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51 - 60 of 160 search results for katalk:za33 24 where 0 match all words and 160 match some words.

  1. Results that match 1 of 2 words

  2. Correction of Probe Pressure Artifactsin Freehand 3D Ultrasound — ...

    mi.eng.cam.ac.uk/reports/svr-ftp/treece_tr411.pdf
    27 Apr 2001: Ultrasound in Medicine and Biology, 24(6):855–869, 1998. [6] W. L. Smith and A. ... Parker. Multilevel and motion model-based ultrasonicspeckle tracking algorithms. Ultrasound in Medicine and Biology, 24(3):427–441, 1998.

  3. E:CURRENT_WORKCRTS DEMONSTRATORREPORT.DVI

    www-civ.eng.cam.ac.uk/dsl/publications/CRTS2001.pdf
    21 Mar 2001: 50 mm. 85 mm. Figure 3.4: Cylindrical mould. 22 23 24 25 26 27 28 29 30 31 3216. ... 17. 18. 19. 20. 21. 22. 23. 24. Rm [mm]. Rr[mm] Rr = 0.4957Rm 6.7181.

  4. sb340206 159..168

    www-civ.eng.cam.ac.uk/cjb/papers/p35.pdf
    9 Nov 2001: condition than misplaced bearings. 24. Imperfection caused by lateral load. While being transported, the beam can be.

  5. EMBO problems/2

    https://www-keeler.ch.cam.ac.uk/lectures/EMBOprobs.pdf
    1 Feb 2001: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately.

  6. CUED/D-SoilsiTR290 title paae Numerical modelling of three-leg…

    www-civ.eng.cam.ac.uk/geotech_new/publications/TR/TR290.pdf
    17 Aug 2001: ID-Soils/- SPUDCAN LOAD-DISPLACEMENT AND ROTATION RESPONSES 9. TR290. I. 0.24 0.16 - I I I. ... TR290. 1. 0.24 1 I I 0.16. 0.16 - 0.08. 8.

  7. 4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...

    https://www-keeler.ch.cam.ac.uk/lectures/phasen_a4.pdf
    1 Feb 2001: 4–1. 4 Coherence Selection: Phase Cycling and Gradient Pulses. A multiple-pulse NMR experiment is designed to manipulate the spins in a certain carefully defined way so as to produce a particular spectrum. However, a given pulse sequence usually

  8. Natural Frequency of a Horizontal Soil LayerPart II: Saturated ...

    www-civ.eng.cam.ac.uk/geotech_new/publications/TR/TR273.pdf
    17 Aug 2001: Max=25.3. Mb=-26.4. Max=O.l. Mill=-0.2. Max=lO.S. Mln=-12.3. Mox=S.O. Mill=-9.4. Max=24.9. Mln=-33.6. ... II. SHORT TERMTIME RECORDS. G L e v e l FIG.NO.5 0 24.

  9. SPECKLE DETECTION INULTRASOUND IMAGES USING FIRST ORDER STATISTICS R. …

    mi.eng.cam.ac.uk/reports/svr-ftp/prager_tr415.pdf
    27 Jul 2001: 1. 00.5. 11.5. 2. 24. 68. 101.6. 1.8. 2. 2.2. 2.4. ... tand. ard. devi. atio. n. (a). 00.5. 11.5. 2. 24. 68.

  10. LAMINAR BOUNDARY-LAYER THEORY:A 20TH CENTURY PARADOX? Stephen J.…

    www.damtp.cam.ac.uk/user/sjc1/papers/ictam2000/short.pdf
    16 Jan 2001: F(α,β,c; Re) = 0. (24). In the case of linear two-dimensional Tollmien-Schlichting (TS) waveson a flat plate, the predictions of OS theory are in very good agreementwith ... Re 1. On the other hand, for the derivation of thelinearised OS equation and

  11. The Study ofRelative Density and Boundary Effects for Cone ...

    www-civ.eng.cam.ac.uk/geotech_new/publications/TR/TR256.pdf
    22 Aug 2001: 1 0. 0 4 8 1 2 1 6 20 24 2 8Corrected Prototype Depth, zpc (m). ... being 0.90. , leakage occurcd vertical stressbefore CPTStarted. 0-i I I I 1 I I 8 I I I I I 1 I0 4 8 12 16 20 24 28.

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