International
Tables for
Crystallography
Volume C
Mathematical, physical and chemical tables
Edited by E. Prince

International Tables for Crystallography (2006). Vol. C. ch. 3.4, pp. 165-166

Section 3.4.1.4. Single crystals of biological macromolecules at ambient temperatures

P. F. Lindleya

a ESRF, Avenue des Martyrs, BP 220, F-38043 Grenoble CEDEX, France

3.4.1.4. Single crystals of biological macromolecules at ambient temperatures

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Crystals of biological macromolecules are normally grown from an aqueous solution (see Subsection 3.1.1.2[link] ), and when growth is complete are in equilibrium with the mother liquor. Changes in this equilibrium may often result in crystal damage, so the most important aspect of crystal mounting in this case is to preserve the crystal in its state of hydration. This is most readily accomplished by sealing the crystal in a thin-walled quartz or glass capillary tube (King, 1954[link]; Holmes & Blow, 1966[link]). The crystal adheres to the inside of the tube by surface-tension effects through a small droplet of liquid, and a further pool of liquid at one end maintains the required degree of hydration. The general principles involved are well described by Rayment (1985[link]). D'Aprile & Moretto (1975[link]) have described two simple devices, a small electric heater for melting the wax used for sealing the capillary and a refrigerating microcell to prevent heat affecting the wet crystal, which are very useful for mounting wet single crystals in capillary tubes.

Alternatively, crystals can be grown directly within capillary tubes (Phillips, 1985[link]) or microdialysis cells such as those described by Zeppezauer, Eklund & Zeppezauer (1968[link]). A further mounting device particularly useful for enzymatic studies is the flow cell (Wyckoff et al., 1967[link]), in which the specimen is immobilized while mother liquor, or buffer with substrates or inhibitors, is allowed to flow over the crystal. A useful account of this device is given by Petsko (1985[link]). More recently, Edwards (1993[link]) has described a yokeless flow cell, which uses a plastic cone fixed to a brass mounting pin with a wire harness to support the quartz capillary. Although the device was originally designed for Laue studies, its simplicity and practicality should make it useful for a wide range of diffraction experiments. Pickford, Garman, Jones & Stuart (1993[link]) have designed a mounting cell that allows the humidity around a protein crystal to be varied in a controlled manner. This may be particularly useful for crystals where the solvent content is high and the molecular packing, and hence the diffraction intensities, highly dependent on the precise amount of solvent present.

The relatively short crystal lifetimes and large volumes of intensity data often dictate that crystals of biological macromolecules be mounted so that data collection can be accomplished in the most efficient manner, for example, with a symmetry axis parallel to the rotation axis of the collection device. Samples crystallizing in the form of thin plates that have to be aligned perpendicular to the capillary axis can be wedged using cotton lint fibres (Narayana, Weininger, Heuss & Argos, 1982[link]), or mounted on a fibre plug (Przybylska, 1988[link]).

One of the key problems in collecting diffraction data from wet crystals is movement of the specimen within the capillary, i.e. crystal slippage. Numerous ways have been suggested to surmount this problem, including flattening of the capillary surface, surrounding the crystal with a thin film of plastic (Rayment, Johnson & Suck, 1977[link]) and supporting the crystal with fibre plugs in contact with the mother liquor.

Pressure cells. Tilton (1988[link]) has described an attachment that can be used on conventional diffractometers for collecting X-ray data from biomolecular crystals under gas pressures up to 300 atm (30 MPa). The crystals are coated with mineral oil to minimize dehydration (see Subsection 3.4.1.5[link]) and mounted in a quartz glass capillary between two layers of cotton fibres. These fibres give mechanical support to the specimen and protect it from shock during gas pressurization. No plugs of mother liquor or oil are used so that the gas flow is unimpeded. Kundrot & Richards (1986[link]) describe an adaptation of the flow cell for hydrostatic pressure studies up to 0.2 GPa. More recently, Kroeger & Kundrot (1994[link]) have described a gas cell that allows data sets at several partial pressures to be collected from the same crystal.

References

First citation D'Aprile, F. & Moretto, R. (1975). Two simple devices for sealing wet single crystals in capillary tubes. J. Appl. Cryst. 8, 696.Google Scholar
First citation Edwards, S. L. (1993). Yokeless flow cell for Laue crystallography. J. Appl. Cryst. 26, 305–306.Google Scholar
First citation Holmes, K. C. & Blow, D. M. (1966). The use of diffraction in the study of protein and nucleic acid structure. New York: John Wiley. Google Scholar
First citation King, M. V. (1954). An efficient method for mounting wet protein crystals for X-ray studies. Acta Cryst. 7, 601–602.Google Scholar
First citation Kroeger, K. S. & Kundrot, C. E. (1994). A gas cell for collecting X-ray diffraction data from proteins. J. Appl. Cryst. 27, 609–612.Google Scholar
First citation Kundrot, C. E. & Richards, F. M. (1986). Collection and processing of X-ray diffraction data from protein crystals at high pressure. J. Appl. Cryst. 19, 208–213.Google Scholar
First citation Narayana, S. V. L., Weininger, M. S., Heuss, K. L. & Argos, P. (1982). A method to increase protein-crystal lifetime during X-ray exposure. J. Appl. Cryst. 15, 571–573.Google Scholar
First citation Petsko, G. A. (1985). Flow cell construction and use. Methods in enzymology, Vol. 114, pp. 141–145. New York: Academic Press.Google Scholar
First citation Phillips, G. N. Jr (1985). Crystallisation in capillary tubes. Methods in enzymology, Vol. 114, pp. 128–131. New York: Academic Press.Google Scholar
First citation Pickford, M. G., Garman, E. F., Jones, E. Y. & Stuart, D. I. (1993). A design of crystal mounting cell that allows the controlled variation of humidity at the protein crystal during X-ray diffraction. J. Appl. Cryst. 26, 465–466.Google Scholar
First citation Przybylska, M. (1988). A novel method of mounting a protein crystal on a surface perpendicular to the X-ray capillary. J. Appl. Cryst. 21, 272–273.Google Scholar
First citation Rayment, I. (1985). Treatment and manipulation of crystals. Methods in enzymology, Vol. 114, pp. 136–140. New York: Academic Press.Google Scholar
First citation Rayment, I., Johnson, J. E. & Suck, D. (1977). A method of preventing crystal slippage in macromolecular crystallography. J. Appl. Cryst. 10, 365.Google Scholar
First citation Tilton, R. F. Jr (1988). A fixture for X-ray crystallographic studies of biomolecules under high gas pressure. J. Appl. Cryst. 21, 4–9. Google Scholar
First citation Wyckoff, H. W., Doscher, M. S., Tsernoglou, D., Inagami, T., Johnson, L. N., Hardman, K. D., Allewell, N. M., Kelley, D. M. & Richards, F. M. (1967). Design of a diffractometer and flowcell system for X-ray analysis of crystalline proteins with applications to the crystal chemistry of ribonuclease-S. J. Mol. Biol. 27, 563–578.Google Scholar
First citation Zeppezauer, M., Eklund, H. & Zeppezauer, E. S. (1968). Micro diffusion cells for the growth of single protein crystals by means of equilibrium dialysis. Arch. Biochem. Biophys. 126, 564–573.Google Scholar








































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