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Normalised equations

Rather than the integral equation approach of Rampazzo [459], the direct simulation from the transport equations is used here. In order to obtain a certain surface concentration T or fractional coverage 0, the substance in question must first arrive at the electrode, by some transport process. As was shown in Chap. 2, the normalised equation describing the accumulation of substance at the electrode is... [Pg.189]

Henry s constant is the standard-state fugacity for any component i whose activity coefficient is normalised by Equation (14). ... [Pg.19]

Fig. 1.12 Three normal distributions with different values of a (Equation (1.55)). The functions are normalised, so the area under each curve is the same. Fig. 1.12 Three normal distributions with different values of a (Equation (1.55)). The functions are normalised, so the area under each curve is the same.
T indicates that the integration is over all space. Wavefunctions which satisfy this condition re said to be normalised. It is usual to require the solutions to the Schrodinger equation to be rthogonal ... [Pg.50]

Q is given by Equation (6.4) for a system of identical particles. We shall ignore any normalisation constants in our treatment here to enable us to concentrate on the basics, and so it does not matter whether the system consists of identical or distinguishable particles. We also replace the Hamiltonian by the energy, E. The internal energy is obtained via Equation (6.20) ... [Pg.327]

The variation of the ia-plane shear modulus normalised with respect to the matrix modulus as a function of the fiber volume fraction is shown ia Figure 11. As noted eadier, it is generally difficult to measure the shear modulus of the fibers, which may themselves be anisotropic. The equation should be used with caution. [Pg.11]

The solution of this equation is in the form of a Bessel function 32. Again, the characteristic length of the cylinder may be defined as the ratio of its volume to its surface area in this case, L = rcJ2. It may be seen in Figure 10.13 that, when the effectiveness factor rj is plotted against the normalised Thiele modulus, the curve for the cylinder lies between the curves for the slab and the sphere. Furthermore, for these three particles, the effectiveness factor is not critically dependent on shape. [Pg.643]

We now transform the eq.(22) in the same way as done for the eq.(14) we assume that the (normalised) optimum orbitals have been determined by some existing Quantum Chemistry program along with the partial waves Rn and with the potential terms J./m, and Gum- Using these quantities we then set up the equation... [Pg.29]

The denominator in this equation represents the area under the curve of Figure 5.12 and serves to normalise the expression, so that f(x) —> 1 as x 0- The absorption correction factor Ea is equal to 1 //(%). [Pg.145]

The next step is to generate all possible and allowed conformations, which leads to the full probability distribution F). The normalisation of this distribution gives the number of molecules of type i in conformation c, and from this it is trivial to extract the volume fraction profiles for all the molecules in the system. With these density distributions, one can subsequently compute the distribution of charges in the system. The charges should be consistent with the electrostatic potentials, according to the Poisson equation ... [Pg.59]

Figure 5. Exact (numerical solution, continuous line) and linearised (equation (24), dotted line) velocity profile (i.e. vy of the fluid at different distances x from the surface) at y = 10-5 m in the case of laminar flow parallel to an active plane (Section 4.1). Parameters Dt = 10 9m2 s-1, v = 10-3ms-1, and v = 10-6m2s-1. The hydrodynamic boundary layer thickness (<50 = 5 x 10 4 m), equation (26), where 99% of v is reached is shown with a horizontal double arrow line. For comparison, the normalised concentration profile of species i, ct/ithe linear profile of the diffusion layer approach (continuous line) and its thickness (<5, = 3 x 10 5m, equation (34)) have been added. Notice that the linearisation of the exact velocity profile requires that <5, Figure 5. Exact (numerical solution, continuous line) and linearised (equation (24), dotted line) velocity profile (i.e. vy of the fluid at different distances x from the surface) at y = 10-5 m in the case of laminar flow parallel to an active plane (Section 4.1). Parameters Dt = 10 9m2 s-1, v = 10-3ms-1, and v = 10-6m2s-1. The hydrodynamic boundary layer thickness (<50 = 5 x 10 4 m), equation (26), where 99% of v is reached is shown with a horizontal double arrow line. For comparison, the normalised concentration profile of species i, ct/ithe linear profile of the diffusion layer approach (continuous line) and its thickness (<5, = 3 x 10 5m, equation (34)) have been added. Notice that the linearisation of the exact velocity profile requires that <5, <c <5o...
The result of equating the steady-state fluxes, equations (14) and (15), is sometimes known as the Best equation [9,13,16,27-31] which we normalise to its most elementary parameters [26] (other normalisations have also been suggested [21]) ... [Pg.156]

This change in the supply flux Jmkm due to changing ro is bound to affect the uptake flux. A decrease in ro implies an increase in /m and a decrease in b (see equation (77)) which results in an increase of the normalised flux / (see equation (17)). However, it must be pointed out that the internalisation step can become rate determining, and then the flux will not change any more below some ro value. [Pg.185]

Figure 2 The normalised polymerization rate, RIKk/n, plotted against the total relative concentration of ions, c/K, according to equation (17). The value of P is... Figure 2 The normalised polymerization rate, RIKk/n, plotted against the total relative concentration of ions, c/K, according to equation (17). The value of P is...
Alternatively, Matlab s built-in function norm can be used to determine normalisation coefficients and perform the same task. An example for column-wise normalisation of a matrix X with orthogonal columns is given below. It is worthwhile to compare X with equation (2.15) the subspace command can be used to determine the angle between the vectors (in rad) and reconfirm orthogonality. ... [Pg.25]

Now we use the information gathered so far for the prediction of the 10 test samples Ys removed from the complete data set at the veiy beginning. The function PCR PLS pred. m does the work according to equation (5.70). Importantly the mean-centring and normalisation have to be performed in exactly the same way as in the calibration. [Pg.302]


See other pages where Normalised equations is mentioned: [Pg.41]    [Pg.158]    [Pg.158]    [Pg.48]    [Pg.364]    [Pg.82]    [Pg.452]    [Pg.41]    [Pg.158]    [Pg.158]    [Pg.48]    [Pg.364]    [Pg.82]    [Pg.452]    [Pg.256]    [Pg.48]    [Pg.52]    [Pg.57]    [Pg.62]    [Pg.64]    [Pg.67]    [Pg.80]    [Pg.328]    [Pg.504]    [Pg.345]    [Pg.11]    [Pg.365]    [Pg.6]    [Pg.366]    [Pg.186]    [Pg.411]    [Pg.459]    [Pg.43]    [Pg.178]    [Pg.59]    [Pg.251]    [Pg.259]   
See also in sourсe #XX -- [ Pg.82 ]




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Integral equation for the box-normalised collision state

Normalising

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