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Current total droplet

Since the current is proportional to the total droplet charge, this means that the addition of A+ to the solution leads only to a small increase in the droplet charge. However, in the charged droplets, the ions A+ compete with the ions B+ in the conversion process to gas-phase ions. A proportionality to concentrations of ions A+ and B+ in the droplets may be expected in this competition51 so that an increase of the concentration of A+ in the solution should lead to a decrease of production of gas-phase ions B+, i.e. to a decrease of /B. This is exactly what is observed in Figure 3. [Pg.273]

Figure 1.1 Schematic of major processes occurring in the atmospheric pressure region of electrospray. TDC stands for total droplet current (/). The figure illustrates major processes occurring in the atmospheric pressure region of an ESI run in the positive ion mode. Penetration of the imposed electric field into the liquid leads to formation of an electric double layer at the meniscus. The double layer is due to the polarizabilty and dipole moments of the solvent molecules and an enrichment near the meniscus of positive ions present in the solution. Figure 1.1 Schematic of major processes occurring in the atmospheric pressure region of electrospray. TDC stands for total droplet current (/). The figure illustrates major processes occurring in the atmospheric pressure region of an ESI run in the positive ion mode. Penetration of the imposed electric field into the liquid leads to formation of an electric double layer at the meniscus. The double layer is due to the polarizabilty and dipole moments of the solvent molecules and an enrichment near the meniscus of positive ions present in the solution.
The dependence of the total droplet current produced at the spray capillary on various parameters was given in Eq. (1.7). Relevant to the present discussion is the dependence of the current ) on the square root of the conductivity of the solution. At the low total electrolyte concentrations generally used in ESI, the conductivity is proportional to the concentration of the electrolyte. Thus, if a single electrolyte (E) was present in the sprayed solution, one would expect that the observed peak intensity Ie will increase with the square root of the concentration of that electrolyte (Cg, see Eq. (1.7)). At flow rates higher than that corresponding to the cone jet mode, the dependence on the concentration is lower than the 0.5 power [36]. Because ESI-MS is a very sensitive method, so that detection of electrolytes down to 10 M is easily feasible, one seldom works in practice with a single electrolyte system. The presence of electrolyte ions E leads to two concentration regimes for the analyte A ... [Pg.17]

Although it is hard to draw a sharp distinction, emulsions and foams are somewhat different from systems normally referred to as colloidal. Thus, whereas ordinary cream is an oil-in-water emulsion, the very fine aqueous suspension of oil droplets that results from the condensation of oily steam is essentially colloidal and is called an oil hydrosol. In this case the oil occupies only a small fraction of the volume of the system, and the particles of oil are small enough that their natural sedimentation rate is so slow that even small thermal convection currents suffice to keep them suspended for a cream, on the other hand, as also is the case for foams, the inner phase constitutes a sizable fraction of the total volume, and the system consists of a network of interfaces that are prevented from collapsing or coalescing by virtue of adsorbed films or electrical repulsions. [Pg.500]

We hope to have convinced the reader by now that the tunneling centers in glasses are complicated objects that would have to be described using an enormously big Hilbert space, currently beyond our computational capacity. This multilevel character can be anticipated coming from the low-temperature perspective in Lubchenko and Wolynes [4]. Indeed, if a defect has at least two alternative states between which it can tunnel, this system is at least as complex as a double-well potential—clearly a multilevel system, reducing to a TLS at the lowest temperatures. Deviations from a simple two-level behavior have been seen directly in single-molecule experiments [105]. In order to predict the energies at which this multilevel behavior would be exhibited, we first estimate the domain wall mass. Obviously, the total mass of all the atoms in the droplet... [Pg.144]

The mechanisms of ion formation are usually studied with measurements of mass separated ion energy distributions using a magnetic sector mass spectrometer.144,145 For a liquid metal ion source, both atomic ions and cluster ions of all sizes are emitted. If the total ion current is large, neutral atoms and small droplets may also be emitted. There is little question that most of the atomic ions in a liquid metal ion source at low... [Pg.362]

ESI has important characteristics for instance, it is able to produce multiply charged ions from large molecules. The formation of ions is a result of the electrochemical process and of the accumulation of charge in the droplets. The ESI current is limited by the electrochemical process that occurs at the probe tip and is sensitive to concentration rather than to total amount of sample. [Pg.46]

Ions, either positive or negative, of an analyte A will be desorbed from the droplets, producing a theoretical ion current a = Ap[A], where k,A is a rate constant depending on the nature of A. Let us suppose that another ion B is produced from the buffer, at a rate IB = kn B, and that no other ions are sprayed. The total ion current for these two ions... [Pg.52]

The electrical current due to the droplets motion can be measured easily by the amperometer (A) shown in Fig. 1.1. This measurement allows to estimate, from a quantitative point of view, the total number of elementary charges leaving the capillary and which, theoretically, may correspond to gas-phase ions. The droplet current I, the droplet radii R, and charge q were originally calculated by Pfeifer and Hendricks (Pfeifer and Hendricks, 1968) ... [Pg.17]

We also studied12 the relationship between the thickness of the tip (apex angle = 90°) and the electrospray performance and found that the parylene thickness does not affect the spray performance. Spray performance from three tips was compared with different thicknesses (3, 5 and 7 pm) whose sizes were the same as the triangular tip in Figure 6.4. The monitored total ion currents for these three tips were 35.5 1.2 nA for the 3 pm thick tip, 35.3 1.5 nA for the 5pm thick tip and 35.8 1.4nA for the 7pm tip. Liquid droplets were confined to the tips in all cases. This indicates clearly that only the top surface of the triangular tip is involved in the ESI activity. [Pg.136]

In 1898 J. J. Thomson produced gaseous ions in moist air by exposure to X-rays, and then produced a cloud of water droplets by cooling by adiabatic expansion. He calculated the size of the droplets by the rate of settling of the cloud, using Stokes s law (see p. 745). The total weight of water precipitated was known from the cooling effect and he measured the current produced in the gas by an applied potential difference. The charge on the drop was found to be 6 5 X 10 e.s.u., later corrected to 3 4 x e.s.u. By a similar method H. A. Wilson found 3 1 x io e.s.u. [Pg.931]

There are three basic stages to the process, shown in Figure 11.9, external to the electrolysis section. SO2 is absorbed and reacts with the bromine. The reactor product solution is then concentrated by evaporation using the sensible heat contained in the entering flue gas. All the HBr and the majority of the water are vaporised and an 80% to 85% sulphuric acid solution is produced. The desulphurised gas leaving the reactor is scrubbed with water to remove the HBr and the acid droplets. In the ISPRA plant the total electrode surface area is 64 m. The current density of operation is 2000 A m and at a temperature of 50°C the cell voltage is between 1.3-1.4 V and the current efficiency for bromine production is 90%. [Pg.383]

The tendency ofkA/kE to approach unity at low CAand Cb indicates [36] that there is a depletion of the ion that has the higher sensitivity k. This is the tetrabutylammonium ion (A) in the present example. At Ca = Cb < Ce 10 M, the current I, the total charge Q of the droplets, and the number of charged droplets are maintained by the presence of the electrolyte E, whose concentration is much higher. Under these conditions, species like A" " and with large coefficients and kB find plenty of droplet surface to go to, and the ions evaporate rapidly even when present at very low concentrations. This results in a depletion of theh concentration. The ion A of higher sensitivity is depleted more than B, and this leads to an apparent finding... [Pg.19]


See other pages where Current total droplet is mentioned: [Pg.149]    [Pg.21]    [Pg.7]    [Pg.198]    [Pg.152]    [Pg.671]    [Pg.162]    [Pg.60]    [Pg.365]    [Pg.672]    [Pg.183]    [Pg.297]    [Pg.821]    [Pg.115]    [Pg.115]    [Pg.120]    [Pg.135]    [Pg.261]    [Pg.255]    [Pg.1338]    [Pg.931]    [Pg.83]    [Pg.228]    [Pg.160]    [Pg.126]    [Pg.18]    [Pg.45]    [Pg.308]    [Pg.1]    [Pg.15]    [Pg.282]    [Pg.980]    [Pg.31]    [Pg.156]    [Pg.671]    [Pg.92]   
See also in sourсe #XX -- [ Pg.21 ]




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