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d# d# = departing train unit #.

If you prefer to place this sliced image compilation into a preexisting page within your site, continue with the following steps. 5. After dragging the sliced images and auto-generated HTML page into the Files tab of the Site Window, open the auto-generated HTML page and the page where you want to place your sliced image. Make sure you can see both pages. 6. On the auto-generated HTML page, select the entire table by dragging across it. 7. Drag the entire table from the HTML page into place on your destination page, as shown in Figure 10-15. As you drag, a wide black line shows you where the image table will land when you release the mouse. Use this guide to position the table, and then release the mouse to place the table. 8. Close the HTML page. This page isn t needed any longer. You can move it to the Site Trash or wait until you clean out your site during the final site check.

You can store useful subroutines in a separate file and import them using the include command. For example, save the Lepto code that follows in Listing 23-5 to a file called shapes.lep, and try the following (the output is shown in Figure 23-3):

Save this information in a file and print it out or save it somewhere. (Unfortunately, you can t save it on the Knoppix CD itself.) Remember to update it if you make any changes to your partition table. Now you can use fdisk to recreate damaged partition tables if necessary.

1. L. Baylor, et al. Improved core fueling with high eld pellet injection in the DIII-D tokamak. Phys. Plasmas, 7:1878 1885, 2000. 2. L. Baylor, et al. Comparison of fueling ef ciency from different fueling locations on DIII-D. J. Nucl. Mater., 313:530 533, 2003. 3. M. Berger and J. Oliger. Adaptive mesh re nement for hyperbolic partial differential equations. J. Comput. Phys., 53:484 512, 1984. 4. M.J. Berger and P. Colella. Local adaptive mesh re nement for shock hydrodynamics. J. Comput. Phys., 82(1):64 84, 1989. 5. P. Colella. Multidimensional upwind methods for hyperbolic conservation laws. J. Comput. Phys., 87:171 200, 1990. 6. P. Colella, et al. Chombo software package for AMR applications design document. 7. R.K. Crockett, P. Colella, R. Fisher, R.I. Klein, and C.F. McKee. An unsplit, cell-centered Godunov method for ideal MHD. J. Comput. Phys., 203:422 448, 2005. 8. P. Gohill, et al. Investigations of H-mode plasmas triggered directly by pellet injection in the DIII-D tokamak. Phys. Rev. Lett., 86:644 647, 2001. 9. R.J. Goldston and P.H. Rutherford. Introduction to Plasma Physics. Institute of Physics Publishing, Bristol, 1997. 10. R. Ishizaki, et al. Two-dimensional simulation of pellet ablation with atomic processes. Phys. Plasmas, 11:4064 4080, 2004. 11. S.C. Jardin, et al. A fast shutdown technique for large tokamaks. Nucl. Fusion, 40:923 933, 2000. 12. J.B. Bell, P. Colella, J.A. Trangenstein, and M. Welcome. Adaptive mesh re nement on moving quadrilateral grids. In Proceedings of the 9th AIAA Computational Fluid Dynamics Conference, Buffalo, NY, June 1989. 13. B.V. Kuteev. Hydrogen pellet ablation and acceleration by current in high temperature plasmas. Nucl. Fusion, 35:431 453, 1995. 14. A.K. MacAulay. Two dimensional time dependent simulation of ablation of hydrogen pellets in hot magnetized fusion plasmas. PhD thesis, Princeton University, 1993. 15. A. K. MacAulay. Geometrical, kinetic and atomic physics effects in a two dimensional time dependent simulation of ablating fuel pellets. Nucl. Fusion, 34:43 62, 1994. 16. H.W. M ller, et al. High plasmoid formation, drift, and striations during pellet ablation in ASDEX u upgrade. Nucl. Fusion, 42:301 309, 2002. 17. P. Parks. Magnetic- eld distortion near an ablating hydrogen pellet. Nucl. Fusion, 20:311 320, 1980. 18. P. Parks. Theory of pellet cloud oscillation striations. Plasma Phys. Control. Fusion, 38:571 591, 1996. 19. P. Parks, L.R. Baylor. Effects of parallel ows and toroidicity on cross eld transport of pellet ablation matter in tokamak plasmas. Phys. Rev. Lett., 94:125002, 2005. 20. P. Parks, et al. Radial displacement of pellet ablation material in tokamaks due to the grad-B effect. Phys. Plasmas, 7:1968 1975, 2000. 21. P. Parks and M. Rosenbluth. Equilibrium pellet and liquid jet shape under high ablation pressures. Phys. Plasmas, 5:1380 1386, 1998. 22. P. Parks and R.J. Turnbull. Effect of transonic ow in ablation cloud on lifetime of a solid hydrogen pellet in a plasma. Phys. Fluids, 21:1735 1741, 1978. 23. D.R. Reynolds, R. Samtaney, and C.S. Woodward. A fully implicit numerical method for single- uid resistive magnetohydrodynamics. J. Comput. Phys., 219:144 162, 2006.

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The impact of obesity on an individual s psychological state is highly variable (see 14). Psychiatric disorders may occur, with depression being commonest in women, subjects with extreme obesity, those who actively seek treatment, and patients with binge-eating disorder (Fabricatore and Wadden, 2004). All obese people should therefore be screened for depression and anxiety, and speci cally for eating disorders ( 20), because all these conditions can impair the patient s quality of life and can also interfere with successful management. Many studies have attempted to identify psychological factors that predict success or failure of obesity management programmes, but no consistently useful guidelines have yet emerged (Teixeira et al., 2005).