Conformational analysis of the full‐length M2 protein of the influenza A virus using solid‐state NMR

The influenza A M2 protein forms a proton channel for virus infection and mediates virus assembly and budding. While extensive structural information is known about the transmembrane helix and an adjacent amphipathic helix, the conformation of the N‐terminal ectodomain and the C‐terminal cytoplasmic tail remains largely unknown. Using two‐dimensional (2D) magic‐angle‐spinning solid‐state NMR, we have investigated the secondary structure and dynamics of full‐length M2 (M2FL) and found them to depend on the membrane composition. In 2D ¹³C DARR correlation spectra, 1,2‐dimyristoyl‐sn‐glycero‐3‐phosphocholine (DMPC)‐bound M2FL exhibits several peaks at β‐sheet chemical shifts, which result from water‐exposed extramembrane residues. In contrast, M2FL bound to cholesterol‐containing membranes gives predominantly α‐helical chemical shifts. Two‐dimensional J‐INADEQUATE spectra and variable‐temperature ¹³C spectra indicate that DMPC‐bound M2FL is highly dynamic while the cholesterol‐containing membranes significantly immobilize the protein at physiological temperature. Chemical‐shift prediction for various secondary‐structure models suggests that the β‐strand is located at the N‐terminus of the DMPC‐bound protein, while the cytoplasmic domain is unstructured. This prediction is confirmed by the 2D DARR spectrum of the ectodomain‐truncated M2(21–97), which no longer exhibits β‐sheet chemical shifts in the DMPC‐bound state. We propose that the M2 conformational change results from the influence of cholesterol, and the increased helicity of M2FL in cholesterol‐rich membranes may be relevant for M2 interaction with the matrix protein M1 during virus assembly and budding. The successful determination of the β‐strand location suggests that chemical‐shift prediction is a promising approach for obtaining structural information of disordered proteins before resonance assignment.     

Crystal structure of the TLDc domain of oxidation resistance protein 2 from zebrafish

The oxidation resistance proteins (OXR) help to protect eukaryotes from reactive oxygen species. The sole C‐terminal domain of the OXR, named TLDc is sufficient to perform this function. However, the mechanism by which oxidation resistance occurs is poorly understood. We present here the crystal structure of the TLDc domain of the oxidation resistance protein 2 from zebrafish. The structure was determined by X‐ray crystallography to atomic resolution (0.97Å) and adopts an overall globular shape. Two antiparallel β‐sheets form a central β‐sandwich, surrounded by two helices and two one‐turn helices. The fold shares low structural similarity to known structures. Proteins 2012. © 2012 Wiley Periodicals, Inc.     

Backbone assignment and secondary structure of the PsbQ protein from Photosystem II

PsbQ is one of the extrinsic proteins situated on the lumenal surface of photosystem II (PSII) in the higher plants and green algae. Its three-dimensional structure was determined by X-ray crystallography with exception of the residues 14–33. To obtain further details about its structure and potentially its dynamics, we approached the problem by NMR. In this paper we report ¹H, ¹⁵N, and ¹³C NMR assignments for the PsbQ protein. The very challenging oligo-proline stretches could be assigned using ¹³C-detected NMR experiments that enabled the assignments of twelve out of the thirteen proline residues of PsbQ. The identification of PsbQ secondary structure elements on the basis of our NMR data was accomplished with the programs TALOS+, web server CS23D and CS-Rosetta. To obtain additional secondary structure information, three-bond H_N-H_α J-coupling constants and deviation of experimental ¹³C_α and ¹³C_β chemical shifts from random coil values were determined. The resulting “consensus” secondary structure of PsbQ compares very well with the resolved regions of the published X-ray crystallographic structure and gives a first estimate of the structure of the “missing link” (i.e. residues 14–33), which will serve as the basis for the further investigation of the structure, dynamics and interactions.     

Structure of the Cdt1 C‐terminal domain: Conservation of the winged helix fold in replication licensing factors

In eukaryotic replication licensing, Cdt1 plays a key role by recruiting the MCM2‐7 complex onto the origin of chromosome. The C‐terminal domain of mouse Cdt1 (mCdt1C), the most conserved region in Cdt1, is essential for licensing and directly interacts with the MCM2‐7 complex. We have determined the structures of mCdt1CS (mCdt1C_small; residues 452 to 557) and mCdt1CL (mCdt1C_large; residues 420 to 557) using X‐ray crystallography and solution NMR spectroscopy, respectively. While the N‐terminal 31 residues of mCdt1CL form a flexible loop with a short helix near the middle, the rest of mCdt1C folds into a winged helix structure. Together with the middle domain of mouse Cdt1 (mCdt1M, residues 172–368), this study reveals that Cdt1 is formed with a tandem repeat of the winged helix domain. The winged helix fold is also conserved in other licensing factors including archaeal ORC and Cdc6, which supports an idea that these replication initiators may have evolved from a common ancestor. Based on the structure of mCdt1C, in conjunction with the biochemical analysis, we propose a binding site for the MCM complex within the mCdt1C.     

Structural and dynamics characterization of norovirus protease

Norovirus protease is an essential enzyme for proteolytic maturation of norovirus nonstructural proteins and has been implicated as a potential target for antiviral drug development. Although X‐ray structural studies of the protease give us wealth of structural information including interactions of the protease with its substrate and dimeric overall structure, the role of protein dynamics in the substrate recognition and the biological relevance of the protease dimer remain unclear. Here we determined the solution NMR structure of the 3C‐like protease from Norwalk virus (NV 3CLpro), a prototype strain of norovirus, and analyzed its backbone dynamics and hydrodynamic behavior in solution. ¹⁵N spin relaxation and analytical ultracentrifugation analyses demonstrate that NV 3CLpro is predominantly a monomer in solution. Solution structure of NV 3CLpro shows significant structural variation in C‐terminal domain compared with crystal structures and among lower energy structure ensembles. Also, ¹⁵N spin relaxation and Carr–Purcell–Meiboom–Gill (CPMG)‐based relaxation dispersion analyses reveal the dynamic properties of residues in the C‐terminal domain over a wide range of timescales. In particular, the long loop spanning residues T123–G133 show fast motion (ps‐ns), and the residues in the bII–cII region forming the large hydrophobic pocket (S2 site) undergo conformational exchanges on slower timescales (μs–ms), suggesting their important role in substrate recognition.     

Structure of a glycoside hydrolase family 50 enzyme from a subfamily that is enriched in human gut microbiome bacteroidetes

The polysaccharide utilization locus in Bacteroides plebeius that confers the ability to catabolize porphyran contains a putative GH50 β‐agarase (BACPLE_01683, BpGH50). BpGH50 did not show any clear activity on agarose or on the related algal galactans porphyran and carrageenan. However, the 1.4 Å resolution X‐ray crystal structure of BpGH50 confirmed its possession of the core (α/β)₈ barrel fold found in GH50 enzymes as well as the structural conservation of the catalytic residues and some substrate binding residues. Examination of the structure supports assignment of this protein as a β‐galactosidase but suggests that it may utilize a different, possibly hybrid, algal galactan substrate. Proteins 2016; 85:182–187. © 2016 Wiley Periodicals, Inc.     

Structural analysis of nested neutralizing and non‐neutralizing B cell epitopes on ricin toxin's enzymatic subunit

In this report, we describe the X‐ray crystal structures of two single domain camelid antibodies (V_HH), F5 and F8, each in complex with ricin toxin's enzymatic subunit (RTA). F5 has potent toxin‐neutralizing activity, while F8 has weak neutralizing activity. F5 buried a total of 1760 Ų in complex with RTA and made contact with three prominent secondary structural elements: α‐helix B (Residues 98–106), β‐strand h (Residues 113–117), and the C‐terminus of α‐helix D (Residues 154–156). F8 buried 1103 Ų in complex with RTA that was centered primarily on β‐strand h. As such, the structural epitope of F8 is essentially nested within that of F5. All three of the F5 complementarity determining regions CDRs were involved in RTA contact, whereas F8 interactions were almost entirely mediated by CDR3, which essentially formed a seventh β‐strand within RTA's centrally located β‐sheet. A comparison of the two structures reported here to several previously reported (RTA‐V_HH) structures identifies putative contact sites on RTA, particularly α‐helix B, associated with potent toxin‐neutralizing activity. This information has implications for rational design of RTA‐based subunit vaccines for biodefense. Proteins 2016; 84:1162–1172. © 2016 Wiley Periodicals, Inc.     

A comparative analysis of the equilibrium dynamics of a designed protein inferred from NMR,X‐ray,and computations

A detailed analysis of high‐resolution structural data and computationally predicted dynamics was carried out for a designed sugar‐binding protein. The mean‐square deviations in the positions of residues derived from nuclear magnetic resonance (NMR) models and those inferred from X‐ray crystallographic B‐factors for two different crystal forms were compared with the predictions based on the Gaussian Network Model (GNM) and the results from molecular dynamics (MD) simulations. GNM systematically yielded a higher correlation than MD, with experimental data, suggesting that the lack of atomistic details in the coarse‐grained GNM is more than compensated for by the mathematically exact evaluation of fluctuations using the native contacts topology. Evidence is provided that particular loop motions are curtailed by intermolecular contacts in the crystal environment causing a discrepancy between theory and experiments. Interestingly, the information conveyed by X‐ray crystallography becomes more consistent with NMR models and computational predictions when ensembles of X‐ray models are considered. Less precise (broadly distributed) ensembles indeed appear to describe the accessible conformational space under native state conditions better than B‐factors. Our results highlight the importance of using multiple conformations obtained by alternative experimental methods, and analyzing results from both coarse‐grained models and atomic simulations, for accurate assessment of motions accessible to proteins under native state conditions. Proteins 2009. © 2009 Wiley‐Liss, Inc.     

Backbone conformations and side chain flexibility of two somatostatin mimics investigated by molecular dynamics simulations

Molecular dynamics simulations with two designed somatostatin mimics, SOM230 and SMS 201‐995, were performed in explicit water for a total aggregated time of 208 ns. Analysis of the runs with SOM230 revealed the presence of two clusters of conformations. Strikingly, the two sampled conformers correspond to the two main X‐ray structures in the asymmetric unit of SMS 201‐995. Structural comparison between the residues of SOM230 and SMS 201‐995 provides an explanation for the high binding affinity of SOM230 to four of five somatostatin receptors. Similarly, cluster analysis of the simulations with SMS 201‐995 shows that the backbone of the peptide interconverts between its two main crystallographic conformers. The conformations of SMS 201‐995 sampled in the two clusters violated two different sets of NOE distance constraints in agreement with a previous NMR study. Differences in side chain fluctuations between SOM230 and SMS 201‐995 observed in the simulations may contribute to the relatively higher binding affinity of SOM230 to most somatostatin receptors. Proteins 2009. © 2008 Wiley‐Liss, Inc.     

Solution structure and dynamics of the single-chain hepatitis C virus NS3 protease NS4A cofactor complex

The backbone assignments, secondary structure, topology, and dynamics of the single-chain hepatitis C virus NS3 protease NS4A cofactor complex have been determined by NMR spectroscopy. Residues I34 to S181 of NS3 and the central three residues of the NS4A cofactor were assigned and the secondary structure was verified for these residues. In several X-ray structures of NS4A-bound NS3 protease, residues 1 to 28 are stabilized by crystal packing, which allows for the formation of the A0 strand and alpha0 helix. In solution, these N-terminal residues are largely unassigned and no evidence of a well-structured A0 strand or alpha0 helix was detected. NOEs between residues in the E1-F1 loop (containing D81) and the alpha1 helix (containing H57) together with the detection of a D81-H57 hydrogen bond indicate that in solution the catalytic triad (D81, H57, S139) of the protease is better ordered in the presence of the NS4A cofactor. This is consistent with the earlier crystallographic results and may explain the observed increase in catalytic activity of the enzyme due to NS4A binding. A model-free analysis of our relaxation data indicates substantial exchange rates for residues V51-D81, which comprise the upper part of the N-terminal beta-barrel. A comparison of chemical-shift differences between NS3 protease and the NS3 protease-NS4A complex shows extensive chemical-shift changes for residues V51-D81 indicating that non-local structural changes occur upon NS4A binding to the NS3 protease that are propagated well beyond the protease-cofactor interaction site. This is consistent with crystallographic data that reveal large structural rearrangements of the strand and loop regions formed by residues V51-D81 as a result of NS4A binding. The coincidence of large exchange rates for the NS3 protease-NS4A complex with chemical-shift differences due to NS4A binding suggests that residues V51-D81 of the NS3 protease NS4A complex are in slow exchange with a NS4A-free conformation of NS3 protease.     

The 1.49 A resolution crystal structure of PsbQ from photosystem II of Spinacia oleracea reveals a PPII structure in the N-terminal region

We report the high-resolution structure of the spinach PsbQ protein, one of the main extrinsic proteins of higher plant photosystem II (PSII). The crystal structure shows that there are two well-defined regions in PsbQ, the C-terminal region (residues 46-149) folded as a four helix up-down bundle and the N-terminal region (residues 1-45) that is loosely packed. This structure provides, for the first time, insights into the crucial N-terminal region. First, two parallel beta-strands cross spatially, joining the beginning and the end of the N-terminal region of PsbQ. Secondly, the residues Pro9-Pro10-Pro11-Pro12 form a left-handed helix (or a polyproline type II (PPII) structure), which is stabilized by hydrogen bonds between the Pro peptide carbonyl groups and solvent water molecules. Thirdly, residues 14-33 are not visible in the electron density map, suggesting that this loop might be very flexible and presumably extended when PsbQ is free in solution. On the basis of the essential role of the N-terminal region of PsbQ in binding to PSII, we propose that both the PPII structure and the missing loop are key secondary structure elements in the recognition of specific protein-protein interactions between PsbQ and other oxygen-evolving complex extrinsic and/or intrinsic proteins of PSII. In addition, the PsbQ crystal coordinates two zinc ions, one of them is proposed to have a physiological role in higher plants, on the basis of the full conservation of the ligand protein residues in the sequence subfamily.     

Exploring the dynamic information content of a protein NMR structure: Comparison of a molecular dynamics simulation with the NMR and X‐ray structures of Escherichia coli ribonuclease HI

The multiconformer nature of solution nuclear magnetic resonance (NMR) structures of proteins results from the effects of intramolecular dynamics, spin diffusion and an uneven distribution of structural restraints throughout the molecule. A delineation of the former from the latter two contributions is attempted in this work for an ensemble of 15 NMR structures of the protein Escherichia coli ribonuclease HI (RNase HI). Exploration of the dynamic information content of the NMR ensemble is carried out through correlation with data from two crystal structures and a 1.7‐ns molecular dynamics (MD) trajectory of RNase HI in explicit solvent. Assessment of the consistency of the crystal and mean MD structures with nuclear Overhauser effect (NOE) data showed that the NMR ensemble is overall more compatible with the high‐resolution (1.48 Å) crystal structure than with either the lower‐resolution (2.05 Å) crystal structure or the MD simulation. Furthermore, the NMR ensemble is found to span more conformational space than the MD simulation for both the backbone and the sidechains of RNase HI. Nonetheless, the backbone conformational variability of both the NMR ensemble and the simulation is especially consistent with NMR relaxation measurements of two loop regions that are putative sites of substrate recognition. Plausible side‐chain dynamic information is extracted from the NMR ensemble on the basis of (i) rotamericity and syn‐pentane character of variable torsion angles, (ii) comparison of the magnitude of atomic mean‐square fluctuations (msf) with those deduced from crystallographic thermal factors, and (iii) comparison of torsion angle conformational behavior in the NMR ensemble and the simulation. Several heterogeneous torsion angles, while adopting non‐rotameric/syn‐pentane conformations in the NMR ensemble, exist in a unique conformation in the simulation and display low X‐ray thermal factors. These torsions are identified as sites whose variability is likely to be an artifact of the NMR structure determination procedure. A number of other torsions show a close correspondence between the conformations sampled in the NMR and MD ensembles, as well as significant correlations among crystallographic thermal factors and atomic msf calculated from the NMR ensemble and the simulation. These results indicate that a significant amount of dynamic information is contained in the NMR ensemble. The relevance of the present findings for the biological function of RNase HI, protein recognition studies, and previous investigations of the motional content of protein NMR structures are discussed. Proteins 1999;36:87–110. © 1999 Wiley‐Liss, Inc.     

Crystal structure of the sensor domain of BaeS from Serratia marcescens FS14

The sensor histidine kinases of two‐component signal‐transduction systems (TCSs) are essential for bacteria to adapt to variable environmental conditions. The two‐component regulatory system BaeS/R increases multidrug and metal resistance in Salmonella and Escherichia coli. In this study, we report the X‐ray structure of the periplasmic sensor domain of BaeS from Serratia marcescens FS14. The BaeS sensor domain (34–160) adopts a mixed α/β‐fold containing a central four‐stranded antiparallel β‐sheet flanked by a long N‐terminal α‐helix and additional loops and a short C‐terminal α‐helix on each side. Structural comparisons revealed that it belongs to the PDC family with a remarkable difference in the orientation of the helix α2. In the BaeS sensor domain, this helix is situated perpendicular to the long helix α1 and holds helix α1 in the middle with the beta sheet, whereas in other PDC domains, helix α2 is parallel to helix α1. Because the helices α1 and α2 is involved in the dimeric interface, this difference implies that BaeS uses a different dimeric interface compared with other PDC domains. Proteins 2017; 85:1784–1790. © 2017 Wiley Periodicals, Inc.     

Structural features of cholesteryl ester transfer protein: A molecular dynamics simulation study

Cholesteryl ester transfer protein (CETP) mediates the net transfer of cholesteryl esters (CEs) from atheroprotective high‐density lipoproteins (HDLs) to atherogenic low‐density lipoproteins (LDLs) or very‐low‐density lipoproteins (VLDLs). Inhibition of CETP raises HDL cholesterol (good cholesterol) levels and reduces LDL cholesterol (bad cholesterol) levels, making it a promising drug target for the prevention and treatment of coronary heart disease. Although the crystal structure of CETP has been determined, the molecular mechanism mediating CEs transfer is still unknown, even the structural features of CETP in a physiological environment remain elusive. We performed molecular dynamics simulations to explore the structural features of CETP in an aqueous solution. Results show that the distal portion flexibility of N‐terminal β‐barrel domain is considerably greater in solution than in crystal; conversely, the flexibility of helix X is slightly less. During the simulations the distal end of C‐terminal β‐barrel domain expanded while the hydrophilic surface increasing more than the hydrophobic surface. In addition, a new surface pore was generated in this domain. This surface pore and all cavities in CETP are stable. These results suggest that the formation of a continuous tunnel within CETP by connecting cavities is permitted in solution. Proteins 2013. © 2012 Wiley Periodicals, Inc.     

C‐terminal β‐strand swapping in a consensus‐derived fibronectin Type III scaffold

The crystal structures of six different fibronectin Type III consensus‐derived Tencon domains, whose solution properties exhibit no, to various degrees of, aggregation according to SEC, have been determined. The structures of the five variants showing aggregation reveal 3D domain swapped dimers. In all five cases, the swapping involves the C‐terminal β‐strand resulting in the formation of Tencon dimers in which the target‐binding surface is blocked. All of the variants differ in sequence in the FG loop, which is the hinge loop in the β‐strand‐swapped dimers. The six tencon variants have between 0 and 5 residues inserted between positions 77 and 78 in the FG loop. Analysis of the structures suggests that a non‐glycine residue at position 77 and insertions of <4 residues may destabilize the β‐turn in the FG loop promoting β‐strand swapping. Swapped dimers with an odd number of inserted residues may be less stable, particularly if they contain proline residues, because they cannot form perfect β‐bridges in the FG regions that link the swapped dimers. The Tencon β‐swapped variants with the longest FG sequences are observed to form higher order hexameric or helical oligomeric structures in the crystal correlating well with the aggregation properties of these domains observed in solution. Understanding the structural basis for domain‐swapped dimerization and oligomerization will support engineering efforts of the Tencon domain to produce variants with desired biophysical properties. Proteins 2014; 82:1359–1369. © 2013 Wiley Periodicals, Inc.     

The effect of calcium on the conformation of cobalamin transporter BtuB

BtuB is a β‐barrel membrane protein that facilitates transport of cobalamin (vitamin B12) from the extracellular medium across the outer membrane of Escherichia coli. It is thought that binding of B12 to BtuB alters the conformation of its periplasm‐exposed N‐terminal residues (the TonB box), which enables subsequent binding of a TonB protein and leads to eventual uptake of B12 into the cytoplasm. Structural studies determined the location of the B12 binding site at the top of the BtuB's β‐barrel, surrounded by extracellular loops. However, the structure of the loops was found to depend on the method used to obtain the protein crystals, which—among other factors—differed in calcium concentration. Experimentally, calcium concentration was found to modulate the binding of the B12 substrate to BtuB. In this study, we investigate the effect of calcium ions on the conformation of the extracellular loops of BtuB and their possible role in B12 binding. Using all‐atom molecular dynamics, we simulate conformational fluctuations of several X‐ray structures of BtuB in the presence and absence of calcium ions. These simulations demonstrate that calcium ions can stabilize the conformation of loops 3–4, 5–6, and 15–16, and thereby prevent occlusion of the binding site. Furthermore, binding of calcium ions to extracellular loops of BtuB was found to enhance correlated motions in the BtuB structure, which is expected to promote signal transduction. Finally, we characterize conformation dynamics of the TonB box in different X‐ray structures and find an interesting correlation between the stability of the TonB box structure and calcium binding. Proteins 2010. © 2009 Wiley‐Liss, Inc.     

Disorder and order in unfolded and disordered peptides and proteins: A view derived from tripeptide conformational analysis. I. Tripeptides with long and predominantly hydrophobic side chains

We performed a conformational analysis of the central residues of three tripeptides glycyl‐L ‐isoleucyl‐glycine (GIG), glycyl‐L ‐tyrosyl‐glycine (GYG) and glycyl‐L ‐arginyl‐glycine (GRG) in aqueous solution, based on a global analysis of amide I′ band profiles and NMR J‐coupling constants. The results are compared with recently reported distributions of GVG, GFG and GEG. For GIG and GYG, we found that even though the polyproline II (pPII) fraction is below 0.5, it is still the most populated conformation, whereas GVG and GFG show both a larger β‐strand fraction. For GRG, we observed a clear dominance of pPII over β‐strand, reminiscent of observations for GEG and GKG. This finding indicates that terminal charges on otherwise hydrophobic residue side chains stabilize pPII over β‐strand conformations. For all peptides investigated we found that a variety of compact and turn‐like conformations constitute nearly 20 percent of their conformational distributions. Attempts to analyze our data with a simple two‐state pPII??β model therefore do not yield any satisfactory reproduction of experimental results. A comparison of the obtained GxG ensembles with conformational distributions of GxG segments in truncated coil libraries (helices and sheets omitted) revealed a much larger fraction of type II β_i+2 and type III β like conformations for the latter. Thus, a comparison of conformational distributions of unfolded peptide segments in solution and in coil libraries reveal interesting information on how the interplay between intrinsic propensities of amino acid residues and non‐local interactions in polypeptide chains determine the conformations of loop segments in proteins. Proteins 2013; © 2012 Wiley Periodicals, Inc.     

Crystal structure of Helicobacter pylori MinE,a cell division topological specificity factor

In Gram‐negative bacteria, proper placement of the FtsZ ring, mediated by nucleoid occlusion and the activities of the dynamic oscillating Min proteins MinC, MinD and MinE, is required for correct positioning of the cell division septum. MinE is a topological specificity factor that counters the activity of MinCD division inhibitor at the mid‐cell division site. Its structure consists of an anti‐MinCD domain and a topology specificity domain (TSD). Previous NMR analysis of truncated Escherichia coli MinE showed that the TSD domain contains a long α‐helix and two anti‐parallel β‐strands, which mediate formation of a homodimeric α/β structure. Here we report the crystal structure of full‐length Helicobacter pylori MinE and redefine its TSD based on that structure. The N‐terminal region of the TSD (residues 19–26), previously defined as part of the anti‐MinCD domain, forms a β‐strand (βA) and participates in TSD folding. In addition, H. pylori MinE forms a dimer through the interaction of anti‐parallel βA‐strands. Moreover, we observed serial dimer–dimer interactions within the crystal packing, resulting in the formation of a multimeric structure. We therefore redefine the functional domain of MinE and propose that a multimeric filamentous structure is formed through anti‐parallel β‐strand interactions.     

LacZ β‐galactosidase: Structure and function of an enzyme of historical and molecular biological importance

This review provides an overview of the structure, function, and catalytic mechanism of lacZ β‐galactosidase. The protein played a central role in Jacob and Monod's development of the operon model for the regulation of gene expression. Determination of the crystal structure made it possible to understand why deletion of certain residues toward the amino‐terminus not only caused the full enzyme tetramer to dissociate into dimers but also abolished activity. It was also possible to rationalize α‐complementation, in which addition to the inactive dimers of peptides containing the “missing” N‐terminal residues restored catalytic activity. The enzyme is well known to signal its presence by hydrolyzing X‐gal to produce a blue product. That this reaction takes place in crystals of the protein confirms that the X‐ray structure represents an active conformation. Individual tetramers of β‐galactosidase have been measured to catalyze 38,500 ± 900 reactions per minute. Extensive kinetic, biochemical, mutagenic, and crystallographic analyses have made it possible to develop a presumed mechanism of action. Substrate initially binds near the top of the active site but then moves deeper for reaction. The first catalytic step (called galactosylation) is a nucleophilic displacement by Glu537 to form a covalent bond with galactose. This is initiated by proton donation by Glu461. The second displacement (degalactosylation) by water or an acceptor is initiated by proton abstraction by Glu461. Both of these displacements occur via planar oxocarbenium ion‐like transition states. The acceptor reaction with glucose is important for the formation of allolactose, the natural inducer of the lac operon.