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Two-timing

There are three changable sensor units for the MH-24/64 magnetic head as like as for MH-24. The units must be changed when rope diameter changes more than two times. The sensor units of the MH-40 and MH-54 are unchangable. So the MH-40 and MH-64 heads are more releable having no connectors for this. [Pg.336]

It is easy to notice, that the protection against a short-circuit failure in the X-ray tube circuit implements due to the "soft" outer characteristic of the apparatus main circuit. The overvoltage protection at emergencies in the control system happens due to the redistribution of the magnetie flow, created by power winding I, between the 3,6 control yokes. Therefore the voltage on the X-ray apparatus anode drops approximately two times. [Pg.431]

The base of this estimation is the signal to noise ratio. The lowest signal to noise ratio S/N which is necessary as a minimum to discern a signal from noise is S/N = 2 1 (4). Referring to the limiting values for the granularity Oj, of the film system classes the smallest density difference AD of an defect which would just be visible should be at least two times greater than On. [Pg.551]

Of our special interest is the thickness measurement of powder coatings. While the sound velocity of the electrostatic applied powder/air mixture is estimated to be two times the velocity in air it is also an estimation that thickness powder / air layer is reduced by a factor of 5 by smelting (burning in process, hardening). [Pg.843]

Figure Al.6.20. (Left) Level scheme and nomenclature used in (a) single time-delay CARS, (b) Two-time delay CARS ((TD) CARS). The wavepacket is excited by cOp, then transferred back to the ground state by with Raman shift oij. Its evolution is then monitored by tOp (after [44])- (Right) Relevant potential energy surfaces for the iodine molecule. The creation of the wavepacket in the excited state is done by oip. The transfer to the final state is shown by the dashed arrows according to the state one wants to populate (after [44]). Figure Al.6.20. (Left) Level scheme and nomenclature used in (a) single time-delay CARS, (b) Two-time delay CARS ((TD) CARS). The wavepacket is excited by cOp, then transferred back to the ground state by with Raman shift oij. Its evolution is then monitored by tOp (after [44])- (Right) Relevant potential energy surfaces for the iodine molecule. The creation of the wavepacket in the excited state is done by oip. The transfer to the final state is shown by the dashed arrows according to the state one wants to populate (after [44]).
Figure Al.7.5(a) shows a larger scale schematic of the Si(lOO) surface if it were to be biilk-tenninated, while figure Al.7.5(b) shows the arrangement after the dimers have been fonned. The dashed boxes outline the two-dimensional surface unit cells. The reconstructed Si(lOO) surface has a unit cell that is two times larger than the bulk unit cell in one direction and the same in the other. Thus, it has a (2 x 1) synnnetry and the surface is labelled as Si(100)-(2 x i). Note that in actuality, however, any real Si(lOO) surface is composed of a mixture of (2 X 1) and (1 x 2) domains. This is because the dimer direction rotates by 90° at each step edge. Figure Al.7.5(a) shows a larger scale schematic of the Si(lOO) surface if it were to be biilk-tenninated, while figure Al.7.5(b) shows the arrangement after the dimers have been fonned. The dashed boxes outline the two-dimensional surface unit cells. The reconstructed Si(lOO) surface has a unit cell that is two times larger than the bulk unit cell in one direction and the same in the other. Thus, it has a (2 x 1) synnnetry and the surface is labelled as Si(100)-(2 x i). Note that in actuality, however, any real Si(lOO) surface is composed of a mixture of (2 X 1) and (1 x 2) domains. This is because the dimer direction rotates by 90° at each step edge.
All the other infonnation needed for this process is contained in the two time correlation matrix because the process is Gaussian. A somewhat involved calculation [18] results (for 2 > in... [Pg.698]

Two applications of the flucUiathig diffusion equation are made here to illustrate tlie additional infonnation the flucUiations provide over and beyond the detenninistic behaviour. Consider an infinite volume with an initial concentration, c, that is constant, Cq, everywhere. The solution to the averaged diffusion equation is then simply (c) = Cq for all t. However, the two-time correlation fiinction may be shown [26] to be... [Pg.704]

The key for optimally extracting infonnation from these higher order Raman experiments is to use two time dimensions. This is completely analogous to standard two-dimensional NMR [136] or two-dimensional 4WM echoes. As in NMR, tire extra dimension gives infonnation on coherence transfer and the coupling between Raman modes (as opposed to spins in NMR). [Pg.1213]

Taking into account the hydration shell of the NA and the possibility of the water content changing we are forced to consider the water -I- nucleic acid as an open system. In the present study a phenomenological model taking into account the interdependence of hydration and the NA conformation transition processes is offered. In accordance with the algorithm described above we consider two types of the basic processes in the system and thus two time intervals the water adsorption and the conformational transitions of the NA, times of the conformational transitions being much more greater... [Pg.117]

The model consists of a two dimensional harmonic oscillator with mass 1 and force constants of 1 and 25. In Fig. 1 we show trajectories of the two oscillators computed with two time steps. When the time step is sufficiently small compared to the period of the fast oscillator an essentially exact result is obtained. If the time step is large then only the slow vibration persists, and is quite accurate. The filtering effect is consistent (of course) with our analytical analysis. Similar effects were demonstrated for more complex systems [7]. [Pg.278]

Charged species are not a special case in RAMSES. As ean be seen from Figure 2-57, rr-electron systems can accommodate any number of electrons between zero and two times the number of atoms involved. [Pg.67]

Now Ictu.s see how the de.scriptor.s bcltavc under rotation of the entire molecule. 1 f the trans isomer used before is rotated by 1and the descriptors are calculated again, a value of (-1 is obtained two times (right-hand side, bottom line of Figure 2-88). [Pg.90]

Most science papers call for things to be extracted 3 times (3X) with a solvent. Strike feels that this is overkill and that one or two times is usually sufficient. Sometimes one has so much product oil that it forms its own heavy layer (usually at the bottom). There is no need to extract such a large amount with solvent. In such a case one would merely drain the oil from the water or, if using a PP container, decant the water from the oil. The water itself can then be extracted once with solvent and the solvent added to the oil. [Pg.27]

Sots i. Prepared by addition as much of a solution of 1.5 g of lithium in 75 ml of liquid NH3 to 1 1 of the commercial product as to cause a uniformly blue solution, for a least 1 min. The liquid is subsequently distilled two times at 10-20 mmHg. [Pg.98]

When the friction coefficient is set to zero, HyperChem performs regular molecular dynamics, and one should use a time step that is appropriate for a molecular dynamics run. With larger values of the friction coefficient, larger time steps can be used. This is because the solution to the Langevin equation in effect separates the motions of the atoms into two time scales the short-time (fast) motions, like bond stretches, which are approximated, and longtime (slow) motions, such as torsional motions, which are accurately evaluated. As one increases the friction coefficient, the short-time motions become more approximate, and thus it is less important to have a small timestep. [Pg.93]

Since a standard additions calibration curve is constructed in the sample, it cannot be extended to the analysis of another sample. Each sample, therefore, requires its own standard additions calibration curve. This is a serious drawback to the routine application of the method of standard additions, particularly in laboratories that must handle many samples or that require a quick turnaround time. For example, suppose you need to analyze ten samples using a three-point calibration curve. For a normal calibration curve using external standards, only 13 solutions need to be analyzed (3 standards and 10 samples). Using the method of standard additions, however, requires the analysis of 30 solutions, since each of the 10 samples must be analyzed three times (once before spiking and two times after adding successive spikes). [Pg.115]

Note The sequence of columns in binary runs 1,2, 4, 8, 16, 32, 64, 128, 256, 512, 1024, 2048, 4096 and so on, each column being two times greater than the previous one. Compare this with the decimal system where each column is 10 times greater than the previous one. [Pg.305]

This last result includes the factor since all segments are counted twice by the combination of Eqs. (1.53) and (1.54). The double summation also makes the two terms in the brackets equal to two times either one of them. This procedure averages over all segments fulfilling the role of center of mass therefore it is appropriate to identify the quantity evaluated by Eq. (1.59) by the symbol rg. ... [Pg.54]

As T Tg, the difference between the two times diminishes, dropping to zero when T = Tg. [Pg.253]

Interference of Waves. The coherent scattering property of x-rays is used in x-ray diffraction appHcations. Two waves traveling in the same direction with identical wavelengths, X, and equal ampHtudes (the intensity of a wave is equal to the square of its ampHtude) can interfere with each other so that the resultant wave can have anywhere from zero ampHtude to two times the ampHtude of one of the initial waves. This principle is illustrated in Figure 1. The resultant ampHtude is a function of the phase difference between the two initial waves. [Pg.372]

In Figure lb, the two waves have a phase difference of 1/4 of the wavelength, X/4, and the resultant ampHtude is the square root of two times that... [Pg.372]

The use of plastics in the U.S. building and constmction sector increased at a rate of nearly 6% per year from 3,077,000 t in 1980 to 5,389,000 t in 1990 as shown in Table 2 (by resin class) and Table 3 (by market appHcation). This advance is almost two times the overall U.S. GNP growth for the same period and is a testimony of plastics increasing popularity as materials within the building and constmction sector. [Pg.328]


See other pages where Two-timing is mentioned: [Pg.312]    [Pg.898]    [Pg.261]    [Pg.697]    [Pg.705]    [Pg.706]    [Pg.1167]    [Pg.1433]    [Pg.1435]    [Pg.1503]    [Pg.1508]    [Pg.1580]    [Pg.2316]    [Pg.327]    [Pg.93]    [Pg.375]    [Pg.156]    [Pg.95]    [Pg.237]    [Pg.117]    [Pg.321]    [Pg.88]    [Pg.220]    [Pg.38]    [Pg.204]    [Pg.102]    [Pg.86]    [Pg.326]   
See also in sourсe #XX -- [ Pg.218 , Pg.236 ]




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