Treat the target as an absorbing sphere of effective capture radius , surrounded by a uniform dilute reservoir of RNA polymerase with number density . The steady diffusion equation, spherical symmetry, and boundary conditions giveBy Fick's laws, the inward capture rate per target is . Multiplying by the target number density and comparing with the bimolecular rate law therefore yields the Smoluchowski association rateIts units here are , since the concentrations count particles rather than moles. The absorbing boundary assumes every encounter is productive; orientation constraints would reduce the effective association rate constant.
The Stokes–Einstein relation, for RNA polymerase radius at an illustrative temperature , givesNeither cell volume nor the effective is specified, so a unique numerical time is unavailable. A representative Escherichia coli volume is . The -base pair target has a DNA contour extent of about ; using this as an order-of-magnitude capture radius gives . For independent searchers, the target's approximately constant encounter hazard is , henceUsing half the target's contour extent for instead gives about ; the spherical capture model is not exact target geometry. One searcher's mean would be about under the first convention, whereas the first arrival among is much faster.
If only a fraction of each searcher's time is available for three-dimensional diffusion, and nonspecific DNA binding neither scans nor delivers the target, the effective searching population is . Thus , about under the stated estimate. This assumes stationarity, well-mixed searchers and no additional target-access route; nonspecific binding alone is sequestration, not facilitated diffusion.
Articles by others on the same topic
There are currently no matching articles.