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Simulation Construction

Due to the noncrystalline, nonequilibrium nature of polymers, a statistical mechanical description is rigorously most correct. Thus, simply hnding a minimum-energy conformation and computing properties is not generally suf-hcient. It is usually necessary to compute ensemble averages, even of molecular properties. The additional work needed on the part of both the researcher to set up the simulation and the computer to run the simulation must be considered. When possible, it is advisable to use group additivity or analytic estimation methods. [Pg.309]

At the beginning of a project, the model system must be determined. Oligomers can be used to model properties that are a function of local regions of the chain only. Simulations of a single polymer strand can be used to determine the tendency to fold in various manners and to hnd mean end-to-end distances and other properties generally considered the properties of a single mol- [Pg.309]

The structure of a polymer, which is actually many structures generated by a sampling of conformation space, can be obtained via a number of techniques. Some of the most widely used techniques are as follows  [Pg.310]

Ah initio calculations of polymer properties are either simulations of oligomers or band-structure calculations. Properties often computed with ah initio methods are conformational energies, polarizability, hyperpolarizability, optical properties, dielectric properties, and charge distributions. Ah initio calculations are also used as a spot check to verify the accuracy of molecular mechanics methods for the polymer of interest. Such calculations are used to parameterize molecular mechanics force fields when existing methods are insulficient, which does not happen too often. [Pg.310]

The property to be predicted must be considered when choosing the method for simulating a polymer. Properties can be broadly assigned into one of two categories material properties, primarily a function of the nature of the polymer chain itself, or specimen properties, primarily due to the size, shape, and phase [Pg.310]


The colors in a computer-processed photo, then, are not false colors in any profound sense they are simply not simulated, constructed, to the usual human visual system standards. The redness you directly experience when looking at a fire is an arbitrary construction of your brain. Hotness could be constructed by the brain so that it would be experienced with the sensations we now think of as coldness. As long as the relation of the experience of coldness to objects and processes associated with higher temperatures in the outside world held constant, so that you knew things that felt cold would burn you, it would be just as useful to our survival as the present experience of hotness being associated with high-temperature objects. [Pg.50]

Try reading upside down for a page or two. Surprisingly, psychological experiments have found that many people can work up to almost normal reading speed within a page or two. After the initial work, automatization of the perceptual simulation/construction process can be surprisingly fast. [Pg.52]

The objeetive of the present work was to evaluate the use of two ligneous-cellulosic materials, a brown seaweed and sugarcane bagasse, as substrates for SRB growth and to investigate their ability to remove heavy metals simulating constructed wetlands. [Pg.463]

Figure 4. EPR (top) and UV/Vis (bottom) spectra of synthetic Hb hybrids. Reductive nitro-sylation [24] of met-Hb (prepared from Hb A<, by potassium ferricyanide oxidation foilowed by G-25 chromatography) with one equivalent of NO give Hb[(a-Fe(III))2(P-Fe(II)NO)2] (left), while limited air oxidation of Hb(NO)4 furnishes Hb[(a-Fe(II)NO)2(P-Fe(III))2] (right). SoUd lines are the experimental spectra, the dotted line on the UVA is spectra represents a simulation constructed from equal mixtures of heme-Fe(lll)and heme-Fe(II)NO standard Hb spectra. EPR spectra were obtained at X-band (9.3 GHz), with sanities at 76 K, and detected with a field modulation anqilitude of 5 G and frequency of 100 kHz. Figure 4. EPR (top) and UV/Vis (bottom) spectra of synthetic Hb hybrids. Reductive nitro-sylation [24] of met-Hb (prepared from Hb A<, by potassium ferricyanide oxidation foilowed by G-25 chromatography) with one equivalent of NO give Hb[(a-Fe(III))2(P-Fe(II)NO)2] (left), while limited air oxidation of Hb(NO)4 furnishes Hb[(a-Fe(II)NO)2(P-Fe(III))2] (right). SoUd lines are the experimental spectra, the dotted line on the UVA is spectra represents a simulation constructed from equal mixtures of heme-Fe(lll)and heme-Fe(II)NO standard Hb spectra. EPR spectra were obtained at X-band (9.3 GHz), with sanities at 76 K, and detected with a field modulation anqilitude of 5 G and frequency of 100 kHz.
Once the flowsheet structure has been defined, a simulation of the process can be carried out. A simulation is a mathematical model of the process which attempts to predict how the process would behave if it was constructed (see Fig. 1.1b). Having created a model of the process, we assume the flow rates, compositions, temperatures, and pressures of the feeds. The simulation model then predicts the flow rates, compositions, temperatures, and pressures of the products. It also allows the individual items of equipment in the process to be sized and predicts how much raw material is being used, how much energy is being consumed, etc. The performance of the design can then be evaluated. [Pg.1]

Hgure 1.1 Synthesis is the creation of a process to transform feed streams into product streams. Simulation predicts how it would behave if it was constructed. [Pg.2]

Reservoir simulation is a technique in which a computer-based mathematical representation of the reservoir is constructed and then used to predict its dynamic behaviour. The reservoir is gridded up into a number of grid blocks. The reservoir rock properties (porosity, saturation, and permeability), and the fluid properties (viscosity and the PVT properties) are specified for each grid block. [Pg.205]

The amount of detail input, and the type of simulation model depend upon the issues to be investigated, and the amount of data available. At the exploration and appraisal stage it would be unusual to create a simulation model, since the lack of data make simpler methods cheaper and as reliable. Simulation models are typically constructed at the field development planning stage of a field life, and are continually updated and increased in detail as more information becomes available. [Pg.206]

The biased-sampling approach may be considerably generalized, to allow the construction of MC moves step-by-step, with each step depending on the success or failure of the last. Such a procedure is biased, but it is then possible to correct for the bias (by considering the possible reverse moves). The technique has dramatically speeded up polymer simulations, and is capable of wider application. [Pg.2265]

Other methods consist of algorithms based on multivariate classification techniques or neural networks they are constructed for automatic recognition of structural properties from spectral data, or for simulation of spectra from structural properties [83]. Multivariate data analysis for spectrum interpretation is based on the characterization of spectra by a set of spectral features. A spectrum can be considered as a point in a multidimensional space with the coordinates defined by spectral features. Exploratory data analysis and cluster analysis are used to investigate the multidimensional space and to evaluate rules to distinguish structure classes. [Pg.534]

Fig. 6.21 The construction of a system of periodic cells in the Ewald method. (Figure adapted from Allen M P and D ] Tildesley 1987. Computer Simulation of Liquids, Oxford, Oxford University Press.)... Fig. 6.21 The construction of a system of periodic cells in the Ewald method. (Figure adapted from Allen M P and D ] Tildesley 1987. Computer Simulation of Liquids, Oxford, Oxford University Press.)...
I Ikcal/mol. From this initial simulation a histogram is constructed which gives the iber of times a state with an energy in the range E to E + 6E is determined. These histo-a values cire stored in an array H( ). Each of the values in this cirray (H(E)) should initially approximate the energy distribution at the temperature Tq ... [Pg.452]


See other pages where Simulation Construction is mentioned: [Pg.309]    [Pg.309]    [Pg.312]    [Pg.2456]    [Pg.215]    [Pg.56]    [Pg.223]    [Pg.240]    [Pg.266]    [Pg.5]    [Pg.309]    [Pg.309]    [Pg.222]    [Pg.309]    [Pg.309]    [Pg.312]    [Pg.2456]    [Pg.215]    [Pg.56]    [Pg.223]    [Pg.240]    [Pg.266]    [Pg.5]    [Pg.309]    [Pg.309]    [Pg.222]    [Pg.2]    [Pg.167]    [Pg.790]    [Pg.756]    [Pg.2254]    [Pg.2365]    [Pg.80]    [Pg.90]    [Pg.92]    [Pg.213]    [Pg.314]    [Pg.349]    [Pg.414]    [Pg.498]    [Pg.498]    [Pg.390]    [Pg.429]    [Pg.295]    [Pg.348]    [Pg.348]    [Pg.411]    [Pg.420]    [Pg.433]    [Pg.440]   


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