The Applicability of Amide Proton Transfer Imaging in the Nervous System: Focus on Hypoxic-Ischemic Encephalopathy in the Neonate

In recent years, magnetic resonance imaging (MRI) has become more widely used in neonatal hypoxic-ischemic encephalopathy (HIE), involving, for example, evaluation of cerebral edema, white matter fiber bundle tracking, cerebral perfusion status, and assessment of brain metabolites. MRI has many imaging modalities. However, its application for assessing changes in the internal environment at the tissue and cellular level after hypoxia–ischemia remains a challenge and is currently the focus of intense research. Based on the exchange between amide protons of proteins and polypeptides and free water protons, amide proton transfer (APT) imaging can display changes in pH and protein concentrations in vivo. This paper is a review of the principles of APT imaging, with a focus on the potential application of APT imaging for neonatal HIE.     

Magnetization Transfer Prepared Gradient Echo MRI for CEST Imaging

Chemical exchange saturation transfer (CEST) is an emerging MRI contrast mechanism that is capable of noninvasively imaging dilute CEST agents and local properties such as pH and temperature, augmenting the routine MRI methods. However, the routine CEST MRI includes a long RF saturation pulse followed by fast image readout, which is associated with high specific absorption rate and limited spatial resolution. In addition, echo planar imaging (EPI)-based fast image readout is prone to image distortion, particularly severe at high field. To address these limitations, we evaluated magnetization transfer (MT) prepared gradient echo (GRE) MRI for CEST imaging. We proved the feasibility using numerical simulations and experiments in vitro and in vivo. Then we optimized the sequence by serially evaluating the effects of the number of saturation steps, MT saturation power (B1), GRE readout flip angle (FA), and repetition time (TR) upon the CEST MRI, and further demonstrated the endogenous amide proton CEST imaging in rats brains (n = 5) that underwent permanent middle cerebral artery occlusion. The CEST images can identify ischemic lesions in the first 3 hours after occlusion. In summary, our study demonstrated that the readily available MT-prepared GRE MRI, if optimized, is CEST-sensitive and remains promising for translational CEST imaging.     

The internal cavities of pike alpha-parvalbumin probably contain water

The kinetics of hydrogen exchange of pike a-parvalbumin was investigated using the method of infrared spectroscopy (sensitive to the amide hydrogen atoms in the peptide) and radioisotope method (sensitive to all labile hydrogen atoms). Ultraslow exchangeable hydrogen atoms were found to be substantially less in the first case than in the second one. Taking into account that the internal cavities in the parvalbumin are formed by hydrophobic amino acid residues, devoid of labile hydrogen atoms, it is possible to make the most appropriate assumption, namely, these cavities contain water molecules, hydrogen atoms of which are ultraslow exchangeable.     

The internal cavities of pike α-parvalbumin probably contain water

The kinetics of hydrogen exchange of pike α-parvalbumin was investigated using the method of infrared spectroscopy (sensitive to the amide hydrogen atoms in the peptide) and radioisotope method (sensitive to all labile hydrogen atoms). Ultraslow-exchangeable hydrogen atoms were found to be substantially fewer in the former case than in the latter. Taking into account that the internal cavities in the parvalbumin are formed by hydrophobic amino acid residues, devoid of labile hydrogen atoms, it is possible to make the most appropriate assumption, namely, these cavities contain water molecules, the hydrogen atoms of which are ultraslow-exchangeable.     

Imaging in vivo extracellular pH with a single paramagnetic chemical exchange saturation transfer magnetic resonance imaging contrast agent

The measurement of extracellular pH (pHe) has potential utility for cancer diagnoses and for assessing the therapeutic effects of pH-dependent therapies. A single magnetic resonance imaging (MRI) contrast agent that is detected through paramagnetic chemical exchange saturation transfer (PARACEST) was designed to measure tumor pH(e) throughout the range of physiologic pH and with magnetic resonance saturation powers that are not harmful to a mouse model of cancer. The chemical characterization and modeling of the contrast agent Yb(3+)-1,4,7,10-tetraazacyclododecane-1,4,7-triacetic acid,10-o-aminoanilide (Yb-DO3A-oAA) suggested that the aryl amine of the agent forms an intramolecular hydrogen bond with a proximal carboxylate ligand, which was essential for generating a practical chemical exchange saturation transfer (CEST) effect from an amine. A ratio of CEST effects from the aryl amine and amide was linearly correlated with pH throughout the physiologic pH range. The pH calibration was used to produce a parametric pH map of a subcutaneous flank tumor on a mouse model of MCF-7 mammary carcinoma. Although refinements in the in vivo CEST MRI methodology may improve the accuracy of pHe measurements, this study demonstrated that the PARACEST contrast agent can be used to generate parametric pH maps of in vivo tumors with saturation power levels that are not harmful to a mouse model of cancer.     

TmDOTA-tetraglycinate encapsulated liposomes as pH-sensitive LipoCEST agents

Lanthanide DOTA-tetraglycinate (LnDOTA-(gly)₄ ⁻) complexes contain four magnetically equivalent amide protons that exchange with protons of bulk water. The rate of this base catalyzed exchange process has been measured using chemical exchange saturation transfer (CEST) NMR techniques as a function of solution pH for various paramagnetic LnDOTA-(gly)₄ ⁻ complexes to evaluate the effects of lanthanide ion size on this process. Complexes with Tb(III), Dy(III), Tm(III) and Yb(III) were chosen because these ions induce large hyperfine shifts in all ligand protons, including the exchanging amide protons. The magnitude of the amide proton CEST exchange signal differed for the four paramagnetic complexes in order, Yb>Tm>Tb>Dy. Although the Dy(III) complex showed the largest hyperfine shift as expected, the combination of favorable chemical shift and amide proton CEST linewidth in the Tm(III) complex was deemed most favorable for future in vivo applications where tissue magnetization effects can interfere. TmDOTA-(gly)₄ ⁻ at various concentrations was encapsulated in the core interior of liposomes to yield lipoCEST particles for molecular imaging. The resulting nanoparticles showed less than 1% leakage of the agent from the interior over a range of temperatures and pH. The pH versus amide proton CEST curves differed for the free versus encapsulated agents over the acidic pH regions, consistent with a lower proton permeability across the liposomal bilayer for the encapsulated agent. Nevertheless, the resulting lipoCEST nanoparticles amplify the CEST sensitivity by a factor of ∼10⁴ compared to the free, un-encapsulated agent. Such pH sensitive nano-probes could prove useful for pH mapping of liposomes targeted to tumors.     

Nuclear magnetic resonance studies of the internal dynamics in Apo, (Cd2+)1 and (Ca2+)2 calbindin D9k. The rates of amide proton exchange with solvent.

The backbone dynamics of the EF-hand Ca(2+)-binding protein, calbindin D9k, has been investigated in the apo, (Cd2+)1 and (Ca2+)2 states by measuring the rate constants for amide proton exchange with solvent. 15N-1H correlation spectroscopy was utilized to follow direct 1H-->2H exchange of the slowly exchanging amide protons and to follow indirect proton exchange via saturation transfer from water to the rapidly exchanging amide protons. Plots of experimental rate constants versus intrinsic rate constants have been analyzed to give qualitative insight into the opening modes of the protein that lead to exchange. These results have been interpreted within the context of a progressive unfolding model, wherein hydrophobic interactions and metal chelation serve to anchor portions of the protein, thereby damping fluctuations and retarding amide proton exchange. The addition of Ca2+ or Cd2+ was found to retard the exchange of many amide protons observed to be in hydrogen-bonding environments in the crystal structure of the (Ca2+)2 state, but not of those amide protons that were not involved in hydrogen bonds. The largest changes in rate constant occur for residues in the ion-binding loops, with substantial effects also found for the adjacent residues in helices I, II and III, but not helix IV. The results are consistent with a reorganization of the hydrogen-bonding networks in the metal ion-binding loops, accompanied by a change in the conformation of helix IV, as metal ions are chelated. Further analysis of the results obtained for the three states of metal occupancy provides insight into the nature of the changes in conformational fluctuations induced by ion binding.     

Hydrogen exchange of individual amide protons in the F helix of cyanometmyoglobin

Hydrogen exchange of the individual amide protons of alanine-90 (F5), glutamine-91 (F6), serine-92 (F7), and histidine-93 (F8) residues in cyanometmyoglobin of sperm whale has been studied by 1H nuclear magnetic resonance spectroscopy at 360 MHz. The amide proton resonance of F5, F6, and F7 have been assigned by use of the selective nuclear Overhauser effect between the consecutive amide protons. At pH 6.8, and in the temperature range of 5-20 degrees C, these protons show a 10(4)-fold retardation compared to the rates in free peptides. Apparent activation enthalpies for hydrogen exchange of F5, F6, and F8 protons are 18.5 +/- 0.4, 9.5 +/- 0.3, and 18.5 +/- 0.3 kcal/mol, respectively. Some implications of these results on the nature of the opening processes involved in hydrogen exchange are considered.     

Differentiation between glioma and radiation necrosis using molecular magnetic resonance imaging of endogenous proteins and peptides

It remains difficult to distinguish tumor recurrence from radiation necrosis after brain tumor therapy. Here we show that these lesions can be distinguished using the amide proton transfer (APT) magnetic resonance imaging (MRI) signals of endogenous cellular proteins and peptides as an imaging biomarker. When comparing two models of orthotopic glioma (SF188/V+ glioma and 9L gliosarcoma) with a model of radiation necrosis in rats, we could clearly differentiate viable glioma (hyperintense) from radiation necrosis (hypointense to isointense) by APT MRI. When we irradiated rats with U87MG gliomas, the APT signals in the irradiated tumors had decreased substantially by 3 d and 6 d after radiation. The amide protons that can be detected by APT provide a unique and noninvasive MRI biomarker for distinguishing viable malignancy from radiation necrosis and predicting tumor response to therapy.     

Rapid amide proton exchange rates in peptides and proteins measured by solvent quenching and two-dimensional NMR.

In an effort to develop a more versatile quenched hydrogen exchange method for studies of peptide conformation and protein-ligand interactions, the mechanism of amide proton exchange for model peptides in DMSO-D2O mixtures was investigated by NMR methods. As in water, H-D exchange rates in the presence of 90% or 95% DMSO exhibit characteristic acid- and base-catalyzed processes and negligible water catalysis. However, the base-catalyzed rate is suppressed by as much as four orders of magnitude in 95% DMSO. As a result, the pH at which the exchange rate goes through a minimum is shifted up by about two pH units and the minimum exchange rate is approximately 100-fold reduced relative to that in D2O. The solvent-dependent decrease in base-catalyzed exchange rates can be attributed primarily to a large increase in pKa values for the NH group, whereas solvent effects on pKW seem less important. Addition of toluene and cyclohexane resulted in improved proton NMR chemical shift dispersion. The dramatic reduction in exchange rates observed in the solvent mixture at optimal pH makes it possible to apply 2D NMR for NH exchange measurements on peptides under conditions where rates are too rapid for direct NMR analysis. To test this solvent-quenching method, melittin was exchanged in D2O (pH 3.2, 12 degrees C), aliquots were quenched by rapid freezing, lyophilized, and dissolved in quenching buffer (70% DMSO, 25% toluene, 4% D2O, 1% cyclohexane, 75 mM dichloroacetic acid) for NMR analysis. Exchange rates for 21 amide protons were measured by recording 2D NMR spectra on a series of samples quenched at different times. The results are consistent with a monomeric unfolded conformation of melittin at acidic pH. The ability to trap labile protons by solvent quenching makes it possible to extend amide protection studies to peptide ligands or labile protons on the surface of a protein involved in macromolecular interactions.     

NMR studies of the influence of dodecyl sulfate on the amide hydrogen exchange kinetics of a micelle-solubilized hydrophobic tripeptide

Backbone amide hydrogen exchange measurements are an important source of information about the internal dynamics of proteins. Before such measurements can be interpreted unambiguously, contributions to hydrogen exchange rates from the chemical and physical environment of the amides must be taken into account. Membrane proteins are often solubilized in detergents, yet there have not been any systematic investigations of the possible effects detergents may have on the amide hydrogen exchange rates of proteins. To address this question, we have measured individual backbone and carboxyl-terminal amide exchange rates for the amphipathic tripeptide Leu-Val-Ile-amide dissolved in water and dodecyl sulfate micelles. 1H NMR spectroscopy was used to measure exchange using the direct exchange-out into D2O technique at 5 degrees C and using an indirect steady-state saturation-transfer technique at 25 degrees C. The broadening effect of micelle-incorporated spin-labeled fatty acid (12-doxylstearate) on the 1H NMR spectra of both the detergent and the peptide resonances was used to demonstrate that the tripeptide is intimately associated with the micelle. The resonance from formate ion, which is excluded from the micelle, was unperturbed by the spin label. The detergent did not retard the exchange rates of either the primary (terminal) or secondary (backbone) amides of the tripeptide. This suggests that the micelle/peptide interaction does not restrict access of charged catalysts and water to these amides and shows that the peptide amides are not hydrogen bonded. However, the pH for the exchange minima of these amides in detergent was increased between 1.2 and 1.7 units compared to exchange in water.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effect of regioisomerism on the coordination chemistry and CEST properties of lanthanide(III) NB-DOTA-tetraamide chelates

Chemical exchange saturation transfer (CEST) offers many advantages as a method of generating contrast in magnetic resonance images. However, many of the exogenous agents currently under investigation suffer from detection limits that are still somewhat short of what can be achieved with more traditional Gd³⁺ agents. To remedy this limitation we have undertaken an investigation of Ln³⁺ DOTA-tetraamide chelates (where DOTA is 1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetic acid) that have unusually rigid ligand structures: the nitrobenzyl derivatives of DOTA-tetraamides with (2-phenylethyl)amide substituents. In this report we examine the effect of incorporating hydrophobic amide substituents on water exchange and CEST. The ligand systems chosen afforded a total of three CEST-active isomeric square antiprismatic chelates; each of these chelates was found to have different water exchange and CEST characteristics. The position of a nitrobenzyl substituent on the macrocyclic ring strongly influenced the way in which the chelate and Ln³⁺ coordination cage distorted. These differential distortions were found to affect the rate of water proton exchange in the chelates. But, by far the greatest effect arose from altering the position of the hydrophobic amide substituent, which, when forced upwards around the water binding site, caused a substantial reduction in the rate of water proton exchange. Such slow water proton exchange afforded a chelate that was 4.5 times more effective as a CEST agent than its isomeric counterparts in dry acetonitrile and at low temperatures and very low presaturation powers.     

pH dependence of hydrogen exchange from backbone peptide amides in apamin

The kinetics of hydrogen exchange of the 11 most protected backbone amides of bee venom apamin have been measured between pH 1 and pH 8.5 by using time-resolved and saturation-transfer NMR spectroscopy. The five amides most protected from base-catalyzed exchange, those of residues 5 and 12-15, show highly correlated exchange behavior in the base-catalyzed regime. It is proposed that the intramolecular hydrogen bonds stabilizing these amides define a stable cooperative unit of secondary structure in apamin (a C-terminal helix and an N-terminal beta-turn). This conformational unit is further stabilized (by 5-6 kJ mol-1) on titration of the Glu-7 side-chain carboxyl group. The relative contributions of specific intramolecular interactions to this conformational stabilization are estimated. The pHminima in the pH-dependent single amide exchange curves are compared with values predicted by correcting for sequence-dependent contributions to amide exchange rates [Molday, R. S., Englander, S. W., & Kallen, R. G. (1972) Biochemistry 11, 150-158]. The lack of correlation suggests that the "open" conformers from which amide exchange occurs are nonrandom. This conclusion is dependent on the assumption that acid-catalyzed exchange occurs via N-protonation so that residual conformational effects on exchange rates in the open conformers will affect acid- and base-catalyzed rates in approximately equal and opposite ways. A strong correlation between the measured pHminima and the amide proton chemical shifts is observed, however, and this may be most easily accommodated if acid-catalyzed exchange occurs by the imidic acid mechanism (via amide O-protonation).     

Measuring rapid hydrogen exchange in the homodimeric 36 kDa HIV-1 integrase catalytic core domain

Measurements of rapid hydrogen exchange (HX) of water with protein amide sites contain valuable information on protein structure and function, but current NMR methods for measuring HX rates are limited in their applicability to large protein systems. An alternate method for measuring rapid HX is presented that is well-suited for larger proteins, and we apply the method to the deuterated, homodimeric 36 kDa HIV-1 integrase catalytic core domain (CCD). Using long mixing times for water-amide magnetization exchange at multiple pH values, HX rates spanning more than four orders of magnitude were measured, as well as NOE cross-relaxation rates to nearby exchangeable protons. HX protection factors for the CCD are found to be large (>10(4)) for residues along the dimer interface, but much smaller in many other regions. Notably, the catalytic helix (residues 152-167) exhibits low HX protection at both ends, indicative of fraying at both termini as opposed to just the N-terminal end, as originally thought. Residues in the LEDGF/p75 binding pocket also show marginal stability, with protection factors in the 10-100 range (～1.4-2.7 kcal/mol). Additionally, elevated NOE cross-relaxation rates are identified and, as expected, correspond to proximity of the amide proton to a rapidly exchanging proton, typically from an OH side chain. Indirect NOE transfer between H(2) O and the amide proton of I141, a residue in the partially disordered active site of the enzyme, suggests its proximity to the side chain of S147, an interaction seen in the DNA-bound form for a homologous integrase.     

The hydration of amides in helices; a comprehensive picture from molecular dynamics,IR, and NMR

We examined the hydration of amides of alpha(3)D, a simple, designed three-helix bundle protein. Molecular dynamics calculations show that the amide carbonyls on the surface of the protein tilt away from the helical axis to interact with solvent water, resulting in a lengthening of the hydrogen bonds on this face of the helix. Water molecules are bonded to these carbonyl groups with partial occupancy ( approximately 50%-70%), and their interaction geometries show a large variation in their hydrogen bond lengths and angles on the nsec time scale. This heterogeneity is reflected in the carbonyl stretching vibration (amide I' band) of a group of surface Ala residues. The surface-exposed amides are broad, and shift to lower frequency (reflecting strengthening of the hydrogen bonds) as the temperature is decreased. By contrast, the amide I' bands of the buried (13)C-labeled Leu residues are significantly sharper and their frequencies are consistent with the formation of strong hydrogen bonds, independent of temperature. The rates of hydrogen-deuterium exchange and the proton NMR chemical shifts of the helical amide groups also depend on environment. The partial occupancy of the hydration sites on the surface of helices suggests that the interaction is relatively weak, on the order of thermal energy at room temperature. One unexpected feature that emerged from the dynamics calculations was that a Thr side chain subtly disrupted the helical geometry 4-7 residues N-terminal in sequence, which was reflected in the proton chemical shifts and the rates of amide proton exchange for several amides that engage in a mixed 3(10)/alpha/pi-helical conformation.     

A globular protein with slower amide proton exchange from an alpha helix than from antiparallel beta sheets

In proteinase inhibitor IIA from bull seminal plasma, which is a small globular protein with 57 amino acid residues, measurements of individual amide proton exchange rates by two-dimensional correlated 1H NMR spectroscopy (COSY) showed that the exchange was slowest for some hydrogen bonded amide groups in an alpha-helix. This contrasts with all other proteins which were so far studied in detail, where the slowest exchange rates were observed for hydrogen bonded amide protons in antiparallel beta-sheets.     

NMR of hydrogen bonding in cold-shock protein A and an analysis of the influence of crystallographic resolution on comparisons of hydrogen bond lengths

Hydrogen bonding in cold-shock protein A of Escherichia coli has been investigated using long-range HNCO spectroscopy. Nearly half of the amide protons involved in hydrogen bonds in solution show no measurable protection from exchange in water, cautioning against a direct correspondence between hydrogen bonding and hydrogen exchange protection. The N to O atom distance across a hydrogen bond, R(NO), is related to the size of the (3h)J(NC') trans hydrogen bond coupling constant and the amide proton chemical shift. Both NMR parameters show poorer agreement with the 2.0-A resolution X-ray structure of the cold-shock protein studied by NMR than with a 1.2-A resolution X-ray structure of a homologous cold-shock protein from the thermophile B. caldolyticus. The influence of crystallographic resolution on comparisons of hydrogen bond lengths was further investigated using a database of 33 X-ray structures of ribonuclease A. For highly similar structures, both hydrogen bond R(NO) distance and Calpha coordinate root mean square deviations (RMSD) show systematic increases as the resolution of the X-ray structure used for comparison decreases. As structures diverge, the effects of coordinate errors on R(NO) distance and Calpha coordinate root mean square deviations become progressively smaller. The results of this study are discussed with regard to the influence of data precision on establishing structure similarity relationships between proteins.     

Sequence-specific 1H NMR assignments and identification of slowly exchanging amide protons in murine epidermal growth factor

Proton nuclear magnetic resonance (1H NMR) assignments for the murine epidermal growth factor (mEGF) in aqueous solution were determined by using two-dimensional NMR at pH 3.1 and 28 degrees C. The assignments are complete for all backbone hydrogen atoms, with the exception of the N-terminal amino group, and for 46 of the 53 side chains. Among the additional seven amino acid residues, three have complete assignments for all but one side-chain proton, and between two and four protons are missing for the remaining four residues. The sequential assignments by nuclear Overhauser effect spectroscopy are consistent with the chemically determined amino acid sequence. The NMR data show that the conformations of both the Tyr3-Pro4 and Cys6-Pro7 peptide bonds are trans in the predominant solution structure. Proton-deuterium exchange rate constants were also measured for 13 slowly exchanging amide protons. The information presented here has been used elsewhere to determine the three-dimensional structure of mEGF in aqueous solution.     

Hydrogen exchange kinetics in a membrane protein determined by 15N NMR spectroscopy: use of the INEPT experiment to follow individual amides in detergent-solubilized M13 coat protein

The coat protein of the filamentous coliphage M13 is a 50-residue polypeptide which spans the inner membrane of the Escherichia coli host upon infection. Amide hydrogen exchange kinetics have been used to probe the structure and dynamics of M13 coat protein which has been solubilized in sodium dodecyl sulfate (SDS) micelles. In a previous 1H nuclear magnetic resonance (NMR) study [O'Neil, J. D. J., & Sykes, B. D. (1988) Biochemistry 27, 2753-2762], multiple exponential analysis of the unresolved amide proton envelope revealed the existence of two slow "kinetic sets" containing a total of about 30 protons. The slower set (15-20 amides) originates from the hydrophobic membrane-spanning region and exchanges at least 10(5)-fold slower than the unstructured, non-H-bonded model polypeptide poly(DL-alanine). Herein we use 15N NMR spectroscopy of biosynthetically labeled coat protein to follow individual, assigned, slowly exchanging amides in or near the hydrophobic segment. The INEPT (insensitive nucleus enhancement by polarization transfer) experiment [Morris, G. A., & Freeman, R. (1979) J. Am. Chem. Soc. 101, 760-762] can be used to transfer magnetization to the 15N nucleus from a coupled proton; when 15N-labeled protonated protein is dissolved in 2H2O, the INEPT signal disappears with time as the amide protons are replaced by solvent deuterons. Amide hydrogen exchange is catalyzed by both H+ and OH- ions. Base catalysis is significantly more effective, resulting in a characteristic minimum rate in model peptides at pH approximately equal to 3. Rate versus pH profiles have been obtained by using the INEPT experiment for the amides of leucine-14, leucine-41, tyrosine-21, tyrosine-24, and valines-29, -30, -31, and -33 in M13 coat protein. The valine residues exchange most slowly and at very similar rates, showing an apparent 10(6)-fold retardation over poly(DL-alanine). A substantial basic shift in the pH of the minimum rate (up to 1.5 pH units) was also observed for some residues. Possible reasons for the shift include accumulation of catalytic H+ ions at the negatively charged micelle surface or destabilization of the negatively charged transition state of the base-catalyzed reaction by either charge or hydrophobic effects within the micelle. The time-dependent exchange-out experiment is suitable for slow exchange rates (kex), i.e., less than (1-2) x 10(-4) s-1.(ABSTRACT TRUNCATED AT 400 WORDS)     

Kinetics of amide proton exchange in helical peptides of varying chain lengths. Interpretation by the Lifson-Roig equation.

The kinetics of amide proton exchange (1H----2H) have been measured by proton nuclear magnetic resonance spectroscopy for a set of helical peptides with the generic formula Ac-(AAKAA)m Y-NH2 and with chain lengths varying from 6 to 51 residues. The integrated intensity of the amide resonances has been measured as a function of time in 2H2O at pH* 2.50. Exchange kinetics for these peptides can be modeled by applying the Lifson-Roig treatment for the helix-to-coil transition. The Lifson-Roig equation is used to compute the probability that each residue is helical, as defined by its backbone (phi, psi) angles. A recursion formula then is used to find the probability that the backbone amide proton of each residue is hydrogen bonded. The peptide helix can be treated as a homopolymer, and direct exchange from the helix can be neglected. The expression for the exchange kinetics contains only three unknown parameters: the rate constant for exchange of a non-hydrogen-bonded (random coil) backbone amide proton and the nucleation (v2) and propagation (w) parameters of the Lifson-Roig theory. The fit of the exchange curves to these three parameters is very good, and the values for v2 and w agree with those derived from circular dichroism studies of the thermally-induced unfolding of related peptides [Scholtz, J.M., Qian, H., York, E.J., Stewart, J.M., & Baldwin, R.L. (1991) Biopolymers (in press]).