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Replicases

According to some remarks concerning the physical interaction between the incident ultrasonic wavelet and the defects [4-6], we consider that an Ascan signal, may be described as a weighted sum of few delayed and phase-shifted replicas of the ultrasonic incident wavelet j(r). We can express this mathematically as ... [Pg.174]

Fig. XV-11. Electron micrograph of a freeze fracture replica of a region inside a mul-tivesicular liposome. Note the tetrahedral coordination nearly every vertex has three edges, and each face is connected to three others. The average number of edges per face is 5.1. (From Ref. 77.)... Fig. XV-11. Electron micrograph of a freeze fracture replica of a region inside a mul-tivesicular liposome. Note the tetrahedral coordination nearly every vertex has three edges, and each face is connected to three others. The average number of edges per face is 5.1. (From Ref. 77.)...
The intensity autocorrelation measurement is comparable to all of the spectroscopic experunents discussed in the sections that follow because it exploits the use of a variably delayed, gating pulse in the measurement. In the autocorrelation experiment, the gating pulse is just a replica of the time-fixed pulse. In the spectroscopic experiments, the gating pulse is used to mterrogate the populations and coherences established by the time-fixed pulse. [Pg.1975]

The average of In Z(X.) is most conveniently done using tire replicas tlirough tire relation... [Pg.2661]

From tire above equation it follows tliat in tire mean-field limit replica symmetry is not broken. This makes tire GLO model conceptually simpler to interirret tlian tire random bond heteropolymer model discussed in tire appendix. [Pg.2662]

Fig. 3. Replica electron micrograph showing "house-of-cards" microstmcture in a machinable fluormica glass-ceramic (white bar = 10 fiva). Fig. 3. Replica electron micrograph showing "house-of-cards" microstmcture in a machinable fluormica glass-ceramic (white bar = 10 fiva).
Note For all practical purposes the stator performance data are only a replica of rotor data for torque and current. The performance of a motor is the performance of its rotor circuit and its design. [Pg.8]

With the help of this equation the thermal curve of a machine can be drawn on a log-log graph for a known r, I versus /j//, for different conditions of motor heating prior to a trip (Figure 3.12). The relay can be set for the most appropriate thermal curve, after assessing the motor s actual operating conditions and hence achieving a true thermal replica protection. [Pg.58]

Note For obtaining a true replica of the motor thermal characteristics, - / and 6 - t more curves may be plotted for th < 0.02. [Pg.62]

The scheme is termed a closed transient switching. A comparison of the two methods in terms of voltage transients and current overshoots is given in Table 4.1. In an AIT starter The same logic can be applied as discussed above. The star point of the AIT is opened and connected through the main contactor C3 to provide a near replica to a Y A switching. Figure 4.7 illustrates the revised scheme. [Pg.76]

Stalling or locked rotor protection. This is also detected by the prolonged starting time as well as overheating of the machine. It is possible that the machine was already under operation and hot when it had stalled. Under such a condition, the rotor operates at a high freqitency and is more vulnerable to damage. Since it is not possible to create a replica of the rotor, separate... [Pg.297]

Overcurrent protection. To provide a thermal replica protection, the relay is set according to motor s heating and cooling (/ - 1) curves supplied by the motor manufacturer. If these curves are not available, they can be established with the help of motor heating and cooling time constants, as in equations (3.2) and (3.4). A brief procedure to establish the motor thermal curves when they are not available is explained in Section 3.6. [Pg.298]

RTDs or thermocouples These are normally embedded in the stator windings as illustrated in Figures 12.42 and 12.39(a). The winding temperature can now be monitored continually and a temperature replica of the machine obtained at any time. Figure 12.39(b) shows... [Pg.307]

With the availability of 3.3 and 6.6 kV vacuum contactors the control of HT motors up to 6.6 kV systems has now become easier and economical, compact and even more reliable. For 11 kV. systems, vacuum as well as SF (Sulphur hexafluoride) breakers can be used. The HT motor s switching and protection through a vacuum contactor provides a replica of an LT system. The earlier practice of using an HT OCB, MOCB, or an air blast circuit breaker for the interruption of an HT circuit is now a concept of the past. [Pg.308]

On the supply side of the interrupter, an equivalent busbar, inductance and lumped capacitance with a provision to connect p.f. correction capacitors, if required, to represent a replica of the actual installation. [Pg.578]

Corona effect All such factors may influence the If and IZnO in different proportions and be detrimental in assessing the actual variation in through IZnO. IZnO therefore cannot be regarded as a true replica of I, monitoring IZnO may not accurately assess the actual condition of the arrester. To use IZnO to assess the condition of an arrester, it is essential to separate from it. [Pg.618]

A silver replica of a holly leaf is to be made by investment casting. (A natural leaf is coated with ceramic slurry which is then dried and fired. During firing the leaf burns away, leaving a mould cavity.) The thickness of the leaf is 0.4 mm. Calculate the liquid head needed to force the molten silver into the mould cavity. It can be assumed that molten silver does not wet the mould walls. [Pg.156]

Figure 2 Snapshot from an MD simulation of a multilamellar liquid crystalline phase DPPC bilayer. Water molecules are colored white, lipid polar groups gray, and lipid hydrocarbon chains black. The central simulation cell containing 64 DPPC and 1792 water molecules, outlined m the upper left portion of the figure, is shown along with seven replicas generated by the periodic boundary conditions. (From Ref. 55.)... Figure 2 Snapshot from an MD simulation of a multilamellar liquid crystalline phase DPPC bilayer. Water molecules are colored white, lipid polar groups gray, and lipid hydrocarbon chains black. The central simulation cell containing 64 DPPC and 1792 water molecules, outlined m the upper left portion of the figure, is shown along with seven replicas generated by the periodic boundary conditions. (From Ref. 55.)...
The feed-back design (Figure 6.3.3 on the next page) was a 2-level, 6-variables central composite plan that required 2 = 64 experiments for the full replica. A 1/4 replica consisting of 16 experiments was made with an additional centerpoint. This was repeated after every 3 to 4 experiments to check for the unchanged condition of the catalyst. The execution of the complete study required six weeks of around the clock work. In the next six weeks, mathematical analysis and model-building was done and some additional check experiments were made. [Pg.129]

The mean field treatment of such a model has been presented by Forgacs et al. [172]. They have considered the particular problem of the effects of surface heterogeneity on the order of wetting transition. Using the replica trick and assuming a Gaussian distribution of 8 Vq with the variance A (A/kT < 1), they found that the prewetting transition critical point is a function of A and... [Pg.279]


See other pages where Replicases is mentioned: [Pg.46]    [Pg.517]    [Pg.271]    [Pg.2242]    [Pg.2661]    [Pg.2663]    [Pg.197]    [Pg.327]    [Pg.45]    [Pg.59]    [Pg.59]    [Pg.132]    [Pg.282]    [Pg.287]    [Pg.294]    [Pg.295]    [Pg.299]    [Pg.299]    [Pg.425]    [Pg.571]    [Pg.582]    [Pg.589]    [Pg.619]    [Pg.729]    [Pg.104]    [Pg.109]    [Pg.109]    [Pg.110]    [Pg.110]    [Pg.171]    [Pg.218]   
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Carbon replicas

DNA replicases

Detachment replicas

Double replica blotting

Extraction replicas

Fractional replica

Franck-Condon vibronic replica

Freeze-fracture replica

Grating replica

Gratings, diffraction replicas

Hamiltonian replica exchange

Irregular replicas

LO-phonon replicas

Metadynamics replica exchange

Microfluidic devices replica molding

Monte Carlo method replica-exchange

Monte replica-exchange

Multidimensional replica-exchange

Multidimensional replica-exchange method

Negative replicas

Oxide replica

Parallel replica

Parallel replica dynamics exchange

Parallel-replica dynamics

Periodic replica

Phonon replica

Platinum shadowed replica

Polymer replica method

Polyurethane replica molding

Regular replicas

Replica Exchange Molecular Dynamics

Replica Hamiltonian

Replica Ornstein-Zernike equations

Replica and shadowing techniques

Replica definition

Replica dipolar fluid

Replica exchange Monte Carlo

Replica exchange molecular dynamics REMD)

Replica exchange with solute tempering

Replica exchange with solute tempering REST)

Replica expressions in the grand canonical ensemble

Replica formation, porous

Replica integral equation

Replica interaction

Replica method

Replica molding

Replica molding process

Replica moulding

Replica parts

Replica plating

Replica plating method

Replica plating of animal cells

Replica polymerization

Replica symmetry breaking

Replica techniques

Replica trick

Replica-casting method

Replica-exchange

Replica-exchange conformational

Replica-exchange conformational sampling

Replica-exchange method

Replica-producing techniques

Replicas platers

Replicas preparation

Replicas problems

Replication carbon replicas

Replication direct replicas

Replication extraction replicas

Replication methods double stage replicas

Replication methods extraction replicas

Shadowed carbon replica

Silica replicas, organic templates

Silicone replica method

Simple Continuous and Discrete Models for Simulating Replica Exchange

Simple replicas

Simulating replica exchange

Single-step replica

Skin surface replicas

Superstate parallel-replica dynamics

Surface replica

Synthesis replica

Templating method replica surfaces

The introduction of replicas

Thermodynamic Integration Versus Expanded Ensemble and Replica-Exchange Monte Carlo Simulation

Thin-film replicas

Two-step replica

Wright Brothers Flying Machine Replica

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