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New page: left|200px<br /><applet load="2j53" size="350" color="white" frame="true" align="right" spinBox="true" caption="2j53" /> '''SOLUTION STRUCTURE OF GB1 DOMAIN PROTEIN G A...
 
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==Overview==
==Overview==
The solution structure of the GB1 domain of protein G at a pressure of 2, kbar is presented. The structure was calculated as a change from an, energy-minimised low-pressure structure using (1)H chemical shifts. Two, separate changes can be characterised: a compression/distortion, which is, linear with pressure; and a stabilisation of an alternative folded state., On application of pressure, linear chemical shift changes reveal that the, backbone structure changes by about 0.2 A root mean square, and is, compressed by about 1% overall. The alpha-helix compresses, particularly, at the C-terminal end, and moves toward the beta-sheet, while the, beta-sheet is twisted, with the corners closest to the alpha-helix curling, up towards it. The largest changes in structure are along the second, beta-strand, which becomes more twisted. This strand is where the protein, binds to IgG. Curved chemical shift changes with pressure indicate that, high pressure also populates an alternative structure with a distortion, towards the C-terminal end of the helix, which is likely to be caused by, insertion of a water molecule. Proteins 2007. (c) 2007 Wiley-Liss, Inc.
The solution structure of the GB1 domain of protein G at a pressure of 2 kbar is presented. The structure was calculated as a change from an energy-minimised low-pressure structure using (1)H chemical shifts. Two separate changes can be characterised: a compression/distortion, which is linear with pressure; and a stabilisation of an alternative folded state. On application of pressure, linear chemical shift changes reveal that the backbone structure changes by about 0.2 A root mean square, and is compressed by about 1% overall. The alpha-helix compresses, particularly at the C-terminal end, and moves toward the beta-sheet, while the beta-sheet is twisted, with the corners closest to the alpha-helix curling up towards it. The largest changes in structure are along the second beta-strand, which becomes more twisted. This strand is where the protein binds to IgG. Curved chemical shift changes with pressure indicate that high pressure also populates an alternative structure with a distortion towards the C-terminal end of the helix, which is likely to be caused by insertion of a water molecule. Proteins 2007. (c) 2007 Wiley-Liss, Inc.


==About this Structure==
==About this Structure==
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[[Category: Streptococcus sp.]]
[[Category: Streptococcus sp.]]
[[Category: Akasaka, K.]]
[[Category: Akasaka, K.]]
[[Category: Kamatari, Y.O.]]
[[Category: Kamatari, Y O.]]
[[Category: Tunnicliffe, R.B.]]
[[Category: Tunnicliffe, R B.]]
[[Category: Williamson, M.P.]]
[[Category: Williamson, M P.]]
[[Category: Wilton, D.J.]]
[[Category: Wilton, D J.]]
[[Category: cell wall]]
[[Category: cell wall]]
[[Category: igg-binding protein]]
[[Category: igg-binding protein]]
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[[Category: protein g]]
[[Category: protein g]]


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