Generation of a third-order folded structure for chromatin

Abstract

A model for the initiation of the diffuse-condensed transition of chromatin induced by a change in the conformation of lysine-rich histones is proposed. Three levels of folded structures are discussed. The first-order folded structure refers to the structure of the repeat unit of chromatin, which is called the nucleosome. The nucleosome contains a nuclease resistant region in which 140 base pairs of DNA are wrapped around the surface of a histone aggregated of two copies each of the histones H2A, H2B, H3 and H4. This DNA-histone aggregate is called a core particle. The nuclease accessible region of the nucleosome is approximately 60 base pairs of DNA which link the core particle, hence the terminology “linker DNA.” The lysine-rich histones, (Hl, H5), which are more loosely bound than the core histones, are associated with the linker DNA. The second-order folded structure refers to the conformation of a polynucleosome. Based on neutron scattering and quasielastic light scattering studies the second-order folded structure is assumed to be an extended helix in solution with 5–7 nucleosome units per turn. The third-order folded structure is defined as that structure resulting from the first stage in the condensation process induced by a conformational change in the lysine-rich histones. Generation of the third-order folded structure in the proposed model is effected by an increased affinity of the lysine-rich histones for super-helical DNA in the core particles in adjacent turns of the second-order folded structure. Since the lysine-rich histones preferentially bind to A-T rich regions in DNA, the distribution of these regions would determine the third-order folded structure. The net effect of a non-random distribution of A-T rich regions as in the proposed model is the generation of a helix for the third-order folded structure. The assumption of a non-random distribution of A-T rich regions is indirectly supported by proflavine binding studies reported herein and by the existence of repetitive and non-repetitive DNA regions inferred from renaturation studies. One consequence of the proposed mechanism is that the majority of the A-T rich regions are in the interior of the third-order folded structure. Promoter sites of high A-T content would then be inaccessible to polymerases. The proposed model also suggests a role for spacer DNA in the genome. Higher order folded structures must also be present in the final state of condensed chromatin since the three orders of folded structures considered in this communication accounts for only 2% of that required in the diffuse-condensed transition.