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Ideal sample capacitance

Figure 18. C(V) curves for a metal-Ba stearate semiconductor structure (multilayer thickness, 1000 A). Capacitance levels are indicated the max/min ratio depends on the parameters of the structure, and the absolute values of the capacitance depend of course on the area of the metal contact (a mercury probe). Different areas of the same sample were used to obtain the curves in the top and bottom figures.------------- an ideal, theoretical C(V) curve. Figure 18. C(V) curves for a metal-Ba stearate semiconductor structure (multilayer thickness, 1000 A). Capacitance levels are indicated the max/min ratio depends on the parameters of the structure, and the absolute values of the capacitance depend of course on the area of the metal contact (a mercury probe). Different areas of the same sample were used to obtain the curves in the top and bottom figures.------------- an ideal, theoretical C(V) curve.
In this book, an explanation of capacitive behaviour in similar and comparable systems is not directly possible with constant-phase elements because such a comparison is only possible if n values are equal, particularly in the study of surfaces covered with polymer coatings where a unification of the envisaged parameters is necessary. The impedances measured match with a relatively large amount of samples, of which the structure can be complex, showing many sources of non-idealities (e.g. variations in thickness of the membrane, pore size and pore density42 7). A good indication if such non-idealities occur can be found in the values of n. If they are not comparable, non-idealities occur. [Pg.56]

Arulepp et al. [81] reported an in situ technique of CDC activation whereby Ti02 was mixed with TiC and chlorinated. During synthesis, titanium in the Ti02 was etched, leaving controlled amounts of oxygen to etch the carbon. It was shown that the oxidation treatment improved the volumetric capacitance but not the gravimetric capacitance. This was perhaps because of unreacted Ti02 in the sample. The carbon was ideally polarizable at E < 2.8 V and showed a power density of 2.5kW/kg. [Pg.85]

Biosensors. Sensors are required to adequately monitor bioreactor performance. Ideally, one would like to have online sensors to minimize the number of samples to be taken from the bioreactor and to automate the bioreactor process. Most bioreactors have autoclavable pH and dissolved oxygen (D.O.) electrodes as online sensors, and use offline detectors to measure other critical parameters such as glucose and glutamine concentration, cell density, and carbon dioxide partial pressure (pC02). An online fiber-optic-based pC02 sensor is commercially available and appears to be robust.37 Probes are also commercially available that determine viable cell density by measuring the capacitance of a cell suspension. Data from perfusion and batch cultures indicate that these probes are reasonably accurate at cell concentrations greater than 0.5 X 106 cells/mL.38,39... [Pg.1435]

Figure 6.3 (a) Schematic representation of equivalent circuit for an ion conductor put between a pair of blocking electrode, and (b) the corresponding Nyquist plot. Ideally the sample-electrode interface is composed only of the double-layer capacitance. However, the practical Nyquist plot that corresponds to this frequency region is not vertical to the real axis. The rate-limiting process of this plot is that the ion diffuses to form a double layer. [Pg.79]

The use of irradiated particles as tracers provides an accurate way to measure particle velocity it allows one to calibrate low-cost flowmeters such as the capacitive flowmeter. Unfortunately, in most industrial environments, it is not possible to produce short-lived radioactive tracers. At ANL, a nuclear research reactor was available for the production of radioactive particles. Ideally, the density and size of the tracer particles and the solids in the flow should be the same so the tracers can be uniformly distributed in the flow and represent the solids velocity distribution. For that purpose, the sample particles to be activated were fabricated from resin, hardener, and indium oxide powder to closely duplicate the size and density of the glass beads used in the flow tests. The particles, after irradiated in the reactor, had a 54-min half-life of y activity. Twenty particles were injected into the flow stream during the reloading of the feed hopper, becoming randomly mixed with the glass beads. [Pg.246]

Impedance interfaces often provide the facility for automatically switching between measurements of the sample to be measured and measurements of a low loss calibrated reference capacitor (Figure 3.2.10). An ideal reference capacitor would have a completely flat response (constant capacitance) across the entire frequency range. This ideal capacitor cannot be achieved in reality since there will always be some parallel resistance in the capacitor even though this can, in practice, be an extremely high value. However, the difference between an ideal and nonideal capacitor is sufficiently small for most purposes and the reference capacitor is a very useful tool that can be used to quantify errors due to cables and instrument measurement errors. The deviation of the capacitor from its ideal response due to cables... [Pg.184]

As shown in Figure 8.7a, for ideal electrolyte sample dense at 100%, a circle is observed. However, in a real cell, additional contributions must be taken into account grain boundary at intermediate frequency and the electrode response at low frequency. The capacity ranges for each contribution are shown in Figure 8.7b. The bulk response, observed at high frequency, is associated with capacitance of about 10 F. The capacitance associated with grain boundaries is in the range of 10 F, whereas the electrode response corresponds to a capacitance of 10 F. From these data, both the electrolyte resistance and the electrode resistance can be derived. [Pg.175]

The atomic emission source provides for sample vaporization, dissociation, and excitation. The ideal excitation source will allow the excitation of all lines of interest for the elements in the sample, and do this reproducibly over enough time to encompass full elemental excitation. Excitation sources include but are not limited to (1) inductively coupled plasma (ICP), (2) direct current plasmas (DCP), (3) microwave induced plasmas (MIP), and (4) capacitively coupled... [Pg.45]

For an ideal insulating dielectric, s measured in the frequency domain is a real quantity and is equal to the ratio of the capacitances measured with sample in and sample out of the active electrode region i.e. [Pg.603]

These examples represent a circuit composed of ideal capacitive and resistive electrical components. The path of least impedance through a real-life sample placed between two conducting metal electrodes can be represented... [Pg.14]


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