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Training of different microsurgical suture techniques with the help of BASYC . a end-to-end anastomosis , d end-to-side anastomosis. Reprinted with permission from

Training ofa Kohonen neural network with a chirality code, The number of weights in a neuron is the same as the number of elements in the chirality code vector, When a chirality code is presented to the network, the neuron with the most similar weights to the chirality code is excited ,

Training set samples in class A-D are displayed in the two-measurement row space. Unknown samples are labeled X, Y, and Z.

Training set spectra from

Training simulator image for an LDPE plant.

Training spray operators to calibrate a sprayer using a Kalibottle . Photo G. A. Matthews

Training to support risk assessment

Training to support the incident response plan

Training using back-propagation.

Traiumission electron micrographs of a mixture of a star diblock copolymer fringes are due to variations in the thickness of the specimen only. Pictures reproduced witti permission from .

Traizole NSC746457 as a novel HDAC-1 inhibitor.

Traj ectories of single resin particle in water computed from the equation on p. 548

Trajecfories that reach the same value of the scattering angle 9for given initial orientation .

Trajectorie.s having subsets of all f-values equal to unity.

Trajectories and power spectra of the same particle with equal initial conditions for Re 0.08 with a volume fraction of 0.14 and dimensionless frquency f 10.0. The figure is a courtesy of Dr. G. Barrios.

Trajectories corresponding to the relative motion of two molecules. The filled circle represents the pseudo-molecule and the cross the fixed center of force. Two trajectories are shown, for the same quantum states of the reactants, but with different phases of the internal degrees of freedom, as explained in the text.

Trajectories flow through the area, S, of an arbitrary 6 V-dimensional closed domain, V.

Trajectories for collisions at different impact parameters showing the deflection at different values of b b Rm- For large initial f the trajectory is a shade pulled in by the long-range force. The deflection is maximal at the rainbow, which is at far Ffm- For closer-in approach the trajectory begins to sample the repulsive potential. At what is called the glorythe net deflection is zero because the initial attraction is fully counterbalanced by the repulsion closer in. Below the glory, fa fag, repulsion dominates and the scattering is backwards. Rq isthe distance of closest approach.

Trajectories for compositions in stillpot.

Trajectories for distillate and bottoms products versus D F for column.

Trajectories for interception by a cylinder. After Spielman, L.A. 1977. Particle capture from low-speed laminar flows. Ann. Rev. Fluid Mech. 9, 297-319. Copyright 1977 by Annual Reviews Inc. With permission.

Trajectories for particle interception by a cylinder with London forces of attraction incorporated. After Spielman, L.A. C Goren, S.L. 1970. Capture of small particles by London forces from low-speed liquid flows. Environ. Sci. Technol. 4, 135-140. Copyright 1970 American Chemical Society. With permission.

Trajectories for region G see

Trajectories for the coupled oscillator system of eqs. . Parameters

Trajectories for two hypothetical spherical molecules. Two trajectories are shown by arrows. Trajectory I is very significant if one of the molecules is charged, since this can give rise to substantial charge-induced dipole attractive forces.



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