Treat the target as a stationary perfectly absorbing sphere of reaction radius , surrounded by an effectively uniform reservoir of protein number density . At steady state the radial diffusion equation givesThe inward capture rate per target is the integral of the Fick's first law:For dilute independent targets of number density , the volume association rate is , soThis is the Smoluchowski association rate, in volume per time because the concentrations are number densities. If the target also diffuses, use the relative diffusion coefficient . Orientation constraints, incomplete absorption and chromosome geometry can reduce the actual association rate relative to this ideal collision limit.
The given sphere has radius . The Stokes–Einstein relation at an illustrative givesFor well-mixed independent searchers in cell volume , the target-arrival rate is . The corresponding mean first arrival time isThe source does not fix , the reaction radius or temperature. For an order-of-magnitude estimate, a bacterial volume around and reaction radius – give about –. A 20-base-pair B-form site is about long, supporting a nanometre-scale capture radius but not uniquely defining its spherical value. The estimate is the ideal diffusion-limited time, not a measured intracellular search time: nonspecific binding, orientational matching, crowding and limited accessibility are excluded.
If the outcome is the first successful binding to any operator, ten well-separated functionally independent unoccupied targets give ten times the total capture rate. Henceor roughly – for the estimates above. This assumes nonoverlapping capture zones and no significant depletion before the first event. The first-arrival time at one designated operator is not divided by ten merely because other sites are added, and filling all ten sites is a different occupancy problem.
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