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Piecewise linear interpolation

ConstPUCling Piecewitee UneaP InterpofaitlOII Piecewise linear interpolation can be presented in a closed form, which simplifies the interpolation process. [Pg.645]

Surface (3D) Reconstruction Surface reconstruction from point clouds is fundamental in many applications. Using the raw point clouds or volumetric data acquired from an unknown surface, an approximation of the surface can be constructed and used to compare it with CAD models or for smface-based automated programming. Reconstruction methods can be classified into two types the computational geometry approach focuses on the piecewise-linear interpolation of unorganised points and defines the surface as a carefiilly chosen sub-set of the Delaunay triangulation in a Cartesian coordinate system, and the computer graphics... [Pg.339]

Here functions R(v) and C(v) can be obtained by piecewise-linear interpolation of the dependence of R and C parameters obtained by fitting the experimental spectra at different voltages (such as in Figure 4.5.4) to the impedance function in Eq. (10). Any other suitable smooth interpolation can be used. The impedance function has to be expressed in terms of electric parameters, as described in Section 4.5.1.3. For use in a discretized equivalent circuit, the values obtained from the fit have to be divided or multiplied by the number of chains, depending on the series or parallel position of the electric element. So, for series resistors it has to be divided, and for parallel, multiplied. It should be considered that the low-frequency limit of Re Z), used as a fitting parameter in the equation, is not always a simple sum of the discrete elements that constitute a transmission line. In particular, in Eq. (10) the Ra is 1/3 of the specific resistance multiplied by the transmission line length, as can be seen from Eq. (8). Therefore resistance of single chain shown in Eig 4.55 will be Ra 3/N. [Pg.441]

Piecewise linear interpolation based on Delaunay triangulation is used to get the surface over the selected shape. A buffer zone is used for 1-dimensional simplexes. [Pg.614]

There are some constraints on the shape functions in order to have a consistent finite element formulation. Equation 8.12 demands that the shape function Nn be at least linear in the spatial coordinates. The simplest and most widely used shape function in our case is perhaps the piecewise linear interpolation function as described in Kennedy (1995). With this shape function, one can achieve C° continuity in pressure, that is, the pressure field variable is continuous at element interface, but its gradients are not. The pressure gradient field is piecewise constant over the elements and is discontinuous across element interfaces. Consequently, the resulting velocity and shear rate fields are not continuous across element boundaries. An example of triangular elements with higher order shape functions can be found in Hieber and Shen (1980). [Pg.116]

A piecewise linear function interpolating a given set of (yi9 xt) values. [Pg.384]

The end points of any linear segment, x(ti) and x(ti+i), are either interpolated from the data or taken as actual data points as in the Boxcar method. These piecewise linear approximation techniques perform well for steady-state process data with little noise, but are inadequate for process data with important low amplitude transients and are inefficient for data with relevant high frequency features. Also, the line segments used in the approximation satisfy a local, not a global error criterion. [Pg.130]

Some standard one-dimensional GC methods use reference peaks to help recognize drift [23]. For more widely varying chromatographic conditions, retention times for targets can be related using a linear retenhon index (LRI) [24], in which retention times are referenced relative to the retention times of marker compounds. A common LRI scheme uses the n-alkanes as marker points with indices equal to 100 times the carbon number (foUowing the Kovats index [24]) then the indices for peaks between marker points are computed using piecewise hnear interpolation. If retention-time windows are defined relative to marker p>eaks that can be located, then any linear retention-time transformation observed in the marker jjeaks can be apphed to the windows used for chemical identification. [Pg.96]

Physical laws often cannot be described in closed form, or their representation in explicit form is very expensive. Frequently, the only information available is a set of measurement data. In these cases the laws are often represented as piecewise smooth interpolating functions (linear, splines,. .. ) or simple tables. [Pg.232]

The assignment between the mean value and the root mean square deviation of the simulated transmission signals, which are influenced by both effects, is shown in Fig. 12.5 for different theoretical relative extinction cross sections. This assignment, which is subsequently referred to as SE-Function, is defined by the results of the simulations described earlier. With the SE-Function each simulated or measured value pair of mean transmission and root mean square deviation is assigned to the associated theoretical relative extinction cross section. By piecewise linear 2D interpolation each simulated or measured value pair of mean transmission and root mean square deviation is assigned to the associated theoretical relative extinctiOTi cross section. [Pg.461]

Basically, the simulations can be performed for a variety of particle size distributions with different widths and shapes to determine the SE-Function. In this case, the correction of the polydispersity effect is carried out together with the correction of the boundary layer and the overlapping effect in one step by piecewise linear 3D interpolation. Thereby, a corrected particle size distribution is determined with an advanced PSD-SE-Method, which requires the measurement of enough independent transmission signals of tight beams with different geometries. [Pg.466]

MATLAB has several functions for interpolation. The function = interpl(x, y, x) takes the values of the independent variable x and the dependent variable y (base points) and does the one-dimensional interpolation based on x, to find yj. The default method of interpolation is linear. However, the user can choose the method of interpolation in the fourth input argument from nearest (nearest neighbor interpolation), linear (linear interpolation), spline (cubic spline interpolation), and cubic (cubic inteipolation). If the vector of independent variable is not equally spaced, the function interplq may be used instead. It is faster than interpl because it does not check the input arguments. MATLAB also has the function sp/ine to perform one-dimensional interpolation by cubic. splines, using nat-a- not method, ft can also return coefficients of piecewise poiynomiais, if required. The functions interp2, inte.rp3, and interpn perform two-, three-, and n-dimensional interpolation, respectively. [Pg.167]

Figure 3 Relationship between activation energy (E) and conversion (x) for capillary dilatometry. The error bars represent the standard errors of the values. The open (blue) symbols represent E values when the temperature corresponding to a desired value of conversion was obtained through linear interpolation of smoothed data (1 data point / K). On the other hand, the solid (red) S5mibols represent the E values when the temperature corresponding to a certain value of conversion was obtained using a piecewise sigmoidal fit of less smoothed data (10 data points / K). Figure 3 Relationship between activation energy (E) and conversion (x) for capillary dilatometry. The error bars represent the standard errors of the values. The open (blue) symbols represent E values when the temperature corresponding to a desired value of conversion was obtained through linear interpolation of smoothed data (1 data point / K). On the other hand, the solid (red) S5mibols represent the E values when the temperature corresponding to a certain value of conversion was obtained using a piecewise sigmoidal fit of less smoothed data (10 data points / K).
To obtain the isosteres, one must interpolate the pressure at a given quantity adsorbed at each temperature. To avoid large interpolation errors, particularly at low pressures, the data were fitted piecewise to well behaved polynomial functions by a least squares method. Typical isosteres are shown in Figure 5. The slope of an isostere was determined by linear regression on the interpolated points. The resulting isosteric heat curves are shown in Figure 6. [Pg.84]

The linear algebraic system consists of 3n - 3 equations and 3n - 3 unknowns that can be solved to produce the optimal piecewise cubic spline. Press, Teukolsky, Vetterling, and Flannery describe a routine for cubic spline interpolation. " ... [Pg.650]


See other pages where Piecewise linear interpolation is mentioned: [Pg.215]    [Pg.183]    [Pg.200]    [Pg.187]    [Pg.215]    [Pg.183]    [Pg.200]    [Pg.187]    [Pg.168]    [Pg.431]    [Pg.1003]    [Pg.265]    [Pg.153]    [Pg.121]    [Pg.650]    [Pg.348]    [Pg.846]    [Pg.1501]    [Pg.466]    [Pg.1110]    [Pg.141]    [Pg.200]    [Pg.2509]    [Pg.2350]    [Pg.121]    [Pg.125]    [Pg.472]    [Pg.1032]    [Pg.2350]    [Pg.415]    [Pg.443]    [Pg.97]    [Pg.1138]    [Pg.192]   
See also in sourсe #XX -- [ Pg.644 , Pg.645 ]




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