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Refined Structure of (alpha)(beta)-Tubulin at 3.5 A Resolution
https://www2.mrc-lmb.cam.ac.uk/groups/JYL/PDF/jmb%20tubulin%20refinement.pdf3 Nov 2001: 24,pp. 255-302, Plenum Press, New York. 26. Wolf, S. G., Nogales, E., Kikkawa, M., Gratzinger,D., Hirokawa, N. & ... S. (1968). RelativisticHartree-Fock X-ray and electron scattering factors.Acta Crystallog. sect. A, 24, 390-397. -
Multiview Geometry: Profiles and Self-Calibration Paulo Ricardo dos…
mi.eng.cam.ac.uk/reports/svr-ftp/mendonca_phd-thesis.pdf22 May 2001: 24. 2.4 Projection of a torus. 25. 3.1 Geometric representation of the epipolar constraint. ... 24 CHAPTER 2. PROJECTIVE GEOMETRY. Figure 2.3. Torus corresponding to the fourth-degree implicit surface rotated by about the axis and translated. -
cde235 2454..2461
https://www2.mrc-lmb.cam.ac.uk/groups/JYL/PDF/MinC%20EMBO%202001.pdf4 May 2001: SeMet-substituted crystals were grown in thesame manner as for the native protein but with 24% PEG 2000, 0.1 Msodium citrate pH 4.8, 3.6% ethanol for the crystallization ... J. Appl. Crystallogr., 24,946950. Laskowski,R.A., Macarthur,M.W., Moss,D.S. and -
Correction of Probe Pressure Artifactsin Freehand 3D Ultrasound — ...
mi.eng.cam.ac.uk/reports/svr-ftp/treece_tr411.pdf27 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. -
EMBO problems/2
https://www-keeler.ch.cam.ac.uk/lectures/EMBOprobs.pdf1 Feb 2001: 1 24 2 2 2+ ( )In a heteronuclear system a coherence order can be assigned to each spinseparately. -
sb340206 159..168
www-civ.eng.cam.ac.uk/cjb/papers/p35.pdf9 Nov 2001: condition than misplaced bearings. 24. Imperfection caused by lateral load. While being transported, the beam can be. -
4–1 4 Coherence Selection: Phase Cycling and Gradient Pulses ...
https://www-keeler.ch.cam.ac.uk/lectures/phasen_a4.pdf1 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 -
Natural Frequency of a Horizontal Soil LayerPart II: Saturated ...
www-civ.eng.cam.ac.uk/geotech_new/publications/TR/TR273.pdf17 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. -
The Study ofRelative Density and Boundary Effects for Cone ...
www-civ.eng.cam.ac.uk/geotech_new/publications/TR/TR256.pdf22 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. -
LAMINAR BOUNDARY-LAYER THEORY:A 20TH CENTURY PARADOX? Stephen J.…
www.damtp.cam.ac.uk/user/sjc1/papers/ictam2000/short.pdf16 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
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