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Travel distance

The Driving Module houses power supply, circuits for determination of travel distance (odometer wheels) and circumferential orientation, and a computer and a storage facility for all data recorded. The Driving Module has cups extending to the pipe wall, thus providing the movement of the tool after its launching into the continuous oil flow. [Pg.1060]

The reaction rates for oxidation of atmospheric SO2 (0.05-0.5 d ) yield a sulfur residence time of several days, at most this corresponds to a transport distance of several hundred to 1000 km. The formation of HNO by oxidation is more rapid and, compared with H2SO2P results in a shorter travel distance from the emission source. H2SO4 can also react with NH to form NH HSO or (NH2 2S04 aerosols. In addition the NH NO aerosols are in equihbrium with NH (g) and HNO (g). [Pg.213]

Speed of containers sliding down a spiral may be controlled by the pitch of the spiral or by banldug the outer or inner edge of the blade. Banldug tends to throw the container to one side of the blade, thus varying its total travel distance. While usually fabricated of steel, blades may be specified in different materials, as required by specific appheations. [Pg.1976]

The events are so fine-tuned and the size of chamber, pressure of gas, travel, distance of the moving contact and the size of blast nozzle so designed and adjusted that a near-slrike-free interruption can be achieved for low reactive currents (inductive or capacitive) as well as fullload and very heavy fault currents. The advance compression of gas through the movement of main contact plays an important role by storing a part of the gas even before opening of the arcing contacts. [Pg.641]

The horizontal dispersion of a plume has been modeled by the use of expanding cells well mixed vertically, with the chemistry calculated for each cell (31). The resulting simulation of transformation of NO to NO2 in a power plant plume by infusion of atmospheric ozone is a peaked distribution of NO2 that resembles a plume of the primary pollutants, SO2 and NO. The ozone distribution shows depletion across the plume, with maximum depletion in the center at 20 min travel time from the source, but relatively uniform ozone concentrations back to initial levels at travel distances 1 h from the source. [Pg.330]

An AC corona discharge in the throat leads to a cloud of charged droplets whose large momentum allows very long travel distances. Multiple devices for eliminating static discharges in powder silos have been tested [41] but the tests did not address typical flow rates for large capacity, dense phase pneumatic transfer operations. [Pg.77]

As described above, the magnitude of Knudsen number, Kn, or inverse Knudsen number, D, is of great significance for gas lubrication. From the definition of Kn in Eq (2), the local Knudsen number depends on the local mean free path of gas molecules,, and the local characteristic length, L, which is usually taken as the local gap width, h, in analysis of gas lubrication problems. From basic kinetic theory we know that the mean free path represents the average travel distance of a particle between two successive collisions, and if the gas is assumed to be consisted of hard sphere particles, the mean free path can be expressed as... [Pg.101]

It is clear that if S> Xj, particle-particle collision happens most probably and X(9,P) = Xh. If Sparticle-wall collision happens within the travel distance of <5/cos 9. Then, the local free path of the test particle, X, is the average oiX 9,0) over the whole ranges of 6 and j3. That is. [Pg.102]

Following the approach similar to that of the atomic-scale model, the evolution of the system state and the lateral force on the asperity can be determined in terms of AUldrj = 0. If we chose V rj)= VQ cos ir rj) as the potential function for the repulsive and attractive pinning center, respectively, the lateral force F=-dy/d7 can be plotted as a function of the traveling distance p, as shown in Fig. 17. [Pg.173]

Fig. 15—Position and force of the moving atom as a function of traveling distance Xq, (a) position x, (b) acting force F with the dotted area corresponding the net work done by the force. Fig. 15—Position and force of the moving atom as a function of traveling distance Xq, (a) position x, (b) acting force F with the dotted area corresponding the net work done by the force.
Fig. 17 —Lateral force acting on the asperity versus the traveling distance r, (a) for repulsive pinning center, the dotted area corresponds to the net work done by the force, (b) for attractive pinning center. Fig. 17 —Lateral force acting on the asperity versus the traveling distance r, (a) for repulsive pinning center, the dotted area corresponds to the net work done by the force, (b) for attractive pinning center.
Another type of flow artifact is due to voxel inflow and outflow problems large velocities make a spin leave its designated voxel in the time between signal encoding and signal readout. As the traveled distance d and the velocity v are related by the expression d = vt, it is obvious that the effect is more severe, the smaller the voxel size is. Slow velocities, on the other hand, may be masked by diffusive displacements. [Pg.214]

For processing, the data on energy consumption were collected, within the trade, it was travel distance, information on cargo and storage time of various foods. All data was obtained primarily from farmers, processors and traders, absent sufficient data, it was supplemented by data from available databases, especially the Ecoinvent database. [Pg.271]

Bennett DH, Mckone TE, Matthies M, Kastenberg WE (1998) General formulation of characteristic travel distance for semivolative organic chemicals in a multimedia environment. Environ Sci Technol 32 4023 -030... [Pg.69]

In a nonattaching gas electron, thermalization occurs via vibrational, rotational, and elastic collisions. In attaching media, competitive scavenging occurs, sometimes accompanied by attachment-detachment equilibrium. In the gas phase, thermalization time is more significant than thermalization distance because of relatively large travel distances, thermalized electrons can be assumed to be homogeneously distributed. The experiments we review can be classified into four categories (1) microwave methods, (2) use of probes, (3) transient conductivity, and (4) recombination luminescence. Further microwave methods can be subdivided into four types (1) cross modulation, (2) resonance frequency shift, (3) absorption, and (4) cavity technique for collision frequency. [Pg.250]

The strain-stress relationship ay = Cykfiki is valid when strain is instantaneously provoked by stress, i.e., no dephasing process occurs. In fact, it was observed that the magnitude of acoustic waves decreased as a function of the travelling distance. Introducing a damping term proportional to the time course of strain variations can solve this discrepancy ... [Pg.212]

We now have an expression for c x, y, z) that depends on the parameter 8, which itself depends on time. The quantity m8 expresses the distance for which a puff emitted at / = 0, and whose center is located at x = iit, has appreciable concentrations. Physically, Eq. (4.9) expresses the concentration emanating from the point source to be a plume composed of many puffs whose concentration distributions are sharply peaked about the puff centroids at all travel distances. We have not specified the parameter 8, although we expect that it should be proportional to aixlu)(u. The assumptions made in deriving Eq. (4.8) require that 8 < xlu. If the proportionality constant relating 8 and aix/u)/u is of order one, as we expect it to be, then the condition of validity of Eq. (4.9) can be stated as... [Pg.227]

Fig. 6. Schematic illustration of the stopped-flow magnetic tweezers experiments to follow single chromatin fiber assembly, (a) Flow diagram of how the experiment was performed, (b) A blow-up of the cuvette, with the bead attached to its side note that the DNA tether is not normal to the wall of the cuvette because of the position of the external magnet, i.e., the z direction is out of the plane of the video frame, (c) A schematic explaining the calculation of the distance traveled by the bead across the videoscreen. The X- and y-coordinates of the bead position on each successive video frame are used to calculate the projected traveled distance, (d) The actual shortening of the fiber can be calculated from the projected shortening (travel of bead across screen) and the cosine of the angle theta. Fig. 6. Schematic illustration of the stopped-flow magnetic tweezers experiments to follow single chromatin fiber assembly, (a) Flow diagram of how the experiment was performed, (b) A blow-up of the cuvette, with the bead attached to its side note that the DNA tether is not normal to the wall of the cuvette because of the position of the external magnet, i.e., the z direction is out of the plane of the video frame, (c) A schematic explaining the calculation of the distance traveled by the bead across the videoscreen. The X- and y-coordinates of the bead position on each successive video frame are used to calculate the projected traveled distance, (d) The actual shortening of the fiber can be calculated from the projected shortening (travel of bead across screen) and the cosine of the angle theta.

See other pages where Travel distance is mentioned: [Pg.534]    [Pg.2301]    [Pg.212]    [Pg.55]    [Pg.60]    [Pg.61]    [Pg.974]    [Pg.59]    [Pg.91]    [Pg.102]    [Pg.173]    [Pg.174]    [Pg.174]    [Pg.142]    [Pg.149]    [Pg.246]    [Pg.71]    [Pg.264]    [Pg.375]    [Pg.42]    [Pg.319]    [Pg.26]    [Pg.93]    [Pg.204]    [Pg.139]    [Pg.216]    [Pg.444]    [Pg.270]    [Pg.110]    [Pg.110]    [Pg.111]    [Pg.92]    [Pg.130]   
See also in sourсe #XX -- [ Pg.72 ]

See also in sourсe #XX -- [ Pg.288 ]

See also in sourсe #XX -- [ Pg.682 , Pg.683 , Pg.700 ]




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