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First Order Schemes

The first order correction function for this scheme is then given by the particular [Pg.291]

The general solution of (7.21) will consist of the sum of the homogeneous solution / jxYzi( P) particular solution/fpYzj Z ) the usual way. However, since pp = 0 has as its only solution oc pp, the homogeneous solution of (7.21) is [Pg.291]

Thus for any first order scheme our line of attack will be to compute the perturbation operator c, plug it into the right hand side and solve the PDE to find the suitable correction function. It turns out that this is not so difficult at leading order, for simple first order schemes such as this. However at higher orders the complexity of the terms often limits our progress. [Pg.291]


A more convincing approach leads to an adaptive method based on the symmetric second order scheme (9). As a first step, we have to introduce a first order scheme substituting p of the previous section. In what follows, we use the following pair of schemes ... [Pg.404]

It should also be remembered that the discretization scheme influences the accuracy of the results. In most CFD codes, different discretization schemes can be chosen for the convective terms. Usually, one can choose between first-order schemes (e.g., the first-order upwind scheme or the hybrid scheme) or second-order schemes (e.g., a second-order upwind scheme or some modified QUICK scheme). Second-order schemes are, as the name implies, more accurate than first-order schemes. However, it should also be remembered that the second-order schemes are numerically more unstable than the first-order schemes. Usually, it is a good idea to start the computations using a first-order scheme. Then, when a converged solution has been obtained, the user can continue the calculations with a second-order scheme. [Pg.1032]

This implementation is second-order accurate with respect to the time and the size step. The scheme is general applicable and as shown in the next section, this scheme is also sensitive for discontinuities in Gn as caused by the R-Z model for fines removal. The oscillations are however less severe than for the method of lines. Also for this method a first-order scheme was Implemented. Here the so-called Lax scheme wcus chosen (8) ... [Pg.164]

A system such as this can readily be solved by using the Solver. The previous example of the isomerization of cis- [Ni(13aneN4)(H20)2] (Figure 23-5),is actually a case of coupled reversible first-order processes. There are two observable rate processes, Afast ai d Aglow/ but each is reversible. Treatment of the data according to the consecutive reversible first-order scheme is shown in Figure 23-6. [Pg.384]

The UDS approximation retains only the first term on the right hand side, hence the leading truncation error term term is of first order in Sxpe = xg — xp) so it is a first order scheme. [Pg.1027]

When the first-order scheme is semi-implicit with 0 < a < 1, this realizability condition is a mix of those found for pure advection and pure diffusion. [Pg.352]

The first-order scheme for convection is exactly the same as the one described in Section 8.3.2. The only difference (which is not strictly necessary) is that we will replace the... [Pg.353]

Equation 6.126 is a forward FDM, as grid points after j (here j + 1) are used for evaluation. It is a first-order scheme, as only one point is used. Higher order... [Pg.355]

The formation of volatile degradation products as observed by non-isothermal thermogravimetry is a complex process. The non-isothermal thermogravimetry curve that is apparently composed of several independent processes was described by the first-order scheme, i.e. — = km where t is time, m is the actual mass of the degraded sample, and k is the rate constant of polyolefin degradation to volatile products. In a non-isothermal mode,... [Pg.306]

Hence we can see that the [ABO scheme gives a first-order error in the variance of q. For significantly small friction (relative to h), the leading order term will be dominated by the term at order h", potentially giving us greater accuracy than we would expect from a first order scheme. [Pg.276]

This is not always the case for first order schemes, however. For example the scheme denoted [AOABJ is consistent with the dynamics, and may be used for integrating the overdamped (y = oo) Langevin equation. [Pg.295]

The procedure then follows just as in the case of the first order schemes. The form of the right-hand side C pp will be dependent on the choice of the update scheme, and can be computed using the BCH formula using Proposition 7.1. More complicated symmetric schemes involving more than five stages can be utilized, but these schemes may require more than one force evaluation per iteration, while increasing the complexity of the PDE to solve. [Pg.298]

The first order schemes of the form XYZ, as well as schemes such as XOYOX] are not consistent in this overdamped limit the errors in computed... [Pg.306]


See other pages where First Order Schemes is mentioned: [Pg.404]    [Pg.340]    [Pg.86]    [Pg.86]    [Pg.129]    [Pg.253]    [Pg.348]    [Pg.250]    [Pg.343]    [Pg.990]    [Pg.419]    [Pg.330]    [Pg.331]    [Pg.351]    [Pg.353]    [Pg.365]    [Pg.365]    [Pg.366]    [Pg.365]    [Pg.258]    [Pg.277]    [Pg.291]    [Pg.291]    [Pg.293]    [Pg.295]    [Pg.295]    [Pg.295]    [Pg.501]    [Pg.6359]    [Pg.150]    [Pg.279]    [Pg.279]    [Pg.280]    [Pg.380]   


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Ordering schemes

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