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A structured stochastic ow model for interpreting ow: follower data from a stirred vessel, Trans Inst Chem Eng, 59, 271 278 Manning, F S, D Wolf, and D L Keairns (1965) Model simulation of stirred tank reactors, AIChE J, 11(4), 723 727 M rkl, H, R Bronnenmeier, and B Wittek (1991) The resistance of micro-organisms to a hydrodynamic stress, Int Chem Eng, 31(2), 185 Martin, T, C M McFarlane, and A W Nienow (1994) The in uence of liquid properties and impeller type on bubble coalescence behaviour and mass transfer in sparged agitated bioreactors, Proc 8th European Conf on Mixing Cambridge, Sept 1994 I ChemE, Rugby, pp 57 64 Meier, S J, T A Hatton, and D I C Wang (1999) Cell death from bursting bubbles: role of cell attachment to rising bubbles in sparged reactors, Biotechnol Bioeng, 62(4), 468 478.

This formula will not work if the Data range consists of noncontiguous cells. In other words, Data must be a rectangular range of cells.

1. Make sure that the element you want to affect is contained within a <div> tag with an ID on your page. 2. Select the object to trigger the effect.

Meijer, J, H ten Hoopen, K Luyben, and R Libbenga (1993) Effects of hydrodynamic stress on cultured plant cells: a literature survey, Enzyme Microb Technol, 15, 234 238 Meijer, J J, H J G ten Hoopen, Y M van Gameren, Ch A M Luyben, and K R Libbenga (1994) Effects of hydrodynamic stress on the growth of plant cells in batch and continuous culture, Enzyme Microb Technol, 16, 467 477 Merchuk, J C (1991) Shear effects on suspended cells, Adv Biochem Eng Biotechnol, 44, 66 95..

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The parallel function to getDirectory() is getFilename(), which extracts a filename from a fully qualified pathname. This code returns seasonal.png:

Some accessory lenses have a flat front surface, such as the Cokin 0.5x Wide-Angle Lens shown in Figure 14-6. Normally it s not an issue to glue the mounting thread of the step-up ring directly to the front surface of a telephoto lens. However, the Cokin 0.5x Wide-Angle Lens is so wide that any additional thickness in the front causes vignette. The only solution is to saw the mounting thread off a 52-77mm step-up ring.

The MIT Mark II display It was apparent to those who worked with Mark I that scaling the system up so that it made a big enough image to get both eyes into the view zone with some amount of look-around required increasing the space-bandwidth product of the diffractive part of the display, and also required a horizontal mirror that was bigger than would be practical with a spinning mirrored drum. The Mark I1 display, designed by St. Hilaire,xiii,xiv brought two major improvements over Mark I. The first was the use of an 18channel TeO, AOM, such that 18 scan lines could be output in parallel (with the vertical mirror moving in 18-line steps instead of a continuous sweep); the second was the replacement of the large horizontal polygonal mirror with a linear array of small galvanometric scanners. The goal of this modular architecture was to be able to scale up the image in size and resolution by adding more AOM channels and more horizontal mirrors. The raster image driving the display is 18 channels of 262144 x 8, and was generated by a compact dataflow supercomputer called Cheops developed at the MIT Media Laboratory, and later by PC graphics cards (see below). Images from Mark I1 have a 30 view angle and a volume of 150mm x 75mm x 150mm (width x height x depth). This is not only large enough to permit both eyes to be in the view zone, but to permit experiments with such concepts as haptic (force-feedback) interfaces, though with only 144 vertical scan lines it still isn t really television quality.

On the other hand, there are no bound states of two solitons or two antisolitons for the SineGordon system. This is confirmed by theoretical scattering experiments performed by Lorentz boosting solitons and allowing them to collide: two solitons or two antisolitons bounce off each other, suggesting a repulsive force, but a soliton and an antisoliton pass through each other with a time delay, suggesting an attraction.

Figure 17-3 shows the effect of the following code:

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