Human apolipoprotein A-I: structure determination and analysis of unusual diffraction characteristics

1999 ◽  
Vol 55 (12) ◽  
pp. 2013-2021 ◽  
Author(s):  
David W. Borhani ◽  
Jeffrey A. Engler ◽  
Christie G. Brouillette

The crystallization and structure determination of recombinant human apolipoprotein A-I (apo A-I), the major protein component of high-density lipoprotein, is described. The fragment crystallized, residues 44–243 of native apo A-I [apo Δ(1–43)A-I], is very similar to intact native apo A-I in its ability to bind lipid, to be incorporated into high-density lipoproteins and to activate lecithin–cholesterol acyl transferase. Apo Δ(1–43)A-I crystallizes from 1.0–1.4 M sodium citrate pH 6.5–7.5 in space group P212121, with unit-cell parameters a = 97.47, b = 113.87, c = 196.19 Å (crystal form I). The crystals exhibit unusual diffraction intensity spikes and axial extinctions that are discussed in the context of the 4 Å crystal structure. When flash-cooled to 100 K, the crystals diffract synchrotron radiation to 3 Å resolution. Radiation sensitivity and crystal-to-crystal variation have hindered the assembly of a complete 3 Å data set.

1999 ◽  
Vol 55 (9) ◽  
pp. 1578-1583 ◽  
Author(s):  
David W. Borhani ◽  
Jeffrey A. Engler ◽  
Christie G. Brouillette

The crystallization of recombinant human apolipoprotein A-I (apo A-I), the major protein component of high-density lipoprotein, in a new crystal form is described. The fragment crystallized, residues 44–243 of native apo A-I [apo Δ(1–43)A-I], is very similar to intact native apo A-I in its ability to bind lipid, to be incorporated into high-density lipoproteins and to activate lecithin–cholesterol acyl transferase. Apo Δ(1–43)A-I crystallizes, in the presence of β-D-octylglucopyranoside, in space group I222 or I212121, with unit-cell parameters a = 37.11, b = 123.62, c = 164.65 Å and a diffraction limit of 3.2 Å. These form II crystals grow under conditions of significantly lower ionic strength than the original form I crystals (space group P212121, a = 97.47, b = 113.87, c = 196.19 Å, diffraction limit 3.0 Å). Packing arguments show that the unusual open conformation of apo Δ(1–43)A-I found in the form I crystals cannot be packed into the smaller oddly proportioned form II unit cell. Monomeric apo Δ(1–43)A-I, as either a four-helix bundle (∼75 × 30 × 30 Å) or an extended helical rod (∼150 × 20 × 20 Å), can be packed into the form II unit cell. It is concluded, therefore, that apo Δ(1–43)A-I may have crystallized in one of these distinct conformations in the form II crystals.


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