Fig. 1.2.4.1. Change of structure amplitude for horse haemoglobin as a function of salt concentration in the suspension medium of the low-order h0l reflections at various lattice shrinkage stages (C, C′, D, E, F, G, H, J) (p. 6) | html | pdf |
Fig. 1.2.5.1. A model of the myoglobin molecule at 6 Å resolution (p. 7) | html | pdf |
Fig. 1.2.5.2. Cylindrical sections through a helical segment of a myoglobin polypeptide chain (p. 7) | html | pdf |
Fig. 1.2.6.1. The 2 Å-resolution map of sperm-whale myoglobin was represented by coloured Meccano-set clips on a forest of vertical rods (p. 8) | html | pdf |
Table 4.2.1.1. Compilation of membrane proteins with known structures, including crystallization conditions and key references for the structure determinations (pp. 95-96) | html | pdf |
Table 4.2.2.1. Potentially useful detergents for membrane-protein crystallizations with molecular weights and CMCs [in water, from Michel (1991) or as provided by the vendor] (p. 97) | html | pdf |
Table 4.2.3.1. Summary of the results of attempts to crystallize the two-subunit cytochrome c oxidase from the soil bacterium Paracoccus denitrificans using different detergents (after Ostermeier et al., 1997) (p. 98) | html | pdf |
4.3. Application of protein engineering to improve crystal properties (pp. 100-110) | html | pdf | chapter contents |
Fig. 6.1.2.1. Section through a sealed X-ray tube (p. 125) | html | pdf |
Fig. 6.1.2.2. Synchrotron radiation emitted by a relativistic electron travelling in a curved trajectory (p. 126) | html | pdf |
Fig. 6.1.2.3. Comparison of the spectra from the storage ring SPEAR (p. 127) | html | pdf |
Fig. 6.1.2.4. Main components of a dedicated electron storage-ring synchrotron-radiation source (p. 127) | html | pdf |
Fig. 6.1.2.5. Electron trajectory within a multipole wiggler or undulator (p. 127) | html | pdf |
Fig. 6.1.2.6. Spectral distribution and critical wavelengths for (a) a dipole magnet, (b) a wavelength shifter and (c) a multipole wiggler at the ESRF (p. 128) | html | pdf |
Fig. 6.1.4.1. Production of a point focus by successive reflections at two orthogonal curved mirrors (p. 130) | html | pdf |
Fig. 6.1.4.2. The `catamegonic' arrangement of Montel (1957), in which two confocal mirrors with orthogonal curvatures lie side-by-side (p. 130) | html | pdf |
Fig. 6.1.4.3. Mirror bender (after Franks, 1955) (p. 130) | html | pdf |
Fig. 6.1.4.4. Triangular mirror bender as described by Lemonnier et al (p. 130) | html | pdf |
Fig. 6.1.4.5. Mirror holder with machined slots for two orthogonal pairs of curved mirrors (after Arndt, Duncumb et al (p. 130) | html | pdf |
Fig. 6.1.4.6. Ellipsoidal mirror for use with a microfocus X-ray tube, where x1 is ∼15 mm (p. 131) | html | pdf |
Fig. 6.1.4.7. A polycapillary collimator (after Bly & Gibson, 1996) (p. 131) | html | pdf |
Tables
Table 6.1.2.1. Standard X-ray tube inserts (p. 125) | html | pdf |