Data Bank contribution: P. Bradshaw, B.E. Launder and J.L. Lumley, "Collaborative Testing of Turbulence Models", J. Fluids Engg vol. 118, pp. 243-247, June 1996 This is CTTM data library disk 0 - introduction and documents. All files in this data bank contribution are in ASCII. CASES15 TXT 31132 01-14-97 12:19p ARCH1 TXT 54072 01-14-97 1:24p CTTMFIN TEX 51447 10-04-96 1:29p FIG1 EPS 13118 01-14-97 1:54p CTTMFIN PS 185700 01-14-97 1:50p 8 file(s) 367644 bytes 1088512 bytes free File ARCH1.TXT is the main description of the library. It contains directory listings for the "data disks" (now subdirectories) D1-D6 and R1-R7, and a table of contents of the data library of the 1980/81 Stanford Conference on Computation of Complex Turbulent Flows, which occupies disks D1-D3 with some material on later disks. It also contains detailed running instructions, as issued to the Collaborators, for the "complex" flows on Disk D6: instructions for the simpler cases on Disks D1 to D5 (only the cases actually used in the Collaboration) are in file CASES15.TXT. CTTMFIN is the final report to the funding agencies, recorded in TeX (not LaTeX) format and also as a PostScript file. The one figure is - necessarily - in a PostScript file, FIG1.EPS. The CTTM project began with "entry" test cases, namely the prediction of skin-friction coefficient in a boundary layer in zero pressure gradient at a momentum-thickness Reynolds number of 10000. The consensus value in low-speed flow is 0.00264, with an uncertainty of no more than +/- 2 percent (the entry cases also included a Mach 5 adiabatic-wall boundary layer and two boundary layers with heat transfer). The "entry" test cases proved invaluable in spotting errors in models or codes. We most strongly recommend that any turbulence model should first be tested in a low-speed constant-pressure boundary layer, and the predicted skin- friction coefficient and logarithmic-law constants checked against standard data. Grid spacing requirements in the near-wall region can also be checked in this simple flow. Codes which converge only at finite Mach number can be run at, say, M=0.3 and M=0.5, and the results extrapolated back to M=0 on the assumption that compressibility effects vary as the square of M.