Abstract
The goal of native mass spectrometry is to obtain information on non-covalent interactions in solution through mass spectrometry measurements in the gas phase. Characterizing intramolecular folding re-quires using structural probing techniques such as ion mobility spectrometry. However, inferring solu-tion structures of nucleic acids is difficult because the low-charge state ions produced from aqueous solutions at physiological ionic strength get compacted during electrospray. Here we explored whether native supercharging could produce higher charge states that would better reflect solution folding, and whether the voltage required for collision-induced unfolding (CIU) could reflect preserved intramolec-ular hydrogen bonds. We studied pH-responsive i-motif structures, with or without a hairpin in the loop, and unstructured controls. We also implemented a multivariate curve resolution procedure to extract physically meaningful pure components from the CIU data and reconstruct unfolding curves. We found that the relative unfolding voltages reflect preserved intramolecular hydrogen bonds, espe-cially at higher charge states. However, we uncovered several caveats in data interpretation: (1) un-structured controls also undergo unfolding, and the base composition influences the unfolding voltage, (2) changing the solution pH also unexpectedly changed the unfolding voltage, and (3) the ion mobility patterns become more complicated when two structures are present simultaneously, such as an i-motif and a harpin, because of opposite effects on the collision cross section upon activation. Reaching phos-phate charging densities over 0.25 makes it easier to discriminate between structures, and the use of native supercharging agents is thus essential. In short, we investigated in detail the potential and limi-tations of native ion mobility to deduce solution folding of nucleic acids structures.
Supplementary materials
Title
supporting information
Description
Supplementary CD melting, NMR spectroscopy, mass spectra, collision cross section distributions, collision-induced unfolding, and full set of components (CCS distributions) and CIU transitions ob-tained by MCR-ALS
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