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. • Synopsis


over again “naturally” during breeding. Anew tool is available, its potential is undeniable. Only time will tell whether it will also bring the blessing of freeing us from hereditary diseases. In December 2023, the rst CRIS­PR-Cas9 gene-editing therapy was approved. Casgevy, launched by Vertex Pharmaceuticals, is aimed at curing sickle cell disease. It does not correct the mutation that causes sickle cell disease (Sect.12.13). Instead, Casgevy is designed to compensate for the loss of adult hemo­globin by inducing fetal hemoglobin, the main oxygen carrier in the fetus, which is normally switched off shortly after birth. The therapy is still very complex and expensive, but it represents apromising new treat­ment option.
Gene technology not only solves problems, but it also creates new ones. The technical barrier for creating ahomo perfectus is as low as it has ever been in human history. The door to possible misuse is now wide open. We can only hope that ethics and common sense will pre­vent this from happening. Draconian legal regulations do more harm to the benecial use of gene technology than to prevent its misuse. Those in positions of responsibil­ity have recognized this and have created aframework within which gene technology can evolve for the benet of humanity.
12.16 Synopsis
Gene technology has developed into akey technology
-
in modern drug research because it allows the pro-
duction of pure proteins, the targeted mutagenesis to
elucidate functional and mechanistic properties of pro-
teins or to conrm and disprove binding modes, pro-
duces animal models by knocking in and out particu-
lar genes, and allows genes to be activated or silenced.
With the PROTAC method, gene technology can be
used to target proteins for cellular degradation. This
makes individualized somatic gene therapy possible.
The elucidation of the genetic code, the recombinant
-
production of genes and gene products, and the poly-
merase chain reaction were milestones in the estab-
lishment of gene technology.
The sequence analysis of the human genome revealed
-
the constitution of our genes, the number of gene
products, and many functional insights. Meanwhile,
hundreds of genomes of other species have been se-
quenced, and the analysis of the genome of individ-
uals is affordable.
The human genome contains about 25,000 genes of
-
which about 21,500 are translated into proteins. Some
sequence segments are noncoding RNAs and they ac
complish important functions in the organism (e.g., in
the ribosome or spliceosome). About 95% of the ge-
nome contains numerous sequences and signals that
control the regulation of the genome. Afunctional
classication of the gene products has been accom­plished for asignicant portion of the genome.
To study the relevance of blocking the function of
-
agene product, that is, aprotein in adisease situation, aparticular gene can be knocked out in an animal model, mostly in mice. Genes can also be knocked in. Such turning on and off of genes is of utmost importance in drug research because it provides de­cisive information about the relevance of aplanned therapeutic intervention.
In vitro models for drug screening could only be de-
-
veloped once proteins could be produced in pure form and high yield. Various expression systems from bac­terial up to mammalian cells can be used for the pro­duction of foreign proteins, which are brought into cells via the corresponding coding DNA.
Genes can be silenced by RNA interference. There-
-
fore, small amounts of double-stranded RNA, usu­ally produced by the enzyme dicer, are incorporated into the enzyme complex RISC. RISC uses one strand of the RNA dimer segments as atemplate to capture mRNA molecules with acomplementary sequence and cleaves them sequentially. By doing this, mRNAs with particular sequences are eliminated.
To copy this principle for therapy, one needs about
-
22-base RNA molecules that have to be transported across the membrane into cells, adifcult task with fragile and highly polar species. Furthermore, these molecules can cause unwanted immune responses. Chemical modications of the RNA molecules are aimed at improvements in the transportation, immu­nogenicity, and stability properties.
The PROTAC process (proteolysis-targeting chime-
-
ras) causes selective proteolytic degradation of patho­genic and, therefore, unwanted proteins into amino acids by the cell’s own protein degradation machine.
The proteome reects the totality of all proteins in
-
acell at agiven point in time under precisely dened conditions. Its composition changes dynamically and differs between healthy or diseased states or under the inuence of therapeutic treatments.
The proteome can be analyzed at any given time by
-
2D gel electrophoresis. This combines aseparation by isoelectric focusing and SDS-PAGE analysis. Differ­ences in expression patterns indicate the involvement of proteins in adisease situation. Back regulation under drug administration can indicate apossible therapeutic strategy.
Pull-down experiments with immobilized drug mol-
-
ecules on a chromatographic solid support allow the trapping of proteins that show interaction with
-
studied drug molecules. Interaction proles for drug molecules in the cell can be determined.
Biomolecules can be immobilized on microarray
-
chips. In particular, RNA, DNA, and their oligonu­cleotides are anchored on these chips to extract com-
Chapter  • Gene Technology in Drug Research
12
plementary RNA or DNA sequences from large mix-
tures. Suitable uorescent labeling of the anchored
decoy sequences or of the sequences to be “shed”
makes it easy to automatically record the detection
of binding. With this, the expression patterns of cells
can be studied.
Polymorphisms, particularly single nucleotide poly-
-
morphisms (SNPs), are variations in the composition
of the genome of aspecies. These changes make indi-
viduals different, and some SNPs confer susceptibil-
ity or resistance to diseases or inuence the cellular
response to adrug.
Differences in the individual genomes might be the
-
key to atailored individual and personalized drug
therapy and can allow asusceptibility to aparticu-
lar disease pattern to be recognized. Intolerance to
agiven drug therapy could become transparent or the
classication of an individual into different metabo-
lizer classes could be achieved.
Genetic differences can be areason for the develop-
-
ment of diseases. In some cases, they are caused by
single amino acid exchanges in one gene product (e.g.,
sickle cell anemia); in other cases multifactorial genetic
causes are responsible for the disease development.
Epigenetics do not alter the sequence of DNA, but
-
regulate the transcription process by changing the
accessibility of genes. Lifestyle, experience, and en-
vironment exert their effect on the genes through the
epigenome.
Methylations, phosphorylations, and acetylations
-
transmit epigenetic information in areversible man-
ner. Either the bases of DNA are directly methylated
or the packing density of stored DNA on the histone
proteins is altered making it more or lesser accessible
to DNA reader domains. The latter process modies
the charges of positively charged Lys and Arg residues
involved in packing via the transfer of acetyl groups.
The goal of gene therapy tries to replace adefective
-
or missing gene in the cells of apatient. This would
make it possible to eliminate the genetic disease for the
individual and their offspring. Anucleic acid segment
is inserted into the genome via viral carriers, and it
codes for the protein that is to be substituted in the
patient. Gene therapy attempts to replace defective or
missing genes in apatient’s body cells. Retroviruses
are used for this purpose and anucleic acid segment
is introduced into their genome that codes for the
protein to be substituted in the patient. Retroviruses
transcribe this information into DNA and integrate
it into the DNA of the cells in the patient. With the
CRISPR-Cas9 method, highly precise gene scissors
are also available, which in the future might make it
easy to exchange diseased genes for healthy ones.

Bibliography and Further Reading

General Literature
B. R. Glick and J. J. Pasternak, Molecular Biotechnology: Principles
and Applications of Recombinant DNA, ASM Press; 6th Edition (2022)
K. B. Mullis, F. Ferré and R. A. Gibbs, Eds., The Polymerase Chain
Reaction, Birkhäuser, Boston (1994)
N. G. Cooper, Ed., The Human Genome Project. Deciphering the
Blueprint of Heredity, University Science Books, Mill Valley, CA,
USA (1994) T. Strachan, The Human Genome, Bios Scientic, Oxford (1992) G. M. Monastersky and J. M. Robel, Eds., Strategies in Transgenic
Animal Science, Blackwell Science, Oxford (1995) M. Békés, D. R. Langley, C. M. Crews, PROTAC targeted protein de-
graders: the past is prologue, Nat. Rev. Drug Discov., 21, 181–200
(2022) J. A. Wolff, Gene Therapeutics. Methods and Applications of Direct
Gene Transfer, Birkhäuser, Boston (1994) L. E. Post, Gene Therapy: Progress, New Directions, and Issues, Ann.
Rep. Med. Chem., 30, 219–226 (1995) J. S. Kiely, Recent Advances in Antisense Technology, Ann. Rep. Med.
Chem., 29, 297–306 (1994) S. B. Pandit, S. Balaji and N. Srinivasan, Structural and Functional
Characterization of Gene Products Encoded in the Human Ge-
nome by Homology Detection, IUBMB Life, 56, 317–331 (2004) P. E. Slagboom and I. Meulenbelt, Organisation of the Human Ge-
nome and our Tools for Identifying Disease Genes, Biological
Psychology, 61, 11–31 (2002) E. S. Lander, etal., Initial Sequencing and Analysis of the Human
Genome, Nature, 409, 860–921 (2001) J. C. Venter, etal., The Sequence of the Human Genome, Science, 291,
1304–1351 (2001) S. L. Salzberg, Open question: How many genes do we have? BMC
Biol., 16, 94 (2018) A. C. Lai and C. M. Crews, Induced protein degradation: An emerging
drug discovery paradigm, Nat. Rev. Drug Discov., 16, 101–114
(2017) L. DeFrancesco, Life Technologies promises $1,000 genome. Nature
Biotech., 30, 126 (2012) J.A. Doudna and E. Charpentier, Genome Editing. The new frontier
of genome engineering with CRISPR-Cas9, Science, 346, 1258096,
1–9 (2014)
Special Literature
K. B. Mullis, The unusual origin of the polymerase chain reaction,
Scient. American, 262(4), 56–61 (1990) R. D. Fleischmann etal., Whole Genome Random Sequencing and As-
sembly of Haemophilus inuenzae Rd, Science, 269, 496–512 (1995) M. D. Adams etal., Initial Assessment of Human Gene Diversity and
Expression Patterns Based Upon 83 Million Nucleotides of cDNA
Sequence, Nature, 377, Suppl., 3–174 (1995) L. Timmons, H. Tabara, C. C. Mello and A. Z. Fire, Inducible Sys-
temic RNA Silencing in Caenorhabditis elegans, Mol Biol Cell.,
14, 2972–2983 (2003) K. M. Sakamoto, K. B. Kim, A. Kumagai, F. Mercurio, C. M. Crews,
R. J. Deshaies, Protacs: chimeric molecules that target proteins to
the Skp1-Cullin-F box complex for ubiquitination and degrada-
tion, Proc Natl Acad Sci USA, 98, 8554–8559 (2001) C. Arnold, PROTAC protein degraders to drug the undruggable enter
phase 3 trials, Nat Med, (2020), https://doi.org/10.1038/d41591-
024-00072-8
Bibliography and Further Reading
M. W. Chang, E. Barr, J. Seltzer, Y.-Q. Jiang, G. J. Nabel, E. G. Nabel,
M. S. Parmacek and J. M. Leiden, Cytostatic Gene Therapy for Vascular Proliferative Disorders with a Constitutively Active Form of the Retinoblastoma Gene Product, Science, 267, 518–522 (1995)
C. Craig, Bristol-Myers to Pay $2.7M for Transgenic Goats that Make
Human Antibodies, BioWorld Today, 6, 1 (1995)
M. S. Gadd etal., Structural basis of PROTAC cooperative recognition
for selective protein degradation, Nat. Chem. Biol., 13, 514–521 (2017)
U. Rix and G. Superti-Furga, Target proling of small molecules by
chemical proteomics, Nat. Chem. Biol., 5, 616–624 (2009)
R. K. Seide and A. Giaccio, Patenting Animals, Chemistry & Industry,
16, 656–659 (1995)
http://www.ensembl.org/Homo_sapiens/index.html (Explore the Homo
sapiens genome) (Last accessed Nov. 16, 2024)
https://www.genecards.org/ (The Human Gene Database with functional
predictions) (Last accessed Nov. 16, 2024)
https://www.proteinatlas.org/search/ (The Human Protein Altas) (Last
accessed Nov. 29, 2024)
J. Wang, S. Yazdani, A. Han, M. Schapira, Structure-based view of the
druggable genome, Drug Discov Today, 25, 561–567 (2020)
S. Adhikari etal., A high-stringency blueprint of the human proteome,
Nat Comm, 11, 5301 (2020). https://doi.org/10.1038/s41467-020-
19045-9
P. Amaral etal., The status of the human gene catalogue, Nature, 622,
41–47 (2023)
J. M. Carlton etal., Draft Genome Sequence of the Sexually Transmit-
ted Pathogen Trichomonas vaginalis, Science, 315, 207–212 (2007)
S. Schneiker etal., Complete Genome Sequence of the Myxobacterium
Sorangium cellulosum. Nature Biotech., 25, 1281–1289 (2007)


Experimental Methods
of Structure Determination
Contents
13.1 Crystals: Aesthetic on the Outside, Periodic on the Inside – 194
13.2 Just Like Wallpaper: Symmetries Govern Crystal Packings – 196
13.3 Crystal Lattices Diract X-Rays – 196
13.4 Crystal Structure Analysis: Evaluating the Spatial Arrangement and Intensity of Diraction Patterns – 197


13.5 Diraction Power and Resolution Determine the Accuracy of aCrystal Structure – 201
13.6 Electron Microscopy: Topographic Images Reveal Macromolecular Structures – 205
13.7 Structures in Solution: The Resonance Experiment in NMR Spectroscopy – 208
13.8 From Spectra to Structure: Distance Maps Evolve into Spatial Geometries – 209
13.9 How Relevant Are Structures in aCrystal or NMR Tube to aBiological System? – 211
13.10 Synopsis – 212
Bibliography and Further Reading – 213
© The Author(s), under exclusive license to Springer-Verlag GmbH, DE, part of Springer Nature 2024 G. Klebe, Drug Design, https://doi.org/10.1007/978-3-662-68998-1_13
Chapter  • Experimental Methods of Structure Determination
13
In this chapter, we will focus on experimental methods used to determine the structure of ligands and proteins. There are three main techniques that provide informa­tion about the three-dimensional structure of small or­ganic molecules up to proteins: crystal structure analysis,
high-resolution NMR spectroscopy, and electron micros­copy. The rst technique is the oldest. It goes back to an
experiment performed by Max von Laue in 1912. Just 17years earlier, Wilhelm Roentgen had discovered an electromagnetic radiation that was later named X-rays or “Roentgen rays” in German in his honor. Together with his collaborators Walter Friedrich and Paul Knip­ping, Laue demonstrated the wave nature of X-rays using acopper sulfate crystal. At the same time, they demon­strated the lattice structure of crystals. Just one year later, William Lawrence Bragg and his father William Henry Bragg reaped the rewards of these experiments. They de­termined the crystal structure of sodium chloride. The technique has evolved over the years. Today, the struc­tures of proteins and nucleic acid complexes containing many thousands of amino acids and nucleosides have been determined.
NMR spectroscopy is likewise arelatively new tech­nique. In 1945, the research group of Felix Bloch and Edward Purcell in the USA rst observed the resonance absorption of hydrogen nuclei in amagnetic eld. From this experiment, the technique has grown, largely due to advances in instrumentation, to the point where the structure of proteins with more than 800 amino acids can be determined. However, this requires the protein to be extensively labeled with different isotopes.
In recent years, electron microscopy has emerged as another very powerful imaging technique, providing direct images for structure determination of very large, often membrane-bound protein complexes and viruses. For this purpose, the samples must be “vitried” (sealed in ice like aglass) in aprocess known as cryo-electron microscopy, so that they can then be studied as individ­ual molecules at low temperatures. On the other hand,
electron beams can also be used for crystallographic dif­fraction experiments to elucidate structures, similar to classical crystallography.
13.1 Crystals: Aesthetic on the Outside,
Periodic on the Inside
The term “crystal” causes one to immediately think of well-formed minerals or sparkling gemstones with amagnicent cut. The association of crystals with the structures of the molecules that determine our lives only occur to us as asecond thought. The crystal is typically associated with “dead” material. When Jack Dunitz took over his chair as professor of organic chemistry at the ETH in Zurich at the end of the 1950s, the famous nat­ural product chemist Leopold Ruzicka dismissively told him that crystals are a“chemical graveyard.” Nonethe­less, Dunitz and his research group showed over many years that acrystal in no way belongs in a“graveyard,” but rather is the key to understanding the structure, dy­namics, and reactivity of molecules.
If amineral is considered, the regular construction of the single crystals stands out. Even organic materials have the ability to form well-shaped crystals. One must only think of the fascinating crystals of candied sugar. Is this external regularity arepresentation of the inner structure? Before this question is answered, the way that crystals are obtained should be claried. Amineralogist got it easy. Nature has already provided well-formed crystals over thousands or millions of years. Organic molecules and proteins rarely occur in Nature in acrystalline state. Conditions must be found under which they crystallize.
In general, crystals are grown from asolution. For sim­ple organic substances, this can also be accomplished from melted material or by sublimation. Both crystallization methods are known from water when alake freezes over or when beautiful hoarfrost crystals form. For crystalliza- tion from solution, asolvent is sought in which the com-
. Fig. 13.1 Paving stones cover asurface without leaving holes (left).
This is only possible if they are derived from aparticular basic geo­metric pattern, for instance aparallelogram, rectangle, square, trian­gle, or hexagon. This basic pattern can by modulated by complemen­tary bulges and recesses. Apath cannot be covered without holes if
equilateral pentagons or octagons are used. If an octagonal stone is combined with asquare stone, however, the surface can be completely covered. It is immediately clear that if asquare stone is cut along its two diagonals, two triangles result. Adding four such pieces an octa­gon can be amended to asquare in this way (right)
. • Crystals: Aesthetic on the Outside, Periodic on the Inside


. Fig. 13.2 In the simplest case, amolecular packing is generated by
purely shifting the molecule in all three spatial directions. The gener­ating unit, the elementary cell, is derived from an irregularly angled body, aparallelepiped (right, magnied image, purple). If apoint near the molecule is picked out and all of the molecules in the crystal pack-
pound is sufciently soluble. By changing the conditions, the saturation point of the solution is exceeded. If this is done slowly, small crystal nuclei will be formed which can grow into large crystals. As arule, the solubility of the compound decreases as the temperature is lowered. The saturation point of the solution can be exceeded by chang­ing the temperature. The solution can also be “thickened,” meaning that some of the solvent is removed. Another possibility is to add asecond solvent in which the com­pound is less soluble. If the ratio of the two solvents is chosen correctly, the saturation point can be approached slowly. For compounds with acidic or basic groups, pH conditions can be found at which the compound exists as asalt. Because of strong ionic interactions, salts of­ten form better crystals. Organic compounds can also be “salted out.” This is done by adding asalt, such as sodium chloride, to an aqueous solution of the compound. The salt “absorbs” the water molecules as it goes into solution. It is surrounded by asolvation shell of water molecules. This removes the water molecules from the surface of the organic compound, which is also surrounded by asolvent sphere. By this, the saturation point of the compound is gradually exceeded and crystallization begins.
Proteins are complex entities that, as ageneral rule,
are only soluble in abuffered aqueous solution. Because
ing are connected via this point, athree-dimensional lattice will result. (7 https://sn.pub/UDQaYm)
of their amino acid composition, they carry charged ionic groups on their surfaces. Similarly, for proteins, it is also necessary to nd conditions under which they associate in periodic arrays. This is achieved by slowly changing the amount of water in which the protein is dis­solved. This can be done in both directions. Hydrophobic proteins begin to aggregate when the amount of water in­creases. Proteins that have stronger polar groups on their surfaces aggregate when the water molecules are removed from their surfaces. The adjustment of the local pH con­ditions to nd an optimal value, the choice of asuitable salt for salting out, and the different temperatures are the conditions that need to be optimized. In addition to salts, surface-active substances (detergents) can also inuence the solvation shell and support crystallization. Despite this, crystallization is akind of ne art. The search for suitable conditions requires creativity and diligence. To­day, however, the crystallization methods are so elaborate that the tedious work of setting up thousands of different test conditions is carried out by robots.
Sometimes considerable effort is invested into struc­ture determination. In 1995, the crystallization and struc­ture determination of HIV integrase, one of the key en­zymes in the life cycle of the virus, was accomplished only after the 40th point mutation of the original protein.
Chapter  • Experimental Methods of Structure Determination
13
These point mutations were made with the goal of alter­ing the surface properties of the protein so that orderly aggregation into acrystal could occur.
Let us return to the original question of whether the
orderly outwards appearance of acrystal is areection
of its inner structure. Chemically, acrystal is homoge­neous. The organic molecule or the protein is the basic building block. It is only when these building blocks are organized in aspatially ordered fashion that aperiodic array emerges which optimally lls space. In everyday life, many solutions to these packing problems are easily seen, for example, sugar cubes that will only t into the box if they are layered in the right direction, or paving stones that must be laid in aneat, periodic fashion to completely cover asidewalk or astreet without gaps (. Fig.13.1).
Asingle paving stone, when correctly tted to the next, represents arepeating unit in the lattice. Acrystallogra­pher refers to this unit as the elementary unit cell, and the orderly setting of one unit upon another in terms of peri­odic translation. In the simplest organic crystal structure, the elementary cell contains one molecule (. Fig.13.2).
13.2 Just Like Wallpaper: Symmetries
Govern Crystal Packings
The contents of an elementary cell can also be more complexly composed, for example, like awallpaper pat­tern. Abasic motif is repeated so that it lls the surface area. Crystallographers call the basic motif the asym- metric unit. In . Fig.13.3, this motif is aower branch. Not all of the motifs can be generated simply by shifting the branch; some must be additionally mirror-reected.
Apair of image and mirror-image branches represent the elementary cell. The surface can now be lled with this building block by simply shifting it. In addition to reecting, basic motifs can also be rotated. By using re­ections and rotations, both so-called symmetry oper- ations, the contents of the elementary cell is generated from the asymmetric unit. This cell is layered on itself in all three spatial directions in an orderly formed crystal lattice. Even as athree-dimensional entity, the elemen­tary cell must take on aparticular form to completely ll all of the space. If the basic types of elementary cells are combined with all of the possible symmetry opera­tions, 230 possibilities result for the basic motif to ll the space. The crystallographer calls them the 230 space groups. For chiral molecules, and proteins belong to this group, mirror reection does not occur. This reduces the number of possible space groups signicantly. Therefore, proteins (and nearly all of the chiral organic molecules) crystallize in only 65space groups.

13.3 Crystal Lattices Diffract X-Rays

Max von Laue used crystals to prove the wave nature of X-rays by diffracting them. For illustration, we shall con-
sider awater wave. When adrop of rain strikes apuddle, circular waves propagate from the center outwards. The drop generates aso-called elementary wave upon sub­mersion. If two drops that are separated by aparticular distance simultaneously strike the water’s surface, circu­lar waves propagate outwardly from both submersion points. It is better to observe this experiment when the surface of the water is constantly “excited,” for exam-
. Fig. 13.3 An area can be covered not only by purely shifting an
object, the asymmetric unit. Additional symmetry operations such as mirror reection and rotation can also be used. This way multiple copies of the object are generated. In the presented case, the ower branch along with its mirror image makes up the unit (the elementary cell is outlined in red) that can be used to cover the surface simply by shifting it regularly
. Fig. 13.4 Two raindrops strike the surface of the water and form
circular, outwardly moving water waves. These superimpose on each other to give aband-like interference pattern. There are areas along these bands where the water surface is quiet. In other areas, it moves that much more strongly
. • Crystal Structure Analysis: Evaluating the Spatial Arrangement and Intensity of Diraction Patterns


ple, by aconstantly dripping tap. The circular outwardly spreading wave fronts meet each other at some point. What happens? Alamellar pattern forms, parts of the water’s surface remain at rest and other parts seem to move vigorously (. Fig.13.4). In the cross section, the water surface moves sinusoidally (. Fig.13.5). How do two waves behave that collide and superimpose with each other? If the wave peak and another wave peak or the wave trough and another wave trough meet, the wave is amplied. If, on the other hand, awave peak meets atrough, they cancel each other out. The water surface remains calm. The lamellar pattern of moving and still water surface between waves that are moving outwardly and inwardly is caused by this superimposition. It is called interference. The band density depends on the dis­tance between the submersion points of the drops. The ensuing interference pattern, therefore, contains informa­tion about the relative position of the points from which the elementary waves were generated.
If parallel water waves (e.g., awave front at the coast) collide with abarrier that has asmall opening (e.g., ahar­bor entrance), semicircular waves spread outwards from the backside. If this barrier has two neighboring open­ings (double slit), semicircular waves develop behind each of the two openings. By this, the same picture as with the two raindrops is achieved (. Fig.13.4). The two waves interfere with each other behind the double-slit barrier, and adiffraction pattern forms. The density of this pat­tern, that is, the progression of the bands, depends on the geometry of the double slit.
Formally, the diffraction sequence on the crystal lat­tice is analogous. The same principles are valid, but the superimposition is more complex. Avery simple lattice shall be considered that has only one type of atoms. An X-ray beam runs as aparallel wave towards this crystal. It collides with an array of atoms and initiates an interaction that is comparable to that between the raindrop and the puddle. Each atom generates aspherical wave because of the interaction between the atom’s electrons and the X-ray. The circular wave on the water’s surface represents, there­fore, the spherical wave in space. The spreading spherical waves superimpose on one another and form awave that leaves the crystal in achanged direction (. Fig.13.6). Formally seen, the incoming and outgoing waves have an angular relationship to each other that is equivalent to the reection of the wave at aplane perpendicular to the con­sidered array of atoms. Therefore, the diffraction of the three-dimensional crystal lattice can be treated formally as areection at aplane in the lattice.
Many parallel sets of such lattice planes can be in­scribed on acrystal with differing relative separation from one another and relative occupation density with atoms (. Fig.13.7). The reected waves contain the in­formation about the geometry (distance) and the relative occupancy (scattering power) in this plane. To record the diffraction properties of acrystal, each set of parallel
planes of the crystal must be oriented in the X-ray beam so that areection is possible. This laborious work is taken over by acomputer-controlled diffractometer.
13.4 Crystal Structure Analysis: Evaluating
the Spatial Arrangement and Intensity of Diffraction Patterns
To demonstrate that different lattices indeed generate dif­ferent diffraction patterns, asimple experiment should be considered. For this purpose, alaser pointer and dif­ferent pinhole lters are needed. The pinhole lters can easily be made. Ablack-and-white printout of the peri­odic arrangements shown in . Fig.13.8 can be greatly reduced and transferred to high-resolution photographic lm. These perforated pinhole masks represent two-di­mensional periodic lattices. When the laser beam passes through these pinhole masks, adiffraction pattern is gen­erated on ascreen, which is shown in . Fig.13.8. The rst two masks change the spacing and symmetry of the pinhole mask. This is clearly reected in the diffraction images obtained. In the third and fourth masks, the re­peating motif of three or ve differently sized holes rep­resents amolecule with two types of atoms. These motifs form aperiodic lattice when arranged side by side. They have the same spacing or “dimension” as the rst image on the left. When the diffraction images are compared, the intensity distribution of the light spots is different in the rst, third, and fourth images. This intensity distri­bution contains the information about the spatial con­struction of the motif that created the lattice. This infor­mation is used to determine the crystal structure and the geometry of the molecule in the crystal.
The reections, that is, the intensity of the individual light spots in the diffraction pattern, contain informa­tion about the spatial geometry of the molecule. There is amathematical technique, the Fourier transform, that can be used to translate the diffraction pattern back to the generating motif expressed as a density in space. AFourier transform is the superposition of many sine and cosine functions to describe the periodicity in space. The intensity of the diffracted reections determines the contribution of the superimposed sine and cosine func­tions, as well as their relative phase. The importance of these aspects for the superposition of waves has already been emphasized in the explanation of interference (. Fig.13.5). Unfortunately, this relative phasing in­formation is lost in the diffraction experiment. The dif­fractometer records only the intensity of the reections. This lack of information is known as the phase problem in crystal structure determination. The relative phases must be reconstructed for the individual reections us­ing computational methods and appropriate measure­ment conditions. Often large electron-rich elements (e.g., heavy metal ions) are embedded in the protein (e.g., by
a
b
c
Chapter  • Experimental Methods of Structure Determination
. Fig. 13.5 The waves are sinusoidal
in cross-section. The distance between two wave peaks is called the wave­length. The height of the water wave at the summit is called the amplitude. The position at which the wave crosses the resting position determines the phase. (a)If two wave trains with the same phase meet, they will add to each other and the amplitude doubles. This situation is found in the places in
. Fig.13.4 where the water’s surface
moves more strongly. (b)If there is aphase difference of exactly one half of awavelength, the wave peaks will meet with the troughs. Both waves can­cel each other out. This represents the parts of . Fig.13.4 where the water surface is very still. (c)Any other su­perimposed phase shift causes awave, the amplitude of which is somewhere between the extremes in(a) and(b)
13
. Fig. 13.6 If awave front (blue) in one plane meets with arow of
atoms (black points on the dotted lines), each atom in this row will become the starting point for athree-dimensional circular wave. This is analogous to those created when the raindrop hits the surface of apuddle. The circular waves that formed from the back row of atoms superimpose upon one another just as in the case with the water waves
. Fig.13.4). All circular waves are generated with the same phase in
( the indicated direction of the incoming wave (left). As aresult of this
superimposition, anew wave front forms (red) that leaves the crystal in an altered direction. Relative to the direction of the incoming wave, they have an angle that is formally areection of the incoming wave front on the atom row that is marked with the green line. If adifferent incoming direction is taken (blue), the circular waves will not be gener­ated from the same place (right), that is, there is aphase difference be­tween them. Their superimposition does not lead to anew wave front leaving the crystal
. • Crystal Lattices Diract X-Rays


. Fig. 13.7 A cluster of parallel planes can be laid through the at-
oms of acrystal lattice(a,b,c). In the rst three images, one sort of
atoms is present. The relative distance of the inscribed planes from one another and their atomic occupation density varies. Each of these planes can give rise to “reections” in an X-ray diffraction experiment. For this, the crystal must be brought into the correct orientation for the incoming beam each time. The X-ray counter must be positioned in away so that it captures the out-going X-ray beam. It is from this geometry that the spatial orientation of the cluster of planes in the crystal is determined. The occupation density of the atoms decides
how “well” aparticular array of planes reects the incoming X-ray beam. This information is contained in the intensity (amplitude) of the outgoing wave. (d)Three different types of atoms in amolecular crystal have different spatial relationships to one another. A paral­lel cluster of planes can be placed through each type of atom in the molecule (here atriatomic molecule). The amplitude of the outgoing beam results as a superposition of three sets of waves reected at these planes. Therefore, the observed intensity contains information about the relative distance of the atoms on the mutually parallel lattice planes and, therefore, their arrangement in the molecule
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