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Molecular Matrices

To date, the melt state linear dynamic oscillatory shear properties of various kinds of nanocomposites have been examined for a wide range of polymer matrices including Nylon 6 with various matrix molecular weights [34], polystyrene (PS) [35], PS-polyisoprene (PI) block copolymers [36,37], poly(e-caprolactone) (PCL) [38], PLA [39,40], PBS [30,41], and so on [42],... [Pg.285]

We have considered scalar, vector, and matrix molecular properties. A scalar is a zero-dimensional array a vector is a one-dimensional array a matrix is a two-dimensional array. In general, an 5-dimensional array is called a tensor of rank (or order) s a tensor of order s has ns components, where n is the number of dimensions of the coordinate system (usually 3). Thus the dipole moment is a first-order tensor with 31 = 3 components the polarizability is a second-order tensor with 32 = 9 components. The molecular first hyperpolarizability (which we will not define) is a third-order tensor. [Pg.348]

Interference from Isobars and Matrix Molecular Ions... [Pg.18]

J. F. Tassin and L. Monnerie, A fluorescence polarization study of matrix molecular weight on the relaxation of a labeled molecule in a stretched polymer melt, J. Polym. Sci. Polym. Phys. Ed., 21,1981 (1983). [Pg.252]

Figure 11.4. Typical stress-strain curve of a PVA/nanotube composite. The material is a fiber containing 25wt% of MWNTs in a PVA matrix (molecular weight 195 000,99% hydrolized). Figure 11.4. Typical stress-strain curve of a PVA/nanotube composite. The material is a fiber containing 25wt% of MWNTs in a PVA matrix (molecular weight 195 000,99% hydrolized).
The formation of polymer-polymer complexes as a rule is observed in aqueous media5,33. The viscosity of complexes in water is about 0.05-0.10 dl/g and close to that of globular proteins. Aqueous solutions have some features low intrinsic viscosity values are independent of the matrix molecular weight, the absence both of the concentration dependence of the reduced viscosity and the polyelectrolyte anomaly, and high values (about 30 s) of the sedimentation constant. [Pg.109]

The PAA-PVP system in methanol and the PMAA-PVP system in DMF display the typical properties of polycomplexes, namely low values of intrinsic viscosity independent of the matrix molecular weight (for PVP with molecular weight of 50 MO and 560000, the intrinsic viscosity [ /], of PA A-PVP complexes in methanol is equal to 0.07 dl/g), the absence both of the concentration dependence of the reduced viscosity, and of the polyelectrolyte anomaly. [Pg.121]

T Vispersions of acrylic polymer beads in rapidly polymerizable liquids are important biomaterials (I, 2). The biocompatibility and functionality of dental restoratives, dental prostheses, and surgical prostheses depend on the mechanical properties of these biopolymers as well as on their physical and chemical constitution. This investigation was part of a continuing program to determine the influence of microstructural parameters on the mechanical properties of these multiphase systems. The effects of the volume fractions of dispersed phase and matrix, molecular weight of the matrix, chain length and concentration of crosslinkers, impact modifiers, and filler were studied in terms of microstructure, hard-... [Pg.295]

Now we compare the variation of the brush thickness L with P, as predicted by Eq. (59), with the available data. The first experimental study of this problem [265], performed by SIMS for a series of very short (as compared to a standard depth resolution of this technique) (COOH)dPS (N=125-413) end-anchored chains annealed at different temperatures and with different matrices used (T= 108 °C for P=63, and 160 °C for P=4460), revealed identical unswollen brush conformation for both used matrix molecular weights. The variation of the brush height L with P, at a constant coverage other groups in experiments performed later [241,243]. On the basis of the cumulative data for the Pl-dPS (N=893) brush in the PS host matrix (P=88,495, and 3173), presented in Fig. 37, we were able to achieve an equi-o situation (o=3.7.10 3, see arrow in Fig. 37 and corresponding symbols (A, ) in Fig. 38 as described in... [Pg.91]


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See also in sourсe #XX -- [ Pg.11 , Pg.12 , Pg.13 , Pg.14 , Pg.15 , Pg.16 , Pg.17 , Pg.18 , Pg.19 , Pg.20 ]




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Augmented molecular matrix

Electrophoresis matrix molecular weight

Elements balance, molecular matrix

Evaluation of the nuclear derivative coupling matrix elements with canonical molecular orbitals

Fock matrix semiempirical molecular orbital theory

Host matrices molecular structure

Inorganic matrices molecularly imprinted

Matrices molecular orbital application

Matrix bond 16 molecular graph

Matrix elements molecular, factorization

Matrix isolation molecular

Matrix molecular weight

Matrix, molecular application

Matrix-assisted laser desorption molecular-weight distribution

Mixed matrix membranes molecular separation

Molecular dynamics matrix diagonalization

Molecular graph matrices

Molecular incidence matrix

Molecular matrices, living systems

Molecular modelling density matrices

Molecular orbital theory overlap matrix

Molecular quantum similarity matrix

Molecular systems transformation matrices

Molecularly biological matrices

Molecularly imprinted matrices using carbohydrates as the precursors

Molecularly imprinted protein matrices for catalysis

Molecularly imprinted protein matrices for recognition and separation

Novel Molecular Matrices

Second-derivative coupling matrix molecular systems

Structure and Molecular Motion of Peroxy Radicals in Polymer Matrices

Three-state molecular system, non-adiabatic minimal diabatic potential matrix

Three-state molecular system, non-adiabatic transformation matrices

Two-state molecular system, non-adiabatic transformation matrices

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