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Triangle function

Fourier transforms boxcar function 274 Cauchy function 276 convolution 272-273 Dirac delta function 277-279 Gaussian function 275-276 Lorentzian function 276-277 shah function 277-279 triangle function 275 fraction, rational algebraic 47 foil width at half maximum (FWHM) 55, 303... [Pg.205]

If we convolve two single-peaked functions, the result is smoother than either component. Two rectangle functions convolved yield a triangle two triangle functions convolved (four rectangles convolved) produce a result that is astonishingly close to a gaussian (Fig. 1). [Pg.8]

Avd Avn Avp c A AW Doppler half-width in hertz natural half-width l/47cyN pressure-broadened half-width 1 /4nyP variable of integration wavelength of radiant flux triangle function of unit height and half-width % scaled ratio (AvN -1- Avc) /ln 2/AvD... [Pg.37]

To eliminate this ringing", apodisation functions are used. The most commonly used is the triangle function which reduces the ringing effect but also the spectral resolution (Fig. I2.8C). [Pg.223]

The most common apodization functions are those proposed by Norton and Beer (1976) and the triangle function (Griffiths and de Haseth 2(X)7). Norton and Beer tested over 1000 functions of the general form... [Pg.25]

Figure 3.5. (a) Discretely sampled sinc function b) its Fourier transform, a series of triangle functions. [Pg.61]

Figure 4. Conical parameters on the relativistic seam, (a) g (open circles), (open squares), h (open triangles). The nonrelativistic quantities, g (filled circle) and h(nr) (filled square) (b) s, w = X (circles), y (squares), z (triangles). Filled (open) markers from nonrelativistic (reladvistic) calculations, (c) Magnitude of the invariant / = g x h as a function of... Figure 4. Conical parameters on the relativistic seam, (a) g (open circles), (open squares), h (open triangles). The nonrelativistic quantities, g (filled circle) and h(nr) (filled square) (b) s, w = X (circles), y (squares), z (triangles). Filled (open) markers from nonrelativistic (reladvistic) calculations, (c) Magnitude of the invariant / = g x h as a function of...
Fig. 5.5 The first few steps of the simplex algorithm with the function + 2i/. The initial simplex corresponds to the triangle 123. Point 2 has the largest value of the function and the next simplex is the triangle 134. The simplex for tire third step is 145. Fig. 5.5 The first few steps of the simplex algorithm with the function + 2i/. The initial simplex corresponds to the triangle 123. Point 2 has the largest value of the function and the next simplex is the triangle 134. The simplex for tire third step is 145.
It can be readily shown that L,J 1,3 satisfy the requirements for shape functions (as stated in Equation 2.3) associated with the triangoilar element. The area of a triangle in tenns of the Cartesian coordinates of its vertices is written as... [Pg.31]

Attach the flask containing the mixture, with capillary in position, to the column make sure that the Perkin triangle (or vacuum distilling adapter ) and receiver are in place. See that the oil pump is functioning... [Pg.100]

The trigonometric functions of angles are the ratios between the various sides of the reference triangles shown in Fig. 3-39 for the various quadrants. Clearly r = /x + y > 0. The fundamental functions (see Figs. 3-40, 3-41, 3-42) are... [Pg.438]

FIG. 3-53 Trial functions for Galerldn finite element method linear polynomial on triangle. [Pg.481]

Step 3 Drawing a Functional GO Chart - The system is represented by the interconnected GO symbols. Independent components are represented by triangle symbols and dependent components are represented by circles. [Pg.122]

FIG. 11 Adsorbed amount as a function of bulk concentration for a non-interacting (empty symbols) and adsorbing (full symbols) wall. Diamonds and triangles correspond to a system with semi-rigid chains, circles and squares for flexible chains [28]. [Pg.533]

Figure 1. The energy of bcc and hep randoiri alloys and the ])ai tially ordered a phase relative to the energy of the fee phase (a), of the Fe-Co alloy as a function of Co concentration. The corresponding mean magnetic moments are shown in (h). The ASA-LSDA-CPA results are shown as a dashed line for the o ])hase, as a full line for the her ]>hase, as a dot-dashed line for the hep phase, and as a dotted line for the fee phase. The FP-GGA results for pure Fe and Co are shown in (a) by the filled circles (bcc-fcc) and triangles (hep-fee). In (b) experimental mean magnetic moments are shown as open circles (bcc), open scpiares (fee) and open triangles (hep). Figure 1. The energy of bcc and hep randoiri alloys and the ])ai tially ordered a phase relative to the energy of the fee phase (a), of the Fe-Co alloy as a function of Co concentration. The corresponding mean magnetic moments are shown in (h). The ASA-LSDA-CPA results are shown as a dashed line for the o ])hase, as a full line for the her ]>hase, as a dot-dashed line for the hep phase, and as a dotted line for the fee phase. The FP-GGA results for pure Fe and Co are shown in (a) by the filled circles (bcc-fcc) and triangles (hep-fee). In (b) experimental mean magnetic moments are shown as open circles (bcc), open scpiares (fee) and open triangles (hep).
Figure 2. Total energies of ordered (LIq structure, squares), random (circles) and segregated (triangles) fee RhsoPdso alloys as a function of the number of neighboring shells included in the local interaction zone. Values obtained by the LSGF-CPA method are shown by filled symbols and full lines. The energies obtained by the reference calculations are shown by a dashed line (LMTO, ordered sample), a dotted line (LMTO-CPA, random sample), and a dot-dashed line (interface Green s function technique, segregated sample). Figure 2. Total energies of ordered (LIq structure, squares), random (circles) and segregated (triangles) fee RhsoPdso alloys as a function of the number of neighboring shells included in the local interaction zone. Values obtained by the LSGF-CPA method are shown by filled symbols and full lines. The energies obtained by the reference calculations are shown by a dashed line (LMTO, ordered sample), a dotted line (LMTO-CPA, random sample), and a dot-dashed line (interface Green s function technique, segregated sample).
Here, we address the more general question of the relative stability of monomers, dimers and triangular trimers on the (111) surface of FCC transition metals of the same chemical species as a function of the d band filling Nd. All possible atomic configurations of the systems are considered monomers and dimers at sites N and F, triangles with A and B borders at sites N and F (Fig. 4). The d band-filling includes the range of stability of the FCC phase (Nd > 7.5e /atom). The densities of states are obtained from... [Pg.378]


See other pages where Triangle function is mentioned: [Pg.209]    [Pg.353]    [Pg.353]    [Pg.2]    [Pg.306]    [Pg.307]    [Pg.222]    [Pg.1540]    [Pg.26]    [Pg.356]    [Pg.52]    [Pg.209]    [Pg.353]    [Pg.353]    [Pg.2]    [Pg.306]    [Pg.307]    [Pg.222]    [Pg.1540]    [Pg.26]    [Pg.356]    [Pg.52]    [Pg.267]    [Pg.668]    [Pg.2647]    [Pg.277]    [Pg.278]    [Pg.457]    [Pg.32]    [Pg.24]    [Pg.28]    [Pg.32]    [Pg.119]    [Pg.423]    [Pg.480]    [Pg.481]    [Pg.44]    [Pg.79]    [Pg.292]    [Pg.185]    [Pg.430]    [Pg.702]    [Pg.14]   
See also in sourсe #XX -- [ Pg.8 , Pg.13 ]




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