No abstract

Huntington's disease (HD) is a heritable neurodegenerative disease that is caused by a CAG expansion in the first exon of the huntingtin gene. This expansion results in an elongated polyglutamine (polyQ) domain that increases the propensity of huntingtin exon-1 (HTTex1) to form cross-β fibrils. While the polyQ domain is important for fibril formation, the dynamic, C-terminal proline-rich domain (PRD) of HTTex1 makes up a large fraction of the fibril surface. Because potential fibril toxicity has to be mediated by interactions of the fibril surface with its cellular environment, we wanted to model the conformational space adopted by the PRD. We ran 800 ns long molecular dynamics (MD) simulations of the PRD using an explicit water model optimized for intrinsically disordered proteins. These simulations accurately predicted our previous solid-state NMR data and newly acquired EPR DEER distances, lending confidence in their accuracy. The simulations show that the PRD generally forms an imperfect polyproline II (PPII) helical conformation. The two polyproline (polyP) regions within the PRD stay in a PPII helix for most of the simulation, whereas occasional kinks in the proline rich linker region cause an overall bend in the PRD structure. The dihedral angles of the glycine at the end of the second polyP region are very variable, effectively decoupling the highly dynamic 12 C-terminal residues from the rest of the PRD.

Huntington's disease (HD) is a heritable neurodegenerative disease that is caused by a CAG expansion in the first exon of the huntingtin gene. This expansion results in an elongated polyglutamine (polyQ) domain that increases the propensity of huntingtin exon-1 (HTTex1) to form cross-β fibrils. While the polyQ domain is important for fibril formation, the dynamic, C-terminal proline-rich domain (PRD) of HTTex1 makes up a large fraction of the fibril surface. Because potential fibril toxicity has to be mediated by interactions of the fibril surface with its cellular environment, we wanted to model the conformational space adopted by the PRD. We ran 800 ns long molecular dynamics (MD) simulations of the PRD using an explicit water model optimized for intrinsically disordered proteins. These simulations accurately predicted our previous solid-state NMR data and newly acquired EPR DEER distances, lending confidence in their accuracy. The simulations show that the PRD generally forms an imperfect polyproline II (PPII) helical conformation. The two polyproline (polyP) regions within the PRD stay in a PPII helix for most of the simulation, whereas occasional kinks in the proline rich linker region cause an overall bend in the PRD structure. The dihedral angles of the glycine at the end of the second polyP region are very variable, effectively decoupling the highly dynamic 12 C-terminal residues from the rest of the PRD. Statement of SignificanceHD is caused by a polyQ expansion in the exon-1 of huntingtin, which results in the formation of fibrillar huntingtin aggregates. Although the polyQ domain is the site of the disease-causing mutation, the PRD domain of HTTex1 is important for fibril toxicity and contains many epitopes of fibril-specific HTTex1 antibodies. Here, we present a structural and dynamic model of the highly dynamic PRD domain using a combination of EPR, solid-state NMR, and MD simulations. This model paves the way for studying known HTTex1 fibril specific binders and designing new ones.

No abstract