| Literature DB >> 31179287 |
David Gnutt1,2, Linda Sistemich2, Simon Ebbinghaus1,2.
Abstract
Cytomimetic media are used to mimic the physicochemical properties of the cellular milieu in an in vitro experiment. The motivation is that compared to entire cells, they can be used efficiently in combination with a broad range of experimental techniques. However, the development and use of cytomimetic media is hampered by the lack of in-cell data that could be used as a hallmark to directly evaluate and improve the performance of cytomimetic media in different applications. Such data must include the study of specific biomolecular reactions in different cell types, different compartments of a single cells and different cellular conditions. In previous studies, model systems such as cancer cell lines, bacteria or oocytes were used. Here we studied how the environment of cells that undergo neuronal differentiation or proteostasis stress modulates the protein folding equilibrium. We found that NGF induced differentiation leads to a decrease of the melting temperature and a change of the folding mechanism. Proteomic changes that occur upon differentiation could explain this effect, however, we found that the crowding effect remained unchanged. Using MG132, a common proteasome inhibitor and inducer of the unfolded protein response, we show that changes to the quality control machinery modulate the folding equilibrium, leading to protein destabilization at prolonged stress exposure. Our study explores the range of protein folding modulation within cells subject to differentiation or stress that must be encountered in the development of cytomimetic media.Entities:
Keywords: Macromolecular crowding; cytomimetic media; fast relaxation imaging (FReI); in-cell spectroscopy; protein folding and stability
Year: 2019 PMID: 31179287 PMCID: PMC6544126 DOI: 10.3389/fmolb.2019.00038
Source DB: PubMed Journal: Front Mol Biosci ISSN: 2296-889X
Figure 1(A) Exemplary SOD1*G41D transfected cell after 7 d incubation with 100 ng L−1 NGF. For better visualization, an intensity scaled version is shown. On the bottom, a control cell is shown without NGF treatment. (B) A/D ratio of the genetic crowding sensor (Boersma et al., 2015) in HeLa as well as PC12 cells (Figure S1) (C) Melting temperatures in differentiated and undifferentiated PC12 cells. (D) Cooperativity parameter δg1 in differentiated and undifferentiated PC12 cells. (E) ΔGf in differentiated and undifferentiated PC12 cells. For comparison, the mean value of HeLa cell measurements is depicted [blue line (3.2 ± 0.5) kJ mol−1 (data shown from reference Gnutt et al., 2019)]. Each data point represents a single cell measurement (B–E). Statistical significance was tested using either Welch's unpaired t-test (B–D) or a non-parametric Kruskal-Wallis test followed by a post-hoc Dunn's test for multiple comparisons (E). **p < 0.01.
Figure 2(A) HeLa cells transfected with SOD1*G41D were treated with 10 μM MG132 for different timepoints. Morphological differences could be observed after ~18 h incubation. Scale bar 30 μm. (B) Melting temperature, ΔGf and cooperativity parameter δg1 in MG132 treated cells. Each data point represents a single cell measurement. Error bars depict mean and s.d. (C) Exemplary D/A unfolding curve for a control cell and a cell treated with 10 μM MG132 for 24 h which showed a temperature triggered aggregation behavior. (D) A/D ratio of the genetic crowding sensor in MG132 treated cells. Each data point represents a single cell measurement (B,D). Statistical significance was tested using a non-parametric Kruskal-Wallis test followed by a post-hoc Dunn's test for multiple comparisons. Asterisks denote differences towards the untreated control (0h). *** p < 0.001, ** p < 0.01.