Structure of the SAM-II riboswitch bound to S-adenosylmethionine
Structure of the SAM-II riboswitch bound to S-adenosylmethionine
Structure of the SAM-II riboswitch bound to S-adenosylmethionine
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10-30 minutes in 30 µl <strong>of</strong> one <strong>of</strong> two heavy-a<strong>to</strong>m derivative solutions. Crystals<br />
designated for isomorphous replacement were backsoaked in mo<strong>the</strong>r liquor<br />
containing 2 mM magnesium chloride, 10 mM <strong>SAM</strong>, and 200 mM cesium chloride<br />
for ~10 minutes. Crystals designated as native were backsoaked for 10-30 minutes in<br />
mo<strong>the</strong>r liquor that only contained 320 mM ammonium acetate (all o<strong>the</strong>r components<br />
remaining <strong>the</strong> same) with <strong>the</strong> addition <strong>of</strong> 2 mM magnesium chloride, 10 mM <strong>SAM</strong>,<br />
and 600 mM lithium chloride also for ~10 minutes. This was followed by a 10-30<br />
minute exchange in<strong>to</strong> <strong>the</strong> same solutions containing <strong>the</strong> addition <strong>of</strong> 8 % (2R,3R)-<br />
butanediol. Crystals were looped and flash-frozen in liquid nitrogen. Diffraction data<br />
was collected on a home X-ray source (Rigaku MSC) using CuK α radiation.<br />
Anomalous diffraction data was collected by an inverse-beam experiment and was<br />
integrated, indexed, and scaled using HKL2000 5 .<br />
Phasing and structure determination. An initial heavy a<strong>to</strong>m solution was<br />
calculated using data from a single anomalous dispersion (SAD) experiment at CuK α<br />
with cesium as <strong>the</strong> anomalous scatterer. The solution containing four heavy a<strong>to</strong>ms<br />
(FOM = 0.27, Z-score = 17) was generated in SOLVE 6 . The heavy a<strong>to</strong>m solution<br />
was <strong>the</strong>n used <strong>to</strong> calculate experimental phases by single isomorphous replacement<br />
with anomalous scattering (SIRAS) experiment and diffraction data extending <strong>to</strong> 2.5<br />
Å resolution for <strong>the</strong> native data set and 2.8 Å resolution for <strong>the</strong> same cesium<br />
derivative set. Phases were calculated using CNS 7 in which a cesium was treated as<br />
<strong>the</strong> heavy a<strong>to</strong>m derivative, (f’ = -1.16, f” = 8.80), while a lithium back soaked crystal<br />
was treated as <strong>the</strong> native data set. Following density modification in CNS 7 , <strong>the</strong> figure