α-Helix-to-random-coil transitions of two-chain coiled coils: Experiments on the thermal denaturation of ββ tropomyosin cross-linked selectively at C-190

A method is described for preparation of a species of β tropomyosin that is sulfhydryl-blocked at C36 and disulfide-cross-linked at C190. Five steps are involved: (1) Rabbit skeletal muscle tropomyosin, comprising αα and αβ species, is oxidized with ferricyanide, disulfide-cross-linking both species at C190. (2) The product is treated with iodoacetamide, blocking the only remaining free sulfhydryl, i.e., C36 of the β-chains. (3) The C36-blocked, C190-cross-linked product is reduced with dithiothreitol (DTT), unfolded in urea, and α and β chains separated by ion-exchange chromatography. (4) The C36-blocked β chains are refolded by dialysis. (5) The refolded, C36-blocked ββ species are cross-linked at C190 by ferricyanide oxidation. The resulting C36-blocked, C190-cross-linked ββ product is separated from contaminating species—mostly completely blocked β-chains and multichain cross-linked molecules—by size-exclusion chromatography in denaturing (guanidinium chloride) solvent. The five-step process and the final product were monitored by titration of free sulfhydryls and by NaDodSO₄/polyacrylamide gel electrophoresis (PAGE). Thermal unfolding curves from CD are reported for the resulting pure, C36-blocked, C190-cross-linked ββ species and for its DTT-reduction product, the noncross-linked C36-blocked species. The latter shows almost the same thermal unfolding transition as intact, noncross-linked ββ species. The former shows a pretransition similar to, but larger in extent than, the one well known to occur in the analogous case of C190-cross-linked αα tropomyosin. These unfolding transitions are compared with one another and with that previously reported for doubly cross-linked (at C36 and C190) ββ species. These comparisons are made in the light of current physical models for coiled-coil unfolding equilibria. It is concluded that although no extent model is demonstrably satisfactory, any successful model must include strain at the cross-link, loop entropy, and regional nonuniformities as essential parts of the physics.