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Active state

Electrochemical iron dissolution is a process in which metal atoms are transferred as ions from the lattice surface sites into the interstices of the [Pg.203]

Modern Aspects of Electrochemistry, Number 29, edited by John O M. Bockris et al. Plenum Press, New York, 1996. [Pg.203]

It is a well-known fact that iron dissolution occurs in four different states, namely, the active, passive, transpassive, and brightening states, determined by the nature and kinetics of the reactions involved, which depend in turn on the potential and electrolyte composition. A schematic polarization curve for anodic dissolution of iron in acid solutions is given in Fig. 1. The shape of the curve depends on the nature of the electrolyte, the polarization program, and hydrodynamics. The Fe/Fe, and [Pg.204]

The overall active range of iron dissolution was subdivided by Lorenz et into the following ranges  [Pg.204]

ACTIVE STATE PASSIVE STATE TRANST SIVEj BRIGHTEN STATE iING STATE [Pg.205]


A quantitative theory of rate processes has been developed on the assumption that the activated state has a characteristic enthalpy, entropy and free energy the concentration of activated molecules may thus be calculated using statistical mechanical methods. Whilst the theory gives a very plausible treatment of very many rate processes, it suffers from the difficulty of calculating the thermodynamic properties of the transition state. [Pg.402]

In many instances tire adiabatic ET rate expression overestimates tire rate by a considerable amount. In some circumstances simply fonning tire tire activated state geometry in tire encounter complex does not lead to ET. This situation arises when tire donor and acceptor groups are very weakly coupled electronically, and tire reaction is said to be nonadiabatic. As tire geometry of tire system fluctuates, tire species do not move on tire lowest potential energy surface from reactants to products. That is, fluctuations into activated complex geometries can occur millions of times prior to a productive electron transfer event. [Pg.2976]

Diltiazem inhibits calcium influx via voltage-operated channels and therefore decreases intracellular calcium ion. This decreases smooth muscle tone. Diltiazem dilates both large and small arteries and also inhibits a-adrenoceptor activated calcium influx. It differs from verapamil and nifedipine by its use dependence. In order for the blockade to occur, the channels must be in the activated state. Diltiazem has no significant affinity for calmodulin. The side effects are headache, edema, and dizziness. [Pg.142]

Additive inhibitors have been developed to reduce the contaminant coke produced through nickel-cataly2ed reactions. These inhibitors are injected into the feed stream going to the catalytic cracker. The additive forms a nickel complex that deposits the nickel on the catalyst in a less catalyticaHy active state. The first such additive was an antimony compound developed and first used in 1976 by Phillips Petroleum. The use of the antimony additive reportedly reduced coke yields by 15% in a commercial trial (17). [Pg.210]

The catalyst is then transferred back to the first process reactor and is reheated to the reforming process temperature at the reactor inlet using a flow of hydrogen-rich process recycle gas, thereby achieving reduction of the platinum to a catalyticaUy active state. [Pg.223]

Electroless reactions must be autocatalytic. Some metals are autocatalytic, such as iron, in electroless nickel. The initial deposition site on other surfaces serves as a catalyst, usually palladium on noncatalytic metals or a palladium—tin mixture on dielectrics, which is a good hydrogenation catalyst (20,21). The catalyst is quickly covered by a monolayer of electroless metal film which as a fresh, continuously renewed clean metal surface continues to function as a dehydrogenation catalyst. Silver is a borderline material, being so weakly catalytic that only very thin films form unless the surface is repeatedly cataly2ed newly developed baths are truly autocatalytic (22). In contrast, electroless copper is relatively easy to maintain in an active state commercial film thicknesses vary from <0.25 to 35 p.m or more. [Pg.107]

In HIC, the hydrophobic interactions are relatively weak, often driven by salts in moderate concentration (I to 2 M), and depend primarily on the exposed residues on or near the protein surface preservation of the native, biologically active state of the protein is an important feature of HIC. Elution can be achieved differentially by decreasing salt concentration or increasing the concentration of polarity perturbants (e.g., ethylene glycol) in the eluent. [Pg.2062]

It follows from this discussion that all of the transport properties can be derived in principle from the simple kinetic dreoty of gases, and their interrelationship tlu ough k and c leads one to expect that they are all characterized by a relatively small temperature coefficient. The simple theory suggests tlrat this should be a dependence on 7 /, but because of intermolecular forces, the experimental results usually indicate a larger temperature dependence even up to for the case of molecular inter-diffusion. The Anhenius equation which would involve an enthalpy of activation does not apply because no activated state is involved in the transport processes. If, however, the temperature dependence of these processes is fitted to such an expression as an algebraic approximation, tlren an activation enthalpy of a few kilojoules is observed. It will thus be found that when tire kinetics of a gas-solid or liquid reaction depends upon the transport properties of the gas phase, the apparent activation entlralpy will be a few kilojoules only (less than 50 kJ). [Pg.112]

Fig. 22.1. (a) The ethylene molecule or monomer (b) the monomer in the activated state, ready to polymerise with others (<)-(f) the ethylene polymer ("polyethylene") the chain length is limited by the addition of terminators like —OH. The DP is the number of monomer units in the chain. [Pg.229]

Rectifiers working according to the control diagram in Fig. 8-6 are used for anodic corrosion protection in passivatable systems that go spontaneously from the passive to the active state when the protection current is switched off [12]. The predetermined nominal voltage between reference electrode and protected object is compared with the actual voltage f/j in a differential display unit D. The difference AU = is amplified in a voltage amplifier SV to VqAU. This... [Pg.235]

The original microscopic rate theory is the transition state theory (TST) [10-12]. This theory is based on two fundamental assumptions about the system dynamics. (1) There is a transition state dividing surface that separates the short-time intrastate dynamics from the long-time interstate dynamics. (2) Once the reactant gains sufficient energy in its reaction coordinate and crosses the transition state the system will lose energy and become deactivated product. That is, the reaction dynamics is activated crossing of the barrier, and every activated state will successfully react to fonn product. [Pg.201]

A number of kinase structures have been determined in various catalytic states. For example, structures of the cyclin-dependent kinase, CDK2, in its inactive state and in a partially active state after cyclin binding have been discussed in Chapter 6. The most thoroughly studied kinase is the cyclic AMP-dependent protein kinase the structure of both the inactive and the active... [Pg.277]

Passivity—a condition of a metal or alloy in which the material is normally thermodynamically unstable in a given electrolytic solution but remains visibly unchanged for a prolonged period. The electrode potential of a passive metal is always appreciably more noble than its potential in the active state. [Pg.49]

Fig. I. Field emission dala from a mounted nanotube. An activated nanotube emits a higher current when heated by the laser than when the laser beam is bloeked (a). When aetivated by exposing the nanotube to oxygen while heating the tip, this behavior is reversed, and the emission current increases dramatically when the laser is blocked. The activated state can also be achieved by laser heating while maintaining a bias voltage of —75 V. Note that the scale of the two plots is different the activated current is always higher than the inactivated current. As discussed in the text, these dala led to the conclusion that the emitting feature is a chain of carbon atoms pulled from a single layer of the nanotube —an atomic wire. Fig. I. Field emission dala from a mounted nanotube. An activated nanotube emits a higher current when heated by the laser than when the laser beam is bloeked (a). When aetivated by exposing the nanotube to oxygen while heating the tip, this behavior is reversed, and the emission current increases dramatically when the laser is blocked. The activated state can also be achieved by laser heating while maintaining a bias voltage of —75 V. Note that the scale of the two plots is different the activated current is always higher than the inactivated current. As discussed in the text, these dala led to the conclusion that the emitting feature is a chain of carbon atoms pulled from a single layer of the nanotube —an atomic wire.
If the vapor pressure of the sorbent in its active state is below that of the gas being dehumidified, moisture is absorbed from the gas stream. As the process continues, the sorbent liecomes diluted due to the moisture increase. See Fig, 9,17,... [Pg.724]

The process for initiating radical formation in aromatic amine-vinyl monomer systems have been studied by Feng et al. [80-86] who proposed the formation of an aminium radical as the active state of an exciplex as intimate ion-pair and then a cyclic transition state which then would undergo a proton transfer process of deprotonation leading to the formation of active radical species for initiation as follows ... [Pg.238]

The end group of the polymers, photoinitiated with aromatic amine with or without the presence of carbonyl compound BP, has been detected with absorption spectrophotometry and fluororescence spectrophotometry [90]. The spectra showed the presence of tertiary amino end group in the polymers initiated with secondary amine such as NMA and the presence of secondary amino end group in the polymers initiated with primary amine such as aniline. These results show that the amino radicals, formed through the deprotonation of the aminium radical in the active state of the exciplex from the primary or secondary aromatic amine molecule, are responsible for the initiation of the polymerization. [Pg.239]

In de-aerated 10sulphuric acid (Fig. 3.45) the active dissolution of the austenitic irons occurs at more noble potentials than that of the ferritic irons due to the ennobling effect of nickel in the matrix. This indicates that the austenitic irons should show lower rates of attack when corroding in the active state such as in dilute mineral acids. The current density maximum in the active region, i.e. the critical current density (/ ii) for the austenitic irons tends to decrease with increasing chromium and silicon content. Also the current densities in the passive region are lower for the austenitic irons... [Pg.601]

Tantalum is severely attacked at ambient temperatures and up to about 100°C in aqueous atmospheric environments in the presence of fluorine and hydrofluoric acids. Flourine, hydrofluoric acid and fluoride salt solutions represent typical aggressive environments in which tantalum corrodes at ambient temperatures. Under exposure to these environments the protective TajOj oxide film is attacked and the metal is transformed from a passive to an active state. The corrosion mechanism of tantalum in these environments is mainly based on dissolution reactions to give fluoro complexes. The composition depends markedly on the conditions. The existence of oxidizing agents such as sulphur trioxide or peroxides in aqueous fluoride environments enhance the corrosion rate of tantalum owing to rapid formation of oxofluoro complexes. [Pg.894]


See other pages where Active state is mentioned: [Pg.402]    [Pg.1688]    [Pg.1976]    [Pg.2536]    [Pg.64]    [Pg.18]    [Pg.532]    [Pg.173]    [Pg.505]    [Pg.2432]    [Pg.365]    [Pg.398]    [Pg.61]    [Pg.475]    [Pg.107]    [Pg.114]    [Pg.469]    [Pg.469]    [Pg.445]    [Pg.12]    [Pg.484]    [Pg.425]    [Pg.207]    [Pg.667]    [Pg.27]    [Pg.591]    [Pg.163]    [Pg.546]    [Pg.766]    [Pg.894]    [Pg.1149]    [Pg.33]   
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Absolute Rate (Transition State) Theory and the Activated Complex

Activated complex or transition state

Activated complex theory transition state

Activated complex, and transition states

Activated complex, transition state

Activated energy state

Activated state

Activated state

Activated state Activation energy

Activated state during diffusion

Activated state theory

Activated state theory, mineral dissolution

Activated state theory, polymer transport

Activation analysis with solid state detectors

Activation energy relation with Transition-state theory

Activation energy solid state regarding

Activation energy states

Activation energy transition-state complex

Activation energy, apparent transition state theory

Activation free energy excited state

Activation state

Activation state

Activation volume excited state

Activation, transition state

Active Association States

Active Dynamic Hand Splints State of the Art

Active pharmaceutical ingredient solid-state characterization

Active pharmaceutical ingredients solid-state properties

Active state, characterization

Active state, iron

Actively caring states

Activities and Standard States An Overall View

Activities and Standard States of Strong Electrolytes

Activities, Activity Coefficients and Standard States

Activity and standard states

Activity and the Standard State

Activity coefficient pure-component standard state

Activity coefficient transition state

Activity coefficients and solution standard states

Activity coefficients in states of uniform composition

Amorphous polymers activated state theory

Anodic dissolution activated state

Brim States as Active Sites in Hydrotreating Catalysts

C-H activation transition state

Catalytic active state

Catalytic properties substrate active states

Complete active space state interaction

Desulfovibrio gigas hydrogenase activity state

Diffusion coefficients activated state theories

Disease states, profiling enzyme activities

Dual activation transition-state model

Electron paramagnetic resonance active spin states

Employment First Activating the British Welfare State

Energetics and Reaction Pathways Metallic Edge States as Active Sites

Enhancing the actively caring person states

Enzyme Active Sites Are Most Complementary to the Transition State Structure

Hydrocarbon activation transition-state energies

Hydrogenase activation states

Ideal solutions calculating state-dependent activity

Initial state preparation chemical activation

Isomeric reactions activated state

Nitrogenase activity states

Optical Properties of the Activated State

Optically active state

Oxidation State of Gold in Active Catalysts

Oxidation state active catalysts

Oxidation state active sites

Partial agonism and the two-state model of receptor activation

Pure components, calculating state-dependent activity

Redox State and Biologic Activity

Redox-Active Solid-State Electrolytes

Resting-state active sites

Shock Activation Enhanced Solid State Reactivity

Solid State Conformations of Drugs and Biologically Active Molecules

Solid state fermentation water activity

Standard State and Thermodynamic Activity

Standard state for activity

Standard state species activity based

State Government Activities

State activation energy and

State of the active catalysts

State-selective active-space methods

Steady-state activation

Steady-state activity

The Active Site and Transition States

The welfare state perspective Is there a contingent convergence of activation policies

Thermally activated reorientations and tunnel relaxation of orientational states in a phonon field

Transient-state kinetic analysis Enzyme active sites

Transition State Theory Molecular Nature of the Activated Complex

Transition state (activated

Transition state activation energy

Transition state and activation energy

Transition state theory , development activated complex

Transition state theory activation energy

Transition state theory enthalpy of activation

Transition state theory entropy activation

Transition state theory entropy of activation

Transition-State or Activated Complex Theory

Transition-state theory catalytic activity

United state activities

Variable state activation theory

Zero-order state, optically active

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