Taylor model

The hot-wire anemometer can be modified for hquid measurements, although difficulties are encountered because of bubbles and dirt adhering to the wire. See Stevens, Borden, and Strausser, David Taylor Model Basin Rep. 953, December 1956 Middlebrook and Piret, Ind. Eng. Chem., 42, 1511-1513 (1950) and Piret et al., Ind. Eng. Chem., 39, 1098-1103 (1947). 

David W. Taylor Model Basin, Washington, September 1953 Jackson, loc. cit. Valentin, op. cit.. Chap. 2 Soo, op. cit.. Chap. 3 Calderbank, loc. cit., p. CE220 and Levich, op. cit.. Chap. 8). A comprehensive and apparently accurate predictive method has been publisned [Jami-alahamadi et al., Trans ICE, 72, part A, 119-122 (1994)]. Small bubbles (below 0.2 mm in diameter) are essentially rigid spheres and rise at terminal velocities that place them clearly in the laminar-flow region hence their rising velocity may be calculated from Stokes law. As bubble size increases to about 2 mm, the spherical shape is retained, and the Reynolds number is still sufficiently small (<10) that Stokes law should be nearly obeyed. 

Myosin as an ATPase Activation of Myosin ATPase by Actin Lymn and Taylor Model 1971 Eisenberg and Hill Model 1985... 

HABERMAN, W. L. and SAYRE, R. M. David Taylor Model Basin Report No 1143 (Oct 1958) Motion of rigid and fluid spheres in stationary and moving liquids inside cylindrical tubes. 

W. L. Haberman R. M. Sayre (1958) Motion of Rigid and Fluid Spheres in Stationary and Moving Liquids Inside Cylindical Tubes, David Taylor Model Basin Report No. 1143, U. S. Navy, Washington, D. C. 

In the so-called Lymm-Taylor model, the actomyosin ATPase reaction proceeds in a stepwise manner ... 

R4. Rosenberg, B., David Taylor Model Basin (Navy Dept., Washington, D.C.), Rept. No. 727 (1950). 

B15. Bryn, T., David Taylor Model Basin Transl. No. 132 (1949). 

Refs 1) W.G. Neall, Radiological Safety Report. Hydra 1 at David Taylor Model Basin, Washington, DC, Naval Radiological Defense Lab Rept USNRDL-TR-423 (May 1960) 2)... 

A. Roosen and J.E. Taylor. Modeling crystal growth in a diffusion field using fully-faceted interfaces. J. Computational Phys., 114(1) 113—128, 1994. 

Cone-Plate Viscometer. Measurements with the cone-plate viscometer were made between 500 and 30,000 dynes/cm2. Evidently, the PU droplets in the emulsions are deformed into long streaks during the experiments at these high stresses. To understand the measured results, the Taylor model for the emulsions must be replaced by another model. For... 

The fourth actin-bound, top-of-powerstroke state is ephemeral. In the original Lymn—Taylor model it is not clear if this fourth state is strongly or weakly bound to actin, but P release, ADP release, and force generation all occur during the transition 4 to 1. Thus, in the following discussion, we attempt to break this transition down into a series of elementary events and to explore if it is possible to order the biochemical and mechanical events and to correlate them with structural changes. 

H.S. Taylor, Models, interpretations, and calculations concerning resonant electron scattering processes in atoms and molecules, Adv. Chem. Phys. 18 (1970) 91. 

Fig. 4.30 In contrast to the (non-reac-tive) Taylor model, the tracer gas speed for a reacting gas is unequal to the carrier gas speed. This can be derived from the exponential term in the solution of the concentration of the tracer gas cA at the channel exit.

SOURCE From Haberman and Sayre, David W. Taylor Model Basin Report 1143, 1958. 

This result was first derived by Aris (1956) using the method of moments. While the resulting model now includes both the effects (axial molecular diffusion and dispersion caused by transerverse velocity gradients and molecular diffusion) it has the same deficiency as the Taylor model, i.e. converting a hyperbolic model into a parabolic equation. 

Rochester, A.B. and White, R.B. (1980). Calculation of turbulent diffusion for the Chirikov-Taylor model, Phys. Rev. Lett. 44, 1586-1589. 

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