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Free proton transport

The protons are dissociated away in contact with the water in the internal channels. Center. A covalent bonding of proton donor-acceptor molecules and a sufficiently dense stacking leads to a solvent free proton transport. Bottom. In the soggy sand electrolytes anions are absorbed at the surfaces of the insulating matrix (e.g., SiOJ. The respective cations (e.g., Li+) are free while far away from the matrix essentially associated in form of ions pairs if the solvent is a weak dielectric. [Pg.39]

As previously mentioned, during flight, the air density changes significantly. The air pressure at 0 MSL (mean sea level) is approximately 1 bar, and at 10,000 m MSL, the air pressure is 260 mbar. Due to water-free proton transport in the HT-PEFC electrolyte, a constant conductivity of the membrane can be expected for low air densities. Figure 23.1a shows a lab test measurement of an HT-PEFC 70 cell stack (49 cm ) at varying ambient pressures from 1 bar to 660 mbar. The decrease in performance at low pressure is moderate compared to a low temperature PEFC, which experiences pronounced drying of the membrane, with an approximately... [Pg.513]

Methods similar to those discussed in this chapter have been applied to determine free energies of activation in enzyme kinetics and quantum effects on proton transport. They hold promise to be coupled with QM/MM and ab initio simulations to compute accurate estimates of nulcear quantum effects on rate constants in TST and proton transport rates through membranes. [Pg.417]

In the case of PEMs, the situation is more complicated because the sulfonate counter-ions (in the case of a PEM such as Nafion ) are bound to the polymer chain and are thus relatively immobile, in contrast to the free counter-ion in a small molecule acid such as sulfuric or acetic acid. Tethering of the sulfonate group can be considered to be an impediment to the mobility of the proton as it traverses the membrane. Proton mobility is also affected by the effective mean-free path of connectivity of the conduction pathway as shown in Figure 3.2. In situation (a), the increased number of dead ends and tortuosity of the aqueous domains through which proton transport occurs over the situation in (b) leads to lower overall mobility. This has been demonstrated by Kreuer and will be discussed later in this section. [Pg.109]

Proton conductivities of 0.1 S cm at high excess water contents in current PEMs stem from the concerted effect of a high concentration of free protons, high liquid-like proton mobility, and a well-connected cluster network of hydrated pathways. i i i i Correspondingly, the detrimental effects of membrane dehydration are multifold. It triggers morphological transitions that have been studied recently in experiment and theory.2 .i29.i ,i62 water contents below the percolation threshold, the well-hydrated pathways cease to span the complete sample, and poorly hydrated channels control the overall transports ll Moreover, the structure of water and the molecular mechanisms of proton transport change at low water contents. [Pg.381]

Cytochrome a + a3 This cytochrome complex is the only electron carrier in which the heme iron has a free ligand that can react directly with molecular oxygen. At this site, the transported electrons, molecular oxygen, and free protons are brought together to produce water (see Figure 6.8). Cytochrome a + 83 (also called cytochrome oxidase) contains bound copper atoms that are required for this complex reaction to occur. [Pg.76]

An anode configuration closely related to the AB approach is the so-called reconfigured anode, in which a thin layer of metal (such as Pt/C) or metal oxide (such as FeOx) is added to the outside of the anode GDL facing the flow field. - Unlike a normal anode electrode layer that is impregnated with ionomers for facile proton transport, this ionomer-free CO oxidation layer is hydrophobic for improved gas diffusion to help maximize the interaction between CO and O2. [Pg.261]

Figure 18.21. Proton Transport by Cytochrome C Oxidase. Four "chemical" protons are taken up from the matrix side to reduce one molecule of O2 to two molecules of H2O. Four additional "pumped" protons are transported out of the matrix and released on the cytosolic side in the course of the reaction. The pumped protons double the efficiency of free-energy storage in the form of a proton gradient for this final step in the electron-transport chain. Figure 18.21. Proton Transport by Cytochrome C Oxidase. Four "chemical" protons are taken up from the matrix side to reduce one molecule of O2 to two molecules of H2O. Four additional "pumped" protons are transported out of the matrix and released on the cytosolic side in the course of the reaction. The pumped protons double the efficiency of free-energy storage in the form of a proton gradient for this final step in the electron-transport chain.
Most of the information on the photoreactions of the chromophores (cf. below) is for the a -trans form. The 13-d5 chromophores produced in the photoreaction are C=N anfi[85] and not as well accommodated by the binding pocket this results in the thermal relaxation to aW-trans and thus the cyclic reaction. Because the position of the 0-ionone ring is fixed, the displacement caused by the bond isomerization around the C13-C14 bond is confined to the chain near the Schiff base. As will be discussed below, it is the movements near the Schiff-base region of the retinal which store excess free energy to drive the reactions of the photocycle and the accompanying proton transport. [Pg.195]

The end use defines the quality and quantity of the gas needed. For our purposes, the end use for the hydrogen generated is a fuel for fuel cells. Most commercial hydrogen generating units incorporate a drying mechanism that removes much of the moisture from the gas. This is not appropriate for a fuel cell system. Free water will be abundant and should be removed by a water filter or series of water filters, but it is not necessary to remove very fine aerosols by coalescer or to use water absorption techniques. The reason is that the hydrogen side of the fuel cell membrane needs to remain hydrated (moist at a certain level) to aid and maintain proton transport for the operation of the fuel cell. [Pg.150]

For each proton transported out of the matrix across the inner membrane and into the inner membrane space of a mitochondrion, how much free energy potential is generated across the inner membrane ... [Pg.309]

The predominating transport mechanism for such protons is by free proton jumps (Grotthus mechanism) between neighboring oxygen ions although, statistically, a concentration of oxygen vacancies will enable some protons to move as OH ions when the host oxygen ions jump to vacancies. [Pg.8]


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