Hydrogen-bonded Secondary Structure Research Articles

Folding of an all-helical Greek-key protein monitored by quenched-flow hydrogen–deuterium exchange and NMR spectroscopy

To advance our understanding of the protein folding process, we use stopped-flow far-ultraviolet (far-UV) circular dichroism and quenched-flow hydrogen-deuterium exchange coupled with nuclear magnetic resonance (NMR) spectroscopy to monitor the formation of hydrogen-bonded secondary structure in the C-terminal domain of the Fas-associated death domain (Fadd-DD). The death domain superfamily fold consists of six α-helices arranged in a Greek-key topology, which is shared by the all-β-sheet immunoglobulin and mixed α/β-plait superfamilies. Fadd-DD is selected as our model death domain protein system because the structure of this protein has been solved by NMR spectroscopy, and both thermodynamic and kinetic analysis indicate it to be a stable, monomeric protein with a rapidly formed hydrophobic core. Stopped-flow far-UV circular dichroism spectroscopy revealed that the folding process was monophasic and the rate is 23.4s(-1). Twenty-two amide hydrogens in the backbone of the helices and two in the backbone of the loops were monitored, and the folding of all six helices was determined to be monophasic with rate constants between 19 and 22s(-1). These results indicate that the formation of secondary structure is largely cooperative and concomitant with the hydrophobic collapse. This study also provides unprecedented insight into the formation of secondary structure within the highly populated Greek-key fold more generally. Additional insights are gained by calculating the exchange rates of 23 residues from equilibrium hydrogen-deuterium exchange experiments. The majority of protected amide protons are found on helices2, 4, and 5, which make up core structural elements of the Greek-key topology.

Structural space of protein–protein interfaces is degenerate, close to complete, and highly connected

At the heart of protein-protein interactions are protein-protein interfaces where the direct physical interactions occur. By developing and applying an efficient structural alignment method, we study the structural similarity of representative protein-protein interfaces involving interactions between dimers. Even without structural similarity between individual monomers that form dimeric complexes, ∼90% of native interfaces have a close structural neighbor with similar backbone C(α) geometry and interfacial contact pattern. About 80% of the interfaces form a dense network, where any two interfaces are structurally related using a transitive set of at most seven intermediate interfaces. The degeneracy of interface space is largely due to the packing of compact, hydrogen-bonded secondary structure elements. This packing generates relatively flat interacting surfaces whose geometries are highly degenerate. Comparative study of artificial and native interfaces argues that the library of protein interfaces is close to complete and comprised of roughly 1,000 distinct interface types. In contrast, the number of possible quaternary structures of dimers is estimated to be about 10(4) times larger; thus, an experimentally determined database of all representative quaternary structures is not likely in the near future. Nevertheless, one could in principle exploit the completeness of protein interfaces to predict most dimeric quaternary structures. Finally, our results provide a structural explanation for the prevalence of promiscuous protein interactions. By side-chain packing adjustments, we illustrate how multiprotein specificity can be attained at a promiscuous interface.

Salt-Specific Stability and Denaturation of a Short Salt-Bridge-Forming α-Helix

The structure of a single alanine-based Ace-AEAAAKEAAAKA-Nme peptide in explicit aqueous electrolyte solutions (NaCl, KCl, NaI, and KF) at large salt concentrations (3-4 M) is investigated using approximately 1 mus molecular dynamics (MD) computer simulations. The peptide displays 71% alpha-helical structure without salt and destabilizes with the addition of NaCl in agreement with experiments of a somewhat longer version. It is mainly stabilized by direct and indirect (" i + 4")EK salt bridges between the Lys and Glu side chains and a concomitant backbone shielding mechanism. NaI is found to be a stronger denaturant than NaCl, while the potassium salts hardly show influence. Investigation of the molecular structures reveals that consistent with recent experiments Na (+) has a much stronger affinity to side chain carboxylates and backbone carbonyls than K (+), thereby weakening salt bridges and secondary structure hydrogen bonds. At the same time, the large I (-) has a considerable affinity to the nonpolar alanine in line with recent observations of a large propensity of I (-) to adsorb to simple hydrophobes, and thereby "assists" Na (+) in its destabilizing action. In the denatured states of the peptide, novel long-lived (10-20 ns) "loop" configurations are observed in which single Na (+) ions and water molecules are hydrogen-bonded to multiple backbone carbonyls. In an attempt to analyze the denaturation behavior within the preferential interaction formalism, we find indeed that for the strongest denaturant, NaI, the protein is least hydrated. Additionally, a possible indication for protein denaturation might be a preferential solvation of the peptide backbone by the destabilizing cosolute (sodium). The mechanisms found in this work may be of general importance to understand salt effects on protein secondary structure stability.

NMR Characterization of a Peptide Model Provides Evidence for Significant Structure in the Unfolded State of the Villin Headpiece Helical Subdomain

The villin headpiece subdomain (HP36) is the smallest naturally occurring protein that folds cooperatively. The protein folds on a microsecond time scale. Its small size and very rapid folding have made it a popular target for biophysical studies of protein folding. Temperature-dependent one-dimensional (1D) NMR studies of the full-length protein together with CD and 1D NMR studies of the 21-residue peptide fragment (HP21) derived from HP36 have shown that there is significant structure in the unfolded state of HP36 and have demonstrated that HP21 is a good model of these interactions. Here, we characterized the model peptide HP21 in detail by two-dimensional NMR. Strongly upfield shifted C(alpha) protons, the magnitude of the 3J(NH,alpha) coupling constants, and the pattern of backbone-backbone and backbone-side chain NOEs indicate that the ensemble of structures populated by HP21 contains alpha-helical structure and native as well as non-native hydrophobic contacts. The hydrogen-bonded secondary structure inferred from the NOEs is, however, not sufficient to confer significant protection against amide H-D exchange. These studies indicate that there is significant secondary structure and hydrophobic clustering in the unfolded state of HP36. The implications for the folding of HP36 are discussed.

Membrane Insertion of a Lipidated Ras Peptide Studied by FTIR, Solid-State NMR, and Neutron Diffraction Spectroscopy

Membrane binding of a doubly lipid modified heptapeptide from the C-terminus of the human N-ras protein was studied by Fourier transform infrared, solid-state NMR, and neutron diffraction spectroscopy. The 16:0 peptide chains insert well into the 1,2-dimyristoyl-sn-glycero-3-phosphocholine phospholipid matrix. This is indicated by a common main phase transition temperature of 21.5 degrees C for both the lipid and peptide chains as revealed by FTIR measurements. Further, (2)H NMR reveals that peptide and lipid chains have approximately the same chain length in the liquid crystalline state. This is achieved by a much lower order parameter of the 16:0 peptide chains compared to the 14:0 phospholipid chains. Finally, proton/deuterium contrast variation of neutron diffraction experiments indicates that peptide chains are localized in the membrane interior analogous to the phospholipid chains. In agreement with this model of peptide chain insertion, the peptide part is localized at the lipid-water interface of the membrane. This is revealed by (1)H nuclear Overhauser enhancement spectra recorded under magic angle spinning conditions. Quantitative cross-peak analysis allows the examination of the average location of the peptide backbone and side chains with respect to the membrane. While the backbone shows the strongest cross-relaxation rates with the phospholipid glycerol, the hydrophobic side chains of the peptide insert deeper into the membrane interior. This is supported by neutron diffraction experiments that reveal a peptide distribution in the lipid-water interface of the membrane. Concurring with these experimental findings, the amide protons of the peptide show strong water exchange as seen in NMR and FTIR measurements. No indications for a hydrogen-bonded secondary structure of the peptide backbone are found. Therefore, membrane binding of the C-terminus of the N-ras protein is mainly due to lipid chain insertion but also supported by interactions between hydrophobic side chains and the lipid membrane. The peptide assumes a mobile and disordered conformation in the membrane. Since the C-terminus of the soluble part of the ras protein is also disordered, we hypothesize that our model for membrane binding of the ras peptide realistically describes the membrane binding of the lipidated C-terminus of the active ras protein.

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Lipophilic Peptide as Novel Building Material of Molecular Sensor

Abstract Lipophilic peptide derivatives 1 - 3 proved to complex with amines in chloroform in 1:1 ratio allowing distinct color change. Peptide 3 as compared with 2 indicated strikingly greater binding affinity, suggesting the importance of subtle modulation in hydrogen-bonded secondary structure of peptide chains in non-polar solvent.

Quench-flow experiments combined with mass spectrometry show apomyoglobin folds through and obligatory intermediate.

Folding of apomyoglobin is characterized by formation of a compact intermediate that contains substantial helicity. To determine whether this intermediate is obligatory or whether the protein can fold directly into the native state via an alternate parallel pathway, we have combined quench-flow hydrogen-exchange pulse labeling techniques with electrospray ionization mass spectrometry. The mass spectra of apomyoglobin obtained at various refolding times suggest that apomyoglobin indeed folds through a single pathway containing an obligatory intermediate with a significant hydrogen-bonded secondary structure content.

Mapping the lifetimes of local opening events in a native state protein.

The rate constants for the processes that lead to local opening and closing of the structures around hydrogen bonds in native proteins have been determined for most of the secondary structure hydrogen bonds in the four-helix protein acyl coenzyme A binding protein. In an analysis that combines these results with the energies of activation of the opening processes and the stability of the local structures, three groups of residues in the protein structure have been identified. In one group, the structures around the hydrogen bonds have frequent openings, every 600 to 1,500 s, and long lifetimes in the open state, around 1 s. In another group of local structures, the local opening is a very rare event that takes place only every 15 to 60 h. For these the lifetime in the open state is also around 1 s. The majority of local structures have lifetimes between 2,000 and 20,000 s and relatively short lifetimes of the open state in the range between 30 and 400 ms. Mapping of these groups of amides to the tertiary structure shows that the openings of the local structures are not cooperative at native conditions, and they rarely if ever lead to global unfolding. The results suggest a mechanism of hydrogen exchange by progressive local openings.

Hydrogen Bonding in Helical Polypeptides from Molecular Dynamics Simulations and Amide Hydrogen Exchange Analysis: Alamethicin and Melittin in Methanol

Molecular dynamics simulations of ion channel peptides alamethicin and melittin, solvated in methanol at 27°C, were run with either regular α-helical starting structures (alamethicin, 1 ns; melittin 500 ps either with or without chloride counterions), or with the x-ray crystal coordinates of alamethicin as a starting structure (1 ns). The hydrogen bond patterns and stabilities were characterized by analysis of the dynamics trajectories with specified hydrogen bond angle and distance criteria, and were compared with hydrogen bond patterns and stabilities previously determined from high-resolution NMR structural analysis and amide hydrogen exchange measurements in methanol. The two alamethicin simulations rapidly converged to a persistent hydrogen bond pattern with a high level of 3 10 hydrogen bonding involving the amide NH's of residues 3, 4, 9, 15, and 18. The 3 10 hydrogen bonds stabilizing amide NH's of residues C-terminal to P2 and P14 were previously proposed to explain their high amide exchange stabilities. The absence, or low levels of 3 10 hydrogen bonds at the N-terminus or for A15 NH, respectively, in the melittin simulations, is also consistent with interpretations from amide exchange analysis. Perturbation of helical hydrogen bonding in the residues before P14 (Aib10-P14, alamethicin; T11-P14, melittin) was characterized in both peptides by variable hydrogen bond patterns that included π and γ hydrogen bonds. The general agreement in hydrogen bond patterns determined in the simulations and from spectroscopic analysis indicates that with suitable conditions (including solvent composition and counterions where required), local hydrogen-bonded secondary structure in helical peptides may be predicted from dynamics simulations from α-helical starting structures. Each peptide, particularly alamethicin, underwent some large amplitude structural fluctuations in which several hydrogen bonds were cooperatively broken. The recovery of the persistent hydrogen bonding patterns after these fluctuations demonstrates the stability of intramolecular hydrogen-bonded secondary structure in methanol (consistent with spectroscopic observations), and is promising for simulations on extended timescales to characterize the nature of the backbone fluctuations that underlie amide exchange from isolated helical polypeptides.

Rapid formation of a molten globule intermediate in refolding of α-lactalbumin

The molten globule state is an intermediate between the native and the fully unfolded states of globular proteins and is purported to be an obligatory on-pathway intermediate of protein folding. The molten globule state of alpha-lactalbumin has been best characterized, but two major issues have yet to be clarified. At which stage of the kinetic refolding is the molten globule state stably organized? And what is the major driving force that stabilizes the molten globule state? We address these questions in this paper. We have investigated the refolding kinetics of alpha-lactalbumin using stopped-flow CD and fluorescence, acrylamide quenching and pulsed hydrogen exchange NMR techniques. A burst-phase intermediate was observed to form within 15 ms. The intermediate was characterized by pronounced, hydrogen-bonded secondary structure, exposure of hydrophobic surfaces and the absence of tertiary structure. Furthermore, the stability of the secondary structure is the same as that in the equilibrium molten globule state. The burst-phase intermediate in alpha-lactalbumin refolding is identical with the molten globule state. Two different models, the hydrophobic collapse model and the secondary-structure coalescence model, of protein folding are discussed on the basis of the present results. The importance of solvent-separated hydrophobic interactions that stabilize the molten globule state is proposed.

Formation of a Molten Globule Intermediate Early in the Kinetic Folding Pathway of Apomyoglobin

Hydrogen exchange pulse labeling and stopped-flow circular dichroism were used to establish that the structure of the earliest detectable intermediate formed during refolding of apomyoglobin corresponds closely to that of a previously characterized equilibrium molten globule. This compact, cooperatively folded intermediate was formed in less than 5 milliseconds and contained stable, hydrogen-bonded secondary structure localized in the A, G, and H helices and part of the B helix. The remainder of the B helix folded on a much slower time scale, followed by the C and E helices and the CD loop. The data indicate that a molten globule intermediate was formed on the kinetic folding pathway.

Hydrogen exchange in native and alcohol forms of ubiquitin.

Ubiquitin adopts a non-native folded structure in 60% methanol solution at low pH. Two-dimensional nuclear magnetic resonance (2D NMR) was used to measure the hydrogen-exchange rates of backbone amide protons of ubiquitin in both native and methanol forms, and to characterize the structure of ubiquitin in the methanol state. Protection factors (the ratios of experimentally determined exchange rates to the rates calculated for an unfolded polypeptide) for protons in the native form of ubiquitin range from less than 10 to greater than 10(5). Most of the protons that are protected from exchange are located in regions of hydrogen-bonded secondary structure. The most strongly protected backbone amide protons are those of residues comprising the hydrophobic core. Hydrogen exchange from ubiquitin in methanol solution was too rapid to measure directly by 2D NMR, so a labeling scheme was employed, in which exchange with solvent occurred while the protein was in methanol solution. Exchange was quenched by dilution with aqueous buffer after the desired labeling time, and proton occupancies were measured by 1H NMR of the native form of the protein. Protection factors for protons in the methanol form of ubiquitin range from 2.6 to 42, with all protected protons located in hydrogen-bonded structure in the native form. Again, the most strongly protected protons are those of residues in the hydrophobic core. Comparison of the patterns of the hydrogen-exchange rates in the native and methanol forms indicates that almost all of the native secondary structure persists in the methanol form, but that it is almost uniformly destabilized by 4-6 kcal/mol.(ABSTRACT TRUNCATED AT 250 WORDS)

Hydrogen bonding in globular proteins

A global census of the hydrogen bonds in 42 X-ray-elucidated proteins was taken and the following demographic trends identified: (1) Most hydrogen bonds are local, i.e. between partners that are close in sequence, the primary exception being hydrogen-bonded ion pairs. (2) Most hydrogen bonds are between backbone atoms in the protein, an average of 68%. (3) All proteins studied have extensive hydrogen-bonded secondary structure, an average of 82%. (4) Almost all backbone hydrogen bonds are within single elements of secondary structure. An approximate rule of thirds applies: slightly more than one-third (37%) form i----i--3 hydrogen bonds, almost one-third (32%) form i----i--4 hydrogen bonds, and slightly less than one-third (26%) reside in paired strands of beta-sheet. The remaining 5% are not wholly within an individual helix, turn or sheet. (5) Side-chain to backbone hydrogen bonds are clustered at helix-capping positions. (6) An extensive network of hydrogen bonds is present in helices. (7) To a close approximation, the total number of hydrogen bonds is a simple function of a protein's helix and sheet content. (8) A unique quantity, termed the reduced number of hydrogen bonds, is defined as the maximum number of hydrogen bonds possible when every donor:acceptor pair is constrained to be 1:1. This quantity scales linearly with chain length, with 0.71 reduced hydrogen bond per residue. Implications of these results for pathways of protein folding are discussed.

Analysis of protein main-chain solvation as a function of secondary structure

We have analysed the hydration of main-chain carbonyl and amide groups in 24 high-resolution well-refined protein structures as a function of the secondary structure in which these polar groups occur. We find that main-chain atoms in β-sheets are as hydrated as those in α-helices, with most interactions involving “free” amide and carbonyl groups that do not participate in secondary structure hydrogen bonds. The distributions of water molecules around these non-bonded carbonyl groups reflect specific steric interactions due to the local secondary structure. Approximately 20% and 4%, respectively of bonded carbonyl and amide groups interact with solvent. These include interactions with carbonyl groups on the exposed faces of α-helices that have been correlated previously with bending of the helix. Water molecules interacting with α-helices occur mainly at the amino and carbonyl termini of the helices, in which case the solvent sites maintain the hydrogen bonding by bridging between residues i and i−3 or i−4 at the amino terminus and between i and i+3 or i+4 at the carbonyl terminus. We also see a number of solvent-mediated N cap and C cap interactions. The water molecules interacting with β-sheets occur mainly at the edges, in which case they extend the sheet structure, or at the ends of strands, in which case they extend the β-ladder. In summary, the solvent networks appear to extend the hydrogen-bonding structure of the secondary structures. In β-turns, which usually occur at the surface of a protein, exposed amide and carbonyl groups are often hydrated, especially close to glycine residues. Occasionally water molecules form a bridge between residues i and i+3 in the turn and this may provide extra stabilization.

Proton NMR study of the solution properties of the polypeptide neurotoxin I from the sea anemone Stichodactyla helianthus

The solution properties of the polypeptide neurotoxin I from the sea anemone Stichodactyla helianthus (Sh I) have been investigated by high-resolution 1H nuclear magnetic resonance (NMR) spectroscopy at 300 MHz. The pH dependence of the spectra has been examined over the range 1.1-12.2 at 27 degrees C. Individual pKa values have been obtained for the alpha-ammonium group of Ala-1 (8.6) and the side chains of Glu-8 (3.7), Tyr-36 (10.9), and Tyr-37 (10.8). For the remaining seven carboxyl groups in the molecule (from five Asp, Glu-31, and the C-terminus), four pKa values, viz., 2.8, 3.5, 4.1 and 6.4, can be clearly identified. The five Lys residues titrate in the range 10.5-11, but individual pKa values could not be obtained because of peak overlap. Conformational changes associated with the protonation of carboxylates occur below pH 4, while in the alkaline pH range major unfolding occurs above pH 10. The molecule also unfolds at elevated temperatures, having a transition temperature of ca. 55 degrees C at pH 5.25. Exchange of the backbone amide protons has been monitored at various values of pH and temperature in the ranges pH 4-5 and 12-27 degrees C. Up to 18 slowly exchanging amides are observed, consistent with the existence of a core of hydrogen-bonded secondary structure, most probably beta-sheet.(ABSTRACT TRUNCATED AT 250 WORDS)

The enzymatic activity of proteinase K is controlled by calcium.

The fungal proteinase K (EC 3.4.21.14) is a very potent unusually stable member of the subtilisin family. Its X-ray structure determined at 0.15-nm resolution shows two bound Ca2+ ions. Ca1 is in near-ideal pentagonal bipyramidal configuration with Asp200 carboxylate and Pro175 peptide C = O in an apical, and Val177 peptide C = O and four water molecules in an equatorial position, whereas Ca2 displays incomplete octahedral coordination with the carboxylate of Asp260, the peptide C = O of Val16 and the two water molecules. Scatchard analysis of the titration of Ca2+-free proteinase K with Ca2+ yields a single dissociation constant (7.6 +/- 2.5) x 10(-8) M associated with the tightly bound Ca1 whereas Ca2 is so weakly bound that it cannot be titrated. If proteinase K is depleted of Ca2+ by treatment with EDTA, followed by gel filtration, its enzymatic activity drops within 6 h to 20% of its original value, without autolysis. Addition of excess Ca2+ immediately raises the residual activity to 28%, but full activity is not achieved. Removal of Ca2+ triggers a conformational change of the substrate recognition site because there is a direct connection, via secondary structure hydrogen bonds, between the Ca1 binding site and the substrate-recognition site. This is indicated further by circular dichroism and fluorescence-spectroscopic data, and by reversed-phase FPLC, carried out in the presence and absence of Ca2+, but the overall structure of the enzyme is not affected. Depletion of Ca2+ also influences binding of longer peptide inhibitors of the chloromethane type, it increases the rate of autolysis after about 48 h, it reduces the thermal stability (measured by activity tests from 65 degrees C to 46 degrees C), and it enhances the deactivation by 8 M urea which inactivates to only 65%, whereas sodium dodecyl sulfate totally inactivates at a concentration of 12.5%.

Nucleotide sequence of the M segment of Germiston virus: Comparison of the M gene product of several bunyaviruses

The complete nucleotide sequence of the M RNA segment of Germiston bunyavirus was determined from plasmids containing overlapping M cDNA inserts. The M segment is 4534 nucleotides long and contains a 50-base-long inverted terminal repeat which can form a stable hydrogen-bonded secondary structure with a ΔG of −45.8 kcal/mol. The RNA molecule complementary to viral RNA contains a single large open reading frame that encodes a 1437 amino acid-long protein with hydrophobic amino and carboxy terminal regions, which could represent signal and anchor sequences, respectively. It is presumed that this gene product is the polyprotein precursor to glycoproteins G1 and G2 and to the nonstructural polypeptide NS M. The nucleotide and amino acid sequences of the M RNA of Bunyamwera virus (prototype of the serogroup) and snowshoe hare and La Crosse viruses (California serogroup) (Lees et al., 1986; Eshita and Bishop, 1984; Grady et al., 1987) were compared to those of Germiston virus. An overall amino acid sequence homology of 44% was found between Germiston and snowshoe hare viruses and of 61 % between Germiston and Bunyamwera viruses. Most of the cysteines, three out of seven of the potential glycosylation sites, as well as the N and C terminal hydrophobic domains, are conserved between the four viruses.

Structure of ubiquitin refined at 1.8Åresolution

The crystal structure of human erythrocytic ubiquitin has been refined at 1.8Åresolution using a restrained least-squares procedure. The crystallographic R-factor for the final model is 0.176. Bond lengths and bond angles in the molecule have root-mean-square deviations from ideal values of 0.016Åand 1.5 °, respectively. A total of 58 water molecules per molecule of ubiquitin are included in the final model. The last four residues in the molecule appear to have partial occupancy or large thermal motion. The overall structure of ubiquitin is extremely compact and tightly hydrogen-bonded; approximately 87% of the polypeptide chain is involved in hydrogen-bonded secondary structure. Prominent secondary structural features include three and one-half turns of α-helix, a short piece of 3 10-helix, a mixed β-sheet that contains five strands, and seven reverse turns. There is a marked hydrophobic core formed between the β-sheet and α-helix. The molecule features a number of unusual secondary structural features, including a parallel Gl β-bulge, two reverse Asx turns, and a symmetrical hydrogen-bonding region that involves the two helices and two of the reverse turns.

The kinetics of bovine growth hormone folding are consistent with a framework model.

The framework model of protein folding requires the hydrogen-bonded secondary structure to be formed early in folding (i.e. the formation of secondary structure precedes the tertiary structure) (Kim, P. S., and Baldwin, R. L. (1982) Annu. Rev. Biochem. 51, 459-489). To test the framework model directly the kinetics of bovine growth hormone (bGH) folding were compared utilizing two methods of detection, one that measures the secondary structure (far ultraviolet circular dichroism) and another that measures the tertiary structure (near ultraviolet absorbance). The results demonstrate that, under identical folding conditions, the kinetics observed by far ultraviolet circular dichroism are faster than those observed by ultraviolet absorption. The faster kinetics observed by circular dichroism indicate the existence of a helix-containing intermediate which is consistent with the framework model. The effect of protein concentration and denaturant concentration on the kinetics of refolding were studied. The rate of refolding measured by absorbance and circular dichroism was dependent on protein concentration. The protein concentration dependence on refolding is due to the transient formation of an associated intermediate. The concentration dependence of folding is taken as evidence that folding is a sequential process with partially folded monomers responsible for the observed association effect. At dilute protein concentrations the refolding can be studied independent of the association phenomena. The growth hormones utilized in this study were derived from Escherichia coli through recombinant DNA technology and from bovine pituitaries. The pituitary-derived bGH has been shown to be heterogeneous at the NH2 terminus (Lorenson, M. F., and Ellis, S. (1975) Endocrinology 96, 833-838), whereas the recombinant DNA-derived bGH contains a single NH2 terminus. No differences in the folding kinetics between the recombinant DNA and pituitary derived-bGH were observed. It is concluded that the heterogeneity of the NH2 terminus of growth hormone obtained from bovine pituitaries does not affect the observed in vitro folding kinetics.