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Transport in solution

For herbicides with low vapor pressures, the major mechanism of transport within the soil is movement in the soil water. The ability of a soil-acting herbicide to provide effective weed control depends upon its ability to move to its target site within the soil profile. Some selectivity between weeds and crops can be achieved by preparation of molecules with appropriate penetration depth within the soil. For the shallow-rooted weeds, the herbicide only needs to move to approximately the top 5 cm of the soil profile further movement takes the chemical beyond its target site and increases the potential for environmental contamination. An understanding of water movement in soils is therefore fundamental in determining the transport of herbicides to their target sites. [Pg.202]

Soils containing a large clay or organic matter content will swell with wetting, and this will reduce the number and continuity of the pore spaces. Darcy s equation (Eq. 7.8) has been used to express the movement of water in soils  [Pg.202]

As water moves through the soil by mass flow, diffusion of herbicide molecules takes place within the moving soil water. Movement by diffusion is much less extensive than by mass flow however, it enables herbicide molecules to penetrate into the smaller pores within aggregates and other areas of the soil that are more isolated from the main stream of mass flow. The process of diffusion is described by Pick s law  [Pg.203]

Herbicides which are taken up by the shoots rely on diffusion, as there is no mass flow of soil water to the shoot. As already discussed, movement in the soil air by diffusion is much greater than that in the soil water, so herbicides with high vapor pressures are more likely to be active via the shoot. These compounds are likely to have low mobility in soil, remaining near the surface to provide weed control. Under cool and wet conditions, some crop damage might be expected. [Pg.205]

Herbicides which are taken up by the root depend upon mass flow of soil water to the root and uptake of the chemical in the water removed from the soil by the plant. The concentration within the root has been shown by Briggs et to be related to the octanol/water partition coefficient. For compounds with a of less than zero, there is virtually no accumulation in the plant root as the rises, so the concentration in the root rises compared to the soil solution concentration. Briggs reported that the optimum for translocation to the leaves is 2. Herbicides with Xow values higher than 4 are accumulated in the roots but not translocated. Soil-acting compounds with systemic activity are, therefore, unlikely to have a Xow greater than 3.5. Further details are discussed in Chapter 9. [Pg.206]


An important result of the concepts discussed in this section and the preceding one is that precipitation and complexation reactions exert joint control over metal ion solubility and transport. Whereas precipitation can limit the dissolved concentration of a specific species (Me ), complexation reactions can allow the total dissolved concentration of that metal to be much higher. The balance between these two competing processes, taking into account kinetic and equilibrium effects, often determines how much metal is transported in solution between two sites. [Pg.391]

Transport in solution or aqueous suspension is the major mechanism for metal movement from the land to the oceans and ultimately to burial in ocean sediments. In solution, the hydrated metal ion and inorganic and organic complexes can all account for major portions of the total metal load. Relatively pure metal ores exist in many places, and metals from these ores may enter an aquatic system as a result of weathering. For most metals a more common sequence is for a small amount of the ore to dissolve, for the metal ions to adsorb onto other particulate matter suspended in flowing water, and for the metal to be carried as part of the particulate load of a stream in this fashion. The very insoluble oxides of Fe, Si, and A1 (including clays), and particulate organic matter, are the most important solid adsorbents on which metals are "carried."... [Pg.415]

The foregoing equations are coupled and are generally nonlinear no general solution exists. However, these equations serve as a starting point for most of the analysis that is relevant to electrophoretic transport in solutions and gels. Of course, the specific geometry and boundary conditions must be specified in order to solve a given problem. Boundary conditions for the electric field include specification of either (1) constant potential, (2) constant current, or (3) constant power. [Pg.561]

The Mechanism of Ion Transport in Solutions, Solids, Melts and Polymers... [Pg.131]

Metal transport and deposition capacities of mineral systems are closely linked to propagation of redox and related physicochemical gradients (pH, aH2, aHCI, aH2S, aS02, aC02, aCH4, aH20, etc) within mineral systems. For metals transported in solution, the rate of mineralization is a product of 3 factors (see Fig. 2) ... [Pg.223]

Zhang Y, de Boer B, Blom PWM (2009) Controllable molecular doping and charge transport in solution-processed polymer semiconducting layers. Adv Funct Mater 19 1901... [Pg.62]

Saudari SR, Frail PR, Kagan CR (2009) Ambipolar transport in solution-deposited pentacene transistors enhanced by molecular engineering of device contacts. Appl Phys Lett 95 023301... [Pg.235]

Fig. 11. Variation ofTc of [3H]PVP360 transport in solutions of dextran of varying molecular weight as a function of the specific viscosity of the dextran solution (n5PM). Dextran M 1.04 x 10 ( ) Klw 2.04xl(P (O) M - 6.94 x 10 (A) Klw = 15.4x 10 (A) 511... Fig. 11. Variation ofTc of [3H]PVP360 transport in solutions of dextran of varying molecular weight as a function of the specific viscosity of the dextran solution (n5PM). Dextran M 1.04 x 10 ( ) Klw 2.04xl(P (O) M - 6.94 x 10 (A) Klw = 15.4x 10 (A) 511...
Once nanoparticles have been formed, whether in an early state of growth or in a more or less final size, their fate depends on the forces between the individual particles and between particles and solid surfaces in the solution. While particles initially approach each other by transport in solution due to Brownian motion, convection, or sedimentation, when close enough, interparticle forces will determine their final state. If the dominant forces are repulsive, the particles will remain separate in colloidal form. If attractive, they will aggregate and eventually precipitate. In addition, they may adsorb onto a solid surface (the substrate or the walls of the vessel in which the reaction is carried out). For CD, both attractive particle-sur-... [Pg.27]

The mobility estimates of Grozema et al. [52] are quite optimistic, at least so far as hole transport in solution is concerned. For what are called realistic rotational force constants and static energy disorder they predict a hole mobility in DNA of 0.1 cm /Vs. However, taking into account the drag effect of the water we obtained a mobility of 3.5x10 cm /Vs, as detailed in Sect. 2.5. This is an upper limit because we included neither scattering nor energetic disorder. [Pg.99]

There is another way of looking at these situations where the lack of a sufficient supply of the needs of the interface compels one to look at the transport processes in solution. The broader view demands that one see the charge-transfer reaction as preceded by adrift of the reaction participants to the interface. In fact, one must think of transport in solution and charge transfer as consecutive steps of an overall reaction. [Pg.494]

The Laplace transfonnation method of solving nonsteady-state diffusion problems was briefly treated in Chapter 4. Thus, one can study all sorts of problems by using various types of current or potential stimuli (as in researches using transients see Section 7.7) and analyzing how transport in solution influences the response of the system. For example, a sinusoidally varying current, density can be used with... [Pg.498]

In volume 1 (Chapters 4 and 5) a fairly detailed treatment of the movement and transport of ions was presented qualitative pictures and quantitative accounts were given of the diffusion and electrical migration of ions in the bulk of the electrolyte. In the treatment of electrodic processes, no mention was made at first of a connection between the transport in solution and processes at electrodes. It was then realized that this neglect of ion transport in solution (ionics) was tantamount to assuming that at no stage in the course of a charge-transfer reaction did the interfacial concentrations of electron acceptors and donors depart from their bulk values. [Pg.537]

There are several places in electrochemical reactions where rate-determining steps can occur. First, if a cathode potential is sufficiently negative, transport of reactants to the electrode will not be able to keep pace with the events that transfer charge as the electrode demands. Then, transport in solution and the electrode events have to be satisfied with what the transport rate can bring to the interface. Transport is the rds. [Pg.543]

Why did we introduce this purely experimental material into a chapter that emphasizes theoretical considerations It is because the ability to replicate Tafel s law is the first requirement of any theory in electrode kinetics. It represents a filter that may be used to discard models of electron transfer which predict current-potential relations that are not observed, i.e., do not predict Tafel s law as the behavior of the current overpotential reaction free of control by transport in solution. [Pg.794]

For the Red/Ox couple, we assume that both species are transported in solution by a convective diffusion process ... [Pg.252]

In the first part, Chapters 2-6, some fundamentals of electrode processes and of electrochemical and charge transfer phenomena are described. Thermodynamics of electrochemical cells and ion transport through solution and through membrane phases are discussed in Chapter 2. In Chapter 3 the thermodynamics and properties of the interfacial region at electrodes are addressed, together with electrical properties of colloids. Chapters 4-6 treat the rates of electrode processes, Chapter 4 looking at fundamentals of kinetics, Chapter 5 at mass transport in solution, and Chapter 6 at their combined effect in leading to the observed rate of electrode processes. [Pg.8]

Fig. 18. Steady-state log j-E curves for H202 reduction and oxidation at a LaNi03 (1.2m2g 1) rotating disk electrode in 0.1 M KOH at 25°C after correction for mass transport in solution. H202 concentration = ImM [48],... Fig. 18. Steady-state log j-E curves for H202 reduction and oxidation at a LaNi03 (1.2m2g 1) rotating disk electrode in 0.1 M KOH at 25°C after correction for mass transport in solution. H202 concentration = ImM [48],...
This text discusses four aspects of ionic electrochemistry ion-solvent interactions, ion-ion interactions, ion transport in solution, and ionic liquids. [Pg.3]


See other pages where Transport in solution is mentioned: [Pg.529]    [Pg.132]    [Pg.161]    [Pg.433]    [Pg.2]    [Pg.291]    [Pg.245]    [Pg.538]    [Pg.368]    [Pg.406]    [Pg.36]    [Pg.361]    [Pg.363]    [Pg.365]    [Pg.367]    [Pg.369]    [Pg.371]    [Pg.373]    [Pg.377]    [Pg.379]    [Pg.381]    [Pg.387]    [Pg.389]    [Pg.393]    [Pg.395]    [Pg.397]    [Pg.399]    [Pg.401]    [Pg.403]    [Pg.405]   


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