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Porod plot

The specific surface area determined from the Porod plot is approximately 10 m /g. This is a very low value and can be attributed to the absence of the Porod limit. [Pg.105]

The relative isotropic scattering intensity /(/ ), (h=4n/ -sm 0), 20=scattering angle, A=0.154 nm) was recorded by use of a Kratky plant. From the tightly packed arrangement of pores and walls the Porod plot of the scattering curve, see Fig. 3, results. Furthermore, for the isotropic two-phase material, for a fixed range order (here L=30 nm), y r) follows via Eq. (1). [Pg.596]

The NA measurement yields a mean chord length of the pores 7=10.8 nm, via Eqs. (2). By use of this value, it follows a normalized Porod plot, defined by... [Pg.596]

Figure 3 Normalized Porod plot P (h) of the scattering intensity 1(h). The resolution limit in real space is marked in the subfigure. Figure 3 Normalized Porod plot P (h) of the scattering intensity 1(h). The resolution limit in real space is marked in the subfigure.
Fig. 18. Porod plot Is versus s of the equatorial SAXS curve of crazes II in polycarbonate... Fig. 18. Porod plot Is versus s of the equatorial SAXS curve of crazes II in polycarbonate...
Rgure 1.11 Porod plots of scattering data of silicates polymerized under a variety of conditions (from a study by Schaefer and Keefer ) (a) two-step acid-catalyzed tetraethoxysilane (TEOS) system (b) two-step acid-and base-catalyzed TEOS system (c) one-step base-catalyzed system TEOS system (W = 1) (d) one-step base-catalyzed system TEOS system (VP = 2) (e) aqueous silicate system. LUDOX . VP is the water/ silica ratio. [Pg.16]

The behavior of I q) at high q is often analyzed using a Porod plot versus q ). [Pg.850]

From equation (8-11), I q)q is expected to become asymptotically constant in the high q limit. Porod plot is used in order to determine (i) the asymptotic value of I q)q and, from it, the interface surface area, S (ii) eventual positive or negative deviations from Porod s law. For example, statistical density fluctuations in the phases produce an additional and constant scattering intensity and thus a deviation of Porod s law, evidenced by a positive slope ofthe linear part ofPorod s plots. On the other hand, a smooth (not sharp) transition in the electron density between the two phases leads to a negative slope (Ruland, 1971). [Pg.850]

A) Slit-smeared Porod plot for spinnable silicate precursor (W2) measured by SAXS. K=iniX(sm0/2). (B) Corresponding SiNMR spectrum. From Drinker and Assink [32]. [Pg.410]

SAXS Porod plots of porous silicates. (A) Aerogel prepared from a particulate precursor, p uik 0.09g/cm . (B) Aerogel prepared from a particulate precursor, Pbuik = 0.21 g/gm. (C) Xerogel prepared from a single-step based-catalyzed hydrolysis of TEOS (r = 2) followed by drying at room temperature [18). [Pg.736]

SANS Porod plot of silica aerogels prepared by single-step hydrolyses of TMOS (r = 4) under neutral (N) or basic ((B) 5 x 10 M NH4OH) conditions followed by supercritical extraction of methanol. Numbers in parentheses are the corresponding bulk densities. The oxidation (heat) treatment for the 0.36-g/cm sample was performed at 500°C 126). [Pg.737]

A) Porod plot for the two-step acid-catalyzed silicate precursor (W1). K is the scattering vector4n/ (sinfl/2). From Schaefer and Keefer [29], (B) Corresponding Si NMR spectrum. From Assink [31]. [Pg.870]

Porod plot of film prepared from monosized particulate silicate precursors (-lO-nm diameters). From Drinker et al. [20]. [Pg.876]

Figure 2. SAXS patterns of PET at 200°C. Hieline (—)istheraw/f9Jversus9 data and has a wetdk peak at qmax tutd a strong optum at low q. The effects of diffuse scattering from the thermal background at high q ate obvious in the uncorrected data, (o) I(q)gp versus q, and their corrected values, ( ) (I(q)-h) versus q. The inset is ite Porod plot used to calculate die thermal backhand fiom the slope of the linear portion in versus... Figure 2. SAXS patterns of PET at 200°C. Hieline (—)istheraw/f9Jversus9 data and has a wetdk peak at qmax tutd a strong optum at low q. The effects of diffuse scattering from the thermal background at high q ate obvious in the uncorrected data, (o) I(q)gp versus q, and their corrected values, ( ) (I(q)-h) versus q. The inset is ite Porod plot used to calculate die thermal backhand fiom the slope of the linear portion in versus...
The quantity/], arises from density fluctuations and Kp is the Porod constant Note the strong positive deviation in the Porod plot (f(q)q versus q ) illustrated as an inset to Figure 2. Positive deviations from Porod s law are caused by thermal density fluctuations [6]. A regression analysis of tiie linear part of the curve gives values of = 0.0S and = 356. A most be subtracted from the raw intensity data before both dj and the invariant are calculated. [Pg.167]

As a result, a plot of the type log ql(q) versus (f-, often designated as a Porod plot, allows determination of r. ... [Pg.58]

Fig. 6.7 Porod plot showing different power-law decays that are common in SAXS interface with a well-defined electron density gradient blue curve), Porod surface scattering red), internal electron density fluctuations black), surface fractal green), Gaussian coil purple), and mass fractal agglomerate orange)... Fig. 6.7 Porod plot showing different power-law decays that are common in SAXS interface with a well-defined electron density gradient blue curve), Porod surface scattering red), internal electron density fluctuations black), surface fractal green), Gaussian coil purple), and mass fractal agglomerate orange)...

See other pages where Porod plot is mentioned: [Pg.265]    [Pg.660]    [Pg.90]    [Pg.362]    [Pg.162]    [Pg.162]    [Pg.622]    [Pg.343]    [Pg.177]    [Pg.177]    [Pg.409]    [Pg.412]    [Pg.457]    [Pg.736]    [Pg.872]    [Pg.873]    [Pg.873]    [Pg.62]    [Pg.110]   
See also in sourсe #XX -- [ Pg.58 , Pg.62 ]




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