Characterization of a double dockerin from the cellulosome of the anaerobic fungus Piromyces equi.

The assembly into supramolecular complexes of proteins having complementary activities is central to cellular function. One such complex of considerable biological and industrial significance is the plant cell wall-degrading apparatus of anaerobic microorganisms, termed the cellulosome. A central feature of bacterial cellulosomes is a large non-catalytic protein, the scaffoldin, which contains multiple cohesin domains. An array of digestive enzymes is incorporated into the cellulosome through the interaction of the dockerin domains, present in the catalytic subunits, with the cohesin domains that are present in the scaffoldin. By contrast, in anaerobic fungi, such as Piromyces equi, the dockerins of cellulosomal enzymes are often present in tandem copies; however, the identity of the cognate cohesin domains in these organisms is unclear, hindering further biotechnological development of the fungal cellulosome. Here, we characterise the solution structure and function of a double-dockerin construct from the P. equi endoglucanase Cel45A. We show that the two domains are connected by a flexible linker that is short enough to keep the binding sites of the two domains on adjacent surfaces, and allows the double-dockerin construct to bind more tightly to cellulosomes than a single domain and with greater coverage. The double dockerin binds to the GH3 beta-glucosidase component of the fungal cellulosome, which is thereby identified as a potential scaffoldin.

Beyond the EX1 limit: probing the structure of high-energy states in protein unfolding.

Hydrogen exchange kinetics in native solvent conditions have been used to explore the conformational fluctuations of an immunoglobulin domain (CD2.domain1). The global folding/unfolding kinetics of the protein are unaltered between pH 4.5 and pH 9.5, allowing us to use the pH-dependence of amide hydrogen/deuterium exchange to characterise conformational states with energies up to 7.2kcal/mol higher than the folded ground state. The study was intended to search for discreet unfolding intermediates in this region of the energy spectrum, their presence being revealed by the concerted exchange behaviour of subsets of amide groups that become accessible at a given free energy, i.e. the spectrum would contain discreet groupings. Protection factors for 58 amide groups were measured across the pH range and the hydrogen-exchange energy profile is described. More interestingly, exchange behaviour could be grouped into three categories; the first two unremarkable, the third unexpected. (1) In 33 cases, amide exchange was dominated by rapid fluctuation, i.e. the free energy difference between the ground state and the rapidly accessed open state is sufficiently low that the contribution from crossing the unfolding barrier is negligible. (2) In 18 cases exchange is dominated by the global folding transition barrier across the whole pH range measured. The relationship between hydroxyl ion concentration and observed exchange rate is hyperbolic, with the limiting rate being that for global unfolding; the so-called EX1 limit. For these, the free energy difference between the folded ground state and any rapidly-accessed open state is too great for the proton to be exchanged through such fluctuations, even at the highest pH employed in this study. (3) For the third group, comprising five cases, we observe a behaviour that has not been described. In this group, as in category 2, the rate of exchange reaches a plateau; the EX1 limit. However, as the intrinsic exchange rate (k(int)) is increased, this limit is breached and the rate begins to rise again. This unintuitive behaviour does not result from pH instability, rather it is a consequence of amide groups experiencing two processes; rapid fluctuation of structure and crossing the global barrier for unfolding. The boundary at which the EX1 limit is overcome is determined by the equilibrium distribution of the fluctuating open and closed states (K(O/C)) and the rate constant for unfolding (k(u)). This critical boundary is reached when k(int)K(O/C)=k(u). Given that, in a simple transition state formalism: k(u)=K(#)k' (where K(#) describes the equilibrium distribution between the transition and ground state and k' describes the rate of a barrierless rearrangement), it follows that if the pH is raised to a level where k(int)=k', then the entire free energy spectrum from ground state to transition state could be sampled.

Cystatin forms a tetramer through structural rearrangement of domain-swapped dimers prior to amyloidogenesis.

The cystatins were the first amyloidogenic proteins to be shown to oligomerize through a 3D domain swapping mechanism. Here we show that, under conditions leading to the formation of amyloid deposits, the domain-swapped dimer of chicken cystatin further oligomerizes to a tetramer, prior to fibrillization. The tetramer has a very similar circular dichroism and fluorescence signature to the folded monomer and dimer structures, but exhibits some loss of dispersion in the 1H-NMR spectrum. 8-Anilino-1-naphthalene sulfonate fluorescence enhancement indicates an increase in the degree of disorder. While the dimerization reaction is bimolecular and most likely limited by the availability of a predominantly unfolded form of the monomer, the tetramerization reaction is first-order. The tetramer is formed slowly (t(1/2)=six days at 85 degrees C), dimeric cystatin is the precursor to tetramer formation, and thus the rate is limited by structural rearrangement within the dimer. Some higher-order oligomerization events parallel tetramer formation while others follow from the tetrameric form. Thus, the tetramer is a transient intermediate within the pathway of large-scale oligomerization.