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Periodicity of amide proton exchange rates in a coiled-coil leucine zipper peptide.

The two-stranded coiled-coil motif, which includes leucine zippers, is a simple protein structure that is well suited for studies of helix-helix interactions. The interaction between helices in a coiled coil involves packing of "knobs" into "holes", as predicted by Crick in 1953 and confirmed recently by X-ray crystallography for the GCN4 leucine zipper [O'Shea, E.K., Klemm, J.D., Kim, P.S., & Alber, T. (1991) Science 254, 539]. A striking periodicity, extending over six helical turns, is observed in the rates of hydrogen-deuterium exchange for amide protons in a peptide corresponding to the leucine zipper of GCN4. Protons at the hydrophobic interface show the most protection from exchange. The NMR chemical shifts of amide protons in the helices also show a pronounced periodicity which predicts a short H-bond followed by a long H-bond every seven residues. This variation was anticipated in 1953 by Pauling and is sufficient to give rise to a local left-handed superhelical twist characteristic of coiled coils. The amide protons that lie at the base of the "hole" in the "knobs-into-holes" packing show slow amide proton exchange rates and are predicted to have short H-bond lengths. These results suggest that tertiary interactions can lead to highly localized, but substantial, differences in stability and dynamics within a secondary structure element and emphasize the dominant nature of packing interactions in determining protein structure.

Amides↗

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]).

Amides↗

Quantitation of the effects of an internal proline residue on individual hydrogen bond stabilities in an alpha-helix: pH-dependent amide exchange in melittin and [Ala-14]melittin.

pH-Dependent amide exchange rates in methanol have been measured for 21 of the 25 exchangeable backbone amides of [Ala-14]melittin (P14A), a synthetic analogue of bee venom melittin having a Pro to Ala substitution at residue 14. P14A, like melittin, adopts an alpha-helical conformation in methanol. As previously found for melittin [Dempsey, C. E. (1988) Biochemistry 27, 6893], the exchange data could be fit to curves calculated assuming acid and base catalysis by solvent from which residue-specific values of kH and kOMe, the acid- and base-catalyzed exchange rate constants, respectively, were determined. From a comparison of kmin values, where kmin is the minimum exchange rate in the curve defining the amide exchange rate as a function of pH, with those previously obtained from melittin, the relative stabilities of individual helical hydrogen bonds in the two peptides were calculated in terms of equilibrium constants for hydrogen-bond-breaking backbone fluctuations. Replacement of P14 in melittin with Ala results in stabilization of amides in a central turn of helix by up to 36-fold (delta delta GPro-Ala = 9 kJ mol-1) and elsewhere throughout the helix (residues 5-21) by 2-10-fold. These data indicate a cooperative effect of the Pro to Ala substitution on helix stability and allow a qualitative description of the fluctuational properties of the melittin and P14A helices in methanol. The effects of proline on the properties of the melittin helix are compared with previous theoretical and empirical studies on the effect of proline on the structure and stability of alpha-helices.

Alanine↗

Helical structure and orientation of melittin in dispersed phospholipid membranes from amide exchange analysis in situ.

A trapping method combined with high-resolution nuclear magnetic resonance spectroscopy is described for the measurement of hydrogen-deuterium exchange rates for individual amides of polypeptides bound to fully hydrated, dispersed phospholipid bilayers. Exchange rates were measured for 22 of the 24 amide hydrogens of bee venom melittin bound to bilayers composed of egg phosphatidylcholine/phosphatidylserine (88:12, mol/mol) dispersed in 20 mM sodium acetate, pH 4.0. Amides of residues 5-11 and 16-22 had exchange rates suppressed by between 30- and 1000-fold, and the rate suppression exhibited a helical periodicity with amides on the hydrophobic helix face up to 20-fold more stable than those on the hydrophilic face of the helix. These results demonstrate that under the conditions studied melittin adopts a helical conformation with stable helical hydrogen bonds extending to residue 22 and that the helix is oriented with the hydrophobic face directed toward the membrane interior.

Amides↗

Inhibition of collagenase from Clostridium histolyticum by phosphoric and phosphonic amides.

Di- and tripeptides with sequences present in collagen that are known to occupy the S1' through S3' subsites at the active site of the collagenase from Clostridium histolyticum do not themselves inhibit this zinc protease. Thus glycylproline, glycylprolylalanine, and their C-terminal amides are not inhibitors. N alpha-Phosphorylglycylproline, N alpha-phosphorylglycyl-L-prolyl-L-alanine, and their C-terminal amides are weak inhibitors with IC50's (concentration causing half-maximal inhibition) of 4.6, 0.8, 3, and 1.5 mM, respectively. Extension of glycyl-L-prolyl-L-alanine to L-leucyl-glycyl-L-prolyl-L-alanine gives a tetrapeptide known to occupy the S1, S1', S2', and S3' subsites of collagenase when present in collagen but that still does not itself inhibit the enzyme. (Isoamylphosphonyl)glycyl-L-prolyl-L-alanine, a peptide containing a tetrahedral phosphorus atom at the position of the amide carbonyl carbon of the L-leucylglycyl amide bond of the parent tetrapeptide, inhibits collagenase with an IC50 of 16 microM, at least 1000-fold more potent than the parent peptide. Substitution of the two-carbon ethyl chain of alanine for the five-carbon isoamyl chain of leucine increases the IC50 to 46 microM. Substitution of the n-decyl chain for the isoamyl chain does not change the IC50. (Isoamylphosphonyl)glycyl-glycyl-L-proline contains a tripeptide that does not occupy the S1' through S3' subsites of collagenase when this peptide is present in collagen and thus has an IC50 of 4.4 mM. (Isoamylphosphonyl)glycyl-L-prolyl-L-alanine may be an analogue of the tetrahedral transition state for the hydrolysis of the natural collagen substrate.(ABSTRACT TRUNCATED AT 250 WORDS)

Amides↗

Protection of amide protons in folding intermediates of ribonuclease A measured by pH-pulse exchange curves.

pH-pulse exchange curves have been measured for samples taken during the folding of ribonuclease A. The curve gives the number of protected amide protons remaining after a 10-s pulse of exchange at pHs from 6.0 to 9.5, at 10 degrees C. Amide proton exchange is base catalyzed, and the rate of exchange increases 3000-fold between pH 6.0 and pH 9.5. The pH at which exchange occurs depends on the degree of protection against exchange provided by structure. Pulse exchange curves have been measured for samples taken at three times during folding, and these are compared to the pulse exchange curves of N, the native protein, of U, the unfolded protein in 4 M guanidinium chloride, and of IN, the native-like intermediate obtained by the prefolding method of Schmid. The results are used to determine whether folding intermediates are present that can be distinguished from N and U and to measure the average degree of protection of the protected protons in folding intermediates. The amide (peptide NH) protons of unfolded ribonuclease A were prelabeled with 3H by a previous procedure that labels only the slow-folding species. Folding was initiated at pH 4.0, 10 degrees C, where amide proton exchange is slower than the folding of the slow-folding species. Samples were taken at 0-, 10-, and 20-s folding, and their pH-pulse exchange curves were measured.(ABSTRACT TRUNCATED AT 250 WORDS)

Amides↗

Ca2+ binding to calbindin D9k strongly affects backbone dynamics: measurements of exchange rates of individual amide protons using 1H NMR.

One- and two-dimensional 1H NMR have been used to study the backbone dynamics in Ca2(+)-free (apo) and Ca2(+)-loaded (Ca2) calbindin D9k at pH 7.5 and 25 degrees C. Hydrogen exchange rates of all 71 backbone amide protons (NH's) have been measured for the Ca2 form by both a direct exchange-out experiment and another experiment that measures the transfer of saturation from water protons to amide protons. A large number of NH's are found to be highly protected against exchange with solvent protons. The results for the Ca2 form are related to solvent accessibility and hydrogen bonding obtained in molecular dynamics simulations of calcium-loaded calbindin. The correlation with these parameters is strong within the N-terminal half of calbindin, which is found to be more stable than the C-terminal half. The amide proton exchange in the apo form is much faster than in the Ca2 form and was studied in a series of experiments in which the exchange was quenched after different times by Ca2+ addition. This experiment is applicable to all amide hydrogens that exchange slowly in the Ca2 form. For these NH's the effects of Ca2+ removal span from a 10(2)-fold decrease to a 10(5)-fold increase of the exchange rate, and the average is a 220-fold increase. The effects on individual NH exchange rates show that the four alpha-helices are almost intact after calcium removal and that the changes in dynamics involve not only the Ca2(+)-binding region. Hydrogen bonds involving backbone NH's in the Ca2+ loops appear to be broken or weakened when calbindin releases Ca2+, whereas the beta-sheet between the Ca2+ loops is found to be present in both the Ca2 and apo forms. Large Ca2(+)-induced effects on NH exchange rates were measured for a few residues at alpha-helix ends far from the two Ca2(+)-binding sites. This may be the result of a change in interhelix angles (or the rate of interhelix angle fluctuations) on calcium binding.

Amides↗

Global disruption of the WASP autoinhibited structure on Cdc42 binding. Ligand displacement as a novel method for monitoring amide hydrogen exchange.

The Cdc42 GTPase, a member of the Rho subfamily of Ras proteins, can signal to the cytoskeleton through its effector, the Wiskott-Aldrich syndrome protein (WASP), activation of which results in localized polymerization of new actin filaments. NMR structures of WASP peptide models in the Cdc42-bound and free states suggest that GTPase binding weakens autoinhibitory contacts between the GTPase binding domain (GBD) and the C-terminal actin regulatory (VCA) region of the protein. In the study presented here, amide hydrogen exchange has been used with NMR spectroscopy to directly examine destabilization of the autoinhibited GBD-VCA conformation caused by GTPase binding. A truncated protein, GBD-C, which models autoinhibited WASP, folds into a highly stable conformation with amide exchange protection factors of up to 3 x 10(6). A novel hydrogen exchange labeling-quench strategy, employing a high-affinity ligand to displace Cdc42 from WASP, was used to examine the amide exchange from the Cdc42-bound state of GBD-C. The GTPase increases exchange rates of the most protected amides by 50-500-fold, with destabilization reducing the differences in the protection of segments in the free state. The results confirm that Cdc42 facilitates the physical separation of the GBD from the VCA in a tethered molecule, indicating this process likely plays an important role in activation of full-length WASP by the GTPase. However, destabilization of GBD-C is not complete in the Cdc42 complex. The data indicate that partitioning of free energy between binding and activation may limit the extent to which GTPases can cause conformational change in effectors. This notion is consistent with the requirement of multiple input signals in order to achieve maximal activation in many effector molecules.

Actins↗

Hydrogen bonding on the ice-binding face of a beta-helical antifreeze protein indicated by amide proton NMR chemical shifts.

The dependence of amide proton chemical shifts on temperature is used as an indication of the hydrogen bonding properties in a protein. The amide proton temperature coefficients of the beta-helical antifreeze protein from Tenebrio molitor are examined to determine their hydrogen bonding state in solution. The temperature-dependent chemical shift behavior of the amides in T. molitor antifreeze protein varies widely throughout the protein backbone; however, very subtle effects of hydrogen bonding can be distinguished using a plot of chemical shift deviation (CSD) versus the backbone amide chemical shift temperature gradient (Deltadelta/DeltaT). We show that differences between the two ranks of ice-binding threonine residues on the surface of the protein indicate that threonine residues in the left-hand rank participate in intrastrand hydrogen bonds that stabilize the flat surface required for optimal ice binding.

Amides↗

Interaction of alpha-and beta-oligoarginine-acids and amides with anionic lipid vesicles: a mechanistic and thermodynamic study.

The interaction of alpha- and beta-oligoarginine amides and acids and of alpha-polyarginine with anionic lipid vesicles was studied. The beta-oligoarginines used were beta3-homologues of the alpha-oligoarginines. Lipid bilayers were composed of POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine) and POPG (1-palmitoyl-2-oleoyl-sn-glycero-3-[phospho-rac-(1-glycerol)]) containing 5 mol % pyrene-PG (1-hexadecanoyl-2-(1-pyrenedecanoyl)-sn-glycero-3-[phospho-rac-1-glycerol]). Kinetic analysis of the binding process onto large unilamellar POPC/POPG (3:7, molar ratio) vesicles (100 nm diameter) shows biphasic time courses for all tested peptides. The first binding step is fast and takes place within approximately 10 s with no disruption of the membrane as indicated by corresponding calcein release measurements. The second binding phase is slow and occurs within the next 30-300 s with substantial membrane disruption. In this context, beta-hexa- and octaarginine amides possess higher second half-times than the beta-hexa- and octaarginine acids of the same chain length. Furthermore beta-octaarginine amide induces a calcein release approximately twice as large as that of the beta-octaarginine acid. Thermodynamic analysis of the binding process, using the complex formation model that assumes that each peptide binds independently to n POPG lipids, reveals apparent binding constants (K(app1)) of approximately 5 x 10(6)-10(8) M(-1) and n-values from 3.7 for beta-hexaarginine acid up to 24.8 for alpha-polyarginine. Although the K(app1)-values are similar, the number of binding sites clearly depends on the chemical nature of the oligoarginine: beta-oligoarginine amides and alpha-oligoarginine acids interact with more lipids than beta-oligoarginine acids of the same length. Calculation of the electrostatic contribution to the total free energy of binding reveals that for all oligoarginines only 25-30% has electrostatic origin. The remaining approximately 70-75% is nonelectrostatic, corresponding to hydrogen bonding and/or hydrophobic interactions. From the obtained data, a mechanism is suggested by which oligoarginines interact with anionic vesicles: (1) initial electrostatic interaction that is fast, nonspecific, and relatively weak; (2) nonelectrostatic interaction that is rate-limiting, stronger, and induces bilayer rigidification as well as release of aqueous contents from the vesicles.

Acids↗

Amide backbone and water-related H/D isotope effects on the dynamics of a protein folding reaction.

The denaturant-dependent relaxation kinetics of folding and unfolding of an isolated all-beta domain of rat CD2 have been measured at 25 degrees C in four isotopic conditions: with a protonated (amide) backbone in H2O and in D2O and with a deuterated backbone in H2O and in D2O. The data show that this structure, which contains no disulfide bonds, folds through a rapidly formed intermediate (pathway U-I-F) and that all free energy changes between states are insensitive to isotopic substitution of the amide groups required for intrachain hydrogen bonding. However, the folding reaction is significantly influenced by the nature of the bulk solvent. In D2O, the stability of each state in the folding pathway, relative to the unfolded molecule, is enhanced to a degree which is proportional to its m value, a measure of the exposure of nonpolar protein groups to the solvent. Together these observations suggest that, at this temperature, the solvent isotope effect arises from enhanced hydrophobic interactions which, in turn, results from an increased strength of the solvent-solvent hydrogen bond in D2O. Apart from emphasizing the role of bonds between solvent molecules in protein folding, the results also have practical implications for amide H/D exchange studies. While the replacement of amide protons by deuterons will not affect the protein's stability during exchange experiments, it is important to account for the isotopic influence of the solvent in which the exchange reaction is performed.

Amides↗

Alkyl amides and nitriles as novel tracers for biomass burning.

The occurrence of n-alkanoic acids, amides, and nitriles in samples of aerosol particulate matter from Kuala Lumpur and Santiago suggests that emissions from cooking and biomass burning are the primary sources of these organic markers in the atmosphere. It is proposed that fatty acids react with ammonia during biomass burning or combustion to produce amides and nitriles, which can be applied as useful biomarker tracers. To test this hypothesis, nonadecanoic acid and hexadecanamide were used as reactants in hydrous pyrolysis experiments. These experiments produced amides and nitriles and indicated that ammonia is an essential agent in their formation. Thus amides and nitriles are of utility as indicators for input from combustion and biomass burning in the ambient atmosphere.

Air Pollutants↗

Factors controlling metal-ion selectivity in the binding sites of calcium-binding proteins. The metal-binding properties of amide donors. A crystallographic and thermodynamic study.

The metal-ion complexing properties of the ligand EDTAM (ethylenediamine-N,N,N',N'-tetraacetamide) are investigated as a model for the role of amide oxygen donors in the binding sites of Ca-binding proteins. The structures of the complexes [Ca(EDTAM)NO3]NO3 (1), [La(EDTAM)(H2O)4](NO3)3.H2O (2), and [Cd(EDTAM)(NO3)]NO3 (3) are reported: 1 monoclinic, P2(1)/c, a = 10.853(2) angstroms, b = 12.893(3) angstroms, c = 13.407(3) angstroms, beta = 103.28(3) degrees, Z = 4, R = 0.0281; 2 triclinic, P, a = 8.695(2) angstroms, b = 9.960(2) angstroms, c = 16.136(3) angstroms, alpha = 95.57(3) degrees, beta = 94.84(3) degrees, gamma = 98.72(3) degrees, Z = 2, R = 0.0394; 3 monoclinic, P2(1)/c, a = 10.767(2) angstroms, b = 12.952(2) angstroms, c = 13.273(2) angstroms, beta = 103.572(3) degrees, Z = 4, R = 0.0167. Compounds 1 and 3 are isostructural, and the EDTAM binds to the metal ion through its two N-donors and four O-donors from the amide groups. Ca(II) in 1 is 8-coordinate with a chelating NO3- group, while Cd(II) in 3 may possibly be 7-coordinate, with an asymmetrically coordinated NO3- that is best regarded as unidentate. The La(III) in 2 is coordinated to the EDTAM in a manner similar to that of 1 and 3, but it is 10-coordinate with four water molecules coordinated to the La(III). The formation constants (log K1) for complexes of a variety of metal ions with EDTAM are reported in 0.1 M NaNO3 at 25.0 +/- 0.1 degrees C. These are compared to the log K1 values for en (ethylenediamine) and THPED (N,N,N',N'-tetrakis(2-hydroxypropyl)-ethylenediamine). For large metal ions, such as Ca2+ or La3+, log K1 increases strongly when the four acetamide groups are added to en to give EDTAM, whereas for a small metal ion, such as Mg2+, this increase is small. The log K1 values for EDTAM compared to THPED suggest that the amide oxygen is a much stronger base than the alcoholic oxygen. Structures of binding sites in 40 Ca-binding proteins are examined. It is shown that the Ca-O=C bond angles involving coordinated amides in these sites are large, commonly being in the 150-180 degrees range. This is discussed in terms of the idea that for purely ionic bonding the M-O=C bond angle will approach 180 degrees, while for covalent bonding the angle should be closer to 120 degrees. How this fact might be used by the proteins to control selectivity for different metal ions is discussed.

Amides↗

Dihedral psi angle dependence of the amide III vibration: a uniquely sensitive UV resonance Raman secondary structural probe.

UV resonance Raman studies of peptide and protein secondary structure demonstrate an extraordinary sensitivity of the amide III (Am III) vibration and the C(alpha)H bending vibration to the amide backbone conformation. We demonstrate that this sensitivity results from a Ramachandran dihedral psi angle dependent coupling of the amide N-H motion to (C)C(alpha)H motion, which results in a psi dependent mixing of the Am III and the (C)C(alpha)H bending motions. The vibrations are intimately mixed at psi approximately 120 degrees, which is associated with both the beta-sheet conformation and random coil conformations. In contrast, these motions are essentially unmixed for the alpha-helix conformation where psi approximately -60 degrees. Theoretical calculations demonstrate a sinusoidal dependence of this mixing on the psi angle and a linear dependence on the distance separating the N-H and (C)C(alpha)H hydrogens. Our results explain the Am III frequency dependence on conformation as well as the resonance Raman enhancement mechanism for the (C)C(alpha)H bending UV Raman band. These results may in the future help us extract amide psi angles from measured UV resonance Raman spectra.

Amides↗

Mechanism and energetics of intramolecular hydrogen transfer in amide and peptide radicals and cation-radicals.

Intramolecular hydrogen transfer in five model amide and peptide radicals and cation-radicals was investigated by combined B3LYP-MP2 calculations. Hypervalent ammonium radicals produced by electron capture in protonated peptides undergo competitive elimination of ammonia, H-atom loss, and H-atom migration to neighboring amide carbonyls. The calculated transition state energies for H-atom migration are slightly but uniformly lower than those for H-atom loss. Transition state theory calculations with inclusion of quantum tunneling effects predict k(H migration)/k(H loss) branching ratios that increase with the ring size of the cyclic transition state for the migration. Intramolecular hydrogen-atom migration in amide and peptide radicals can be described by the proton-coupled electron transfer mechanism. The migrating hydrogen atom shows a negligible spin density and substantial positive charge that are typical of a proton migration. Electron transfer occurs through a pi-orbital system and proceeds in the same (clockwise) or opposite (counterclockwise) direction as the proton motion, depending on the electronic properties of the chain connecting the ammonium group and the amide bond.

Alanine↗

Effects of hydrogen bonding on metal ion-promoted intramolecular electron transfer and photoinduced electron transfer in a ferrocene-quinone dyad with a rigid amide spacer.

A ferrocene-quinone dyad (Fc-Q) with a rigid amide spacer and Fc-(Me)Q dyad, in which the amide proton acting as a hydrogen-bonding acceptor is replaced by the methyl group, are employed to examine the effects of hydrogen bonding on both the thermal and the photoinduced electron-transfer reactions. The hydrogen bonding of the semiquinone radical anion with the amide proton in Fc-Q(.-) produced by the electron-transfer reduction of Fc-Q is indicated by the significant positive shift of the one-electron reduction potential of Fc-Q. The hyperfine coupling constants of Fc-Q(.-) also indicate the existence of hydrogen bonding, agreeing with those predicted by the density functional calculation. The hydrogen-bonding dynamics in the photoinduced electron transfer from the ferrocene (Fc) to the quinone moiety (Q) in Fc-Q have been successfully detected in the femtosecond laser flash photolysis experiments. Thermal intramolecular electron transfer from Fc to Q in Fc-Q and Fc-(Me)Q also occurs efficiently in the presence of metal ions in acetonitrile at 298 K. The hydrogen bond formed between the semiquinone radical anion and the amide proton in Fc-Q results in remarkable acceleration of the rate of metal ion-promoted electron transfer as compared to the rate of Fc-(Me)Q in which hydrogen bonding is prohibited. The metal ion-promoted electron-transfer rates are well correlated with the binding energies of superoxide ion-metal ion complexes, which are derived from the g(zz) values of the ESR spectra.

Amides↗

Synthesis and properties of RNA analogues having amides as interuridine linkages at selected positions.

Oligoribonucleotide analogues having amide internucleoside linkages (AM1: 3'-CH(2)CONH-5' and AM2: 3'-CH(2)NHCO-5') at selected positions have been synthesized and the thermal stability of duplexes formed by these analogues with complementary RNA fragments has been evaluated by UV melting experiments. Two series of oligomers with either 2'-OH or 2'-OMe vicinal to the amide linkages were studied. Monomeric synthons (3' and 5'-C amines and carboxylic acids) were synthesized as follows: For synthesis of the AM1 analogue, the known sequence of radical allylation followed by the cleavage of the double bond was adopted. For synthesis of the AM2 analogue, novel routes via addition of nitromethane followed by conversion of the nitro function to either amino or carboxyl groups were developed. Coupling of monomeric amines and carboxylic acids followed by protecting group manipulation and phosphonylation gave dimeric 3'-hydrogenphosphonate building blocks for oligonucleotide synthesis. Monomeric model compounds having 3'-amide and 2'-OH or 2'-OMe groups were also prepared and their conformational equilibrium was determined by (1)H NMR. The AM1 and AM2 models showed equal preferences for the North conformers (at 40 degrees C, 88-89% with 2'-OH, and 92-93% with 2'-OMe). At physiological salt concentration (0.1 M NaCl) the duplexes between AM1 modified oligonucleotides and RNA had stability similar to unmodified RNA-RNA duplexes (Delta t(m)= -0.2 to +0.7 degrees C per modification). However, the AM2 modification resulted in substantial stabilization of duplexes: Delta t(m)= +1 to +2.4 degrees C per modification compared to all RNA. A 2'-O-methyl vicinal to the AM2 linkage further increased the duplex stability. Our results suggest that RNA analogues having amide internucleoside bonds are very promising candidates for medicinal applications.

Amides↗

Intramolecular migration of amide hydrogens in protonated peptides upon collisional activation.

Presently different opinions exist as to the degree of scrambling of amide hydrogens in gaseous protonated peptides and proteins upon collisional activation in tandem mass spectrometry experiments. This unsettled controversy is not trivial, since only a very low degree of scrambling is tolerable if collision-induced dissociation (CID) should provide reliable site-specific information from (1)H/(2)H exchange experiments. We have explored a series of unique, regioselectively deuterium-labeled peptides as model systems to probe for intramolecular amide hydrogen migration under low-energy collisional activation in an orthogonal quadrupole time-of-flight electrospray ionization (Q-TOF ESI) mass spectrometer. These peptides contain a C-terminal receptor-binding sequence and an N-terminal nonbinding region. When the peptides form a receptor complex, the amide hydrogens of the interacting sequences are protected against exchange with the solvent, while the amide hydrogens of the nonbinding sequences exchange rapidly with the solvent. We have utilized such long-lived complexes to generate peptides labeled with deuterium in either the binding or nonbinding region, and the expected regioselectivity of this labeling was confirmed after pepsin proteolysis. CID of such deuterated peptides, [M + 2H](2+), yielded fragment ions (b- and y-ions) having a deuterium content that resemble the theoretical values calculated for 100% scrambling. Thus, complete randomization of all hydrogen atoms attached to nitrogen and oxygen occurs in the gaseous peptide ion prior to its dissociation.

Amides↗