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Pressure experiments

Even though the rates of initiation span almost a 10-fold range, the values of k, show a standard deviation of only 4%, which is excellent in view of experimental errors. Note that the rotating sector method can be used in high-pressure experiments and other unusual situations, a characteristic it shares with many optical methods in chemistry. [Pg.380]

The phenomena we discuss, phase separation and osmotic pressure, are developed with particular attention to their applications in polymer characterization. Phase separation can be used to fractionate poly disperse polymer specimens into samples in which the molecular weight distribution is more narrow. Osmostic pressure experiments can be used to provide absolute values for the number average molecular weight of a polymer. Alternative methods for both fractionation and molecular weight determination exist, but the methods discussed in this chapter occupy a place of prominence among the alternatives, both historically and in contemporary practice. [Pg.505]

As noted above, all of the colligative properties are very similar in their thermodynamics if not their experimental behavior. This similarity also extends to an application like molecular weight determination and the kind of average obtained for nonhomogeneous samples. All of these statements are also true of osmotic pressure. In the remainder of this section we describe osmotic pressure experiments in general and examine the thermodynamic origin of this behavior. [Pg.544]

Figure 8.7 Schematic representation of an osmotic pressure experiment. Figure 8.7 Schematic representation of an osmotic pressure experiment.
First, we consider the experimental aspects of osmometry. The semiperme-able membrane is the basis for an osmotic pressure experiment and is probably its most troublesome feature in practice. The membrane material must display the required selectivity in permeability-passing solvent and retaining solute-but a membrane that works for one system may not work for another. A wide variety of materials have been used as membranes, with cellophane, poly (vinyl alcohol), polyurethanes, and various animal membranes as typical examples. The membrane must be thin enough for the solvent to pass at a reasonable rate, yet sturdy enough to withstand the pressure difference which can be... [Pg.548]

Osmotic pressure experiments provide absolute values for Neither a model nor independent calibration is required to use this method. Experimental errors can arise, of course, and we note particularly the effect of impurities. Polymers which dissociate into ions can also be confusing. We shall return to this topic in Sec. 8.13 for now we assume that the polymers under consideration are nonelectrolytes. [Pg.552]

We shall have occasion to refer to conditions in the next two chapters as well, so the ideas of the past few sections have applications beyond merely describing the nonideality of osmostic pressure experiments. [Pg.568]

We consider this system in an osmotic pressure experiment based on a membrane which is permeable to all components except the polymeric ion P that is, solvent molecules, M" , and X can pass through the membrane freely to establish the osmotic equilibrium, and only the polymer is restrained. It does not matter whether pure solvent or a salt solution is introduced across the membrane from the polymer solution or whether the latter initially contains salt or not. At equilibrium both sides of the osmometer contain solvent, M , and X in such proportions as to satisfy the constaints imposed by electroneutrality and equilibrium conditions. [Pg.569]

What makes the latter items particularly important is the fact that the charge and electrolyte content of an unknown polymer may not be known hence it is important to design an osmotic pressure experiment correctly for such a system. It is often easier to add swamping amounts of electrolyte than to totally eliminate all traces of electrolyte. Under the former conditions a true molecular weight is obtained. Trouble arises only when the experimenter is indifferent toward indifferent electrolyte this sort of carelessness can be the source of much confusion. [Pg.574]

In some lUPAC-sponsored researchf, samples of the same polystyrene preparation were distributed among different laboratories for characterization. The following molecular weights were obtained for one particular sample by osmotic pressure experiments using the solvents, membranes, and temperatures listed below ... [Pg.578]

As in osmotic pressure experiments, polymer concentations are usually expressed in mass volume units rather than in the volume fraction units indicated by the Einstein equation. For dilute solutions, however, Eq. (8.100) shows that

partial molar volume of the polymer in solution, and M is the molecular weight of the polymer. Substituting this relationship for (pin Eq. (9.9)gives... [Pg.591]

Table 9.3 lists the intrinsic viscosity for a number of poly(caprolactam) samples of different molecular weight. The M values listed are number average figures based on both end group analysis and osmotic pressure experiments. Tlie values of [r ] were measured in w-cresol at 25°C. In the following example we consider the evaluation of the Mark-Houwink coefficients from these data. [Pg.605]

Traditionally, the average specific cake and medium resistances have been deterrnined from constant pressure experiments and the solution of the basic filtration equation for constant pressure which relates filtrate volume to time. This relationship is, in theory, paraboHc but deviations occur in practice. [Pg.392]

Water loss in operating an HDR faciUty may result from either increased storage within the body of the reservoir or diffusion into the rock body beyond the periphery of the reservoir (38). When a reservoir is created, the joints which are opened immediately fill with water. Micropores or microcracks may fill much more slowly, however. Figure 11 shows water consumption during an extended pressurization experiment at the HDR faciUty operated by the Los Alamos National Laboratory at Fenton Hill, New Mexico. As the microcracks within the reservoir become saturated, the water consumption at a set pressure declines. It does not go to zero because diffusion at the reservoir boundary can never be completely elirninated. Of course, if a reservoir joint should intersect a natural open fault, water losses may be high under any conditions. [Pg.271]

After the reactor, a filter protects the flow controller from any catalyst dust. Caution must be applied because, if significant catalyst dust collects, results can be ruined even if the filter is at a lower temperature than the reactor. The flow controller also indicates the volumetric flow of the experiment. To operate properly, the flow controller needs a minimum 5 psig pressure at the gauge before the controller. This is important at low pressure experiments. [Pg.86]

At high pressure experiments the reactor should be installed in a pressure cell. All check valves before it, and the filter with the flow controller after it, can be kept in the vented operating room. As a minimum, the bypass valve and the flow controller must be accessible to the operator. This can be done by extended valve stems that reach through the protecting wall. Both the operating room and the pressure cell should be well ventilated and equipped by CO alarm instruments. [Pg.86]

In the perfectly elastic, perfectly plastic models, the high pressure compressibility can be approximated from static high pressure experiments or from high-order elastic constant measurements. Based on an estimate of strength, the stress-volume relation under uniaxial strain conditions appropriate for shock compression can be constructed. Inversely, and more typically, strength corrections can be applied to shock data to remove the shear strength component. The stress-volume relation is composed of the isotropic (hydrostatic) stress to which a component of shear stress appropriate to the... [Pg.31]

FIG. 6 Equilibrium volume of N2 solids versus temperature at zero pressure. Experiments [289] and PIMC results [260] lines are for visual help. (Reprinted with permission from Ref. 260, Fig. 1 1998, American Physical Society.)... [Pg.97]

The most frequent cause of damage and even explosion in boilers is a low-water condition. This will expose the heating surfaces, which ultimately overheat and rupture under the operating pressure. Experience has shown that since the introduction of controls for unattended automatic operation of boilers the accident rate has increased. Investigation invariably shows that lack of maintenance has been the main contributing factor. It is therefore imperative that personnel responsible for the running of the boiler plant be fully trained and conversant with its safe operation. [Pg.365]

Recent work has allowed values of A," and a for bulk polymerization in dilute solution to be estimated. This work suggests values of A Ar,1 1 1x10s M"1 and a 0.15-0.25 for both MMA and S.17,50 Some values of A 1 and a for S and methacrylates estimated from SP-PLP at high pressure experiments arc shown in Table 5.1. [Pg.246]

Volumes of activation for fast reactions are determined from the effects of high pressure on rate constants, as presented in Chapter 7. Several versions of stopped-flow instruments suitable for high-pressure experiments have been described.7-10... [Pg.256]

Sample obtained from p-S in high-pressure experiments, wavenumbers extrapolated to ambient pressure [58, 109, 119]... [Pg.81]

The use of SCCO2 as a reaction solvent is an area of current significant research activity. The previous lack of attention is at least in part due to the difficulties of carrying out such high-pressure experiments in university... [Pg.140]

The validity of this approximation is comprehensible from an experimental point of view if it is granted that the elastic behavior should be independent of the external pressure P for moderate pressures. Experiments performed at zero pressure, where the term P dV/dL)T, p is literally equal to zero, should on this basis yield results equivalent to those actually obtained at one atmosphere hence omission of the term in question appears justified. [Pg.441]

For the open valve case (CONFLOl), make a step change in Pj and observe the transients in flow rate and liquid level. Try this for a sinusoidally varying inlet pressure. Experiment with a sudden change in the outlet valve setting. [Pg.489]

Tatsumi Y, Hamilton DL, Nesbitt RW, (1986) Chemical characteristics of fluid phase released from a subducted lithosphere and origin of arc magmas evidence from high-pressure experiments and natural rocks. J Volcanol Geotherm Res 29 293-309... [Pg.308]

Flanagan, S., and A. R. Edwards, 1978, Some Nonequilibrium Effects in De-Pressurization Experiments of Water-Filled Systems, in Transient Two-Phase Flow, Proc. 2nd CSNI Specialists Meeting, Vol. 2, 487-516, M. Reocreux and G. Katz Eds., Commissariat a I Energie Atomnizue, Fontenay aux Roses, France. (3)... [Pg.533]

In order to increase the flow rate without too much pressure, Experiment 4 was performed with a Fann filter press which has a wider cross sectional area. A constant air pressure of 100 psi was applied, the flow rate was 26 times that of Experiment 1 while the NaCl concentration was only slightly higher than that of Experiment 1. Although the flow rate was much increased in Experiment 4, the result was similar to Experiment 1. The water retained in the clay (Column 8) determined by drying was found to be close to the amount of anion-free water. The porosity of the sediment was 0.4 and the average pore diameter was 4466 X. It was concluded from this experiment, that the anion-free water was immobile even at 100 psi and 7.4 ft/day. The pore size distributionQof the sample showed 90% of the pores to have a diameter above 350 A and less than 3% of the pores to have a diameter below 100 X (Figure 4). [Pg.601]

As mentioned above, the particular characteristics of the spin crossover process in dinuclear compounds is the appearance of a plateau in the spin transition curve. From the analysis of the results of the pressure experiments, it is inferred that the plateau results from successive ST in the two metal centres, leading first to the formation of relatively stable [HS-LS] pairs and then, above a critical pressure, to the formation of [LS-LS] pairs on further lowering of the temperature. The intermolecular interactions between [HS-LS] pairs leads to domains that contribute to the stability of the... [Pg.190]


See other pages where Pressure experiments is mentioned: [Pg.302]    [Pg.41]    [Pg.41]    [Pg.507]    [Pg.544]    [Pg.617]    [Pg.686]    [Pg.689]    [Pg.100]    [Pg.130]    [Pg.96]    [Pg.138]    [Pg.50]    [Pg.713]    [Pg.80]    [Pg.236]    [Pg.196]    [Pg.198]    [Pg.1119]    [Pg.120]    [Pg.407]    [Pg.548]   
See also in sourсe #XX -- [ Pg.65 ]




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Drop pressure experiment

Experiments in argon at atmospheric pressure

Experiments in methane at 10 bar pressure

High pressure experiments

High-pressure experiments, phase transitions

High-pressure liquid methane bubble point experiments

High-pressure liquid oxygen bubble point experiments

Maximum bubble pressure experiment

Mossbauer high-pressure experiments

Optical activity high-pressure experiments

Optical high-pressure experiments

Optical methods, high-pressure experiments

Phase high-pressure experiments

Pressure cell experiments

Pressure cell experiments composites

Pressure jump experiments

Pressure tuning experiment

Pressure-jump kinetic experiments

Pressurization experiments, silicon

Temperature and Pressure Experiments

The Pressure-Drop Experiment

Ultra high pressure experiments

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