Evidence for pyroelectric and piezoelectric sensory mechanisms in the insect integument.

Quantitative pyroelectric (PE) and piezoelectric (PZE) measurements were carried out on the insect integument of live Blaberus giganteus (cockroach) and on dry integument preparations of the same species. Voltage responses to optical pulses of 10--500 ms, absorbed in the live integument, were PE: interference filter measurements showed the responses to be proportional to the absorbed thermal radiation flux and independent of the wavelength. The voltage/time-course of the responses was in agreement with theoretically calculated PE signals. Voltage responses to mechanical pulses were PZE. The responses of the inner and outer integument surfaces always had opposite electric signs. The polar character of the integument was confirmed by means of a separate dielectric heating method. To explain these results, we hypothesize that the PE properties are for the most part localized in the two outermost layers (outer and inner epicuticle) of the integument, which consists mainly of polar lipids and proteins. Parallel alignment of these polar molecules perpendicular to the integument surface is very likely. PE and PZE responses, therefore, will not only occur in live insects but will also be measurable in dead, dry integument preparations as long as the polar tissue texture remains intact. Due to its polar texture, the insect integument will react to rapid changes in temperature, illumination, or uniaxial pressure in the same way as nonbiological PE materials, where the voltage responses depend on dX/dt (X, pressure or temperature). It seems clear, therefore, that the well-known physiological reactions of various arthropods to such physical outside influences may be related to the PE property of their integument.     

Evidence of inherent spontaneous polarization in the metazoan integument epithelia.

The live integument epithelia of the metazoa have an inherent spontaneous polarization (an inherent permanent electric dipole moment) of corresponding direction perpendicular to the integument surface. The existence of the inherent polarization was proved by their temperature dependence, i.e., by the pyroelectric (PE) effect. Quantitative PE measurements were carried out on a number of integument epithelia of vertebrates (a) in vivo, (b) on fresh epidermis preparations, and (c) on dead, air-dried epidermis specimens of the same species. The demonstrated spontaneous polarization is not dependent on the living state and not caused by a potential difference between the outer and inner integument surface. Dead, dry epidermis samples (potential difference less than 0.01 mV) as well as dead, dry integument appendages (bristles, hairs), and dead cuticles (of arthropoda, annelida, nematoda) showed an inherent dipole moment of the same orientation as the live epidermis. The findings reveal a relationship between the direction (vector) of inherent spontaneous polarization and that of growth (morphogenesis) in the animal epidermis, their appendages, and cuticles. We conclude (a) that the inherent spontaneous polarization is present in live individual epithelial cells of the metazoan integument, and (b) that this physical property is related to the structural and functional cell polarity of integument epithelia and possibly of other epithelia.     

Tight junction structure and ZO-1 content are identical in two strains of Madin-Darby canine kidney cells which differ in transepithelial resistance

The relationship of tight junction permeability to junction structure and composition was examined using two strains of Madin-Darby canine kidney (MDCK) cells (I and II) which differ greater than 30-fold in transepithelial resistance. This parameter is largely determined by paracellular, and hence junctional, permeability under most conditions. When these two strains of cells were grown on permeable filter supports, they formed monolayers with equivalent linear amounts of junction/area of monolayer. Ultrastructural analysis of these monolayers by thin section EM revealed no differences in overall cellular morphology or in tight junction organization. Morphometric analysis of freeze-fractured preparations indicated that the tight junctions of these two cell strains were similar in both number and density of junctional fibrils. Prediction of transepithelial resistance for the two strains from this freeze-fracture data and a published structure-function formulation (Claude, P. 1978, J. Memb. Biol. 39:219- 232) yielded values (I = 26.5 omega/cm2, II = 35.7 omega/cm2) that were significantly lower than those observed (I = 2,500-5,000 omega/cm2, II = 50-70 omega/cm2). Consistent with these structural studies, a comparison of the distribution and cellular content of ZO-1, a polypeptide localized exclusively to the tight junction, revealed no significant differences in either the localization of ZO-1 or the amount of ZO-1 per micron of junction (I = 1,415 +/- 101 molecules/micron, II = 1,514 +/- 215 molecules/micron).     

Transient quinonimines and 1,4-benzothiazines of pheomelanogenesis: new pulse radiolytic and spectrophotometric evidence.

Biosynthetic and model in vitro studies have shown that pheomelanins, the distinctive pigments of red human hair, arise by oxidative cyclization of cysteinyldopas mainly 5-S-cysteinyldopa (1) via a critical o-quinonimine intermediate, which rearranges to unstable 1,4-benzothiazines. To get new evidence for these labile species, fast time resolution pulse radiolytic oxidation by dibromide radical anion of a suitable precursor, the dihydro-1,4-benzothiazine-3-carboxylic acid 7 was performed in comparison with that of 1. In the case of 7, dibromide radical anion oxidation leads over a few microseconds (k = 2.1 x 10(9) M(-1) s(-1)) to a phenoxyl radical (lambda(max) 330 nm, epsilon = 6300 M(-1) cm(-1)) which within tens of milliseconds gives rise with second-order kinetics (2k = 2.7 x 10(7) M(-1) s(-1)) to a species exhibiting an absorption maximum at 540 nm (epsilon = 2200 M(-1) cm(-1)). This was formulated as the o-quinonimine 3 arising from disproportionation of the initial radical. The quinonimine chromophore is converted over hundreds of milliseconds (k = 6.0 s(-1)) to a broad maximum at around 330 nm interpreted as due to a 1,4-benzothiazine or a mixture of 1,4-benzothiazines, which as expected are unstable and subsequently decay over a few seconds (k = 0.5 s(-1)). Interestingly, the quinonimine is observed as a labile intermediate also in the alternative reaction route examined, involving cyclization of the o-quinone (lambda(max) 390 nm, epsilon = 6900 M(-1) cm(-1)) arising by disproportionation (2k = 1.7 x 10(8) M(-1) s(-1)) of an o-semiquinone (lambda(max) 320 nm, epsilon = 4700 M(-1) cm(-1)) directly generated by dibromide radical anion oxidation of 1. Structural formulation of the 540 nm species as an o-quinonimine was further supported by rapid scanning diode array spectrophotometric monitoring of the ferricyanide oxidation of a series of model dihydrobenzothiazines.     

Food intake,conversion and swimming activity in the air-breathing catfish Heteropneustes fossilis

Summary Reared in tubular aquaria containing 20, 40 and 60 cm depth 0f water, Heteropneustes fossilis (20 g; 17 cm body length), an air-breathing catfish, swam 40, 80 and 120 cm/surfacing to exchange atmospheric air. With decreasing Po₂, the starving groups reduced the surfacing, whereas, the decrease in the Po₂ beyond 70 mm Hg induced the feeding groups to surface more frequently. Feeding groups exposed to 20 and 40 cm depth surfaced 353 and 423 times, travelling distances of 141 and 338 m/day, at the energy cost of 8.5 and 9.7 mg dry fish substance/g live fish/day, respectively. The corresponding starving groups surfaced only 163 times/ day and swam 65 and 130 m/day at the expense of 1.2 and 1.6 mg/g/day. Feeding and starving groups reduced the number of surfacing, when the distance they have to swim exceeded 0.8 m/day and increased the proportion of O₂ taken up branchially; the starving and feeding groups exposed to 60 cm depth surfaced only 70 and 271 times, swimming 84 and 325 m/day, at the energy cost of 2.9 and 17.6 mg/g/day. Feeding and conversion rates steadily increased from 16.9 mg dry liver/g live fish/day and 6.7 mg dry fish substance/g live fish/day in those exposed to the shallowest aquarium to 27.4 mg/g/day and 7.0 mg/g/day in those exposed t0 the maximum depth, respectively; conversion efficiency was 44% in the former and 28% in the latter; hence culturing H. fossilis in the shallow waters is profitable.     

Active and passive electrical properties of single bullfrog atrial cells

Single cells from the bullfrog (Rana catesbeiana) atrium have been prepared by using a modification of the enzymatic dispersion procedure described by Bagby et al. (1971. Nature [Long.]. 234:351--352) and Fay and Delise (1973. Proc. Natl. Acad. Sci. U.S.A. 70:641--645). Visualization of relaxed cells via phase-contrast or Nomarski optics (magnification, 400--600) indicates that cells range between 150 and 350 micrometers in length and 4 and 7 micrometers in diameter. The mean sarcomere length in relaxed, quiescent atrial cells in 2.05 micrometer. Conventional electrophysiological measurements have been made. In normal Ringer's solution (2.5 mM K+, 2.5 mM Ca++) acceptable cells have stable resting potentials of about -88 mV, and large (125 mV) long- duration (approximately 720 ms) action potentials can be elicited. The Vm vs. log[K+]0 relation obtained from isolated cells is similar to that of the intact atrium. The depolarizing phase of the action potential of isolated atrial myocytes exhibits two pharmacologically separable components: tetrodotoxin (10(-6) g/ml) markedly suppresses the initial regenerative depolarization, whereas verapamil (3 x 10(-6) M) inhibits the secondary depolarization and reduce the plateau height. A bridge circuit was used to estimate the input resistance (220 +/- 7 M omega) and time constant 20 +/- 7 ms) of these cells. Two- microelectrode experiments have revealed small differences in the electrotonic potentials recorded simultaneously at two different sites within a single cell. The equations for a linear, short cable were used to calculate the electrical constants of relaxed, single atrial cells: lambda = 921.3 +/- 29.5 micrometers; Ri = 118.1 +/- 24.5 omega cm; Rm = 7.9 +/- 1.2 x 10(3) omega cm2; Cm = 2.2 +/- 0.3 mu Fcm-2. These results and the atrial cell morphology suggest that this preparation may be particularly suitable for voltage-clamp studies.     

Vascular effects of caffeic acid phenethyl ester (CAPE) on isolated rat thoracic aorta

This study was aimed to investigate the vascular activity of caffeic acid phenethylester (CAPE), one of the major components of honeybee propolis. Experiments were performed on rat thoracic aortic rings, mounted in an isolated organ bath and connected to an isometric force transducer. The effect of CAPE (0.1-300 microM) was evaluated on tissue pre-contracted with phenylephrine (PE, 1 microM) or with KCl (100 mM). In another set of experiments, tissue was incubated with CAPE (1-100 microM) and responses to PE (0.01-3 microM) or KCl (60 mM) were evaluated. The effect of CAPE on cytosolic Ca(2+) concentration in aortic smooth muscle cells stimulated with PE or KCl was also evaluated. CAPE (0.1-300 microM) caused a concentration-dependent relaxation (pEC(50) 4.99 +/- 0.19; Emax 100.75 +/- 1.65%; n = 4) of tissue pre-contracted with PE that was reduced by endothelium removal or by incubation with N(omega)-nitro-L-arginine methyl ester (L-NAME, 100 microM). CAPE also relaxed KCl-precontracted tissue (pEC(50) 4.40 +/- 0.08; n = 4). CAPE inhibited contractile responses to PE or to KCl, and also inhibited the contractile response to PE obtained in a Ca(2+)-free medium. In addition, CAPE inhibited the increase in cytosolic Ca(2+) concentration triggered by stimulation of aortic smooth muscle cells with PE or KCl. Our results demonstrate a vascular activity for CAPE, that is only partially dependent on nitric oxide. Indeed, at high concentrations, CAPE vasorelaxant effect occurs also in absence of endothelium and it is likely due to an inhibitory effect on calcium movements through cell membranes.     

Cooperativity and intermediates in the equilibrium reactions of Fe(II,III) with ethanethiolate in N-methylformamide solution

The reaction of FeCl(2) or FeCl(3) with sodium ethanethiolate (SEt) in N-methylformamide (NMF) has been reevaluated to rectify a previous Fe(II) oxidation artifact. On titrating Fe(II) with EtS(-) concentrations up to 12 mol Eq, new features in the UV/vis spectrum (epsilon(344)=(3.1+/-0.2)x10(3) M(-1) cm(-1); epsilon(486)=(4.5+/-0.1)x10(2) M(-1) cm(-1)) indicated that the first observable step was the formation of a single complex different from the known tetrahedral tetrathiolate, [Fe(SEt)(4)](2-) . As the EtS(-) concentration increased past 12.5 mol Eq the UV/vis spectrum gradually transformed to that of [Fe(SEt)(4)](2-) (lambda(max)=314 nm). A Hill-formalism fit to the titration data of the initially formed complex indicated cooperative ligation by three ethanethiolate ions, with K(coop)=(1.7+/-0.1)x10(3) M(-3) and Hill "n"=2.4+/-0.1 (r=0.997). The 3:1 EtS(-)-Fe(II) complex is proposed to be [Fe(2)(SEt)(6)](2-). Titration of Fe(III) with EtS(-) showed direct cooperative formation of [Fe(SEt)(4)](-) [epsilon(340)=(3.4+/-0.5)x10(3) M(-1) cm(-1)] with a Hill-formalism K(coop)=(4.3+/-0.1)x10(2) M(-4) and a Hill coefficient "n"=3.7+/-0.2 (r=0.996). Further ligation past [Fe(SEt)(4)](-) was observed at EtS(-) concentrations above 35 mol Eq. The Fe(III) Hill constants are at variance with our previous report. However, the UV/vis spectrum of Fe(III) in NMF solution was found to change systematically over time, consistent with a slow progressive deprotonation of [Fe(nmf)](3+). The observed time-to-time differences in the equilibrium chemistry of Fe(III) with ethanethiolate in NMF thus reflect variation in the microscopic solution composition of FeCl(3) in alkaline NMF solvent. These results are related to the chemistry of nitrogenase FeMo cofactor in alkaline NMF solution.     

pH-induced conformational changes of the Fe(2+)-N epsilon (His F8) linkage in deoxyhemoglobin trout IV detected by the Raman active Fe(2+)-N epsilon (His F8) stretching mode.

To investigate heme-protein coupling via the Fe(2+)-N epsilon (His F8) linkage we have measured the profile of the Raman band due to the Fe(2+)-N epsilon (His F8) stretching mode (nu Fe-His) of deoxyHb-trout IV and deoxyHbA at various pH between 6.0 and 9.0. Our data establish that the band of this mode is composed of five different sublines. In deoxyHb-trout IV, three of these sublines were assigned to distinct conformations of the alpha-subunit (omega alpha 1 = 202 cm-1, omega alpha 2 = 211 cm-1, omega alpha 3 = 217 cm-1) and the other two to distinct conformations of the beta-subunit (omega beta 1 = 223 cm-1 and omega beta 2 = 228 cm-1). Human deoxyHbA exhibits two alpha-chain sublines at omega alpha 1 = 203 cm-1, omega alpha 2 = 212 cm-1 and two beta-chain sublines at omega beta 1 = 217 cm-1 and omega beta 2 = 225 cm-1. These results reveal that each subunit exists in different conformations. The intensities of the nu Fe-His sublines in deoxyHb-trout IV exhibit a significant pH dependence, whereas the intensities of the corresponding sublines in the deoxyHbA spectrum are independent on pH. This finding suggests that the structural basis of the Bohr effect is different in deoxyHbA and deoxyHb-trout IV. To analyse the pH dependence of the deoxyHb-trout IV sublines we have applied a titration model describing the intensity of each nu Fe-His subline as an incoherent superposition of the intensities from sub-sublines with the same frequency but differing intrinsic intensities due to the different protonation states of the respective subunit. The molar fractions of these protonation states are determined by the corresponding Bohr groups (i.e., pK alpha 1 = pK alpha 2 = 8.5, pK beta 1 = 7.5, pK beta 2 = 7.4) and pH. Hence, the intensities of these sublines reflect the pH dependence of the molar fractions of the involved protonation states. Fitting this model to the pH-dependent line intensities yields a good reproduction of the experimental data.(ABSTRACT TRUNCATED AT 400 WORDS)     

A cleft model for cardiac Purkinje strands.

Conduction of the action potential in cardiac muscle is complicated by its multicellular structure, with narrow intercellular clefts and cell-to-cell coupling. A model is developed from anatomical data to describe cardiac Purkinje strands of variable diameter and different internal arrangements of cells. The admittance of the model is solved analytically and fit to results of cable analysis. Using the extracted specific membrane and cell electrical parameters (Rm = 13 K omega cm2, Cm = 1.5 mu F/cm2, Ri = 100 mu cm, and Re = 50 omega cm), the model correctly predicted conduction velocity and filling of capacitance at the onset of a voltage step. The analysis permits more complete studies of the factors controlling conduction velocity; for instance, the effect on conduction velocity of a capacity in the longitudinal current circuit is discussed. Predictions of the impedance and phase angle were also made. Measurements of the frequency dependence of phase angle may provide a basis for separating cleft membrane properties from those of the surface membrane and may aid the measurement of nonlinear membrane properties in muscle.     

Effect of glycerin removal on the electrical resistance of isolated muscle fiber in the frog

Fibres isolated from iliofibularis muscles of the frog Rana esculenta were studied under current-clamp conditions with a double sucrose-gap technique. An increase of membrane resistance in muscle fibres (Rm) was demonstrated during the first 10-15 min of glycerol removal in K2SO4 solution. After a 30 min treatment in glycerol-containing K2SO4 Rm was 1.40 +/- 0.12 k omega X X cm2. The transfer of muscles from the glycerol-K2SO4 solution to an isotonic K2SO4 solution resulted in a progressive increase in the Rm which after a 15 minutes removal of glycerol reached the mean value of 2.02 +/- 0.22 k omega X cm2. It is suggested that this increase may reflect detubulation of the fibres caused by glycerol removal in muscles.     

A study of vibrational relaxation of B-state carbon monoxide in the heme pocket of photolyzed carboxymyoglobin.

The vibrational energy relaxation of dissociated carbon monoxide in the heme pocket of sperm whale myoglobin has been studied using equilibrium molecular dynamics simulation and normal mode analysis methods. Molecular dynamics trajectories of solvated myoglobin were run at 300 K for both the delta- and epsilon-tautomers of the distal histidine, His64. Vibrational population relaxation times were estimated using the Landau-Teller model. For carbon monoxide (CO) in the myoglobin epsilon-tautomer, for a frequency of omega0 = 2131 cm-1 corresponding to the B1 state, T1epsilon(B1) = 640 +/- 185 ps, and for a frequency of omega0 = 2119 cm-1 corresponding to the B2 state, T1epsilon(B2) = 590 +/- 175 ps. Although the CO relaxation rates in both the epsilon- and delta-tautomers are similar in magnitude, the simulations predict that the vibrational relaxation of the CO is faster in the delta-tautomer. For CO in the myoglobin delta-tautomer, it was found that the relaxation times were identical within error for the two CO substate frequencies, T1delta(B1) = 335 +/- 115 ps and T1delta(B2) = 330 +/- 145 ps. These simulation results are in reasonable agreement with experimental results of Anfinrud and coworkers (unpublished results). Normal mode calculations were used to identify the dominant coupling between the protein and CO molecules. The calculations suggest that the residues of the myoglobin pocket, acting as a first solvation shell to the CO molecule, contribute the primary "doorway" modes in the vibrational relaxation of the oscillator.     

Structural heterogeneity of the Fe(2+)-N epsilon (HisF8) bond in various hemoglobin and myoglobin derivatives probed by the Raman-active iron histidine stretching mode.

We have examined the Fe(2+)-N epsilon (HisF8) complex in hemoglobin A (HbA) by measuring the band profile of its Raman-active nu Fe-His stretching mode at pH 6.4, 7.0, and 8.0 using the 441-nm line of a HeCd laser. A line shape analysis revealed that the band can be decomposed into five different sublines at omega 1 = 195 cm-1, omega 2 = 203 cm-1, omega 3 = 212 cm-1, omega 4 = 218 cm-1, and omega 5 = 226 cm-1. To identify these to the contributions from the different subunits we have reanalyzed the nu Fe-His band of the HbA hybrids alpha(Fe)2 beta(Co)2 and alpha(Co)2 beta(Fe)2 reported earlier by Rousseau and Friedman (D. Rousseau and J. M. Friedman. 1988. In Biological Application on Raman Spectroscopy. T. G. Spiro, editor, 133-216). Moreover we have reanalyzed other Raman bands from the literature, namely the nu Fe-His band of the isolated hemoglobin subunits alpha SH- and beta SH-HbA, various hemoglobin mutants (i.e., Hb(TyrC7 alpha-->Phe), Hb(TyrC7 alpha-->His), Hb M-Boston and Hb M-Iwate), N-ethylmaleimide-des(Arg141 alpha) hemoglobin (NES-des(Arg141 alpha)HbA) and photolyzed carbonmonoxide hemoglobin (Hb*CO) measured 25 ps and 10 ns after photolysis. These molecules are known to exist in different quaternary states. All bands can be decomposed into a set of sublines exhibiting frequencies which are nearly identical to those found for deoxyhemoglobin A. Additional sublines were found to contribute to the nu Fe-His band of NES-des(Arg141 alpha) HbA and the Hb*CO species. The peak frequencies of the bands are determined by the most intensive sublines. Moreover we have measured the nu Fe-His band of deoxyHbA at 10 K in an aqueous solution and in a 80% glycerol/water mixture. Its subline composition at this temperature depends on the solvent and parallels that of more R-like hemoglobin derivatives. We have also measured the optical charge transfer band III of deoxyHbA at room temperature and found, that at least three subbands are required to fit its asymmetric band shape. This corroborates the findings on the nu Fe-His band in that it is indicative of a heterogeneity of the Fe(2+)-N epsilon(HisF8) bond. Finally we measured the nu Fe-His band of horse heart deoxyMb at different temperatures and decomposed it into three different sublines. In accordance with what was obtained for HbA their intensities rather than their frequencies are temperature-dependent.(ABSTRACT TRUNCATED AT 400 WORDS)     

The effect of local UVB skin irradiation on the rate of formazan deposition in the epidermis of hairless mice studied by means of a tetrazolium-reduction method

One-hundred-and-twenty hairless mice were irradiated with UVB (310 nm, exposure 60 mJ/cm2) on a limited area of the dorsal skin. At different time intervals after irradiation, the rate of endogenous dehydrogenase activity per mg dry epidermis was measured by the tetrazolium reduction method. The amount of formazan deposited remained normal for 18 h, and then increased, reaching a peak significantly higher than normal at 24 h, and thereafter returned to normal. At day 8 there was a new, probably significant peak. The reaction was followed for 14 days. It was concluded that UVB irradiation provokes a period of increased formazan deposition in the epidermis, similar to what has been observed after ionizing radiation and chemical carcinogens. The validity of the tetrazolium test for skin carcinogenic irritaments was thus also confirmed.     

Measurement of Electric Charges Carried by Bees: Evidence of Biological Variations

Various insects, especially social insects, possess electric charges. Erickson (1982, 1983) shows their involvement in the odor receptor efficiency of honey bee antenna. Also, the author suggests the importance of charges in the transfer of pollen grains from flowers to pollinator insects. To measure directly electric charges, we fit a sensor used to determine the charges of raindrops. Strongly clustered wintering bees and foraging bees were measured. The individual values range between ?400pC to +600pC (m = 153 +/105pC) during winter time. The foraging bees possess variable charges, generally smaller than wintering bees (m = 29 +/? 40pC). 7.0% of measured bees whole are charged negatively and less than 1% of these have no charges. The presence of electric charges throughout bees yearly cycle is significant for the insect society. Moreover electric forces contribute to explain some aspects of bee-parasite relationships.     

Thermal fluctuations between conformational substates of the Fe(2+)-HisF8 linkage in deoxymyoglobin probed by the Raman active Fe-N epsilon (HisF8) stretching vibration.

We have measured the VFe-His Raman band of horse heart deoxymyoglobin dissolved in an aqueous solution as a function of temperature between 10 and 300 K. The minimal model to which these data can be fitted in a statistically significant and physically meaningful way comprises four different Lorentzian bands with frequencies at 197, 209, 218, and 226 cm-1, and a Gaussian band at 240 cm-1, which exhibit halfwidths between 10 and 12.5 cm-1. All these parameters were assumed to be independent of temperature. The temperature dependence of the apparent total band shape's frequency is attributed to an intensity redistribution of the subbands at omega 1 = 209 cm-1, omega 2 = 218 cm-1, and omega 3 = 226 cm-1, which are assigned to Fe-N epsilon (HisF8) stretching modes in different conformational substrates of the Fe-HisF8 linkage. They comprise different out-of-plane displacements of the heme iron. The two remaining bands at 197 and 240 cm-1 result from porphyrin modes. Their intensity ratio is nearly temperature independent. The intensity ratio I3/I2 of the vFe-His subbands exhibits a van't Hoff behavior between 150 and 300 K, bending over in a region between 150 and 80 K, and remains constant between 80 and 10 K, whereas I2/I1 shows a maximum at 170 K and approaches a constant value at 80 K. These data can be fitted by a modified van't Hoff expression, which accounts for the freezing into a non-equilibrium distribution of substates below a distinct temperature Tf and also for the linear temperature dependence of the specific heat of proteins. The latter leads to a temperature dependence of the entropic and enthalpic differences between conformational substates. The fits to the intensity ratios of the vFe-His subbands yield a freezing temperature of Tf = 117 K and a transition region of delta T = 55 K. In comparison we have utilized the above thermodynamic model to reanalyze earlier data on the temperature dependence of the ratio Ao/A1 of two subbands underlying the infrared absorption band of the CO stretching vibration in CO-ligated myoglobin (A. Ansari, J. Berendzen, D. Braunstein, B. R. Cowen, H. Frauenfelder, M. K. Kong, I. E. T. Iben, J. Johnson, P. Ormos, T. B. Sauke, R. Scholl, A. Schulte, P. J. Steinbach, R. D. Vittitow, and R. D. Young, 1987, Biophys. Chem. 26:237-335).(ABSTRACT TRUNCATED AT 400 WORDS)