Epstein-Barr virus latency switch in human B-cells: a physico-chemical model-2
Copyright information:Taken from "Epstein-Barr virus latency switch in human B-cells: a physico-chemical model"http://www.biomedcentral.com/1752-0509/1/40BMC Systems Biology 2007;1():40-40.Published online 31 Aug 2007PMCID:PMC2164963.ssary to switch from latency I to III and vice versa, as...
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Zusammenfassung: | Copyright information:Taken from "Epstein-Barr virus latency switch in human B-cells: a physico-chemical model"http://www.biomedcentral.com/1752-0509/1/40BMC Systems Biology 2007;1():40-40.Published online 31 Aug 2007PMCID:PMC2164963.ssary to switch from latency I to III and vice versa, as a function of the number of Oct-2+Grg/TLR proteins. For small numbers only the latency III state exists, while for large numbers only latency I state exists, compare Figure 3 and Figure 4. Left figure: red lines are at the reference parameter values, in particular Oct-2 complex binding with affinity = 2.5 and an EBNA-1 dimerization dissociation constant of 1 nM. Blue lines show a five-fold weaker Oct-2 affinity (= 12.5 ). Similar behaviour is then displayed at approximately five-fold higher Oct-2 level. Right figure: red solid and dotted lines at reference parameter values. Blue solid and dotted lines at a tenfold stronger EBNA-1 dimerization, and green solid and dotted lines at a tenfold greater volume. The latency III state is relatively robust towards either of these changes, while the latency I state changes more. Black solid and dotted lines show both a tenfold stronger EBNA-1 dimerization and a tenfold greater volume. This influences the latency III state more, essentially because EBNA-1 concentration in the latency III state is then comparable to the EBNA-1 dimerization dissociation constant. |
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DOI: | 10.6084/m9.figshare.67090 |