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Sampling diagram

Fig. 1.1. A sample diagram showing batch, fractional and dynamic melting models. Filled circles represent melts in equilibrium with the residual solid. There is no residual melt for the fractional melting model. Fig. 1.1. A sample diagram showing batch, fractional and dynamic melting models. Filled circles represent melts in equilibrium with the residual solid. There is no residual melt for the fractional melting model.
Fig. 4. Sampling diagram of sodium-24 in human liver homogenate Reprint l with i rmission from S. H. Harrison, R. Zeisler, NBS Internal Report 80-2164, p. 66, 1980. Copyright 1980 National Bureau of Standards... Fig. 4. Sampling diagram of sodium-24 in human liver homogenate Reprint l with i rmission from S. H. Harrison, R. Zeisler, NBS Internal Report 80-2164, p. 66, 1980. Copyright 1980 National Bureau of Standards...
Figure 28-3 Sampling diagram of experimental results for 24Na in liver homogenate. Figure 28-3 Sampling diagram of experimental results for 24Na in liver homogenate.
Figure 8.1. A sample diagram showing proposed chromatography system layouts. Figure 8.1. A sample diagram showing proposed chromatography system layouts.
Only two metal oxide lines (2Fe + 02 = 2FeO and 4/3 A1 + O2 = 2/3 AI2O3) are shown in the sample diagram (Fig. 5.4). In reality there are a large number of nearly parallel lines (for, say, CaO, MgO, Si02, BaO, K2O, Na20, etc.). All these lines are plotted on the basis of involvement of one mole of oxygen utilisation, e g. [Pg.56]

Figure 7.21. Isocratic (A) and gradient (B) separations of a diet cola sample. Diagram courtesy of Dionex Corporation. Figure 7.21. Isocratic (A) and gradient (B) separations of a diet cola sample. Diagram courtesy of Dionex Corporation.
Fig. 9.13. Sample diagrams of free energy density tp ) versus fractional composition 5 of constituent B for a disordered substitutional solid solution The free... Fig. 9.13. Sample diagrams of free energy density tp ) versus fractional composition 5 of constituent B for a disordered substitutional solid solution The free...
FIGURE 3 Diagram metadata labels for a sample diagram. Some labels, such as title and legend, are found in different places for different graphics. [Pg.72]

The sample should be liquid or in solution. It is pumped and nebulized in an argon atmosphere, then sent through a plasma torch that is, in an environment where the material is strongly ionized resulting from the electromagnetic radiation produced by an induction coil. Refer to the schematic diagram in Figure 2.8. [Pg.37]

The above experiment was conducted for a single fluid only. In hydrocarbon reservoirs there is always connate water present, and commonly two fluids are competing for the same pore space (e.g. water and oil in water drive). The permeability of one of the fluids is then described by its relative permeability (k ), which is a function of the saturation of the fluid. Relative permeabilities are measured in the laboratory on reservoir rock samples using reservoir fluids. The following diagram shows an example of a relative permeability curve for oil and water. For example, at a given water saturation (SJ, the permeability... [Pg.202]

Fig. 3. A diagram of the sample with residual austenite tor calibrating eddy current devices... Fig. 3. A diagram of the sample with residual austenite tor calibrating eddy current devices...
As it was determined by the test, the stretch diagram at the uniaxial load carrying ability of the carbon plastic UKN-5000 is almost linear until the destruction point. The samples are breaking brittle, and the relative deformation is small (E < 2%). [Pg.83]

Thus, carrying out tests of the samples shows that the acoustic emission method is quite effective at the quality estimation of carbon plastic and its adhesive joints. Depending on the chosen diagnostic diagram of the construction material loading, the criteria parameters are K, S or AS (a C). [Pg.85]

Figure 9 Slowness diagram At the interface between isotropic steel and a V-bntt weld with 10° inclination and perpendicular grain orientation the incident 45° (with regard to the sample top surface) shea.r wave will split into two quasi shear waves qSV and qSV( 2.)... Figure 9 Slowness diagram At the interface between isotropic steel and a V-bntt weld with 10° inclination and perpendicular grain orientation the incident 45° (with regard to the sample top surface) shea.r wave will split into two quasi shear waves qSV and qSV( 2.)...
Phase transitions in binary systems, nomially measured at constant pressure and composition, usually do not take place entirely at a single temperature, but rather extend over a finite but nonzero temperature range. Figure A2.5.3 shows a temperature-mole fraction T, x) phase diagram for one of the simplest of such examples, vaporization of an ideal liquid mixture to an ideal gas mixture, all at a fixed pressure, (e.g. 1 atm). Because there is an additional composition variable, the sample path shown in tlie figure is not only at constant pressure, but also at a constant total mole fraction, here chosen to be v = 1/2. [Pg.613]

Figure Bl.23.4. Schematic diagram of TOE scattermg and recoiling spectrometry (TOF-SARS) illustrating the plane of scattering fonned by the ion beam, sample and detector. TOE spectra (a) are collected with fixed... Figure Bl.23.4. Schematic diagram of TOE scattermg and recoiling spectrometry (TOF-SARS) illustrating the plane of scattering fonned by the ion beam, sample and detector. TOE spectra (a) are collected with fixed...
Figure Bl.24.1. Schematic diagram of the target chamber and detectors used in ion beam analysis. The backscattering detector is mounted close to the incident beam and the forward scattering detector is mounted so that, when the target is tilted, hydrogen recoils can be detected at angles of about 30° from the beam direction. The x-ray detector faces the sample and receives x-rays emitted from the sample. Figure Bl.24.1. Schematic diagram of the target chamber and detectors used in ion beam analysis. The backscattering detector is mounted close to the incident beam and the forward scattering detector is mounted so that, when the target is tilted, hydrogen recoils can be detected at angles of about 30° from the beam direction. The x-ray detector faces the sample and receives x-rays emitted from the sample.
Figure Bl.24.14. A schematic diagram of x-ray generation by energetic particle excitation, (a) A beam of energetic ions is used to eject inner-shell electrons from atoms in a sample, (b) These vacancies are filled by outer-shell electrons and the electrons make a transition in energy in moving from one level to another this energy is released in the fomi of characteristic x-rays, the energy of which identifies that particular atom. The x-rays that are emitted from the sample are measured witli an energy dispersive detector. Figure Bl.24.14. A schematic diagram of x-ray generation by energetic particle excitation, (a) A beam of energetic ions is used to eject inner-shell electrons from atoms in a sample, (b) These vacancies are filled by outer-shell electrons and the electrons make a transition in energy in moving from one level to another this energy is released in the fomi of characteristic x-rays, the energy of which identifies that particular atom. The x-rays that are emitted from the sample are measured witli an energy dispersive detector.
The main cost of this enlianced time resolution compared to fluorescence upconversion, however, is the aforementioned problem of time ordering of the photons that arrive from the pump and probe pulses. Wlien the probe pulse either precedes or trails the arrival of the pump pulse by a time interval that is significantly longer than the pulse duration, the action of the probe and pump pulses on the populations resident in the various resonant states is nnambiguous. When the pump and probe pulses temporally overlap in tlie sample, however, all possible time orderings of field-molecule interactions contribute to the response and complicate the interpretation. Double-sided Feymuan diagrams, which provide a pictorial view of the density matrix s time evolution under the action of the laser pulses, can be used to detenuine the various contributions to the sample response [125]. [Pg.1980]

Fig. 4.25 Adsorption isotherms showing low-pressure hysteresis, (a) Carbon tetrachloride at 20°C on unactivated polyacrylonitrile carbon Curves A and B are the desorption branches of the isotherms of the sample after heat treatment at 900°C and 2700°C respectively Curve C is the common adsorption branch (b) water at 22°C on stannic oxide gel heated to SOO C (c) krypton at 77-4 K on exfoliated graphite (d) ethyl chloride at 6°C on porous glass. (Redrawn from the diagrams in the original papers, with omission of experimental points.)... Fig. 4.25 Adsorption isotherms showing low-pressure hysteresis, (a) Carbon tetrachloride at 20°C on unactivated polyacrylonitrile carbon Curves A and B are the desorption branches of the isotherms of the sample after heat treatment at 900°C and 2700°C respectively Curve C is the common adsorption branch (b) water at 22°C on stannic oxide gel heated to SOO C (c) krypton at 77-4 K on exfoliated graphite (d) ethyl chloride at 6°C on porous glass. (Redrawn from the diagrams in the original papers, with omission of experimental points.)...
Schematic diagram of a sample thief. Rotating the inner cylinder opens and closes the openings along the outer cylinder s shaft. Schematic diagram of a sample thief. Rotating the inner cylinder opens and closes the openings along the outer cylinder s shaft.

See other pages where Sampling diagram is mentioned: [Pg.12]    [Pg.140]    [Pg.1612]    [Pg.492]    [Pg.1004]    [Pg.1029]    [Pg.125]    [Pg.253]    [Pg.12]    [Pg.140]    [Pg.1612]    [Pg.492]    [Pg.1004]    [Pg.1029]    [Pg.125]    [Pg.253]    [Pg.218]    [Pg.121]    [Pg.84]    [Pg.154]    [Pg.517]    [Pg.1206]    [Pg.1214]    [Pg.1329]    [Pg.1426]    [Pg.1695]    [Pg.1837]    [Pg.1876]    [Pg.1916]    [Pg.2534]    [Pg.568]    [Pg.25]    [Pg.211]    [Pg.384]    [Pg.390]    [Pg.393]   
See also in sourсe #XX -- [ Pg.83 , Pg.88 ]




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