The interactions of several water-soluble ionic porphyrins with different ionic or neutral surfactants in aqueous solutions were studied as a function of surfactant concentration. The interaction leads to the formation of porphyrin aggregates and/or micelle-encapsulated monomers with the exception of those porphyrin−surfactant pairs for which the interaction is Coulombically repulsive. The premicellar surfactant−porphyrin aggregate is identified by absorption and fluorescence spectroscopy, fluorescence lifetime and anisotropy, and resonance light scattering. The spectroscopic results are used to characterize the premicellar aggregates as J-type, H-type, or nonspecific aggregates. All premicellar surfactant−porphyrin aggregates dissociate to form micelle-encapsulated monomers when the surfactant concentration approaches cmc (critical micellar concentration). The interaction of tetrakis-(4-sulfanatophenyl)porphine dianion (H4TPPS2-) at pH <3.5 with cetyltrimethylammonium cation (CTAB) is described by the following sequential equlibria controlled by the surfactant concentration: M ⇌ J ⇌ H ⇌ Mm. The stoichiometric ratio of porphyrin/surfactant is 1:2 for the J-aggregate and ∼1:4 for the H-aggregate. Kinetic intermediates were also observed prior to the formation of the J-aggregate. The J-aggregate exhibits circular dichroism (spontaneous chirality, not seen in H-type or micellar aggregates), intense resonance light scattering, low fluorescence quantum yield and lifetime, and unusually high fluorescence anisotropy.
Detailed circular dichroism and fluorescence studies at different pHs have been carried out to monitor thermal unfolding of horseradish peroxidase isoenzyme c (HRPc). The change in CD in the 222 nm region corresponds to changes in the overall secondary structure of the enzyme, while that in the 400 nm region (Soret region) corresponds to changes in the tertiary structure around the heme in the enzyme. The temperature dependence of the tertiary structure around the heme also affected the intrinsic tryptophan fluorescence emission spectrum of the enzyme. The results suggested that melting of the tertiary structure to a pre-molten globule form takes place at 45 degrees C, which is much lower than the temperature (T(m) = 74 degrees C) at which depletion of heme from the heme cavity takes place. The melting of the tertiary structure was found to be associated with a pK(a) of approximately 5, indicating that this phase possibly involves breaking of the hydrogen-bonding network of the heme pocket, keeping the heme moiety still inside it. The stability of the secondary structure of the enzyme was also found to decrease at pH below 4.5. A 'high temperature' unfolding phase was observed which was, however, independent of pH. The stability of the secondary structure was found to drastically decrease in the presence of DTT (dithiothreitol), indicating that the 'high temperature' form is possibly stabilized due to interhelical disulfide bonds. Depletion of Ca(2+) ions resulted in a marked decrease in the stability of the secondary structure of the enzyme.
The mechanism of unfolding of ferricytochrome c induced by the surfactant sodium dodecyl sulfate has been studied by heme absorption, tryptophan fluorescence, circular dichroism, resonance Raman scattering, stopped-flow and time-resolved resonance energy transfer to obtain a comprehensive view of the whole process. Unfolding occurred at an almost specific molecular ratio of SDS/cytochrome c in the concentration range (20Ϫ50 µM) studied here. However there appears to be a point at Ϸ0.6 mM SDS where unfolding begins to occur for lower cytochrome c concentrations. The kinetics of unfolding revealed only a single transition with a rate constant of 33 s Ϫ1 (at 298 K, [SDS] ϭ 8.7 mM) and activation energy barrier of Ϸ 16 kJ/mol, indicating that other associated steps, if any, are too fast to be significantly populated. The free energy change (∆G°) involved with the unfolding transition was estimated to be about 16.8 kJ/mol. The CD spectrum at 220 nm of SDS-unfolded cytochrome c shows only a partial decrease (25%), indicating that a significant amount of helical structure remains folded in contrast to a complete loss of helical structure in GdnHCl-denatured cytochrome c. The heme structure in SDS-unfolded cytochrome c, as deduced from heme absorption and resonance Raman spectra, shows a major population (Ϸ95%) of mis-ligated histidine to the heme which acts as a kinetic trap in the folding process. The structural changes associated with cytochrome c unfolding were also monitored by time-resolved resonance energy transfer which shows a drastic increase in tryptophan fluorescence lifetime from 12 ps in the native protein to 0.63 ns in the unfolded one, associated with a movement of Trp59 by 10 Å away from heme. The maximum entropy method analysis of fluorescence decay indicated the growth of various conformational substates in SDS-unfolded cytochrome c in contrast to narrowly distributed conformations in the native protein. The refolding was comprised of three kinetic steps; the first was significantly fast (Ϸ8 ms) and was assigned to the dissociation of His26 that paves the protein towards correct folding pathway. The other two slower steps probably arise from chain misorganization and prolyl isomerization. The absence of a burst-phase amplitude supports the idea that the burst phase observed in the folding from completely unfolded cytochrome c corresponds to a molecular collapse that produces significant secondary structure. The partially unfolded state represents a unique intermediate state in the folding pathway.
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