Abstract
In this work, we examine how volume exclusion caused by regions of high chromatin density might influence the time required for proteins to find specific DNA binding sites. The spatial variation of chromatin density within mouse olfactory sensory neurons is determined from soft X-ray tomography reconstructions of five nuclei. We show that there is a division of the nuclear space into regions of low-density euchromatin and high-density heterochromatin. Volume exclusion experienced by a diffusing protein caused by this varying density of chromatin is modeled by a repulsive potential. The value of the potential at a given point in space is chosen to be proportional to the density of chromatin at that location. The constant of proportionality, called the volume exclusivity, provides a model parameter that determines the strength of volume exclusion. Numerical simulations demonstrate that the mean time for a protein to locate a binding site localized in euchromatin is minimized for a finite, nonzero volume exclusivity. For binding sites in heterochromatin, the mean time is minimized when the volume exclusivity is zero (the protein experiences no volume exclusion). An analytical theory is developed to explain these results. The theory suggests that for binding sites in euchromatin there is an optimal level of volume exclusivity that balances a reduction in the volume searched in finding the binding site, with the height of effective potential barriers the protein must cross during the search process.
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Acknowledgements
S.A. Isaacson, D.M. McQueen, and C.S. Peskin were supported by the Systems Biology Center New York (National Institutes of Health Grant P50GM071558). S.A. Isaacson was also supported by National Science Foundation Grant DMS-0920886. M.A. Le Gros and C.A. Larabell were supported by the Department of Energy Office of Biological and Environmental Research Grant DE-AC02-05CH11231, the NIH National Center for Research Resources (5P41 RR019664-08), and the National Institute of General Medical Sciences (8P41 GM103445-08) from the National Institutes of Health.
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Appendix: Soft X-ray Tomography Measurement Error
Appendix: Soft X-ray Tomography Measurement Error
The X-ray microscope employs monochromatic X-rays and, therefore, the values obtained from computed tomography measurements are equal to the LAC values calculated from the atomic composition of the specimen. The SXT technique avoids the beam hardening effects commonly found in polychromatic tomographic imaging (see Tsuchiyama et al. 2005). The measurement error for each pixel of a single projection image is of order 3 %, determined by photon shot noise. The LAC value of each 32 nm voxel is obtained from tomographic reconstruction of many such projections and is typically less than 1 %. LAC measurement errors are insignificant compared to the observed cell-to-cell variation.
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Isaacson, S.A., Larabell, C.A., Le Gros, M.A. et al. The Influence of Spatial Variation in Chromatin Density Determined by X-Ray Tomograms on the Time to Find DNA Binding Sites. Bull Math Biol 75, 2093–2117 (2013). https://doi.org/10.1007/s11538-013-9883-9
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DOI: https://doi.org/10.1007/s11538-013-9883-9