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Multiplier

For such components, as the composition of the solution approaches that of the pure liquid, the fugacity becomes equal to the mole fraction multiplied by the standard-state fugacity. In this case,the standard-state fugacity for component i is the fugacity of pure liquid i at system temperature T. In many cases all the components in a liquid mixture are condensable and Equation (13) is therefore used for all components in this case, since all components are treated alike, the normalization of activity coefficients is said to follow the symmetric convention. ... [Pg.18]

According to Equation (14), the fugacity of component i becomes equal to the mole fraction multiplied by the standard-... [Pg.18]

The total enthalpy correction due to chemical reactions is the sum of all the enthalpies of dimerization for each i-j pair multiplied by the mole fraction of dimer i-j. Since this gives the enthalpy correction for one mole of true species, we multiply this quantity by the ratio of the true number of moles to the stoichiometric number of moles. This gives... [Pg.136]

Multiplying both sides of this equation by (1 + i) gives... [Pg.420]

See chemical equivalent, equivalent conductivity The specific conductance multiplied by the volume (ml) which contains 1 g equivalent of the electrolyte. [Pg.161]

Fuller s equation, applied for the estimation of the coefficient of diffusion of a binary gas mixture, at a pressure greater than 10 bar, predicts values that are too high. As a first approximation, the value of the coefficient of diffusion can be corrected by multiplying it by the compressibility of the gas /... [Pg.147]

The values of common hydrocarbon solubility parameters vary between 300 and 600 (kJ/m3) /2 Several tables are available where the solubility parameters are shown as (cal/cm ) / Jq convert these values, it is necessary to multiply by 64.69. Thus a solubility parameter value of 10 (cal/cm ) / jg equal to 646.9 (kJ/m ) / ... [Pg.154]

Cases 3 and 4 are both exploration prospects, since the volumes of potential oil present are multiplied by a chance factor which represents the probability of there being oil there at all. For example, case 3 has an estimated probability of oil present of 65%, i.e. low risk of failure fo find oil (35%). However, even if there is oil present, the volume is small no greater than 130 MMstb. This would be a low risk, low reward prospect. [Pg.162]

When an explorationist constructs an expectation curve, the above approach for the volumetries of an accumulation is taken, but one important additional parameter must be taken into account the probability of there being hydrocarbons present at all. This probability is termed the Probability of Success" (POS), and is estimated by multiplying together the probability of there being ... [Pg.164]

The estimated probabilities of each of these events occurring are multiplied together to estimate the POS, since they must a//occur simultaneously if a hydrocarbon accumulation is to be formed. If the POS is estimated at say 30%, then the probability of failure must be 70%, and the expectation curve for an exploration prospect may look as shown in figure 6.9. [Pg.164]

This is the method used by the commercial software packages Crystal Ball and RISK . The method is ideally suited to computers as the description of the method will reveal. Suppose we are trying to combine two independent variables, say gross reservoir thickness and net-to-gross ratio (the ratio of the net sand thickness to the gross thickness of the reservoir section) which need to be multiplied to produce a net sand thickness. We have described the two variables as follows ... [Pg.166]

A random number (between 0 and 1) is picked, and the associated value of gross reservoir thickness (T) is read from within the range described by the above distribution. The value of T close to the mean will be randomly sampled more frequently than those values away from the mean. The same process is repeated (using a different random number) for the net-to-gross ratio (N/G). The two values are multiplied to obtain one value of net sand thickness. This is repeated some 1,000-10,000 times, with each outcome being equally likely. The outcomes are used to generate a distribution of values of net sand thickness. This can be performed simultaneously for more than two variables. [Pg.166]

The method allows variables to be added or multiplied using basic statistical rules, and can be applied to dependent as well as independent variables. If input distributions can be represented by a mean, and standard deviation then the following rules are applicable for independent variables ... [Pg.168]

To estimate the product of the two variables below, a short cut method is to multiply the low, medium and high values in a matrix (in which numbers have been selected). [Pg.171]

The volume fraction would typically be used to represent the make up of a gas at a particular stage in a process line and describes gas composition e.g. 70% methane and 30% Ethane (also known as mol fractions) at a particular temperature and pressure. Gas composition may also be expressed in mass terms by multiplying the fractions by the corresponding molecular weight. [Pg.242]

The actual flowrate of each component of the gas (in for example cubic mefres), would be determined by multiplying the volume fraction of that component by the total flowrate. [Pg.242]

For the case of a double-D coil we multiply each matrix element with an element shifted by a constant distance of the same line. This is done in x- and y-direction. The distance between the two elements is the correlation length X for filtering in x-direction and a second correlation length for the movement in y-direction. Thus one gets two new matrices Ax and Ax for the filtering from the left to the right (positiv x-direction) and vice versa (negativ x-direction). [Pg.261]

To demodulate the signal, it is then necessary to multiply the carrier by itself. Of eourse, the carrier of the driver must be exactly the same as the demodulator one. But, as it is modified to be demodulated, we nevertheless need a common frequency reference for the driver and for the DSP. This reference is delivered by a quartz oscillator. [Pg.281]

The demodulation algorithm is very simple the DSP multiplies the received signal by each carrier, and then filters the result using a FIR filter. This kind of digital filter is phase linear, (constant group delay important for the EC combinations). Other filters may be programmed, other demodulation algorithms may be used. [Pg.281]

The resistance R is given by the relation. Here, the second term with the amplitude of very little flux in the tube cannot be neglected because it is multiplied by the pulsation (n=27tf. [Pg.353]

Use now this equation to describe liquid film flow in conical capillary. Let us pass to spherical coordinate system with the origin coinciding with conical channel s top (fig. 3). It means that instead of longitudinal coordinate z we shall use radial one r. Using (6) we can derive the total flow rate Q, multiplying specific flow rate by the length of cross section ... [Pg.617]

In general a thickness measurement using ultrasound is done by measuring the time of flight of the ultrasonic pulse and calculating the thickness of the objeet multiplying the time and the known constant sound velocity in the material. [Pg.762]

Figure 3 Feature relevance. The weight parameters for every component in the input vector multiplied with the standard deviation for that component are plotted. This is a measure of the significance of this feature (in this case, the logarithm of the power in a small frequency region.)... Figure 3 Feature relevance. The weight parameters for every component in the input vector multiplied with the standard deviation for that component are plotted. This is a measure of the significance of this feature (in this case, the logarithm of the power in a small frequency region.)...
This is exact—see Problem 11-8. Notice that Eq. 11-14 is exactly what one would write, assuming the meniscus to be hanging from the wall of the capillary and its weight to be supported by the vertical component of the surface tension, 7 cos 6, multiplied by the circumference of the capillary cross section, 2ar. Thus, once again, the mathematical identity of the concepts of surface tension and surface free energy is observed. [Pg.13]

A method that has been rather widely used involves the determination of the force to detach a ring or loop of wire from the surface of a liquid. It is generally attributed to du Noiiy [42]. As with all detachment methods, one supposes that a first approximation to the detachment force is given by the surface tension multiplied by the periphery of the surface detached. Thus, for a ring, as illustrated in Fig. II-ll,... [Pg.21]

Fig. IV-25. The evaporation resistance multiplied by the square root of temperature versus area per molecule for monolayers of octadecanol on water illustrating agreement with the accessible area model. (From Ref. 290.)... Fig. IV-25. The evaporation resistance multiplied by the square root of temperature versus area per molecule for monolayers of octadecanol on water illustrating agreement with the accessible area model. (From Ref. 290.)...
Returning to the complete calculation, is then given by u multiplied by the number of atoms per unit area in the particular crystal plane. [Pg.266]

The last identity follows from the orthogonality property of eigenfunctions and the assumption of nomralization. The right-hand side in the final result is simply equal to the sum over all eigenvalues of the operator (possible results of the measurement) multiplied by the respective probabilities. Hence, an important corollary to the fiftli postulate is established ... [Pg.11]

If the structure factor vanishes, the corresponding fonn factor is irrelevant as it is multiplied by a zero... [Pg.110]


See other pages where Multiplier is mentioned: [Pg.304]    [Pg.314]    [Pg.14]    [Pg.263]    [Pg.359]    [Pg.65]    [Pg.184]    [Pg.378]    [Pg.444]    [Pg.591]    [Pg.738]    [Pg.891]    [Pg.124]    [Pg.201]    [Pg.553]    [Pg.607]    [Pg.610]    [Pg.622]    [Pg.11]    [Pg.13]    [Pg.33]    [Pg.39]   
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See also in sourсe #XX -- [ Pg.49 , Pg.51 , Pg.52 , Pg.53 , Pg.54 , Pg.55 , Pg.60 , Pg.63 , Pg.65 , Pg.67 , Pg.69 , Pg.70 , Pg.77 , Pg.78 , Pg.81 , Pg.84 , Pg.89 ]

See also in sourсe #XX -- [ Pg.28 , Pg.319 , Pg.360 ]

See also in sourсe #XX -- [ Pg.182 ]

See also in sourсe #XX -- [ Pg.182 ]

See also in sourсe #XX -- [ Pg.281 ]

See also in sourсe #XX -- [ Pg.224 ]

See also in sourсe #XX -- [ Pg.112 , Pg.115 , Pg.125 , Pg.127 , Pg.204 , Pg.219 , Pg.261 , Pg.414 , Pg.476 ]




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Active film multipliers

Affixes, multiplying

Align sequences, multiplying

Analog multiplier signal processing

Application of One-velocity Model to Multiplying Media

Array, Multichannel Electron Multiplier

Array, electron multiplier

BOOTH multiplier

Bifurcation of periodic orbits with multiplier

Capacitor frequency multiplier

Changing the multiplying constant

Channel electron multiplier

Channel electron multiplier arrays

Channel electron multiplier arrays CEMA)

Channel electron multipliers (CEM

Channel plate electron multiplier

Channel plate electron multiplier detector

Channeltron electron multiplier

Channeltron multiplier, mass spectrometry

Characteristic multipliers

Charge transfer in neutral atom-multiply charged ion collisions

Charge transfer multiply charged ions

Coefficient multiplying

Collectors electron multiplier

Complex-conjugate multipliers

Complexes not containing multiply bonded

Complexes not containing multiply bonded ligands

Constrained optimization Lagrange multiplier method

Constraint Lagrange multipliers

Continuous-dynode electron multiplier

Costs of equipment installed cost multipliers

Countercurrent multiplier system

Daly-Multiplier

Dealing with Multiply Charged Ions

Detector secondary electron multiplier

Detectors channel electron multiplier

Detectors electron multipliers

Diameters, 146 Electron multipliers)

Discrete dynode multiplier

Discrete dynode secondary electron multipliers

Discrete-dynode electron multiplier

Distillation multipliers

Distribution multiply labeled

Dynode Electron Multiplier

Dynode multipliers

EMIT (enzyme-multiplied immunoassay

Effective charge weight multiplier

Electrochemistry and electric field as origins of multiply charged ions

Electron multiplier

Electron multiplier analogue

Electron multiplier dead time

Electron multiplier dual mode

Electron multiplier noise

Electron multiplier operating principles

Electron multiplier pulse counting

Electron multipliers with continuous dynodes

Electron multipliers with discrete dynodes

Electron multiplying

Electron multiplying CCD

Electron multiplying CCDs

Electron multiplying charge-coupled device EMCCD)

Electron-multiplier tubes

Electron-multiplying charge-coupled devices EMCCDs)

Electron-multiplying charge-coupled, device

Electrospray ionization generated, multiply charged

Electrospray ionization multiply charged ions produced

Energy Values of Multiply Ionized States

Enhanced multiply charged

Enhanced multiply charged scan

Enzyme multiplied immunoassay

Enzyme multiplied immunoassay technique

Enzyme multiplied immunoassay technique EMIT)

Equality Lagrange multipliers

Exponential Multiplied By Time

Exponential multiplier

Field ionization multiply charged ions

Floquet multiplier

Frequency multipliers

Friction multipliers

Gauges multiplying

General Characteristics of Multiplier Phototubes

General Multiply Periodic Systems. Uniqueness of the Action Variables

Global LaGrange multipliers

Grid multiplier

Hermitian-Lagrange multipliers

How to Multiply Align Sequences

Hydrogenation of Multiply Unsaturated Hydrocarbons

Infinite Homogeneous Multiplying Media

Infinity zero multiplied

Ion detectors channel electron multiplier

Ionization methods, mass multiply charged ions

Jacobi multiplier

John Multiplier Theorem

John Multiplier Theorem for Inequality Constraints

Kalecki multiplier

Kuhn-Tucker conditions Lagrange multipliers

Kuhn-Tucker multipliers

Lagrange Multiplier Rule

Lagrange Multiplier Rule constraints

Lagrange Multiplier Rule controls

Lagrange Multiplier Rule functions

Lagrange Multiplier Theorem

Lagrange Multiplier and Objective Functional

Lagrange multiplier

Lagrange multiplier linear constraints

Lagrange multiplier method

Lagrange multiplier orbital energy

Lagrange multipliers Subject

Lagrange multipliers constrained

Lagrange multipliers energy surfaces

Lagrange multipliers enforcing

Lagrange multipliers enforcing constraints

Lagrange multipliers existence

Lagrange multipliers functional

Lagrange multipliers interpretation

Lagrange multipliers linear

Lagrange multipliers molecular structure

Lagrange multipliers nonlinear

Lagrange multipliers, applications

Lagrange undetermined multiplier technique

Lagrange undetermined multipliers

Lagrange undetermined multipliers maximization

Lagrange undetermined multipliers method

Lagrange’s method of undetermined multipliers

Lagrange’s multipliers

Lagrangian multiplier

Lagrangian multiplier expansion

Lagrangian multiplier method

Lagrangian vector multiplier

Large numbers, multiplying

Leading multipliers

Ligands, multiply bonded

Local LaGrange multiplier

Magnetic electron multiplier

Mass Spectrometry Electron multiplier

Measurement prefix multipliers

Metallanes of multiply-substituted

Method of Lagrangian multipliers

Method of undetermined multipliers

MicroChannel plate electron multiplier

Microprobe multipliers

Momentum Velocity multiplied

Multichannel electron multiplier

Multiplier Circuits

Multiplier amplification

Multiplier detector

Multiplier function

Multiplier method

Multiplier processing element

Multiplier representation

Multiplier terms

Multiplier transformation problem

Multiplier, pneumatic

Multiplier, resistors

Multipliers channel

Multipliers crossed-field

Multipliers, addition compounds

Multipliers, mass spectrometry

Multiply

Multiply

Multiply Branched Polymers

Multiply Charged Molecules

Multiply Substituted Isotopologues

Multiply bonded

Multiply bonded complexes

Multiply bonded dimolybdenum complexes

Multiply bonded silicon compounds

Multiply charged analytes

Multiply charged ions

Multiply charged ions isotopic patterns

Multiply charged ions resolving isotopic patterns

Multiply charged metal ions

Multiply charged negative ions

Multiply charged negative ions anions)

Multiply charged secondary ions

Multiply charged species

Multiply connected

Multiply damaged sites

Multiply enriched systems

Multiply excited states

Multiply functionalized fullerenes

Multiply functionalized system

Multiply instantiated properties

Multiply ionized systems

Multiply operator

Multiply periodic function

Multiply periodic motion

Multiply periodic system

Multiply substituted oxazolines

Multiply twinned particle, gold

Multiply twinned particles

Multiply-Charged Ions in FI-MS

Multiply-accumulate

Multiply-bonded Group 14 compounds

Multiply-bonded Group 14 compounds theoretical studies

Multiply-bonded species

Multiply-bonded species structure

Multiply-bound species

Multiply-charged

Multiply-charged anions

Multiply-charged cations

Multiply-charged molecular ions

Multiply-charged precursor ions

Multiply-charged reagent ions

Multiply-protonated polypeptides

Multiplying

Multiplying

Multiplying both sides of an equation

Multiplying operators

Multiplying prefixes

Multiplying prefixes examples

Multiplying prefixes hyphenation

Multiplying proportions

Multiplying success, defined

Multiplying vectors

Multiplying with scientific notation

Negative Resistance Oscillators, Multipliers and BWOs

Negative number, multiplying inequalities

Neutron multiplier

On the Boundary Condition Between Two Multiplying Media

Peculiarities of multiply charged ions

Penalty function methods multipliers)

Peptide cation, multiply-charged

Peptide ions multiply-protonated

Peptide, multiply charged ions

Photo multiplier

Photo-multiplier tube

Photoelectric multiplier

Photon detectors photo-multiplier

Photon multiplier

Photon multiplier detector

Polymer patterns, multiply

Powers multiplying them

Predefined multiplier

Prefix multipliers

Process multiplier implementation

Protein multiply charged

Protein, analysis multiply-protonated

Quantum Conditions for Simply and Multiply Periodic Motions

Rates experience multiplier

Recognising multiply charged species

Reducing the Multiplier

Repayment multiplier

Resonance multiply excited states

Secondary electron multiplier

Secondary electron multiplier (SEM

Separable Multiply Periodic Systems

Shadow price multiplier

Signed number multiplier

Silyl multiply metalated

Single-channel electron multipliers

Single-point electron multipliers

Small numbers, multiplying

Solving proportions by multiplying or flipping

Stanford vector matrix multiplier

Subtracting and multiplying solutions

Symmetry multiplying

Tandem of multiply charged ions

Technetium not containing multiply bonded ligands

Temperature multipliers

The Electron Multiplier

The Kalecki multiplier

The Keynesian multiplier

The Lagrange Multiplier Method

The Multiplier

The Multiplier as an Indicator of Cost Competitiveness

The method of Lagrangian multipliers

Time multiplier setting

Two Floquet Multiplier at

Two-phase friction multipliers

Two-phase frictional multiplier

Two-phase multiplier

Undetermined multipliers

Undetermined multipliers, method

Units multipliers

Unsaturated hydrocarbons multiply, hydrogenation

Unstable leading multipliers

User-built multiplier

Vector matrix multiplier

Venetian blind multiplier

Voltage multiplier circuits

Voltage multiplier input circuits

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