Vladimir A. Shirokov

Membrane Protein Expression in Cell-Free Systems

Cell-free expression has emerged as a promising tool for the fast and efficient production of membrane proteins. The rapidly growing number of successfully produced targets in combination with the continuous development of new applications significantly promotes the distribution of this technology. Membrane protein synthesis by cell-free expression does not appear to be restricted by origin, size or topology of the target, and its global application is therefore a highly valuable characteristic. The technology is relatively fast to establish in standard biochemical labs, and it does not require expensive equipment. Moreover, it enables the production of membrane proteins in completely new modes, like the direct translation into detergent micelles, which is not possible with any other expression system. In this protocol, we focus on the currently most efficient cell-free expression system for membrane proteins based on Escherichia coli extracts.

Strategies for the cell-free expression of membrane proteins.

Cell-free expression offers an interesting alternative method to produce membrane proteins in high amounts. Elimination of toxicity problems, reduced proteolytic degradation and a nearly unrestricted option to supply potentially beneficial compounds like cofactors, ligands or chaperones into the reaction are general advantages of cell-free expression systems. Furthermore, the membrane proteins may be translated directly into appropriate hydrophobic and membrane-mimetic surrogates, which might offer significant benefits for the functional folding of the synthesized proteins. Cell-free expression is a rapidly developing and highly versatile technique and several systems of both, prokaryotic and eukaryotic origins, have been established. We provide protocols for the cell-free expression of membrane proteins in different modes including their expression as precipitate as well as their direct synthesis into detergent micelles or lipid bilayers.

Continuous-exchange protein-synthesizing systems.

Protein synthesis in cell-free systems is an emerging technology already competing with in vivo expression methods. In this chapter the basic principles of continuous-exchange protein synthesizing systems, and protocols for Escherichia coli and wheat germ translation and transcription-translation systems are described. The ways to improve substrate supply in cell-free systems and mRNA design for eukaryotic system are discussed. Correct folding of the synthesized protein is demonstrated and discussed in detail.

The molecular structure of the left-handed supra-molecular helix of eukaryotic polyribosomes.

During protein synthesis, several ribosomes bind to a single messenger RNA (mRNA) forming large macromolecular assemblies called polyribosomes. Here we report the detailed molecular structure of a 100 MDa eukaryotic poly-ribosome complex derived from cryo electron tomography, sub-tomogram averaging and pseudo-atomic modelling by crystal structure fitting. The structure allowed the visualization of the three functional parts of the polysome assembly, the central core region that forms a rather compact left-handed supra-molecular helix, and the more open regions that harbour the initiation and termination sites at either ends. The helical region forms a continuous mRNA channel where the mRNA strand bridges neighbouring exit and entry sites of the ribosomes and prevents mRNA looping between ribosomes. This structure provides unprecedented insights into protein- and RNA-mediated inter-ribosome contacts that involve conserved sites through 40S subunits and long protruding RNA expansion segments, suggesting a role in stabilizing the overall polyribosomal assembly.

Formation of circular polyribosomes on eukaryotic mRNA without cap-structure and poly(A)-tail: a cryo electron tomography study

The polyribosomes newly formed on recombinant GFP-encoding mRNAs in a wheat germ cell-free translation system were analyzed using cryo-electron tomography, with sub-tomogram averaging of polysomal ribosomes and reconstruction of 3D structures of individual polyribosomes. The achieved level of resolution in the reconstructed polyribosomes allowed deducing the mRNA path by connecting adjacent exit and entry sites at the ribosomes inside each polyribosome. In this way, the circularity of a significant fraction (about 50%) of translating polyribosomes was proved in the case of the capped poly(A)-tailed mRNA, in agreement with the existing paradigm of the circularization via interaction of cap-bound initiation factor eIF4F with poly(A)-binding protein. However, translation of the capped mRNA construct without poly(A) tail, but with unspecific 3′-UTR derived from non-coding plasmid sequence, also led to the formation of circular polyribosomes in similar proportion (40%). Moreover, the polyribosomes formed on the uncapped non-polyadenylated mRNA with non-synergistic 5′- and 3′-UTRs proved to be circular as well, and appeared in the same proportion as in the previous cases. Thus, the formation of circular polyribosomes was found to be virtually independent of the presence of cap structure and poly(A) tail in mRNA, in contrast to the longstanding paradigm in the field.

Conformation transitions of eukaryotic polyribosomes during multi-round translation

Using sedimentation and cryo electron tomography techniques, the conformations of eukaryotic polyribosomes formed in a long-term cell-free translation system were analyzed over all the active system lifetime (20–30 translation rounds during 6–8 h in wheat germ extract at 25°C). Three distinct types of the conformations were observed: (i) circular polyribosomes, varying from ring-shaped forms to circles collapsed into double rows, (ii) linear polyribosomes, tending to acquire planar zigzag-like forms and (iii) densely packed 3D helices. At the start, during the first two rounds of translation mostly the circular (ring-shaped and double-row) polyribosomes and the linear (free-shaped and zigzag-like) polyribosomes were formed (‘juvenile phase’). The progressive loading of the polyribosomes with translating ribosomes induced the opening of the circular polyribosomes and the transformation of a major part of the linear polyribosomes into the dense 3D helices (‘transitional phase’). After 2 h from the beginning (about 8–10 rounds of translation) this compact form of polyribosomes became predominant, whereas the circular and linear polyribosome fractions together contained less than half of polysomal ribosomes (‘steady-state phase’). The latter proportions did not change for several hours. Functional tests showed a reduced translational activity in the fraction of the 3D helical polyribosomes.

Topology of mRNA chain in isolated eukaryotic double-row polyribosomes

In the process of protein synthesis, the translating ribosomes of eukaryotic cells form polyribosomes that are found to be multiplex functional complexes possessing elements of ordered spatial organization. As revealed by a number of electron microscopy studies, the predominant visible configurations of the eukaryotic polyribosomes are circles (circular polyribosomes) and two-stranded formations (so-called double-row polyribosomes). The “long” (i.e. heavy loaded) polyribosomes are usually represented by double-row structures, which can be interpreted as either topologically circular (“col-lapsed rings”), or topologically linear (zigzags or helices). In the present work we have analyzed the mRNA path within the eukaryotic polyribosomes, isolated from a wheat germ cell-free translation system, by integrating two approaches: the visualization of mRNA ends in polyribosomes by marking them with gold nanoparticles (3′-end) and initiating 40S subunits (5′-end), as well as by the cryoelectron tomography. Examination of the location of the mRNA markers in polyribosomes and mutual orientation of ribosomes in them has shown that the double-row polyribosomes of the same sample can have both circular and linear arrangements of their mRNA.

Anomalies of piezoelectric coefficients in barium titanate thin films

Modeling of electromechanical devices involves the use of different material coefficients, whose measurement is a difficult task, especially when the problem concerns thin films. Required coefficients of thin films could be found theoretically, using known values of the bulk constants. Electromechanical coefficients of barium titanate thin films are still unknown; therefore, it is expedient to carry out their calculations. We give here the full set of electromechanical coefficients of barium titanate thin films for the whole range of technologically available misfit strains. In the present paper, piezoelectric coefficients as functions of a misfit strain were calculated. It was revealed that piezoelectric coefficients exhibit anomalies at phase boundaries and inside the monoclinic r-phase as well. The obtained results allow finding the required values of the thin-film parameters, varying the misfit strain.

Continuous-Flow and Continuous-Exchange Cell-Free Translation Systems and Reactors

Progress in biotechnology generates a growing demand for convenient and productive technologies of gene expression on preparative scale. In vivo systems for expression of foreign genes in bacterial or eukaryotic cells are efficient and widely used. However, difficulties associated with cytotoxicity, proteolytic degradation or improper folding and aggregation of synthesized proteins are often encountered in vivo. The in vivo expression systems are restricted by mechanisms of cell control and allow limited opportunities for solving these problems. On the other hand, gene expression in vitro, in cell-free translation or transcription-translation systems, is an alternative that allows full control and high flexibility of conditions.

Control of acoustic properties of a BaTiO3 thin film by a planar electric field

An influence of a planar electric field on material coefficients of a barium titanate film has been studied. Electric-field dependences of dielectric constants, elastic and piezoelectric moduli were built for the (001)-oriented film on a cubic substrate with a misfit strain value equal to . It was revealed that an electromechanical coupling coefficient, k 11, has a maximum at some value of the electric field, which depends on the clamping stress. The misfit strain dependence of the maximum value of the k 11 coefficient was studied at strains below (c-phase).