reasons (this leads to seemingly unsaturated oxygen atoms, which form the oxygen bridges in the three-dimensional case). A simplified silicone resin network on quartz could be composed of covalently bound polysiloxane chains, incompletely crosslinked polysiloxane, and embedded silsesquioxanes or homosilsesquioxanes (cages and ladders), going from the bottom (quartz) to the top [28, 42, 75, 78, 79]. The network has been optimized from graphical aspects. Total height approx. SO A.
Why are water drops rounded Substances are liquids instead of gases because the cohesive forces between the particles are strong enough to pull the particles together so that they are in contact. Below the surface of the liquid, the particles are pulled equally in all directions by these forces. However, particles at the surface are pulled only sideways and downward by neighboring particles, as shown in the model of a water drop in Figure 4. [Pg.398]

Figure 3. Two models describing the microphases of swollen Nation membranes. Top Gierke s [48] suggestion of aqueous inverse spherical micelles connected by water-filled cylindrical channels. Bottom Yeager and Steck s [49] three-region model of a water/ionomer mixture without regular structure. Regions A, B and C are the hydrophobic polymer, the solvent bridges and the hydrophilic regions, respectively. Figure 3. Two models describing the microphases of swollen Nation membranes. Top Gierke s [48] suggestion of aqueous inverse spherical micelles connected by water-filled cylindrical channels. Bottom Yeager and Steck s [49] three-region model of a water/ionomer mixture without regular structure. Regions A, B and C are the hydrophobic polymer, the solvent bridges and the hydrophilic regions, respectively.
How would you build a gumdrop model of a water molecule First, you would draw the electron dot diagram. Remember that the dot diagram models the arrangement of valence electrons in the molecule in two dimensions. The electron dot diagram for a water molecule shows that each hydrogen shares a pair of electrons with the oxygen. [Pg.318]

In this gumdrop model of a water molecule, you can see that the three atoms form a bent structure. ... [Pg.319]

A water molecule forms a drop because of surface tension, which is the force needed to overcome intermolecular attractions and break through the surface of a liquid or spread the liquid out. The higher the surface tension of a liquid is, the more resistant the liquid is to having its surface broken. Figure 13.8 shows a molecular model of a water drop. The net inward force makes the surface of the drop contract and seem to toughen, behaving like a sort of skin. [Pg.442]

FIGURE 3.2 Structure of water, (a) Model of a water molecule. The distance between the nuclei of O and H is l 0.1 nm, the net charges q are 0.24 times the charge of an electron, and the bond angles 6 are 109°. After Israelachvilli (see Bibliography), (b) Example of how water molecules form H-bonds with one another schematic and not to scale. (After O. R. Fennema. Food Chemistry, 3d ed. Marcel Dekker, New York, 1996 (Chapter 2). [Pg.70]

Fig. 2.6. Double layer model of a water surface, after Vogel Mdbius (1988a)... Fig. 2.6. Double layer model of a water surface, after Vogel Mdbius (1988a)...
Figure 6.6 Model of a water-cooled PAFC stack. (Courtesy of The Royal Society). Figure 6.6 Model of a water-cooled PAFC stack. (Courtesy of The Royal Society).
Figure 1. Schematic diagrams of (a) 3-point, (b) 4-point, and (c) 5-point models of a water molecule. Figure 1. Schematic diagrams of (a) 3-point, (b) 4-point, and (c) 5-point models of a water molecule.
A collection of magnetic marbles provides a good physical model of a water drop. Each magnetic marble is like a water molecule, attracted to the marbles around it. If you agitate these marbles slightly, so that they can find their preferred configuration, they tend toward a spherical shape (T Figure 12.10) because the attractions between the marbles cause them to minimize the number of marbles at the surface. [Pg.415]

Model OF A Water-Filled Nanopore with Charged Metal Walls... [Pg.216]

The permeation rate of ions across membranes can be estimated using a continuum dielectric model of a water-membrane system. In this model, both water and membrane are represented as homogeneous, isotropic media, characterized by dielectric constants and ej, respectively, and separated by a sharp planar boundary. If the ion is represented as a point charge q located at the center of a cavity of radius a, the change in the excess chemical potential associated with the transfer of the ion from bulk water to the center of the membrane (the free energy barrier), is expressed in this model as [58,59] ... [Pg.502]

Several molecular dynamics simulations have addressed this issue [14,74, 75], however the simplest model of a water wire consists of an hydrogen-bonded chain of water molecules in vacuum, constrained in space by harmonic poten-... [Pg.505]


See other pages where Model of a Water is mentioned: [Pg.31]    [Pg.4]    [Pg.128]    [Pg.1659]    [Pg.139]    [Pg.319]    [Pg.69]    [Pg.792]    [Pg.306]    [Pg.509]    [Pg.349]    [Pg.350]    [Pg.52]    [Pg.55]    [Pg.278]    [Pg.111]    [Pg.126]   


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