Next Wednesday I'll be visiting Guelph University (Ontario, Canada) to give a lecture on "Evolution as a Fact and a Theory." The hosts are Guelph Skeptics [Lecture].Maybe I'll see some of you there?
Next Wednesday I'll be visiting Guelph University (Ontario, Canada) to give a lecture on "Evolution as a Fact and a Theory." The hosts are Guelph Skeptics [Lecture].
As a general rule, the primary structure of a protein (amino acid sequence) ultimately determines it's final three-dimensional shape1. Proteins fold spontaneously to adopt a specific structure that minimizes free energy. The folded protein occupies the bottom of a free energy well [How Proteins Fold, The Anfinsen Experiment in Protein Folding, Disulfide Bridges Stabilize Folded Proteins, Heat Shock and Molecular Chaperones].
Myoglobin is a small protein with a bound heme group (shown as a space-filling molecule). It carries oxygen in the bloodstream and tissues. The oxygen molecule binds to the active site of the protein near one side of the heme group. There are specific amino acid residues at the active site that are absolutely required for binding oxygen. As you might expect, these amino acids are highly conserved—they will be found at that position in myoglobin from humans or any other species.
The class of proteins to which myoglobin belongs is called "globins." There are two other globins that you are probably familiar with: α-globin and β-globin are the two polypeptides that come together to form an α2β2 hemoglobin tetramer.
Let's go to the Pfam (protein family) database at the Sanger Institute in Cambridge (UK). The entry for the globin family is Globin PF00041. Click on "Alignments" in the left sidebar. This link takes you to the alignment page where you can create an alignment of all the known globin sequences. Choose 75 seeds (default) in the first table and select "Pfam viewer" from the pull-down menu under "Viewer." Click "View" to see the alignments.

1. Other factors that contribute are bound ligands, such as heme groups, and interactions with other proteins as in multimeric proteins with sifferent subunits.
Using U.S. Consumer Product Safety Commission data, the researchers found nearly 40,000 older adults were injured on escalators between 1991 and 2005. The most frequent cause of injury was a slip, trip or fall resulting in a bruise or contusion. The most common injuries were to the lower extremities. However, most injuries were not serious. Only 8 percent of the 39,800 injured were admitted to the hospital after evaluation in an emergency department.
"Although escalators are a safe form of transportation, fall-related injuries do occur. Older adults, especially those with mobility, balance or vision problems, should use caution while riding an escalator and especially when stepping on or off. They should not try to walk up or down a moving escalator, carry large objects, or wear loose shoes or clothing while riding since these appear to be associated with an increased risk of falling," said Dr. O'Neil, associate professor of clinical pediatrics at the IU School of Medicine.


Fractal Wrongness
The state of being wrong at every conceivable scale of resolution. That is, from a distance, a fractally wrong person's worldview is incorrect; and furthermore, if you zoom in on any small part of that person's worldview, that part is just as wrong as the whole worldview.
Debating with a person who is fractally wrong leads to infinite regress, as every refutation you make of that person's opinions will lead to a rejoinder, full of half-truths, leaps of logic, and outright lies, that requires just as much refutation to debunk as the first one. It is as impossible to convince a fractally wrong person of anything as it is to walk around the edge of the Mandelbrot set in finite time.
If you ever get embroiled in a discussion with a fractally wrong person on the Internet--in mailing lists, newsgroups, or website forums--your best bet is to say your piece once and ignore any replies, thus saving yourself time.
The image is "borrowed" from Jeffrey Shallit's blog Recursivity [Fractal Wrongness]

Horton, H.R., Moran, L.A., Scrimgeour, K.G., perry, M.D. and Rawn, J.D. (2006) Principles of Biochemisty. Pearson/Prentice Hall, Upper Saddle River N.J. (USA)
There are four levels of protein structure. The primary structure refers to the sequence of amino acid residues in the polypeptide chain written left-to-right from the N-terminus to the C-terminus.
The tertiary structure of a polypeptide is the three-dimensional conformation. Typical proteins contain α helices, β strands, and turns, although there are some proteins that only have α helices and turns, and others that have only β sheets and turns. In many cases, the final structure consists of distinct, independently folded regions called domains.
An example of a protein with multiple domains is shown on the left. This protein is the enzyme pyruvate kinase from cat (Felix domesticus). There are three separate domains indicated by the square brackets on the side. Note that each of the domains is connected to another by a short stretch of unordered polypeptide chain.
There are certain motifs that occur over and over again in different proteins. The helix-loop-helix motif, for example, consists of two α helices joined by a reverse turn. The Greek key motif consists of four antiparallel β strands in a β sheet where the order of the strands along the polypeptide chain is 4, 1, 2, 3. The β sandwich is two layers of β sheet [see β Strands and β Sheets].
Larger motifs are often called domain folds because they make up the core of a domain. The parallel twisted sheet is found in many domains that have no obvious relationship other than the fact that they share this very stable core structure. The β barrel structure is found in many membrane proteins. There are dozens of enzymes that have adapted to an α/β barrel. These enzymes are not evolutionarily related. (The β helix is much less common.)[Figure Credit: The figures are from Horton et al. (2006)]
Horton, H.R., Moran, L.A., Scrimgeour, K.G., perry, M.D. and Rawn, J.D. (2006) Principles of Biochemisty. Pearson/Prentice Hall, Upper Saddle River N.J. (USA)

Reverse turns. (left) Type I β turn. The structure is stabilized by a hydrogen bond between the carbonyl oxygen of the first N-terminal residue (Phe) and the amide hydrogen of the fourth residue (Gly). Note the proline residue at position n + 1 (right) Type II β turn. This turn is also stabilized by a hydrogen bond between the carbonyl oxygen of the first N-terminal residue (Val) and the amide hydrogen of the fourth residue (Asn). Note the glycine residue at position n + 2 [PDB 1AHL (giant sea anemone neurotoxin)]. (Horton et al. 2006)The two most common common types of β turn are the type I and type II turns shown above. The key point about turns is that they are highly ordered structures stabilized by internal hydrogen bonds. This is why they are counted as the third form of secondary structure (along with the α helix and β strand).
Horton, H.R., Moran, L.A., Scrimgeour, K.G., perry, M.D. and Rawn, J.D. (2006) Principles of Biochemisty. Pearson/Prentice Hall, Upper Saddle River N.J. (USA)

In 1915, Sir William Henry Bragg (1862 - 1942) and William Lawrence Bragg (1890 - 1971) were awarded the Nobel Prize in Physics for their work on the structure of crystals as determined by X-ray crystallography. The Physics prize in 1914 had been awarded to Max von Laue for his discovery of the diffraction of X-rays by crystals.Von Laue's epoch-making discovery of the diffraction of the X-rays in crystals, on the one hand established wave motion as the essential quality of those rays and, on the other, afforded the experimental proof of the existence of molecular gratings in the crystals. The problem, however, of calculating the crystal structures from von Laue's formulae was an exceedingly complicated one, in as much as not only the space lattices, but also the wavelengths and the intensity-distribution over the various wavelengths in the spectra of the X-rays, were unknown quantities. It was consequently a discovery of epoch-making significance when W.L. Bragg found out that the phenomenon could be treated mathematically as a reflection by the successive parallel planes that may be placed so as to pass through the lattice points, and that in this way the ratio between the wavelengths and the distances of the said planes from each other can be calculated by a simple formula from the angle of reflection.
It was only by means of that simplification of the mathematical method that it became possible to attack the problem of the crystal structures, but to attain the end in view it was further necessary that the photographic method employed by von Laue should be replaced by an experimental one, based on the reflection principle, which admitted of a definite, even though at first unknown, wavelength being made use of. The instrument requisite for the said purpose, the so-called X-ray spectrometer, was constructed by Professor W.H. Bragg, W.L. Bragg's father, and it has been with the aid of that instrument that father and son have carried out, in part conjointly, in part each on his own account, a series of extremely important investigations respecting the structure of crystals.
If a number of cubes are laid on and beside each other in such a way that one cube face coincides in every case with the face of an adjoining cube, whereby consequently eight vertices always meet in one point, those angular points give a visual picture of the lattice points in the so-called simple cubic lattice. If again a lattice point is placed so as to coincide with the central point of each cube face, the so-called face-centred cubic lattice is obtained, whereas the centred cubic lattice has one lattice point in every cube-centre. With the exception of these three cases there is no cubic lattice that fulfils the condition that parallel planes placed in any direction whatever so as to pass through all the lattice points, shall also be at a constant distance from each other. The space lattice in the regular or cubic system must therefore coincide with one of those three, or constitute combinations of them. In such lattice combinations, on the other hand, in which the condition just mentioned is not fulfilled, where consequently parallel planes placed to pass through all the lattice points in certain directions are not equidistant, that circumstance is revealed by an abnormal intensity distribution among spectra of different orders, when the reflection takes place by those planes.
From crystallographical data it is always known how the face of a cube is situated in any given regular crystal, and there is consequently no difficulty in fixing the crystal on the spectrometer table in such a way that the reflection shall take place by planes with any prescribed orientation.
The rays falling on the crystal were produced by X-ray tubes, platinum being at first used for the anticathode. The characteristic X-radiation of the metals consists, as is well known, of a few strong lines or narrow bands, and the very first experiments with the spectrometer revealed the X-radiation that is characteristic of platinum. However, in the research undertaken to find out the nature of complicated space lattices, in which an abnormal intensity distribution among spectra of varying orders constitutes one of the most important of the results observed, it soon proved desirable to have available an X-radiation of approximately half the wavelength of the strongest platinum-line. From theoretical considerations W.H. Bragg regarded it as probable that a metal whose atomic weight was somewhere near the figure 100, would give a characteristic radiation of the desired wavelength. Accordingly anticathodes of palladium and rhodium were produced, which fully answered the purpose in view, so that spectra ev en of the fifth order could be obtained and measured. In order to take practical advantage, however, of those results, it was essential to have a method for calculating the intensity in the case of a complicated space lattice, that would prove simpler than the one given by von Laue's theory, and W.L. Bragg developed one.
The above is a brief sketch of the methods discovered by the two Braggs for investigating crystal structures. The results of their investigations embrace a large number of crystals belonging to various systems and can only be cursorily summarized in this place.
To begin with, the two investigators applied themselves to the simplest types of the regular system, represented by the alkaline haloid salts. It then proved that potassium bromide and potassium iodide showed the spectra that are characteristic of a face-centred cubic lattice, while the spectra of potassium chloride represented a simple cubic lattice, sodium chloride occupying an intermediate position. As it must be assumed, on the strength of the analogy of these salts, both in a chemical and a crystallographical sense, that they are possessed of a corresponding space lattice, which could also be corroborated in another way, it was proved by those researchers that the lattice of the crystals in question consists of two face-centred cubic lattices corresponding to the two atoms, which interpenetrate in such a way that they together constitute one single cubic lattice.
From these investigations it follows that a metal atom in the crystals of the alkaloid salts is situated at one and the same distance from the six haloid atoms nearest to it, and vice versa - a relationship that was found to prevail, mutatis mutandis, in all the crystals examined. That means the exceedingly important discovery, both for molecular physics and chemistry, that the crystals consist of atomic lattices and not, as has been always imagined, of molecular ones.
Two face-centred cubic lattices can also interpenetrate in such a way that every point belonging to the one lattice is at the centre of gravity of a tetrahedron whose vertices are points belonging to the other lattice. That structure was found by the two Braggs in the diamond, and afforded an experimental support for the tetrahedral arrangement that chemists postulate for the four-coordinate carbon. On the other hand, the explanation became evident of why crystallographers have not been able to agree regarding the class in the regular system to which the diamond should be referred.
It would carry us too far and be quite too complicated a proceeding to give an account here of the further investigations into the space lattices of the crystals. It will suffice to add that, in the course of their investigations, the two Braggs have also discovered important relations between the amplitude and the phase difference of the diffracted rays on the one hand and the atomic weights on the other, and have also shown experimentally the influence of heat on the space lattice.
Finally it may be mentioned that the two investigators have also determined the wavelengths of the X-rays and the distances between the successive planes placed to pass through the lattice points with such exactitude, that the error, if any, is probably a t most some few units per cent and is more due to the general physical constant entering into the calculations than to the measurements themselves.
Thanks to the methods that the Braggs, father and son, have devised for investigating crystal structures, an entirely new world has been opened and has already in part been explored with marvellous exactitude. The significance of these methods, and of the results attained by their means, cannot as yet be gauged in its entirety, however imposing its dimensions already appear to be. In consideration of the great importance that these methods possess for research in the realm of physics, the Swedish Royal Academy of Sciences decided that the 1915 Nobel Prize in Physics should be divided between Professor W.H. Bragg and his son W.L. Bragg, in recognition of their services in promoting the investigation of crystal structures by means of X-rays.
The &alpha helix is one form of secondary structure in proteins. When a polypeptide chain contains the right sequence of amino acids it can adopt a helical conformation.
β sheets can also be formed when antiparallel β strands align edge to edge. As a matter of fact, the antiparallel conformation is more stable, and more common, than the parallel conformation. 
In order to appreciate why this is such a stable (and common) motif we need to add in the amino acid side chains. (They are usually ignored in the kinds of structures shown above so we can trace the polypeptide backbone.) In the figure on the right I've drawn the hydrophobic side chains in blue so you can see how they cluster together to form the interior "filling" of the sandwhich. You can think of these hydrophobic regions as being like the oil in a mixture of oil and water. The oil droplets tend to come together to exclude the water molecules. Similarly, the hydrophobic residues tend to come together in the middle of the protein and exclude water molecules. This is called hydrophobic interaction and it's one of the dominent weak forces n biochemistry.[Figures are from Horton et al. (2006) © Laurence A. Moran, Pearson/Prentice Hall]
Horton, H.R., Moran, L.A., Scrimgeour, K.G., perry, M.D. and Rawn, J.D. (2006) Principles of Biochemisty. Pearson/Prentice Hall, Upper Saddle River N.J. (USA)
Today's molecule isn't really a molecule. It's an indirect representation of a molecule. It would be amazing if one of you could guess the molecule by looking at the figure but that's probably beyond the ability of most Sandwalk readers. (I know I can't do it.) Your task is to identify what that strange picture is all about and how is it generated. SELECTION AND ADAPTATION REFORMEDIt looks pretty interesting. Some, but not all, of these topics need to be incorporated into modern evolutionary theory. It's too bad they're missing some other topics that should be there (group selection, species sorting, speciation). This conference would be much better if Stephen Jay Gould were still alive and could attend.
* Drift: John Beatty, University of British Columbia
* Neutralism: Sergey Gavrilets, University of Tennessee
* Multilevel selection: David Sloan Wilson, Binghamton University
NEW VIEWS ON GENOMES AND INHERITANCE
* Gene regulatory networks: Greg Wray, Duke University
* Genomes and post-genomes: Michael Purugganan, New York University
* Epigenetic inheritance: Eva Jablonka, Tel-Aviv University
* Niche inheritance: John Odling-Smee, Oxford University
UNDERSTANDING THE PHENOTYPE
* Dynamics of macroevolution: David Jablonski, University of Chicago
* Phenotypic plasticity: Massimo Pigliucci, Stony Brook University
* Origins of form: Stuart Newman, New York Medical College
CONTRIBUTIONS FROM EVO-DEVO
* Innovation: Gerd Müller, University of Vienna
* Modularity: Günter Wagner, Yale University
* Evolvability: Marc Kirschner, Harvard University
CHARACTERISTICS OF EXTENDED SYNTHESIS
* Non-centrality of the gene: Werner Callebaut, Hasselt University
* Principles of transition: Eörs Szathmary, Collegium Budapest
* Conceptual differences in the two syntheses: Alan Love, University of Minnesota

1. The photo is a bit grainy because my camera was on movie mode. Trust me, you don't want to see the complete movie.