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Linear energy transfer equations

Stopping power or linear energy transfer (LET) is the energy lost per unit path length. Equation 6-2 expresses this relationship. [Pg.26]

The application of the calculation method based on derived relationships between the yields of some radiolysis products and the amounts of linear energy transfer (LET) made it possible to determine the value of the observed yield of water decomposition in aerated solutions. The value obtained is in agreement with the quantity G(—H20)02, found by the equation of material balance. [Pg.290]

Here Sons is the Onsager slope-to-intercept ratio (see Equation 41 of Chapter 4). dE/dx denotes the linear energy transfer. In order to determine Tgj the amplitude is measured as a function of E and the values are compared to calculated values with t and of the particular liquid and Xgi as a parameter (Gonidec et al., 1988). [Pg.321]

Steady-State Fluorescence Depolarization Spectroscopy. For steady state depolarization measurements, the sample is excited with linearly polarized lig t of constant intensity. Observed values of P depend on the angle between the absorption and emission dipole moment vectors. In equation 2 (9), Po is the limiting value of polarization for a dilute solution of fluorophores randomly oriented in a rigid medium that permits no rotation and no energy transfer to other fluorophores ... [Pg.183]

This equation shows that the ratio between the acceptor and donor fluorescence quantum yields is directly proportional to the energy-transfer rate constant kET. We have shown that this leads to the following linear relation between the fluorescence intensity of the acceptor 70x and that of the donor 7py, and the occupation probability pQx of the acceptor [3, 77] ... [Pg.52]

Evaporated PDA(12-8) film was used as a nonlinear optical medium in a layered guided wave directional coupler. The directional coupling phenomenon happens in two adjacent waveguide by periodical energy transfer. The theory of linear directional coupler was exactly established [11]. It can be reduced to coupled mode equations ... [Pg.328]

Here, T is the appropriate state variable conjugate to the flux J and X, and depends on the thermodynamic state of the system. These linear, phenomenological laws are fundamental to all processes involving the transfer of mass, momentum or energy but, in many practical circumstances encountered in industry, the fundamental transport mechanisms arise in parallel with other means of transport such as advection or natural convection. In those circumstances, the overall transport process is far from simple and linear. However, the description of such complex processes is often rendered tractable by the use of transfer equations, which are expressed in the form of linear laws such as... [Pg.122]

You saw how the equations governing energy transfer, mass transfer, and fluid flow were similar, and examples were given for one-drmensional problems. Examples included heat conduction, both steady and transient, reaction and diffusion in a catalyst pellet, flow in pipes and between flat plates of Newtonian or non-Newtonian fluids. The last two examples illustrated an adsorption column, in one case with a linear isotherm and slow mass transfer and in the other case with a nonlinear isotherm and fast mass transfer. Specific techniques you demonstrated included parametric solutions when the solution was desired for several values of one parameter, and the use of artificial diffusion to smooth time-dependent solutions which had steep fronts and large gradients. [Pg.169]

As long as r > 3R0, the fluorescence decay is close to exponential, the lifetime of the donor fluorescence decreases linearly with increasing concentration of A and fluorescence quenching obeys Stern Volmer kinetics (Section 3.9.8, Equation 3.36). However, the bimolecular rate constants ket of energy transfer derived from the observed quenching of donor fluorescence often exceed the rate constants of diffusion kd calculated by Equation 2.26, because resonance energy transfer does not require close contact between D and A. Finally, when r < 3R0, at high concentrations and low solvent viscosity, the kinetics of donor fluorescence become complicated, but an analysis is possible,109,110 if required. [Pg.57]


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Linearization, linearized equations

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