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Point Properties

Melting-point properties. The precipitated wax consists mainly of paraffins and some naphthenes the aromatics are absent. Lighter hydrocarbons from Cl to Ci5 are also absent in the wax (Philp, 1994), As [Pg.302]

Melting-point temperature Tj. Won (1986) has given a correlation for the melting point of pure n-alkanes  [Pg.303]

Enthalpy of fusion Ahf. Won (1986) developed a correlation for calculating the melting-point enthalpies (enthalpy of fusion) of paraffin hydrocarbons  [Pg.304]

The enthalpy of fusion for naphthenes and iso-paraffins is given by (Lira-Galena et al., 1996), [Pg.304]

The enthalpy of fusion for aromatic species is given by (Pan et aL, 1997b)  [Pg.304]


To calculate the properties of a molecule, you need to generate a well-defined structure. A calculation often requires a structure that represents a minimum on a potential energy surface. HyperChem contains several geometry optimizers to do this. You can then calculate single point properties of a molecule or use the optimized structure as a starting point for subsequent calculations, such as molecular dynamics simulations. [Pg.8]

Calculating single point properties and energies provides information about chemical pathways and mechanisms. [Pg.9]

Critical Point Properties for Selected Supercritical Fluids... [Pg.597]

Since the boiling point properties of the components in the mixture being separated are so critical to the distillation process, the vapor-liquid equilibrium (VLE) relationship is of importance. Specifically, it is the VLE data for a mixture which establishes the required height of a column for a desired degree of separation. Constant pressure VLE data is derived from boiling point diagrams, from which a VLE curve can be constructed like the one illustrated in Figure 9 for a binary mixture. The VLE plot shown expresses the bubble-point and the dew-point of a binary mixture at constant pressure. The curve is called the equilibrium line, and it describes the compositions of the liquid and vapor in equilibrium at a constant pressure condition. [Pg.172]

With the availabihty of computers, the transfer matrix method [14] emerged as an alternative and powerful technique for the study of cooperative phenomena of adsorbates resulting from interactions [15-17]. Quantities are calculated exactly on a semi-infinite lattice. Coupled with finite-size scaling towards the infinite lattice, the technique has proved popular for the determination of phase diagrams and critical-point properties of adsorbates [18-23] and magnetic spin systems [24—26], and further references therein. Application to other aspects of adsorbates, e.g., the calculation of desorption rates and heats of adsorption, has been more recent [27-30]. Sufficient accuracy can usually be obtained for the latter without scaling and essentially exact results are possible. In the following, we summarize the elementary but important aspects of the method to emphasize the ease of application. Further details can be found in the above references. [Pg.446]

For both statistical and dynamical pathway branching, trajectory calculations are an indispensable tool, providing qualitative insight into the mechanisms and quantitative predictions of the branching ratios. For systems beyond four or five atoms, direct dynamics calculations will continue to play the leading theoretical role. In any case, predictions of reaction mechanisms based on examinations of the potential energy surface and/or statistical calculations based on stationary point properties should be viewed with caution. [Pg.261]

Suppose we now assign a physical meaning to the velocity v, representing it as the velocity of matter in the volume, V. Then if V always contains the same mass, it is a system volume. The properties defined for each point of the system represent those of a continuum in which the macroscopic character of the system is retained as we shrink to a point. Properties at a molecular or atomic level do not exist in this continuum context. Furthermore, since the system volume is fixed in mass, we can regard volume V to always enclose the same particles of matter as it moves in space. Each particle retains its continuum character and thermodynamic properties apply. [Pg.53]

Remark 2 It is worthwhile to mention that the breaking point of the M-estimator, the fraction of outliers that can be tolerated without the estimator potentially breaking down, is about 1 /(g + 1), where g is the dimension of the data (Maronna, 1976). In data reconciliation, outliers refer to the abnormal observations and are a small fraction of the whole data set. In our view, the breaking point property is reasonably good for practical implementations. [Pg.211]

The increase in stability resulting from resonance or electron delocalization is important in the discussion of a great variety of chemical questions. A partial list of topics should stress this point. Properties of dyes, ultraviolet absorption, bond strengths, thermal stabilities, free radical reactions, heats of reaction, and rates of chemical reactions in general may be influenced by resonance stabilization in the chemical species involved. [Pg.107]

IV. BOND CRITICAL POINT PROPERTIES OF THE ELECTRON DENSITY... [Pg.103]

More recently, Yates and Lester230 fitted Liu s surface with a slightly modified form of the Porter-Karplus formulas after first fitting Liu s H2 potential to a simple Morse function. They then use the resulting surface to calculate the three-dimensional classical trajectory of the system. Their empirical fit very closely duplicates Liu s saddle-point properties. Reaction probabilities on this surface are compared with those on the PK surface. [Pg.54]

For the adsorption of antibodies, virtually all ion-exchangers compatible with proteins can be used. Anion-exchangers have been used extensively for the isolation of polyclonal IgG from human plasma and from that of different mammals in a single step with a high degree of purity in a single pass, as shown in Fig. 8. They have also been used to isolate isoforms of monoclonal IgG after optimization of adsorption and elution conditions to fit with isoelectric point properties of the antibody.91... [Pg.562]

The and elements reference namespaces other than CML. This is done to facilitate aggregation with other XML components, such as dictionaries, and by this means to reduce what has been called tag soup . For example, defines a namespace for a dictionary reference called chem mpt. Any processing software that might need to process a melting point property would be directed to this dictionary for further information on the semantics of this term. Similarly, the... [Pg.93]

Feedstock. A hydrotreated, straight-run naphtha from a North Sea crude was used as a base feedstock in the test program. By distillation (according to ASTM D-2892, with 15 theoretical plates and a reflux ratio of 5 1) three naphthas with different initial boiling points (IBP) and three naphthas with different final boiling points were produced. The boiling point properties of the base and the derived naphthas are given in Table I. The composition of the different naphthas was determined by GC analysis. [Pg.270]

Table I The boiling point properties of the base naphtha and the naphthas... Table I The boiling point properties of the base naphtha and the naphthas...
By varying both initial and final boiling points of the feedstock, octane numbers, reformate yields and composition as well as gas yields were measured in a once-through, isothermal pilot reactor. The effect of the feedstock boiling point properties on catalyst deactivation was also studied. [Pg.281]

Table A-2 Boiling and freezing point properties 843 Table A-3 Properties of solid metals 844 846 Table A-4 Properties of solid nonmetals 847 Table A-5 Properties of building materials 848-849 Table A-6 Properties of insulating materials 850 Table A-] Properties of common foods 851-852 Table A-8 Properties of miscellaneous materials 853 TableA-9 Properties of saturated water 854 Table A 10 Properties of saturated refrigerant-134a 855 Table A-11 Properties of saturated ammonia 856 Table A-12 "Properties of saturated propane 857 Table A-13 Properties of liquids 858 Table A-14 Properties of liquid metals 859 Table A- 5 Properties of air at 1 atm pressure 860 TableA-16 Properties of gases at 1 atm pressure 861-862 Table A-17 Properties of the atmosphere at high altitude 863 Table A-18 Emissivities of surfaces 864-865 Table A-19 Solar radiative properties of materials 866 Figure A-20 The Moody chart for friction factor for fully developed flow in circular pipes 867... Table A-2 Boiling and freezing point properties 843 Table A-3 Properties of solid metals 844 846 Table A-4 Properties of solid nonmetals 847 Table A-5 Properties of building materials 848-849 Table A-6 Properties of insulating materials 850 Table A-] Properties of common foods 851-852 Table A-8 Properties of miscellaneous materials 853 TableA-9 Properties of saturated water 854 Table A 10 Properties of saturated refrigerant-134a 855 Table A-11 Properties of saturated ammonia 856 Table A-12 "Properties of saturated propane 857 Table A-13 Properties of liquids 858 Table A-14 Properties of liquid metals 859 Table A- 5 Properties of air at 1 atm pressure 860 TableA-16 Properties of gases at 1 atm pressure 861-862 Table A-17 Properties of the atmosphere at high altitude 863 Table A-18 Emissivities of surfaces 864-865 Table A-19 Solar radiative properties of materials 866 Figure A-20 The Moody chart for friction factor for fully developed flow in circular pipes 867...

See other pages where Point Properties is mentioned: [Pg.483]    [Pg.198]    [Pg.177]    [Pg.125]    [Pg.130]    [Pg.109]    [Pg.213]    [Pg.291]    [Pg.39]    [Pg.93]    [Pg.140]    [Pg.483]    [Pg.497]    [Pg.11]    [Pg.318]    [Pg.127]    [Pg.104]    [Pg.113]    [Pg.115]    [Pg.232]    [Pg.195]    [Pg.271]    [Pg.281]    [Pg.856]    [Pg.66]    [Pg.127]   


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