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Batteries potential difference

A battery produces a potential difference between its two electrodes that is brought about by a decrease in potential energy as one coulomb moves from the... [Pg.116]

If the circuit is broken after the e.m.f. has been applied, it will be observed that the reading on the voltmeter is at first fairly steady, and then decreases, more or less rapidly, to zero. The cell is now clearly behaving as a source of current, and is said to exert a back or counter or polarisation e.m.f., since the latter acts in a direction opposite to that of the applied e.m.f. This back e.m.f. arises from the accumulation of oxygen and hydrogen at the anode and cathode respectively two gas electrodes are consequently formed, and the potential difference between them opposes the applied e.m.f. When the primary current from the battery is shut off, the cell produces a moderately steady current until the gases at the electrodes are either used up or have diffused away the voltage then falls to zero. This back e.m.f. is present even when the current from the battery passes through the cell and accounts for the shape of the curve in Fig. 12.1. [Pg.505]

As a reaction proceeds toward equilibrium, the concentrations of its reactants and products change and AG approaches zero. Therefore, as reactants are consumed in a working electrochemical cell, the cell potential also decreases until finally it reaches zero. A dead battery is one in which the cell reaction has reached equilibrium. At equilibrium, a cell generates zero potential difference across its electrodes and the reaction can no longer do work. To describe this behavior quantitatively, we need to find how the cell emf varies with the concentrations of species in the cell. [Pg.626]

A battery must use cell reactions that generate and maintain a large electrical potential difference. This requires two half-reactions with substantially different standard reduction potentials. The ideal battery would be compact, inexpensive, rechargeable, and environmentally safe. This is a stringent set of requirements. No battery meets all of them, and only a few come close. [Pg.1400]

The electricity-producing system of electric fishes is built as follows. A large number of flat cells (about 0.1 mm thick) are stacked like the flat unit cells connected in series in a battery. Each cell has two membranes facing each other. The membrane potentials of the two membranes compensate for each other. In a state of rest, no electrostatic potential difference can be noticed between the two sides of any cell or, consequently, between the ends of the stack. The ends of nerve cells come up to one of the membranes of each cell. When a nervous impulse is applied from outside, this membrane is excited, its membrane potential changes, and its permeability for ions also changes. Thus, the electrical symmetry of the cell is perturbed and a potential difference of about 0.1 V develops between the two sides. Since nervous impulses are applied simultaneously to one of the membranes in each cell, these small potential differences add up, and an appreciable voltage arises between the ends of the stack. [Pg.589]

While the voltage of the cell represents the potential difference between the two terminals of the battery, in reality it relates to the separation in energy between the two half-cells. We call this separation the emf where the initials derive from the archaic phrase electromotive force. An emf is defined as always being positive. [Pg.288]

There has been considerable progress in developing in vitro tests (a.25). The most success has been in local effects testing in biologically less complex systems, such as testing for skin and eye irritation. In contrast, efforts to develop in vitro tests to evaluate potential systemic toxicants have been hindered by the complexity of the systems involved, and it seems likely that a battery of different in vitro assays will be needed. [Pg.15]

The eleotrolysis is carried out in a medium-sized filter jar two moderately thiok oarbon rods serve as electrodes. The oathode dips into the solution, the anode into 2A7-sulphuric acid contained in a small porous cell, which also dips into the liquid. The eleotrodes are fixed a short distanoe apart and the current is obtained from two units, arranged in series, of an aooumulator battery of the usual capaoity. At a potential difference of 4 volts 1-5-2 amperes pass through the solution. [Pg.317]

In the circuit in Figure 14-3, the battery generates a potential difference of 3.0 V, and the resistor has a resistance of 1 Of) fl. We assume that the resistance of the wire connecting the battery and the resistor is negligible. How much current and how much power are delivered by the batteiy in this circuit ... [Pg.274]

Even when a system is in a steady state other than equilibrium certain physical quantities may be stationary Markov processes. An example are the current fluctuations in the circuit of fig. 7 when a battery is added, which maintains a constant potential difference and therefore a non-zero average current. Another example is a Brownian particle in a homogeneous gravitational field its vertical velocity is a stationary process, but not its position. [Pg.82]

Alessandro Volta built the first battery in 1800 permitting future research and applications to have a source of continuous electrical current available. The SI unit of electric potential difference is named after him. [Pg.228]

A dendrimer consisting of multiple identical and non-interacting redox units, able to reversibly exchange electrons with another molecular substrate or an electrode, can perform as a molecular battery [64, 65]. The redox-active units should exhibit chemically reversible and fast electron transfer processes at easily accessible potential difference and chemical robustness under the working conditions. [Pg.89]

The reaction centre found in many purple non-sulphur bacteria is a simple example of a group of proteins that are natureis solar batteries. The reaction centre uses the energy of sunlight to generate positive and negative charges on opposite sides of the bacterial cytoplasmic membrane. This potential difference drives a circuit of electron transfer reactions that are linked to proton translocation across this membrane. [Pg.621]


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See also in sourсe #XX -- [ Pg.649 ]




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