Douglas J. Tobias’s research while affiliated with University of California, Irvine and other places

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Publications (298)


Snapshots of restrained fibers consisting of c) 100% CSSC with all CSSC restrained and a,b) 70% CSSC with (b) all CSH/CSSC and (c) only CSSC heavy atoms restrained radially at 27 Å. d) Volume fraction, defined as the ratio between the volume of all atoms from CSH/CSSC in the largest aggregate, as determined by network analysis, and that of a 27 Å radius fiber cylinder, over time in each simulation. The cylinder length is determined using half of the maximum heavy atom number density along the axis at the two ends of the fibers. Fibers, created under cryo‐EM‐informed restraints, are stable and exhibit densities similar to aggregates observed in unrestrained simulations.[⁸]
Snapshots illustrating the definitions of a) axial and b) radial directions. Heavy atom distribution of CSSC, CSH, and water for each of the three simulations: c,d) for 100% CSSC, e,f) for 70% CSSC, and g,h) for 70% CSSC with only CSSC restrained, along the axial and radial directions, respectively. The distributions of CSH and CSSC are uniform along both the axial and radial directions of the fiber. Water is present throughout the fiber and shows an enhanced presence near the center. The smooth drop‐off in the density profile around the restrained distance value (≈27 Å) is typical of a fluid interface, which suggest that the applied restraints do not influence the configuration of the fiber/solvent interface.
Heavy atom distribution of small moieties (see Scheme 1) for each of the two simulations: a,b) for 100% CSSC, and c,d) for 70% CSSC, along the axial and radial directions, respectively. The distribution of moieties is largely uniform, and the number density of amide groups is higher than that of the phenyl and thiol near the edges of the fibers.
Direct comparison of fibers observed in real cryo‐EM images and their corresponding simulated images. In the first row, the simulated images have a defocus value of −16.5 μm. For the second and third rows, the simulated images are shown at the same defocus value. Scale bar: 20 nm.
a) Simulated cryo‐TEM images generated from a single MD simulation snapshot of 100% CSSC with all CSSC restrained. Defocus values are set at −16, −12, −8, and −4 μm (from left to right) to illustrate the influence of the defocus value. b) Simulated cryo‐TEM images generated from a single MD simulation snapshot of 100% CSSC with all CSSC restrained at water thicknesses of 10, 40, 80, and 150 nm (from left to right) to demonstrate the influence of water thickness. Scale bars: 20 nm.

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Cryogenic Electron Microscopy Informed Molecular Dynamics Simulations to Investigate the Disulfide Hydrogel Self‐Assembly
  • Article
  • Publisher preview available

May 2025

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2 Reads

Yuanming Song

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Zhaoxu Li

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Justin T. Mulvey

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[...]

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Douglas J. Tobias

Disulfide hydrogels, derived from cysteine‐based redox systems, exhibit active self‐assembly properties driven by reversible disulfide bond formation, making them a versatile platform for dynamic material design. Detailed cryogenic electron microscopy (cryo‐EM) analysis reveals a consistent fiber diameter of 5.4 nm for individual fibers. Using cryo‐EM‐informed radial positional restraints, all‐atom molecular dynamics (MD) simulations are employed to reproduce fibers with dimensions closely matching experimental observations, validated further through simulated cryo‐EM images. The MD simulations reveal that the disulfide gelator (CSSC) predominantly adopts an open conformation, with hydrogen bonds emerging as the key intermolecular force stabilizing the fibers. Notably, intermolecular interactions are found to be higher at 70% conversion to the disulfide gelator compared with 100%, comparable with past unrestrained simulations. Water molecules and solute‐water hydrogen bonds are present throughout the fiber, indicating that the fiber remains hydrated. These findings underscore the potential role of the thiol precursor CSH in stabilizing the transient phase and highlight the importance of CSH‐CSSC interplay. Herein, it provides novel insights into molecular mechanisms governing active self‐assembly and offers strategies for designing tunable materials through controlled assembly conditions.

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Insights into Dermal Permeation of Skin Oil Oxidation Products from Enhanced Sampling Molecular Dynamics Simulation

February 2025

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7 Reads

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1 Citation

The Journal of Physical Chemistry B

The oxidation of human sebum, a lipid mixture covering our skin, generates a range of volatile and semivolatile carbonyl compounds that contribute largely to indoor air pollution in crowded environments. Kinetic models have been developed to gain a deeper understanding of this complex multiphase chemistry, but they rely partially on rough estimates of kinetic and thermodynamic parameters, especially those describing skin permeation. Here, we employ atomistic molecular dynamics simulations to study the translocation of selected skin oil oxidation products through a model stratum corneum membrane. We find these simulations to be nontrivial, requiring extensive sampling with up to microsecond simulation times, in spite of employing enhanced sampling techniques. We identify the high degree of order and stochastic, long-lived temporal asymmetries in the membrane structure as the leading causes for the slow convergence of the free energy computations. We demonstrate that statistical errors due to insufficient sampling are substantial and propagate to membrane permeabilities. These errors are independent of the enhanced sampling technique employed and very likely independent of the precise membrane model.


Molecular Dynamics Simulations of the Interactions of Organic Compounds at Indoor Relevant Surfaces

February 2025

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11 Reads

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2 Citations

Annual Review of Physical Chemistry

With markedly different reaction conditions compared to the chemistry of the outside atmosphere, indoor air chemistry poses new challenges to the scientific community that require combined experimental and computational efforts. Here, we review molecular dynamics simulations that have contributed to the mechanistic understanding of the complex dynamics of organic compounds at indoor surfaces and their interplay with experiments and indoor air models. We highlight the rich interactions between volatile organic compounds and silica and titanium dioxide surfaces, serving as proxies for glasses and paints, as well as the dynamics of skin oil lipids and their oxidation products, which sensitively affect the quality of indoor air in crowded environments. As the studies we review here are pioneering in the rapidly emerging field of indoor chemistry, we provide suggestions for increasing the potentially important role that molecular simulations can continue to play.









Citations (65)


... [1][2][3][4][5] Reaction conditions in indoor environments, such as temperature or relative humidity, are usually markedly different than outside, but the most striking difference is the large surface-tovolume ratio and the chemical variety of both surfaces and compounds found in indoor air. 6,7 Previous research has shown that not only human activities, such as cooking, cleaning, or personal care, transform the composition of indoor air, 8 but also the mere presence of people in indoor environments. 9 A prominent example is the oxidation of the oily-to-waxy mixture of lipids covering our skin, the sebum, through atmospheric oxidants, notably ozone. ...

Reference:

Insights into Dermal Permeation of Skin Oil Oxidation Products from Enhanced Sampling Molecular Dynamics Simulation
Molecular Dynamics Simulations of the Interactions of Organic Compounds at Indoor Relevant Surfaces
  • Citing Article
  • February 2025

Annual Review of Physical Chemistry

... Kv1.1. We previously found that gallic acid enhances Kv1.1 but not Kv1.2 activity, and used this to identify residues in S1, within the voltage-sensing domain (VSD) unique to Kv1.1 and not Kv1.2 that formed the gallic acid binding site (Fig. 6 A and B) (11). Here, we found that unlike gallic acid (11), pisiferic acid was able to negative-shift the voltage dependence of Kv1.1 carrying a triple mutant that disrupts the gallic acid binding site (Fig. 6 C-F). ...

Native American ataxia medicines rescue ataxia-linked mutant potassium channel activity via binding to the voltage sensing domain

... The reduced solubility of these mutant proteins promotes protein aggregation by significantly increasing protein−protein interactions. 28 Various biochemical processes involve proteins in a partially unfolded or folded conformation, making them susceptible to aggregation and thus inhibiting the formation of a functional structure. Mechanisms to combat such processes have emerged through evolution to ensure survival. ...

Insights into the solubility of γ γ \gamma D-crystallin from multiscale atomistic simulations
  • Citing Article
  • April 2023

Journal of Computational Chemistry

... [8] While unrestrained MD simulations have offered valuable insights into the molecular interactions driving self-assembly in CSH-CSSC and similar systems, they remain limited in their capacity to simulate large-scale fiber structures. [3,[8][9][10] These fiber structures, observed experimentally, typically form on time scales well beyond the reach of conventional MD techniques. [3] However, MD simulations constructed based on cryogenic transmission electron microscopy (cryo-EM) images have proven effective in elucidating the intermolecular interactions and dynamics underlying molecular assembly, as demonstrated in studies of the self-assembly of proteins into large-scale structures such as viral capsids. ...

Stimuli responsive hierarchical assembly of supramolecular conductive fibers from coiled-coil building blocks
  • Citing Article
  • February 2023

Biophysical Journal

... To this end, we simulate their formation using a method of network Hamiltonian described by Butts et al. for the formation of disordered protein aggregates. 71 In brief, the structure of a complex nanoscale system produced by self-assembling NPs can be described by a graph interconnecting them. The energy of this system is given by its Hamiltonian. ...

Network Hamiltonian Models for Unstructured Protein Aggregates, with Application to γD-Crystallin
  • Citing Article
  • January 2023

The Journal of Physical Chemistry B

... PIEZO1 has been shown to be mobile in the plasma membrane 30,32,42,43 and we confirmed this in hiPSC-derived neural stem cells, keratinocytes, and endothelial cells differentiated from PIEZO1-HaloTag hiPSCs and labeled with JF646 HTL (Supplemental Videos 1, 2, and 3). Studies on the mobility of the endogenous channel have utilized cells harvested from a PIEZO1-tdTomato knock-in mouse 30,42 where the tdTomato fluorescent protein is limited by rapid photobleaching and low signal-to-noise ratio. ...

Single-particle tracking and machine-learning classification reveals heterogeneous Piezo1 diffusion

... This is due to both the high reactivity of its two double bonds in the 1,2 and 8,9 positions which can be oxidized to its corresponding oxides and to its extraction in enormous amounts derived from waste of the orange juice industry, such as orange peels [1,2]. Oxidation of limonene (encompassing epoxidation) over metal-based catalysts with hydrogen peroxide or t-Butyl hydroperoxide or molecular oxygen [3] is one of the primary methods of converting it into useful compounds [4][5][6][7][8][9]. However, many side-reaction products such as 1,2-epoxylimonene diol, carveol, 8,9-epoxylimonene diol, carvone, and diepoxide can be obtained together with limonene 1,2-epoxide, which renders this process complex [10]. ...

Interactions of Limonene and Carvone on Titanium Dioxide Surface

Physical Chemistry Chemical Physics

... 45,46 V H H-pHLIP displays a similar CD spectrum in solution ( Figure S3b). However, when large unilamellar vesicles (an established membrane mimic environment used with pHLIP 47,48 ) are added, and the pH is decreased to 6.0, it transitions to a more α-helical structure, as indicated by the appearance of a second negative peak. We attribute this pH-mediated change to the characteristic folding pHLIP as an α-helix upon acidi cation. ...

Ca‐dependent interactions between lipids and the tumor‐targeting peptide pHLIP

... It has often been utilized as a model aerosol system to better understand the heterogeneous oxidation process of unsaturated carboxylic acids and their environmental consequences [4]. Although the heterogeneous oxidation of oleic acid by O 3 has been extensively studied with respect to its kinetics, mechanism, and product identification [4][5][6][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28], kinetic data such as the uptake coefficient γ obtained from different experimental approaches sometimes differ by over one order of magnitude. In addition, although some reports on effects of temperature, physical state, and component mixing [6,13,27], how droplet size and relative humidity (RH) affect the ozone-initiated reaction kinetics have not been well explored. ...

Multiphase Ozonolysis of Oleic Acid-Based Lipids: Quantitation of Major Products and Kinetic Multilayer Modeling
  • Citing Article
  • June 2022

Environmental Science and Technology

... In contrast to their work, we simplified the model by focusing on the PAL (100) surface, specifically the Si-OH groups, the SiO 4 units connected to them, and the Si-O-Si framework linked to AlO 8 . These simplifications allowed us to strike a balance between computational feasibility and maintaining the accuracy and reliability of the model while ensuring logical consistency throughout the study [49][50][51][52]. Initially, the crystal structure of PAL was optimized to ensure stability. ...

Heterogeneous Interactions between Carvone and Hydroxylated SiO 2
  • Citing Article
  • March 2022

The Journal of Physical Chemistry C