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. 2011 Oct 5;101(7):1569–1579. doi: 10.1016/j.bpj.2011.08.041

Figure 2.

Figure 2

Illustration of the energy levels and the kinetic model for the two TF species system with a nonspecific genomic background. (A) Binding of TFs to the DNA reduces the energy by Ens < 0 compared to the unbound reference state with energy Efree = 0. Additional energy can be gained through sequence-specific contacts (not shown). Upon dimerization of TFs in solution or on the DNA, the energy is further reduced by the interaction energy Eint ≤ 0. The TFs bind to their target site with a specific binding energy ET. At small dimerization energies Eint, full promoter activation will be reached via the monomer pathway, where TFs arrive at their target independently and consecutively. At large Eint, on the other hand, TFs will predimerize in the DNA-background or in solution and arrive to the targets simultaneously through the dimer pathway. (B) Transcription factors dimerize in solution and bind to the DNA in diffusion-limited binding reactions with a rate constant ka. The dissociation rate of a free dimer kd and the dissociation rate koff of a TF from a DNA site depend on the corresponding energies and follow from detailed balance as explained in the main text. Dimers and monomers can randomly diffuse along the DNA with a rate ksl, which becomes site-dependent when the binding energy is sequence-specific. When the dissociation of a monomer requires the simultaneous dissociation from a cooperatively bound partner, its off-rate koff decreases by a factor 1/ω.