Determination of enantiomerization barriers of hypericin and pseudohypericin by dynamic high‐performance liquid chromatography on immobilized polysaccharide‐type chiral stationary phases and off‐column racemization experiments

Direct enantiomer separation of hypericin, pseudohypericin, and protohypericin was accomplished by high‐performance liquid chromatography (HPLC) using immobilized polysaccharide‐type chiral stationary phases (CSPs). Enantioselectivities up to 1.30 were obtained in the polar‐organic elution mode whereby for hypericin and pseudohypericin Chiralpak IC [chiral selector being cellulose tris(3,5‐dichlorophenylcarbamate)] and for protohypericin Chiralpak IA (chiral selector being the 3,5‐dimethylphenylcarbamate of amylose) gave favorable results. Enantiomers were distinguished by on‐line electronic circular dichroism detection. Optimized enantioselective chromatographic conditions were the basis for determining stereodynamic parameters of the enantiomer interconversion process of hypericin and pseudohypericin. Rate constants delivered by computational simulation of dynamic HPLC elution profiles (stochastic model, consideration of peak tailing) were used to calculate averaged enantiomerization barriers (ΔG) of 97.6–99.6 kJ/mol for both compounds (investigated temperature range 25–45°C). Complementary variable temperature off‐column (i.e., in solution) racemization experiments delivered ΔG = 97.1–98.0 kJ/mol (27–45°C) for hypericin and ΔG = 98.9–101.4 kJ/mol (25–55°C) for pseudohypericin. An activation enthalpy of ΔH^# = 86.0 kJ/mol and an activation entropy of ΔS^# = ?37.7 J/(K mol) were calculated from hypericin racemization kinetics in solution, whereas for pseudohypericin these figures amounted to 74.1 kJ/mol and ?82.6 J/(K mol), respectively. Although the natural phenanthroperylene quinone pigments hypericin and pseudohypericin as well as their biological precursor protohypericin are chiral and can be separated by enantioselective HPLC low enantiomerization barriers seem to prevent the occurrence of an excess of one enantiomer under typical physiological conditions—at least as long as stereoselective intermolecular interactions with other chiral entities are absent. Chirality 2010. © 2009 Wiley‐Liss, Inc.     

Order–Disorder conformation change of xanthan in 0.01M aqueous sodium chloride: Dimensional behavior

Weight-average molecular weights M_w, second virial coefficients, and z-average radii of gyration 〈S²〉 were determined by light scattering as a function of temperature T for four sodium salt samples of xanthan in 0.01M aqueous NaCl, in which the polysaccharide undergoes an order–disorder conformation change with increasing T. The data for 〈S²〉 and M_w at 25 and 80°C, the lowest and highest temperatures studied, confirmed the previous conclusion that the predominant conformation at the former T, i.e., in the ordered state, is a double helix, while that at the latter T, i.e., in the disordered state, is a dimerized coil expanded by electrostatic repulsions between charged groups of the polymer. As T was increased from 25 to 80°C, 〈S²〉 sigmoidally decreased or increased depending on the dimer's molecular weight. This temperature dependence of 〈S²〉 and that determined elsewhere for a high molecular weight sample were found to be described almost quantitatively by a simple dimer model in which the double helix melts from both ends, when the double-helical fraction in the dimer at a given T estimated previously from optical rotation data was used.     

Heat capacity changes and partial molal heat capacities of some di- and tripeptides in water

Integral enthalpies of solution of several dipeptides and tripeptides in water at low concentrations have been determined at 25 and 35°C. These data have been used to derive the changes in heat capacity on dissolution at infinite dilution ΔC at 30°C. Limiting partial molal heat capacities ΔC have been determined by combining ΔC with C_p2 (heat capacity of pure solid peptides). Using the data on ω-amino acids and these peptides, the partial molal heat capacity of a peptide group ? CONH? was semiquantitatively estimated.     

Apparent molar volumes of some amino acids and peptides in aqueous urea solutions

Densities of solutions of several α-amino acids and peptides in 3 and 6m aqueous urea solvents have been determined at 298.15 K. These data have been used to evaluate the infinite-dilution apparent molar volumes of the solutes and the volume changes due to transfer (V ) of the α-amino acids and peptides at infinite dilution from water to aqueous urea solutions. The sign and magnitude of the V values have been rationalized in the framework of Friedman's cosphere-overlap model. The V values for the glycyl group (? CH₂CONH? ) and alkyl side chains have been estimated.     

Effects of cavity-creating mutations on conformational stability and structure of the dimeric 4-α-helical protein ROP: Thermal unfolding studies

The structural and energetic perturbations caused by cavity-creating mutations (Leu-41 → Val and Leu-41 → Ala) in the dimeric 4-α-helical-bundle protein ROP have been characterized by CD spectroscopy and differential scanning calorimetry (DSC). Deconvolution of the CD spectra showed a decrease in α -helicity as a result of the amino acid exchanges that follows qualitatively the overall decrease in conformational stability. Transition enthalpies are sensitive probes of the energetic change associated with point mutations. ΔH⁰ values at the respective transition temperatures, T_1/2 (71.0, 65.3, and 52.9°C at 0.5 mg/ml) decrease from 580 ± 20 to 461 ± 20 kJ/(mol of dimmer) and 335 ± 20 kJ/(mol of dimmer) for wildtype ROP (Steif, C., Weber, P., Hinz, H.-J., Flossdorf, J., Cesareni, G., Kokkinidis, M. Biochemistry 32:3867-3876, 1993), L⁴¹V, and L⁴¹A, respectively. The conformational stabilities at 25°C expressed by the standard Gibbs energies of denaturation, ΔG, are 71.7, 61.1, and 46.1 kJ/(mol of dimmer). The corresponding transition enthalpies have been obtained from extrapolation using the c(T)and c(T) functions. Their values at 25°C are 176.3, 101.9, and 141.7 kJ/(mol of dimmer) for wild-type ROP, L⁴¹V, and L⁴¹A, respectively. When the stability perturbation resulting from the cavity creating mutations is referred to the exchange of 1 mol of CH₂ group, the average ΔΔG value is ?5.0 ± 1 kJ/(mol of CH₂ group). This decrease in conformation stability suggests that dimeric ROP exhibits the same susceptibility to Leu → Yal and Leu → Ala exchanges as small monomeric proteins. Careful determinations of the partial specific heat capacities of wild-type and mutated protein solutions suggest that the mutational effects are predominantly manifested in the native rather than the unfolded state. © 1995 Wiley-Liss, Inc.     

Kinetics of ethidium's intercalation in packaged bacteriophage T7 DNA: effects of DNA packing density

The kinetics of ethidium's intercalative binding to DNA packaged in bacteriophage T7 and two T7 deletion mutants have been determined, using enhancement of fluorescence to quantitate binding. At a constant ethidium concentration, the results can be described as first-order binding with two different rate constants, k (= k₁ + k_?1) and k (= k₂ + k_?2). The larger rate constant (k) was at least four orders of magnitude smaller than the comparable first-order forward rate constant for binding to DNA released from its capsid. At 25°C values of k decreased as the amount of DNA packaged per internal volume increased. This latter observation indicates that the rate of ethidium's binding to packaged T7 DNA is limited by an event that occurs inside of the DNA-containing region of T7, not by the crossing of T7 capsid's outer shell. Arrhenius plots of kM are biphasic, indicating a transition for packaged DNA at a temperature of 20°C. The data indicate that k s are limited by either sieving of ethidium during its passage through the packaged DNA or subsequent hindered intercalation.     

Intrinsic viscosity of native and single-stranded T7 DNA and its relationship to sedimentation coefficient

The intrinsic viscosity and sedimentation coefficient, of native and single-stranded T7 DNA have been determined at 25°C as a function of ionic strength in neutral and alkaline NaCl. The relationship between [η] and S_,w is well represented by the Mandelkern-Flory equation over the entire range of conditions between 0.0013 and 1M Na⁺. An apparent discrepancy between the two methods at moderate to high ionic strengths is probably due to a change in V with ionic strength. It appears that [η] is a more sensitive and reliable measure of molecular expansion for native DNA, S_,w but is a better index of conformational change in single strands, since [η] becomes too small to measure conveniently at high ionic strengths. At moderate to high ionic strengths, denaturation leads to a decrease in [η], although unfolded single strands retain considerable viscosity. At sufficiently low ionic strength, the intrinsic viscosity of the single strands becomes higher than that of native DNA, and the effective volume of a single strand approaches that of the native molecule.     

Dynamic light scattering as a probe of superhelical DNA-intercalating agent interaction

Polarized dynamic light-scattering measurements on superhelical pBR322-plasmid DNA solutions in 0.2M NaCl, 2 mM NaPi, pH 7.0, 2 mM EDTA result in a translational diffusion coefficient D = (3.77 ± 0.10) × 10^?8 cm²/s for the native molecule. Modeling the DNA, in the simplest approximation, as a 10 × 440-nm effective hydrodynamic rigid rod yields a good fit to the apparent diffusion coefficient angular-dependence data up to 70°; the model fails at higher angles, probably due to the effects of flexibility or branching of the rod. Diffusion coefficient titration experiments with a platinum complex intercalating agent (PtTS) result in a titratable superhelix density of σ = ?0.079 ± 0.008 under our experimental conditions, corresponding to about 34 superhelical turns in the native DNA. The DNA contour length predicted by our two independent results, the rod dimensions and the number of superhelical turns, is in excellent agreement with the contour length calculated from the number of base pairs, supporting the hydrodynamic approximation of an effective rodlike structure for this small DNA molecule in solution.     

Study of salt effects on adenosine–polyuridylic acid interaction

Complex formation between poly(U) and adenosine in solutions of salts that stabilize (Na₂SO₄), destabilize (NaClO₄), or have little effect on the water structure (NaCl), as well as the poly(U)·poly(A) interaction in NaClO₄, was studied by equilibrium dialysis and uv spectroscopy. At 3°C and neutral pH, Ado·2 poly(U) is formed in 1M NaCl and 0.33M Na₂SO₄. In NaClO₄ solutions under the same conditions, an Ado·poly(U) was found over the whole range of salt concentration investigated (10 mM?1M), which has not been previously observed under any conditions. The Ado-poly(U) was also found in a NaCl/NaClO₄ mixture, the transition from the triple- to the double-helical complex occurring within a narrow range of concentration of added NaClO₄. In the presence of 1M NaCl this transition is observed on adding as little as 10 mM NaClO₄, i.e., at a [ClO]/[Cl^?] ratio of about 1:100. However, when NaClO₄ is added to a 1M solution of the stabilizing salt Na₂SO₄, no transition occurs even at a [ClO]/[SO] ratio of 1:4. Investigation of melting curves and uv spectra has shown that in an equimolar mixture of the polynucleotides, only a double-helical poly(U)·poly(A) exists in 1M NaClO₄ at low temperatures; this also holds for 1M NaCl. This changes to a triple-helical 2 poly(U)·poly(A) and then dissociates as the temperature increases. At low temperatures and the poly(U)/poly(A) concentration ratio of 2:1, a mixture of 2 poly(U)·poly(A) and poly(U)·poly(A) was observed in 1M NaClO₄, in contrast to the case of 1M NaCl. Thus, sodium perchlorate, a strong destabilizer of water structure, promotes formation of double-helical complexes both in the polynucleotide–monomer and the polynucleotide–polynucleotide systems. Beginning with a sufficiently high ionic strength (μ ? 0.9), a further increase in the salt molarity results in an increase of the poly(U)·adenosine melting temperature in both stabilizing and neutral salts and a decrease in the destabilizing salt. In Na₂SO₄ concentrations higher than 1.2M Ado·2 poly(U) precipitates at room temperature. Analysis of the binding isotherms and melting profiles of the complexes between poly(U) and adenosine according to Hill's model shows that the cooperativity of binding, due to adenosine stacking on poly(U), increases in the order NaClO₄ < NaCl < Na₂SO₄. The free energy of adenosine stacking on the template is similar to that of hydrogen bonding between adenosine and poly(U) and ranges from ?1 to ?2 kcal/mol. The values of ΔH_t [the effective enthalpy of adenosine binding to poly(U) next to an occupied site, obtained from the relationship between complex melting temperature and free monomer concentration at the midpoint of the transition] are ?14.2, ?18.3, and ?16.8 kcal/mol for 1M solutions of NaClO₄, NaCl, and Na₂SO₄, respectively. The results indicate that the effects of anions of the salts studied are related to water structure alterations rather than to their direct interaction with the complexes between poly(U) and adenosine.     

Laser light-scattering analysis of the dimerization of transfer ribonucleic acids with complementary anticodons

Photon-correlation spectroscopy is a powerful technique for measuring the translational diffusion coefficient of particles and macromolecules in solution. In the study described here, this technique was used to analyze a specific dimerization process involving the association of two tRNA molecules through complementary anticodons. The tRNAs used in the analysis were E. coli tRNA and yeast tRNA^Phe. The experimental data on the concentration dependence of the observed diffusion constants are shown to agree well with theoretical predictions. From these data, the equilibrium constant of the association reaction was determined for dimers formed over a wide range of temperatures and in several different solution conditions. In solutions of 0.1M ionic strength at 22°C, the equilibrium constants vary from 1 × 10⁵M^?1 in the absence of magnesium to 1.5 × 10⁶M^?1 in 10 mM Mg⁺². The enthalpy and entropy changes for dimer formation in the absence and presence, 5 and 10 mM, of magnesium have been obtained from the temperature dependence of the equilibrium constant. The results show that both ΔH and ΔS contribute to the free energy of binding and that their relative contributions are similar for each solution condition evaluated.     

Hetero-α-helical,two-chain coiled-coils. Clam–worm hybrid paramyosins

The specificity of the interaction between the α-helices in two-chain coiled-coils is investigated by studying the formation of hybrid molecules in which one α-helix is a clam paramyosin chain and the other a worm paramyosin chain. Hybrids are formed by mixing, denaturation, and subsequent renaturation. Comparison is made with a blank solution in which renaturation precedes mixing, thus precluding hybridization. Hybrids are detected by a ruse based on the presence of free sulfhydryl functions on calm chains. This allows molecules comprising two clam chains to be covalently crosslinked by oxidation with 5,5′-dithiobis(2-nitrobenzoate). Worm paramyosin chains have no sulfhydryl, so molecules comprising two worm chains or hybrid molecules comprising one chain of each type cannot crosslink. When run on sodium dodecyl sulfate polyacrylamide gel electrophoresis, therefore, the protein separates into two well-resolved regions, one containing one-chain species and the other two-chain species. When the gels are scanned and quantitated, the hybrids show up as an increase in the fraction of material in the one-chain band compared with the fraction in the blank solution. When renaturation is direct, we find that the fraction of renaturated molecules that are hybrids varies from ～10% at 5°C to ～5% at 25°C. These are judged to be nonequilibrium (quenched) values. When renaturation is by slow annealing, the equilibrium fraction hybrids are ～4% and show a modest, but measurable, increase with increasing temperature. These data allow calculation of the equilibrium constant K_h and standard free energy for the hybridization reaction: (1/2)CC + (½)WW = CW, in which C(W) stands for an α-helical clam (worm) polypeptide chain. The temperature dependence gives the standard enthalpy and entropy of the reaction. We find ΔH ? 1800 cal mol^?1 and ΔH ? 1.4 cal mol^?1 K^?1, using molarity concentration units and the infinitely dilute solution in NaCl/phosphate buffer as reference state. The possible molecular significance of these values is discussed, and it is concluded that the observed standard entropy arises essentially entirely from the rotational dissymmetry of the hybrids.     

Identification of the Blue Pigment Formed in a D-Glucose-Glycine Reaction System

D-Glucose (0.7 M), glycine (0.3 M), and sodium hydrogencarbonate (0.1 M) were dissolved in aqueous 30% ethanol at pH 8.0 and left at 50 °C for 4 d in a dark room under nitrogen displacement. The resulting blue pigment was isolated and purified from the blue solution by anionic exchange and gel filtration chromatography. This blue pigment, which is designated Blue-G1, was identified as 5-[1,4-bis-carboxymethyl-5-(2,3,4-trihydroxybutyl)-1,4-dihydropyrrolo[3,2-b]pyrrol-2-ylmethylene]-1,4-bis-carboxymethyl-2-(2,3,4-trihydroxybutyl)-4,5-dihydropyrrolo[3,2-b]pyrrol-1-ium. Blue-G1 had two symmetrical pyrrolopyrrole structures with a trihydroxybutyl group. Blue-G1 had a polymerizing activity, suggesting it to be an important Maillard reaction intermediate through the formation of melanoidins.     

Thermodynamics of stabilization of RNA pseudoknots by cobalt(III) hexaammine

Equilibrium unfolding (folding) studies reveal that the autoregulatory RNA pseudoknots derived from the bacteriophage T2 and T4 gene 32 mRNAs exhibit significant stabilization by increasing concentrations of divalent metal ions in solution. In this report, the apparent affinities of exchange inert trivalent Co(NH₃) have been determined, relative to divalent Mg²⁺, for the folded, partially folded (K_f), and fully unfolded (K_u) conformations of these molecules. A general nonspecific, delocalized ion binding model was developed and applied to the analysis of the metal ion concentration dependence of individual two‐state unfolding transitions. Trivalent Co(NH₃) was found to associate with the fully folded and partially unfolded pseudoknotted forms of these RNAs with a K_f of 5–8 × 10⁴ M⁻¹ in a background of 0.10 M K⁺, or 3‐ to 5‐fold larger than the K_f obtained for two model RNA hairpins and hairpin unfolding intermediates, and ≈ 40–50‐fold larger than K_f for Mg²⁺. The magnitude of K_f was found to be strongly dependent on the monovalent salt concentration in a manner qualitatively consistent with polyelectrolyte theory, with K_f reaching 1.2 × 10⁵ M⁻¹ in 50 mM K⁺. Two RNA hairpins were found to have affinities for Co(NH₃) and Ru(NH₃) of 1–2 ×10⁴ M⁻¹, or ≈ 15‐fold larger than the K_f of ∼ 1000 M⁻¹ observed for Mg²⁺. Additionally, the K_u of 4,800 M⁻¹ for the trivalent ligands is ≈ 8‐fold larger than the K_u of 600 M⁻¹ observed for Mg²⁺. These findings suggest that the T2 and T4 gene 32 mRNA pseudoknots possess a site(s) for Mg²⁺ and Co(NH₃) binding of significantly higher affinity than a “duplexlike” delocalized ion binding site that is strongly linked to the thermodynamic stability of these molecules. Imino proton perturbation nmr spectroscopy suggests that this site(s) lies near the base of the pseudoknot stem S2, near a patch of high negative electrostatic potential associated with the region where the single loop L1 adenosine crosses the major groove of stem S2. © 1999 John Wiley & Sons, Inc. Biopoly 50: 443–458, 1999     

Polyiodine units in starch–iodine complex: INDO CI study of spectra and comparison with experiments

The starch–iodine blue complex formation does not involve negatively charged iodine species like I, I, or I; rather, neutral iodine units are involved. The heat of reaction is determined to be about ?110 kJ for every mole of I-I unit in the amylose helix, which suggests that the dissociation of I₂ (binding energy 149 kJ/mol) does not take place during the complex formation. Quantum mechanical (INDO CI) calculations indicate that the linear as well as nonlinear polyiodine units, I₆, with interiodine distance of 3.0 Å are responsible for characteristic absorbance bands of the starch–iodine complex. Based on our previous article [(1989) J. Polym. Sci. A 27 , 4161] and the present studies we identify (C₆H₁₀O₅)_16.5I₆ to be the polymeric unit responsible for the characteristic blue color of the complex.     

Thermal properties of collagen in helical and random coiled states in the temperature range from 4° to 300°K

The low-temperature heat capacity of collagen (in the hydrated and dehydrated states) and the large entropy of collagen in the coiled state relative to the same protein in the helical state were investigated. The heat capacity for collagen in the solid state in the temperature range 4°–50° K changes proportionally to the square of temperature (C_p ～ T²). Above 50°K there is a linear dependence (C_p ～ T). The differences in the character of temperature dependence of heat capacity for the hydrated and dehydrated collagen show the importance of the specific interaction of water molecules with polypeptide chains of this protein. The peculiarities of the temperature dependence of the heat capacity difference (ΔC_p) of hydrated denatured (random coiled) and hydrated native (helical) collagen are observed at 15°, 120°, and 240°K. These differences are caused by the varying degree of ordering of the hydrate water molecules in native and denatured collagen macromolecules. At all temperatures (4°–300°K) the entropy of the random coiled state is higher than that of collagen in the native state and at 298°K ΔS = ∫ (ΔC_p/T)dT = 0.8 cal/100 g °K.     

Construction of Equi-replicated Balanced Block Designs with Block Sizes Exceeding the Number of Treatments

In this note it is shown that the block design with incidence matrix Ñ = [NN… N], where N = c_1hN_h + c_oh (11′–N_h). c_oh and c_1h are any non-negative integers and N_h,h = 1, 2,…,p, are incidence matrices of balanced incomplete block designs with the same number of treatments t, is a balanced block design with the block sizes exceeding the number of treatments. In derivation the matrix M₀, introduced by CALIński (1971) is utilized.     

Cathodic electrochemiluminescence of Ru(bpy)/Nafion coated on graphite oxide electrode in purely aqueous solution

Two cathodic electrochemiluminescence (ECL) peaks have been obtained at ?0.99 and ?1.80 V (vs. SCE), respectively, from Ru(bpy)/Na?on coated onto a graphite oxide electrode in purely aqueous solution under cyclic voltammetric (CV) conditions, without addition of any reducing or oxidative reagents. These two ECL peaks were found to correlate to initial scan direction, pH, and reversal potential. Na?on played an important role in the generation of these two ECL peaks because no cathodic emission was observed in the system without Na?on. It seems that a part of Ru(bpy) electrogenerated at positive potential can remain in the Na?on, even at negative potentials. It was con?rmed that Ru(bpy)⁺ was formed at ?1.80 V by addition of S₂O. The ECL peak at ?0.99 V is attributed to the reaction of Ru(bpy)³⁺ and OH^?. The ECL peak at ?1.80 V is probably due to the annihilation reaction of Ru(bpy)³⁺ and Ru(bpy)⁺. Copyright © 2003 John Wiley & Sons, Ltd.     

Number of binding sites of DNA and polynucleotides with tris(2,2'-dipyridyl)ruthenium(II) cations

The binding of tris(2,2′-bipyridyl)ruthenium(II) cations [Ru(bpy)] with single- and double-stranded (ss and ds) DNA, and the polynucleotides poly(A), poly(C), poly(G), poly(I), poly(I) · poly(C), and poly(U), was studied in aqueous solution. Steady-state electrical conductivity measurements with the polynucleotides, ssDNA, and dsDNA reveal that approximately three nucleotides offer one binding site. This may be compared with the ratio [nucleotide]/[Mg²⁺] of 2.4 : 1 for dsDNA. After laser excitation (353 nm), the luminescence of Ru(bpy) bound to nucleic acids shows two decay components. The contribution of the fast component, which is interpreted as resulting from quenching processes of the absorbed ruthenium complex, exhibits a maximum with increasing [nucleotide]/[Ru(bpy)] at a ratio of about three to one. Bound Ru(bpy) can be released from the strand by addition of NaClO₄ [half-concentration: 2.5 and ≤ 10 mM for poly(U) and dsDNA, respectively].     

Characterization of the transition state of Lysozyme unfolding. I. Effect of protein-solvent interactions on the transition state

The influence of proline cis-trans isomerization on the kinetics of lysozyme unfolding was examined carefully according to the theory of Hagerman and Baldwin [(1976) Biochemistry 15, 1462–1473]. As a result, the kinetics of lysozyme unfolding was found to follow the two-state transition model well. The temperature dependencies of k_uf and k_f over a wide temperature range showed that ΔC = 0 and ΔC = ?6.7 kJ K^?1 mol^?1 in solutions of different concentrations of GuHCl. The data observed in solutions containing other denaturants also supported the conclusion that ΔC is nearly equal to zero. The activation enthalpies of unfolding (ΔH) were observed at various concentrations of several kinds of denaturants. They were independent of species and concentrations of denaturants ΔH = 200 kJ mol^?1). These facts indicate that the aspect of interaction between protein and different kinds of solvent molecules varies only slightly during the unfolding to the transition state, that is, the transition state is at compact as the native one. Therefore, it is also suggested that ΔH of 200 kJ mol^?1 is primarily required for the disruption of long-range interactions among different structural domains through a subtle conformational change. We compared the effects of several kinds of denaturants on the unfolding rate. The addition of PrOH more remarkably increases the unfolding rate than do other hydrophilic denaturants. This is probably because PrOH molecules can penetrate into the hydrophobic core of lysozyme, but hydrophilic reagents cannot because of the compactness of the transition state.     

Physicochemical studies of amylose and its derivatives in aqueous solutions: Thermodynamics of the iodine–triiodide complex

Thermodynamic properties of the amylose–iodine–triiodide complex have been studied by spectrophotometry and by calorimetry using previously studied samples of amylose ionic derivatives, carboxymethylamylose and diethylaminoethylamylose. The ratio of triiodide to total molecular iodine ([I₃]_b/[I]_b + [I₂]_b) in the complex is ca. 0.3 over a range of iodide concentration from 10^?5 to 10^?4M, and there is no evidence for an increasing charge at slightly higher iodide concentration. Direct calorimetric experiments have been carried out in different conditions of polymer, iodine, and iodide concentration in order to study the dependence of the heat of the complexation as a function of the above parameters. It is shown that the dependence of the measured ΔH on the iodide concentration simply derives from the rearrangement of the triiodide equilibrium because of the uptake of a fixed ratio of iodine and triiodide molecules in the complex.