Conformational Effects of a Cancer-Linked Mutation in Pri-miR-30c RNA.

MicroRNAs (miRNAs) are small, noncoding RNAs that mediate post-transcriptional downregulation of specific target genes. These transcripts are the products of a two-step processing pathway; primary miRNAs (pri-miRNAs) are processed by Drosha into individual precursor miRNA (pre-miRNA) hairpins, which are subsequently processed by Dicer into mature miRNAs. Single nucleotide polymorphisms (SNPs) that occur in pri-miRNAs, pre-miRNAs and mature miRNAs have been shown to affect the processing of specific target genes by modulating Drosha and Dicer processing or interactions with RNA binding proteins (RBPs). Using NMR and single-molecule optical tweezer experiments, we have investigated the conformational effects of a cancer-linked G/A mutation in the terminal loop of pri-miR-30c RNA, and how this influences binding by the SRSF3 and hnRNP A1 RBPs, which are implicated in its processing. Our results reveal that the wildtype and G/A variant pri-miR-30c RNAs adopt very similar elongated stem-loop structures, both of which are bound by SRSF3. However, while both wildtype and G/A pri-miR-30c RNAs can form dimeric kissing hairpin structures, the G to A mutation results in partial destabilization of the dimer in the variant transcript. This promotes recognition and binding by hnRNP A1, an RBP that enhances pri-miR-30c processing. Our data provide structural insight into the conformational effects of a G/A mutation in pri-miR-30c RNA and how this could affect processing and promote cancer.

Mechanotransduction in hippocampal neurons operates under localized low picoNewton forces.

There is growing evidence suggesting that mechanical properties of CNS neurons may play an important regulatory role in cellular processes. Here, we employ an oscillatory optical tweezers (OOT) to exert a local indentation with forces in the range of 5-50 pN. We found that single local indentation above a threshold of 13 ± 1 pN evokes a transient intracellular calcium change, whereas repeated mechanical stimulations induce a more sustained and variable calcium response. Importantly, neurons were able to differentiate the magnitude of mechanical stimuli. Chemical perturbation and whole-cell patch clamp recordings suggest that mechanically evoked response requires the influx of extracellular calcium through transmembrane ion channels. Moreover, we observed a mechanically evoked activation of the CAMKII and small G protein RhoA. These results all together suggest that mechanical signaling among developed neurons fully operates in neuronal networks under physiological conditions.

Calcium flares and compartmentalization in rod photoreceptors.

Rod photoreceptors are composed of a soma and an inner segment (IS) connected to an outer segment (OS) by a thin cilium. OSs are composed of a stack of ∼800 lipid discs surrounded by the plasma membrane where phototransduction takes place. Intracellular calcium plays a major role in phototransduction and is more concentrated in the discs, where it can be incorporated and released. To study calcium dynamics in rods, we used the fluorescent calcium dye CaSiR-1 AM working in the near-infrared (NIR) (excitation at 650 and emission at 664 nm), an advantage over previously used dyes. In this way, we investigated calcium dynamics with an unprecedented accuracy and most importantly in semidark-adapted conditions. We observed light-induced drops in [Ca2+]i with kinetics similar to that of photoresponses recorded electrophysiologically. We show three properties of the rods. First, intracellular calcium and key proteins have concentrations that vary from the OS base to tip. At the OS base, [Ca2+]i is ∼80 nM and increases up to ∼200 nM at the OS tip. Second, there are spontaneous calcium flares in healthy and functional rod OSs; these flares are highly localized and are more pronounced at the OS tip. Third, a bright flash of light at 488 nm induces a drop in [Ca2+]i at the OS base but often a flare at the OS tip. Therefore, rod OSs are not homogenous structures but have a structural and functional gradient, which is a fundamental aspect of transduction in vertebrate photoreceptors.

Mechanosensitivity is an essential component of phototransduction in vertebrate rods.

Photoreceptors are specialized cells devoted to the transduction of the incoming visual signals. Rods are able also to shed from their tip old disks and to synthesize at the base of the outer segment (OS) new disks. By combining electrophysiology, optical tweezers (OTs), and biochemistry, we investigate mechanosensitivity in the rods of Xenopus laevis, and we show that 1) mechanosensitive channels (MSCs), transient receptor potential canonical 1 (TRPC1), and Piezo1 are present in rod inner segments (ISs); 2) mechanical stimulation-of the order of 10 pN-applied briefly to either the OS or IS evokes calcium transients; 3) inhibition of MSCs decreases the duration of photoresponses to bright flashes; 4) bright flashes of light induce a rapid shortening of the OS; and 5) the genes encoding the TRPC family have an ancient association with the genes encoding families of protein involved in phototransduction. These results suggest that MSCs play an integral role in rods' phototransduction.

Corrigendum: Cell Mechanotransduction With Piconewton Forces Applied by Optical Tweezers.

[This corrects the article on p. 130 in vol. 12, PMID: 29867363.].

Cell Mechanotransduction With Piconewton Forces Applied by Optical Tweezers.

Mechanical stresses are always present in the cellular environment and mechanotransduction occurs in all cells. Although many experimental approaches have been developed to investigate mechanotransduction, the physical properties of the mechanical stimulus have yet to be accurately characterized. Here, we propose a mechanical stimulation method employing an oscillatory optical trap to apply piconewton forces perpendicularly to the cell membrane, for short instants. We show that this stimulation produces membrane indentation and induces cellular calcium transients in mouse neuroblastoma NG108-15 cells dependent of the stimulus strength and the number of force pulses.