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Distribution statistical

There is no such thing as a pure polymer. All polymers comprise molecules that exhibit chemical and physical distributions of many variables these include molecular weight, branching, steric defects, molecular configuration, preferential chain orientation, and crystallite size and shape. The properties and characteristics that we exploit in polymers are controlled by the overall balance of these distributions. [Pg.13]

In addition to the statistical distributions inherent in an individual polymer, distributions are further broadened by the commercial practice of blending. We commonly blend two, three, four, or even more polymers of similar or dissimilar types in order to achieve the specific properties required. [Pg.13]

When a given measurement (length, temperature, velocity, etc.) is made several times, a number of different values may be obtained due to random errors of measurement. In general, the observed magnitudes will tend to cluster about a central value and be less numerous with displacement from this central value. When the frequency of occurrence (y) of a given observed value is plotted vs the value of the variable of interest (x), a bell shaped curve will often be obtained particularly when the number of determinations (N) is large. In statistical parlance, such curves are called distributions. [Pg.376]

The central value of a distribution may be expressed in several ways. The arithmetic mean (x) is the most widely used measure of central tendency. This is the sum of all of the individual values divided by the munber of values (N) and is expressed as follows  [Pg.376]

Sometimes some of the A values ofx involved in calculating the mean are more important than others. This is taken care of by determining a weighted mean value Equation (14.1) is then written as follows  [Pg.376]

The median is another way of expressing the central value of a distribution. This is the measurement for which equal munbers of measurements lie above and below the value. The mode is still another method of measuring central tendency. This is the most frequently observed value. For a distribution that is perfectly symmetrical, the arithmetic mean, Ihe median, and the mode are all equal. However, this will not be the case for distributions that are not S5mimetrical. [Pg.377]

The extent of a distribution is another characteristic that is of importance. This may be expressed as the spread which is the difference between the maximum and minimum values (x ,ax min)- extent may also be [Pg.377]


Case 1. The particles are statistically distributed around the ring. Then, the number of escaping particles will be proportional both to the time interval (opening time) dt and to the total number of particles in the container. The result is a first-order rate law. [Pg.767]

One may justify the differential equation (A3.4.371 and equation (A3.4.401 again by a probability argument. The number of reacting particles VAc oc dc is proportional to the frequency of encounters between two particles and to the time interval dt. Since not every encounter leads to reaction, an additional reaction probability has to be introduced. The frequency of encounters is obtained by the following simple argument. Assuming a statistical distribution of particles, the probability for a given particle to occupy a... [Pg.768]

Miller W H, Hernandez R, Moore C B and Polik W F A 1990 Transition state theory-based statistical distribution of unimolecular decay rates with application to unimolecular decomposition of formaldehyde J. Chem. Phys. 93 5657-66... [Pg.1043]

The two exponential tenns are complex conjugates of one another, so that all structure amplitudes must be real and their phases can therefore be only zero or n. (Nearly 40% of all known structures belong to monoclinic space group Pl c. The systematic absences of (OlcO) reflections when A is odd and of (liOl) reflections when / is odd identify this space group and show tiiat it is centrosyimnetric.) Even in the absence of a definitive set of systematic absences it is still possible to infer the (probable) presence of a centre of synnnetry. A J C Wilson [21] first observed that the probability distribution of the magnitudes of the structure amplitudes would be different if the amplitudes were constrained to be real from that if they could be complex. Wilson and co-workers established a procedure by which the frequencies of suitably scaled values of F could be compared with the tlieoretical distributions for centrosymmetric and noncentrosymmetric structures. (Note that Wilson named the statistical distributions centric and acentric. These were not intended to be synonyms for centrosyimnetric and noncentrosynnnetric, but they have come to be used that way.)... [Pg.1375]

When the rate measurement is statistically distributed about the mean, the distribution of events can be described by the Poisson distribution, Prrf O, given by... [Pg.1421]

Using this expression, the standard 5=1 equilibrium average properties may be calculated over a trajectory which samples the generalized statistical distribution for 5 7 1 with the advantage of enhanced sampling for g > 1. [Pg.202]

A comparison of Fig. 4 and Fig. 3 shows that this uncoupled QCMD bundle reproduces the disintegration of the full QD solution. However, there are minor quantitative differences of the statistical distribution. Fig. 5 depicts... [Pg.392]

It is important to realize that many important processes, such as retention times in a given chromatographic column, are not just a simple aspect of a molecule. These are actually statistical averages of all possible interactions of that molecule and another. These sorts of processes can only be modeled on a molecular level by obtaining many results and then using a statistical distribution of those results. In some cases, group additivities or QSPR methods may be substituted. [Pg.110]

The modeling of amorphous solids is a more dilhcult problem. This is because there is no rigorous way to determine the structure of an amorphous compound or even dehne when it has been found. There are algorithms for building up a structure that has various hybridizations and size rings according to some statistical distribution. Such calculations cannot be made more efficient by the use of symmetry. [Pg.319]

Boltzmann distribution statistical distribution of how many systems will be in various energy states when the system is at a given temperature Born-Oppenbeimer approximation assumption that the motion of electrons is independent of the motion of nuclei boson a fundamental particle with an integer spin... [Pg.361]

Fig. 25. Reverse osmosis, ultrafiltration, microfiltration, and conventional filtration are related processes differing principally in the average pore diameter of the membrane filter. Reverse osmosis membranes are so dense that discrete pores do not exist transport occurs via statistically distributed free volume areas. The relative size of different solutes removed by each class of membrane is illustrated in this schematic. Fig. 25. Reverse osmosis, ultrafiltration, microfiltration, and conventional filtration are related processes differing principally in the average pore diameter of the membrane filter. Reverse osmosis membranes are so dense that discrete pores do not exist transport occurs via statistically distributed free volume areas. The relative size of different solutes removed by each class of membrane is illustrated in this schematic.
If the initiation reaction is much faster than the propagation reaction, then all chains start to grow at the same time. Because there is no inherent termination step, the statistical distribution of chain lengths is very narrow. The average molecular weight is calculated from the mole ratio of monomer-to-initiator sites. Chain termination is usually accompHshed by adding proton donors, eg, water or alcohols, or electrophiles such as carbon dioxide. [Pg.517]

Gaussian Distribution The best-known statistical distribution is the normal, or Gaussian, whose equation is... [Pg.2085]

Unknown Statistical Distributions Sixth, despite these problems, it is necessaiy that these data be used to control the plant and develop models to improve the operation. Sophisticated numerical and statistical methods have been developed to account for random... [Pg.2550]

This is a formidable analysis problem. The number and impact of uncertainties makes normal pant-performance analysis difficult. Despite their limitations, however, the measurements must be used to understand the internal process. The measurements have hmited quahty, and they are sparse, suboptimal, and biased. The statistical distributions are unknown. Treatment methods may add bias to the conclusions. The result is the potential for many interpretations to describe the measurements equaUv well. [Pg.2562]

The more common approach is the actual positioning of random lines on a surface to create a statistical distribution of fragment sizes. One example of this, suggested by Mott and Linfoot (1943), is a construction of randomly positioned and oriented infinite lines as illustrated in Fig. 8.23. If the random lines are restricted to horizontal or vertical orientation an analytic solution can be obtained for the cumulative fragment number (Mott and Linfoot,... [Pg.302]

Statistical methods for probabilistic design 4.2.1 Modelling data using statistical distributions... [Pg.137]

Some important considerations in the use of statistical distributions have been highlighted, both in terms of the initial data and, more importantly, when modelling the stress and strength for determining the reliability. Stress-Strength Interference (SSI) analysis, which is the main technique used in this connection, will be discussed later. [Pg.140]

Bury, K. V. 1999 Statistical Distributions in Engineering. Cambridge Cambridge University Press. [Pg.383]

Weibull, W. 1951 A Statistical Distribution Function of Wide Applicability. Journal of Applied Mechanics, 73, 293-297. [Pg.393]

Another recent database, still in evolution, is the Linus Pauling File (covering both metals and other inorganics) and, like the Cambridge Crystallographic Database, it has a "smart software part which allows derivative information, such as the statistical distribution of structures between symmetry types, to be obtained. Such uses are described in an article about the file (Villars et al. 1998). The Linus Pauling File incorporates other data besides crystal structures, such as melting temperature, and this feature allows numerous correlations to be displayed. [Pg.495]

A microscopic description characterizes the structure of the pores. The objective of a pore-structure analysis is to provide a description that relates to the macroscopic or bulk flow properties. The major bulk properties that need to be correlated with pore description or characterization are the four basic parameters porosity, permeability, tortuosity and connectivity. In studying different samples of the same medium, it becomes apparent that the number of pore sizes, shapes, orientations and interconnections are enormous. Due to this complexity, pore-structure description is most often a statistical distribution of apparent pore sizes. This distribution is apparent because to convert measurements to pore sizes one must resort to models that provide average or model pore sizes. A common approach to defining a characteristic pore size distribution is to model the porous medium as a bundle of straight cylindrical or rectangular capillaries (refer to Figure 2). The diameters of the model capillaries are defined on the basis of a convenient distribution function. [Pg.65]

Weibull, W. A Statistical Distribution Function of Wide Application. 7. Appl. Mech., Vol. 18, 1951, pp. 293. [Pg.237]


See other pages where Distribution statistical is mentioned: [Pg.165]    [Pg.1421]    [Pg.2132]    [Pg.2803]    [Pg.2993]    [Pg.197]    [Pg.202]    [Pg.204]    [Pg.62]    [Pg.225]    [Pg.483]    [Pg.502]    [Pg.824]    [Pg.2085]    [Pg.2547]    [Pg.2578]    [Pg.295]    [Pg.97]    [Pg.490]    [Pg.244]    [Pg.315]    [Pg.360]    [Pg.147]    [Pg.194]    [Pg.129]   
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See also in sourсe #XX -- [ Pg.218 , Pg.289 ]

See also in sourсe #XX -- [ Pg.4 , Pg.83 , Pg.282 ]




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Basic Statistics Summary for Normal Distribution

Bell-shaped distribution, statistics

Boltzmann distribution Statistical mechanics

Common Statistical Distributions

Conformational distributions statistical properties

Descriptive statistics distribution)

Descriptive statistics skewness, distribution

Distribution functions statistics

Distribution statistics

Distribution statistics

Distribution, sampling (statistical

Distribution, statistical Statistics

Distribution-free statistics

Engineering statistics probability distributions

Equilibrium Statistical Distribution of Diatomic Molecules over Vibrational-Rotational States

Frequency distribution, statistical

Geochemical data statistical distribution

Gumbel statistics/distribution

Material state statistical distribution functions

Maxwell-Boltzmann distribution statistics

Non-statistical distribution

Particle size, statistics Gaussian distribution

Particle size, statistics cumulative distribution

Particle size, statistics distribution, characterization

Poisson distribution/statistics

Polymer molecular weight distribution statistics

Properties of distribution in SAW statistics

Quantum statistical mechanics probability distribution

Relating Current and Future Air Pollutant Statistical Distributions

Sequence distribution statistics

Some Statistical Distributions of Interest

Spectral function statistical distributions

Statistical Distributions Boltzmann Distribution Function

Statistical Moments of the Particle Radius Distribution

Statistical Representation of Molecular States and Boltzmann Distribution

Statistical analysis of copolymer sequence distribution

Statistical distribution directions

Statistical distribution functions

Statistical distribution laws

Statistical distribution of the contour length

Statistical distribution over vibrational-rotational

Statistical distribution over vibrational-rotational states

Statistical distributions Binomial distribution

Statistical distributions Gaussian distribution

Statistical distributions Lorentzian distribution

Statistical distributions Normal distribution

Statistical distributions Poisson distribution

Statistical distributions Porter-Thomas

Statistical distributions continuous

Statistical distributions maximum likelihood

Statistical distributions neutron widths

Statistical distributions parameters

Statistical distributions plotting positions

Statistical mechanics Maxwell velocity distribution

Statistical mechanics and distribution functions

Statistical mechanics radial distribution function

Statistical methods probability distribution

Statistical normal distribution

Statistical thermodynamics Boltzmann energy distribution

Statistical thermodynamics Maxwell-Boltzmann distribution

Statistically generated distribution

Statistics Gaussian distribution

Statistics bimodal distribution

Statistics distribution types

Statistics frequency distributions

Statistics negatively skewed distribution

Statistics normal distribution

Statistics parametric distributions

Statistics positively skewed distribution

Statistics skewed distribution

Statistics standard normal distribution

Statistics test distribution

Weibull Statistical Distribution

Weibull statistics/distribution

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