Resolving intrinsically disordered proteins of the cancer genome with ion mobility mass spectrometry

For proteins the link between their structure and their function is a central tenet of biology. A common approach to understanding protein function is to ‘solve’ its structure and subsequently probe interactions between the protein and its binding partners. The first part of this approach is non-trivial for proteins where localised regions or even their entire structure fail to fold into a three-dimensional structure and yet they possess function. These so called intrinsically or inherently disordered proteins (IDP’s) or intrinsically disordered regions (IDR’s) constitute up to 40% of all expressed proteins. IDPs which have crucial roles in molecular recognition, assembly, protein modification and entropic chain activities, are often dynamic with respect to both conformation and interaction, so in the course of a protein’s ‘lifespan’ it will sample many configurations and bind to several targets. For these proteins, there is a need to develop new methods for structure characterization which exploit their biophysical properties. The solvent free environment of a mass spectrometer is ideally suited to the study of intrinsic interactions and how they contribute to structure. Ion mobility mass spectrometry is uniquely able to observe the range of structures an IDP can occupy, and also the effect of selected binding partners on altering this conformational space. This thesis details the technique of ion mobility mass spectrometry and illustrates its use in assessing the relative disorder of p53 protein. The tumour suppressor p53 is at the hub of a plethora of signalling pathways that maintain the integrity of the human genome and regulate the cell cycle. Deregulation of this protein has a great effect on carcinogenesis as mutated p53 can induce an amplified epigenetic instability of tumour cells, facilitating and accelerating the evolution of the tumour. Herein mass spectrometry provides a compelling, detailed insight into the conformational flexibility of the p53 DNA-binding domain. The plasticity of the p53 DNA-binding domain is reflected in the existence of more than one conformation, independent of any conformational changes prompted by binding. The in vacuo conformational phenotypes exhibited by common cancer-associated mutations are determined and the second-site suppressor mutation from loop L1, H115N, is probed whether it could trigger conformational changes in p53 hotspot cancer mutations. The structural basis of the binding promiscuity of p53 protein is investigated; of particular interest is the molecular interaction of the p53 N-terminus with the oncoprotein murine double minute 2, as well as with the antiapoptotic factor B-cell lymphoma-extralarge

Structural studies of metal ligand complexes by ion mobility-mass spectrometry

Collision cross sections (CCS) have been measured for three salen ligands, and their complexes with copper and zinc using travelling-wave ion mobility-mass spectrometry (TWIMS) and drift tube ion mobility-mass spectrometry (DTIMS), allowing a comparative size evaluation of the ligands and complexes. CCS measurements using TWIMS were determined using peptide and TAAH calibration standards. TWIMS measurements gave significantly larger CCS than DTIMS in helium, by 9 % for TAAH standards and 3 % for peptide standards, indicating that the choice of calibration standards is important in ensuring the accuracy of TWIMS-derived CCS measurements. Repeatability data for TWIMS was obtained for inter- and intra-day studies with mean RSDs of 1. 1 % and 0. 7 %, respectively. The CCS data obtained from IM-MS measurements are compared to CCS values obtained via the projection approximation, the exact hard spheres method and the trajectory method from X-ray coordinates and modelled structures using density functional theory (DFT) based methods. © 2013 Springer-Verlag Berlin Heidelberg

Structural studies of metal ligand complexes by ion mobility-mass spectrometry

The final publication is available at Springer via http://dx.doi.org/10.1007/s12127-013-0122-8Collision cross sections (CCS) have been measured for three salen ligands, and their complexes with copper and zinc using travelling-wave ion mobility-mass spectrometry (TWIMS) and drift tube ion mobility-mass spectrometry (DTIMS), allowing a comparative size evaluation of the ligands and complexes. CCS measurements using TWIMS were determined using peptide and TAAH calibration standards. TWIMS measurements gave significantly larger CCS than DTIMS in helium, by 9 % for TAAH standards and 3 % for peptide standards, indicating that the choice of calibration standards is important in ensuring the accuracy of TWIMS-derived CCS measurements. Repeatability data for TWIMS was obtained for inter- and intra-day studies with mean RSDs of 1. 1 % and 0. 7 %, respectively. The CCS data obtained from IM-MS measurements are compared to CCS values obtained via the projection approximation, the exact hard spheres method and the trajectory method from X-ray coordinates and modelled structures using density functional theory (DFT) based methods. © 2013 Springer-Verlag Berlin Heidelberg

The use of Ion Mobility Mass Spectrometry to probe Modulation of Function of p53 and of MDM2 by Small Molecule Inhibitors

Developing drug-like molecules to inhibit the interactions formed by disordered proteins is sought after but challenging due in part to the lack of solved structures from conformationally dynamic systems. Ion Mobility Mass Spectrometry (IM-MS) is well positioned to assess protein ligand interactions along with the effect of a given inhibitor on conformation. Here we demonstrate the use of IM-MS to characterize the effect of two inhibitors RITA and Nutlin-3 on their respective binding partners: p53 and MDM2. RITA binds N-terminal transactivation domain of p53 (Np53) weakly, preventing direct observation of the complex in the gas phase. Nonetheless, upon incubation with RITA, we observe an alteration in the charge state distribution and in the conformational distributions adopted by Np53 in the gas phase. This finding supports the hypothesis that RITAs mode of action is via a conformational change in p53. Circular dichroism corroborates our gas phase findings, showing a slight increase in secondary structure content on ligand incubation, and HDX-MS experiments also highlight the dynamic properties of this protein. Using the same approach we present data to show the effect of Nutlin-3 binding to MDM2. MDM2 presents as two conformational families in the absence of Nutlin-3. Upon Nutlin-3 binding, the protein undergoes a compaction event similar to that exhibited by RITA on Np53. This multi-technique approach highlights the inherent disorder in these systems; and exemplifies the power of IM-MS as a technique to study transient interactions between small molecule inhibitors and oncogenic intrinsically disordered proteins

Intrinsic disorder in proteins: a challenge for (un)structural biology met by ion mobility-mass spectrometry

The link between structure and function of a given protein is a principal tenet of biology. The established approach to understand the function of a protein is to ‘solve’ its structure and subsequently investigate interactions between the protein and its binding partners. However, structure determination via crystallography or NMR is challenging for proteins where localized regions or even their entire structure fail to fold into a three-dimensional form. These so called IDPs (intrinsically disordered proteins) or intrinsically disordered regions constitute up to 40% of all expressed proteins, and a much higher percentage in proteins involved in the proliferation of cancer. For these proteins, there is a need to develop new methods for structural characterization which exploit their biophysical properties. IM (ion mobility)–MS is uniquely able to examine both absolute conformation(s), populations of conformation and also conformational change, and is therefore highly applicable to the study of IDPs. The present article details the technique of IM–MS and illustrates its use in assessing the relative disorder of the wild-type p53 DNA-core-binding domain of cellular tumour antigen p53. The IM data were acquired on a Waters Synapt HDMS instrument following nESI (nanoelectrospray ionization) from ‘native’ and low-pH solution conditions.</jats:p

Effects of Drift Gas on Collision Cross Sections of a Protein Standard in Linear Drift Tube and Traveling Wave Ion Mobility Mass Spectrometry

There has been a significant increase in the use of ion mobility mass spectrometry (IM-MS) to investigate conformations of proteins and protein complexes following electrospray ionization. Investigations which employ traveling wave ion mobility mass spectrometry (TW IM-MS) instrumentation rely on the use of calibrants to convert the arrival times of ions to collision cross sections (CCS) providing “hard numbers” of use to structural biology. It is common to use nitrogen as the buffer gas in TW IM-MS instruments and to calibrate by extrapolating from CCS measured in helium via drift tube (DT) IM-MS. In this work, both DT and TW IM-MS instruments are used to investigate the effects of different drift gases (helium, neon, nitrogen, and argon) on the transport of multiply charged ions of the protein myoglobin, frequently used as a standard in TW IM-MS studies. Irrespective of the drift gas used, recorded mass spectra are found to be highly similar. In contrast, the recorded arrival time distributions and the derived CCS differ greatly. At low charge states (7 ≤ <i>z</i> ≤ 11) where the protein is compact, the CCS scale with the polarizability of the gas; this is also the case for higher charge states (12 ≤ <i>z</i> ≤ 22) where the protein is more unfolded for the heavy gases (neon, argon, and nitrogen) but not the case for helium. This is here interpreted as a different conformational landscape being sampled by the lighter gas and potentially attributable to increased field heating by helium. Under nanoelectrospray ionization (nESI) conditions, where myoglobin is sprayed from an aqueous solution buffered to pH 6.8 with 20 mM ammonium acetate, in the DT IM-MS instrument, each buffer gas can yield a different arrival time distribution (ATD) for any given charge state