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Sampling effects

If errors in both the 100% and 0% lines are commonplace in FT-IR spectrometers, it is reasonable for users of these instruments to question the photometric accuracy between these extreme values. Fortunately, the situation here appears not to give cause for concern. Richardson et al. [18] have shown that the transmittance scale appears to be linear after correction for errors in the 0% line. [Pg.194]

Most of the errors discussed in this chapter are relatively small. Provided that mid-infrared spectra are measured with an instrument that is equipped with a DTGS or DLATGS detector and care is taken to ensure that the peak absorbance of bands in the spectral region of interest is not excessive, the photometric accuracy of contemporary FT-IR spectrometers is remarkably high. The transmittance scale of these instruments should be accurate to better than 0.001 ( 0.1 %T). [Pg.194]

Standard Practice for Describing and Measuring Performance of Fourier Tranrform Infrared (FT-IR) Spectrometers Level Zero and Level One Tests, ASTM E 1421-91, American Society for Testing and Materials, Philadelphia, PA, 1991. [Pg.195]

Keens and A. Simon, Correction of the non-linear response of infrared detectors, in Proceedings of the 9th International Conference on Fourier Tranrform Spectroscopy, J. E. Bertie and H. Wieser, Eds., Society of Photo-Optical Instrumentation Engineers, Bellingham, WA, 1993, Vol. 2089, p. 222. [Pg.195]

Keens and A. Simon, Correction of non-linearities in detectors in Fourier transform spectroscopy, U.S. patent 4,927,269 (assigned to Bruker Spectrospin Ltd., Milton, Ontario, Canada, May 22, 1990). [Pg.195]


The gas temperature of the Ar plasma in the range of 600 100 K effects temperatures of water or LN2 cooled samples of 350 30 or 200 30 K, respectively. In addition, C, N, and O species are desorbed from the chamber walls and introduced samples, effecting a plasma contamination level in the 0.01-0.1% range. [Pg.126]

The position of the peak (Figure 16) is of critical importance in distinguishing a composition based separation. The large axial dispersion in GPC 1 was attributed to the sample loadings being more than the 9 silica filled columns could handle. This had potentially serious consequences in terms of chromatogram sampling effects. [Pg.177]

Another sampling effect which deserves mention is that since the molecular weight distribution shifl towards higher molecular weights with conversion, a slice will not in general contain proportionate amounts of polymer from all conversions. This dufting can be accounted for in the theoretical predictions by incorporating it into cumulation of the instantaneous property distributions (e.g. Equation 8). [Pg.177]

Several peaks of interest (ideally higher order reflections of the same type hkl, 2h, 2k, 21, 3h, 3k, 31,. .., nh, nk, nl) are fitted by Fourier series the same procedure is applied to the diffraction lines of a reference sample, in which size and strain effects are negligible, in order to determine the instrumental line broadening. Such information is used in order to deconvolute instrumental broadening from sample effects (Stokes-Fourier deconvolution [36]). [Pg.133]

Ogundele, M.O., Cytotoxicity of EDTA used in biological samples Effect on some human breast-milk studies, J Appl Toxicol, 19 (6), 395-400, 1999. [Pg.428]

The results of the experiments are evaluated by means of three-way ANOVA in its simplest form, m = n = p and q = 1. The significance of the sample effect can principally be guaranteed also in the case that both testers and days have significant influence (Sharaf et al. [1986]). [Pg.134]

This section is used to introduce the momentum-enhanced hybrid Monte Carlo (MEHMC) method that in principle converges to the canonical distribution. This ad hoc method uses averaged momenta to bias the initial choice of momenta at each step in a hybrid Monte Carlo (HMC) procedure. Because these average momenta are associated with essential degrees of freedom, conformation space is sampled effectively. The relationship of the method to other enhanced sampling algorithms is discussed. [Pg.293]

Sample Effects The recovery of an analyte from a complex matrix may be affected by other components of the matrix. The homogeneity of the sample will also influence the results. This is related to the issue of sampling mentioned above. Physical or chemical form can lead to incomplete recovery of the analyte. For example, an element may exist in more than one oxidation state in a sample and hence be incompletely determined by a method that requires it to be in one particular state only (speciation). The sample and/or analyte may be unstable, causing a change in the composition of the sample during the course of the analysis. [Pg.164]

R.L. Green, G. Thurau, N.C. Pixley, A. Mateos, R.A. Reed and J.P. Higgins, In-line monitoring of moisture content in fluid bed dryers using near-IR spectroscopy with consideration of sampling effects on method accuracy. Anal. Chem., 77(40), 4515 522 (2005). [Pg.458]

Acute static bioassays are employed to evaluate sample effects on fish and microinvertebrates. Fathead minnows and Daphnia pulex are the freshwater species employed, while sheepshead minnows and grass shrimp are used for marine assays. In all cases, the test organisms are exposed for 96 hours to prescribed concentrations of the sample introduced into holding tanks maintained at the same environmental conditions as a control population. [Pg.42]

Qualitative and visual analyses of overall sampling effectiveness... [Pg.37]

These properties carry back to the discrete formulation. We shall use both discrete and continuous formulations in this volume, changing back and forth as needs require. The continuous regime allows us to avoid consideration of sampling effects when such consideration is not of immediate concern. Deconvolution algorithms, on the other hand, are numerically implemented on sampled data, and we find the discrete representation indispensable in such cases. [Pg.7]

By applying the convolution theorem, we see that replication in the x domain has produced a sampling effect in the frequency domain. The wider the replication interval, the finer is the frequency sampling. Sampling in the x domain, on the other hand, appears in Fourier space as replication. Fine sampling in x produces wide spacing between cycles in co. The area under each scaled Dirac function of co may be taken as the numerical value of a sample. [Pg.24]

It is difficult to specify accuracy in this experiment. One reason is that there may be sampling effects, i.e., wide variability in the samples used. Consequently, the sample should be homogeneous and representative. There is a strong dependence of the modulus and damping behavior on molecular and structural parameters. Entrapped air/gas may affect the results obtained using powder or pellet samples. [Pg.203]

For far-UV spectra, it is usual to scan between 250 nm—where the ellipticities of the baseline and sample effectively coincide, given the scale of ellipticity being used—and as near to 180 nm as the absorbance of the solution will permit. The lower limit may be dictated by the absorbance of the sample or buffer, as indicated by the value of the dynode voltage (see step 2e). [Pg.231]

Jean-Louis G, Kripke DF, Ancoli-Israel S, Klauber MR, Sepulveda RS. Sleep duration, illumination, and activity patterns in a population sample effects of gender and ethnicity. Biol Psychiatry 2000 47 921-927. [Pg.208]

Another example often quoted is that there is no sample effect when measuring the length of a table. First, this is an incomplete definition of a measurand, since it is not clear what is meant by the length. But if, for example, the table forms a part of a measuring system to measure the precise shape of objects then the shape of the table can have an influence on the result. Then such factors as the material of the table, its temperature coefficient, the temperature gradients across the table, the loading of the table, the friction between its feet and the floor are sample effects that need to be taken into account. [Pg.71]

It could be claimed that these are examples of sample effects on precise measurements that do not have their equivalents in chemical measurements, but they were introduced to show the universality of sample effects. [Pg.71]

Just in case some are not convinced that sample effects in physical measurements can be as great in chemical ones, as a further example consider the measurement of absorbed neutron dose in a patient undergoing radiation therapy. [Pg.71]

The differences between physical and chemical measurements should not be over emphasised. Many of the basic problems are very similar, e.g. sample effects are important in all types of measurement. Also similar error structures occur in both types of measurements and not... [Pg.72]


See other pages where Sampling effects is mentioned: [Pg.102]    [Pg.27]    [Pg.177]    [Pg.177]    [Pg.30]    [Pg.132]    [Pg.107]    [Pg.19]    [Pg.22]    [Pg.379]    [Pg.644]    [Pg.55]    [Pg.72]    [Pg.449]    [Pg.130]    [Pg.1]    [Pg.232]    [Pg.753]    [Pg.735]    [Pg.647]    [Pg.36]    [Pg.112]    [Pg.113]    [Pg.307]    [Pg.239]    [Pg.48]    [Pg.70]    [Pg.71]    [Pg.71]   
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Anisokinetic sampling, effect

Biological effects samples

Cost-effective sample size

Cost-effective sample size model

Effect of Sample Concentration on Response

Effect of Sample Treatment

Effect of Sampling

Effect of sample concentration

Effect of sample thickness

Effect of sample thickness (gap)

Effect of the sampling matrix

Effect on Sco when Diluting a Blood Sample Containing HbCO and HbO

Effective frozen samples

Effective sample length

Effective sample size

Effects involved in ultrasound-assisted sample digestion

Effects of Phase Separation, Sample Preparation, Grain Size

Effects of Sample Geometry

Effects of Sample Pretreatment on Calculations

Effects of Sample Tumbling and Rotation

Effects of sample collection

Effects of sample preparation on powder diffraction data

Effects of separating sample from the living system

Fracture toughness sample thickness effect

Matrix Effects and Sample Preparation

Measurement of sample properties without unwanted annealing effects

Measurements without Sample Inertia Effects

Miscellaneous sample effects

Oscillatory) Measurements without Sample Inertia Effects (Gap Loading)

Peak area sample mass effects

Photoacoustic spectroscopy effective sampling depth

Retention times internal standards, sample matrix effect

Reversed-phase HPLC sample concentration effects

Sample Effects

Sample Effects

Sample Problems on Mean Stress Effect and Fatigue Strength Diagrams

Sample application solvent effects

Sample handling matrix effects

Sample harmful effects

Sample heating effects

Sample matrix effects

Sample purity effects

Sample size effects, degrees

Sample size, effects

Sample size, effects independent samples

Sample solution effects

Sample solvent, effect

Sample tumbling effects

Sample volume, effect on dispersion equation for

Sample, load, effect

Sample, load, effect precision

Sample, load, effect volume, maximum

Sample-injection effects

Sampling efficiency, effect

Sampling rate effect

The Effect of Sample Volume

Tip-sample interaction effects

Treatment effects/differences sample size

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