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The Chemistry of Signal Transduction in the TetR ... - Beilstein-Institut

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178<br />

Lanig, H. and Clark, T.<br />

<strong>The</strong> red region <strong>of</strong> <strong>the</strong> plot from 0 – 20 ns has a mean R(a3-a3’) distance <strong>of</strong> 36.9 A˚ , but<br />

shows oscillations that appear to <strong>in</strong>crease <strong>in</strong> amplitude with time. Between 20 and 62 ns,<br />

R(a3-a3’) <strong>in</strong>creases steadily to a f<strong>in</strong>al value (green region, 62 – 108 ns, mean R(a3a3’)<br />

= 45.3 A˚ ) <strong>in</strong> which R(a3-a3’) no longer exhibits <strong>the</strong> strong oscillations seen at <strong>the</strong><br />

beg<strong>in</strong>n<strong>in</strong>g <strong>of</strong> <strong>the</strong> simulation. Thus, <strong>the</strong> simulation rema<strong>in</strong>s stable at a non-<strong>in</strong>duced value <strong>of</strong><br />

R(a3-a3’) for <strong>the</strong> first 20 ns before undergo<strong>in</strong>g a transition over 40 ns to achieve a f<strong>in</strong>al,<br />

apparently stable, <strong>in</strong>duced conformation. We emphasize that this process does not necessarily<br />

correspond to a real <strong>in</strong>duction event <strong>in</strong> <strong>the</strong> biological system, but strictly speak<strong>in</strong>g only<br />

to <strong>the</strong> relaxation <strong>of</strong> <strong>the</strong> stra<strong>in</strong>ed 2O7O X-ray structure. Never<strong>the</strong>less, <strong>the</strong> fact that <strong>the</strong> <strong>in</strong>itial<br />

conformation rema<strong>in</strong>s stable for 20 ns (<strong>the</strong> complete length <strong>of</strong> many simulations reported <strong>in</strong><br />

<strong>the</strong> current literature) is very significant. This is as far as we are aware <strong>the</strong> first direct<br />

observation <strong>in</strong> an MD simulation <strong>of</strong> <strong>the</strong> pre-equilibrium mechanism <strong>of</strong> <strong>in</strong>duction [25]. In<br />

this mechanism, which has found wide acceptance, <strong>the</strong> <strong>in</strong>ducer first docks <strong>in</strong>to <strong>the</strong> non<strong>in</strong>duced<br />

conformation <strong>of</strong> <strong>the</strong> repressor to form a metastable complex, which eventually<br />

relaxes to <strong>the</strong> <strong>in</strong>duced conformation <strong>of</strong> <strong>the</strong> repressor-<strong>in</strong>ducer complex. In <strong>the</strong> reverse process,<br />

<strong>the</strong> <strong>in</strong>ducer dissociates from <strong>the</strong> <strong>in</strong>duced complex to form a metastable, uncomplexed<br />

<strong>in</strong>duced conformation <strong>of</strong> <strong>the</strong> repressor, which <strong>the</strong>n can relax to <strong>the</strong> stable non-<strong>in</strong>duced<br />

conformation.<br />

Conclusions<br />

We have shown that MD simulations <strong>of</strong> 50 – 100 ns are an effective tool for identify<strong>in</strong>g <strong>the</strong><br />

mechanism <strong>of</strong> <strong>in</strong>duction <strong>of</strong> <strong>TetR</strong> and for detect<strong>in</strong>g its state <strong>of</strong> <strong>in</strong>duction. <strong>The</strong>se conclusions<br />

are presumably also valid for o<strong>the</strong>r signal-transduction prote<strong>in</strong>s that vary <strong>the</strong>ir b<strong>in</strong>d<strong>in</strong>g<br />

aff<strong>in</strong>ity by an allosteric rearrangement. Perhaps predictably, X-ray structures are not well<br />

suited for determ<strong>in</strong><strong>in</strong>g <strong>the</strong> <strong>in</strong>duction state <strong>of</strong> signal-transduction prote<strong>in</strong>s because we believe<br />

<strong>the</strong> crystal-pack<strong>in</strong>g forces to be <strong>of</strong> <strong>the</strong> same order <strong>of</strong> magnitude as those that cause <strong>the</strong><br />

allosteric rearrangement.<br />

It is perhaps mislead<strong>in</strong>g to discuss ‘‘<strong>the</strong> mechanism <strong>of</strong> <strong>in</strong>duction’’. Figure 9 illustrates this<br />

po<strong>in</strong>t.<br />

Thus, not <strong>in</strong>duction is unique, but ra<strong>the</strong>r <strong>the</strong> fact that signal-transduction prote<strong>in</strong>s can b<strong>in</strong>d so<br />

strongly to <strong>the</strong> promoter and that this bound conformation is so robust to environmental<br />

factors such as temperature, pH, ion concentrations etc. that should not be able to cause<br />

<strong>in</strong>duction. Induction can be caused by just about any structural change, <strong>in</strong>clud<strong>in</strong>g denaturation,<br />

that lowers <strong>the</strong> b<strong>in</strong>d<strong>in</strong>g aff<strong>in</strong>ity. Thus, one and <strong>the</strong> same signal-transduction prote<strong>in</strong><br />

may be <strong>in</strong>duced <strong>in</strong> many ways. This is <strong>in</strong> fact true <strong>of</strong> <strong>TetR</strong>, which is <strong>in</strong>duced by tetracycl<strong>in</strong>es<br />

<strong>in</strong> <strong>the</strong> presence <strong>of</strong> magnesium, by 5a,6-anhydrotetracycl<strong>in</strong>e [26] and <strong>the</strong> <strong>TetR</strong>-<strong>in</strong>duc<strong>in</strong>g<br />

prote<strong>in</strong> TIP [22] <strong>in</strong> its absence. In <strong>the</strong> latter case, a different mechanism <strong>of</strong> <strong>in</strong>duction is<br />

observed to that found with tetracycl<strong>in</strong>e-magnesium complexes [27].

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