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	<title>Comments for LettsScience</title>
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	<link>http://lettsscience.com</link>
	<description>Biochemistry and biophysics blog.</description>
	<lastBuildDate>Fri, 15 Mar 2013 20:32:56 +0000</lastBuildDate>
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		<title>Comment on The importance of charge compensation in the membrane by lettsscience</title>
		<link>http://lettsscience.com/2012/09/15/the-importance-of-charge-compensation-in-the-membrane/#comment-431</link>
		<dc:creator><![CDATA[lettsscience]]></dc:creator>
		<pubDate>Fri, 15 Mar 2013 20:32:56 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=1196#comment-431</guid>
		<description><![CDATA[Thanks for the comment. Of course I agree that if a VSD is still capable of gating in response to voltage it suggests that the structure can&#039;t be completely disrupted. However, many mutations have large effects on both the kinetics and midpoint of the voltage-gating in ways that we are still unable to fully explain. I completely agree that we need more structural information on VSDs in order to better understand mechanism and how the gating is altered by the mutations.
Every serious scientist worries about potential nonspecific or global effects of their mutations, however, because of the nature of scientific publishing sometimes these concerns are not fully addressed in the papers. That is why I wanted to start this blog so we could discuss these issues that don&#039;t always make it into the literature.
Looking forward to seeing your paper when it comes out. Please post a link to it here when it comes out.]]></description>
		<content:encoded><![CDATA[<p>Thanks for the comment. Of course I agree that if a VSD is still capable of gating in response to voltage it suggests that the structure can&#8217;t be completely disrupted. However, many mutations have large effects on both the kinetics and midpoint of the voltage-gating in ways that we are still unable to fully explain. I completely agree that we need more structural information on VSDs in order to better understand mechanism and how the gating is altered by the mutations.<br />
Every serious scientist worries about potential nonspecific or global effects of their mutations, however, because of the nature of scientific publishing sometimes these concerns are not fully addressed in the papers. That is why I wanted to start this blog so we could discuss these issues that don&#8217;t always make it into the literature.<br />
Looking forward to seeing your paper when it comes out. Please post a link to it here when it comes out.</p>
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		<title>Comment on The importance of charge compensation in the membrane by Tom DeCoursey</title>
		<link>http://lettsscience.com/2012/09/15/the-importance-of-charge-compensation-in-the-membrane/#comment-430</link>
		<dc:creator><![CDATA[Tom DeCoursey]]></dc:creator>
		<pubDate>Fri, 15 Mar 2013 19:17:29 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=1196#comment-430</guid>
		<description><![CDATA[One small comment, mainly in response to the thread from the previous comment.  We worry a lot about whether our mutations have global effects, or change things in ways we did not imagine.  Whenever there is a way to test the overall integrity of the protein, we are happy to do it.  If you mutate a voltage-gated channel and it still gates in response to voltage, this supports the general integrity of the protein - voltage-gating seems a fairly complex activity.  In our in-press JGP paper, we point out that our MD simulations produce a similar water profile for the mutant as for WT channels, which also argues that the overall structure is reasonably intact. Once someone (hint, hint) determines the structure of Hv1, they will be able to determine structures for all the important mutants, too!  Mark Paddock did this with the bacterial reaction center - whenever he made a mutant, he determined the crystal structure, just to be sure!]]></description>
		<content:encoded><![CDATA[<p>One small comment, mainly in response to the thread from the previous comment.  We worry a lot about whether our mutations have global effects, or change things in ways we did not imagine.  Whenever there is a way to test the overall integrity of the protein, we are happy to do it.  If you mutate a voltage-gated channel and it still gates in response to voltage, this supports the general integrity of the protein &#8211; voltage-gating seems a fairly complex activity.  In our in-press JGP paper, we point out that our MD simulations produce a similar water profile for the mutant as for WT channels, which also argues that the overall structure is reasonably intact. Once someone (hint, hint) determines the structure of Hv1, they will be able to determine structures for all the important mutants, too!  Mark Paddock did this with the bacterial reaction center &#8211; whenever he made a mutant, he determined the crystal structure, just to be sure!</p>
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		<title>Comment on Is the S4 helix of Hv Short? by Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience</title>
		<link>http://lettsscience.com/2012/06/01/is-the-s4-helix-of-hv-short/#comment-402</link>
		<dc:creator><![CDATA[Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience]]></dc:creator>
		<pubDate>Sat, 23 Feb 2013 23:37:53 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=547#comment-402</guid>
		<description><![CDATA[[...] recall, I weighed in on this topic last summer in a series of posts (The Problem of aligning S4, Is the S4 helix of Hv short? and Biochemical Data Constraining the S4 of Hv). In my final entry in this series, I examined [...]]]></description>
		<content:encoded><![CDATA[<p>[...] recall, I weighed in on this topic last summer in a series of posts (The Problem of aligning S4, Is the S4 helix of Hv short? and Biochemical Data Constraining the S4 of Hv). In my final entry in this series, I examined [...]</p>
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		<title>Comment on Biochemical Data Constraining the S4 of Hv by Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience</title>
		<link>http://lettsscience.com/2012/06/20/biochemical-data-constraining-the-s4-of-hv/#comment-401</link>
		<dc:creator><![CDATA[Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience]]></dc:creator>
		<pubDate>Sat, 23 Feb 2013 23:37:50 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=712#comment-401</guid>
		<description><![CDATA[[...] avid readers of this blog may recall, I weighed in on this topic last summer in a series of posts (The Problem of aligning S4, Is the S4 helix of Hv short? and Biochemical Data Constraining the S4 of Hv). In my final entry [...]]]></description>
		<content:encoded><![CDATA[<p>[...] avid readers of this blog may recall, I weighed in on this topic last summer in a series of posts (The Problem of aligning S4, Is the S4 helix of Hv short? and Biochemical Data Constraining the S4 of Hv). In my final entry [...]</p>
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		<title>Comment on Human Hv1: Architectural Overview by Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience</title>
		<link>http://lettsscience.com/2012/06/12/human-hv1-architectural-overview/#comment-400</link>
		<dc:creator><![CDATA[Proton Channels at the Biophysical Society Meeting &#8211; 2013 &#124; LettsScience]]></dc:creator>
		<pubDate>Sat, 23 Feb 2013 23:37:43 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=655#comment-400</guid>
		<description><![CDATA[[...] the N-terminus has a significant impact on the channel gating (Musset et al. 2010; see my post Human Hv1: Architectual Overview to learn more). Specifically, they showed that, upon phosphorylation of Thr29, the opening of the [...]]]></description>
		<content:encoded><![CDATA[<p>[...] the N-terminus has a significant impact on the channel gating (Musset et al. 2010; see my post Human Hv1: Architectual Overview to learn more). Specifically, they showed that, upon phosphorylation of Thr29, the opening of the [...]</p>
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		<title>Comment on My Work by Sandipan Chowdhury</title>
		<link>http://lettsscience.com/my-work/#comment-386</link>
		<dc:creator><![CDATA[Sandipan Chowdhury]]></dc:creator>
		<pubDate>Sat, 17 Nov 2012 12:32:48 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?page_id=338#comment-386</guid>
		<description><![CDATA[congrats on your recent pnas paper - nicely done!]]></description>
		<content:encoded><![CDATA[<p>congrats on your recent pnas paper &#8211; nicely done!</p>
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		<title>Comment on The importance of charge compensation in the membrane by Sandipan Chowdhury</title>
		<link>http://lettsscience.com/2012/09/15/the-importance-of-charge-compensation-in-the-membrane/#comment-367</link>
		<dc:creator><![CDATA[Sandipan Chowdhury]]></dc:creator>
		<pubDate>Wed, 19 Sep 2012 22:59:48 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=1196#comment-367</guid>
		<description><![CDATA[Absolute fantabulous reply :)

The points which I had raised and you further commented on were not to say that charge-pairing does not occur. Rather that, although such a concept was proposed in the mid 1980s (or may be even earlier), even after 25yrs our understanding of such a basic proposition remains fraught with equal amounts of uncertainties!

Anyhow, the Pless et. al. paper - initially the paper actually does seem to be very exciting. But honestly after you&#039;ve actually seen the supplementary materials as well, I just can&#039;t help being left bewildered. Here&#039;s why:
E293 neutralization with Nha: no effect GV. But kinetics of GV and FV are slowed down. Through some funny/unexplained calculations, the authors concluded that the pronounced deceleration of the kinetics (which by some weird way corresponded to a 3-fold change in the activation/deactivation kinetics) suggests its role as a &quot;modest catalyst&quot;. The way the paper is written it is worded in such a way so as to suggest that E to Nha substitution does not apart from change the charge, but E to Q makes a H-bond donor, a H-bond acceptor, thereby suggesting that solvation at the site plays an important role. 
Dougherty&#039;s group have clearly shown that the H-bonding capacity of Nha, relative to E, is ~2-3 kcal/mol weaker. If the effects observed on perturbation of the site are largely via solvation, then Nha would&#039;ve had more of an effect (this is just speculation on my part). 
The next point in this regard is that, E293 when mutated to Q produces steady-state GV, QV and FV curves which aren&#039;t signficantly different from WT. The effect of E to Q mutation is large seen in the limiting slope analysis (Seoh et. al. Neuron 1996), where it was seen that this negative charge neutralization reduces Qmax from 13 to ~9. So my point is a similar experiment needs to be done with E293 to Nha to actually say whatever Pless et. al. want to say about this site. 
Finally, about the role of this E293 in reducing Qmax - if you compare Aggarwal and Mackinnon&#039;s values to Seoh et. al.&#039;s values, there is a consistent discrepancy of 2-3 charge units for almost all the charge neutralizations. (The charge add back experiments by Ahern and Horn in JGP actually support Aggarwal and Mackinnon and are not in agreement with Seoh et al). Is the reduction of Qmax due to E293Q, real to begin with? Also it must be mentioned that the comparable site in the BK channels is a Tyr. Ma and Horrigan (JGP 2006) found that mutating this site to E does not have any effect on Qmax. 
So, where are we about really understanding the role of E293 in the functional cycle of the VSDs - for me, actually nowhere!!!

Next for E283, Pless at. al.&#039;s data and analysis is more palatable (but only slightly so). If you see the crystal structure of 2R9R, there are water molecules everywhere around the E283 site. How can charge pairing occur if there is water all around? 

About the D316 site, I wouldn&#039;t know what to make of it, if you consider the data in the supplementary information. 

The other thing which I just want to mention that while stabilizing the charge is important. Keeping it a bit unstable is also as important, so that things can happen at the millisecond time scale. It is almost reminiscent of Dr. Mackinnon&#039;s Nobel Lecture Video, where he talks about the paradox between flux of ions and the high selectivity of K ions. While the charges need some stabilization, I firmly believe that it is necessary to have forces attenuating such stabilizations as well, so that the energy barriers for the transitions are relatively smaller such that the charges can move up and down quickly as the voltage-changes.]]></description>
		<content:encoded><![CDATA[<p>Absolute fantabulous reply <img src='http://s0.wp.com/wp-includes/images/smilies/icon_smile.gif' alt=':)' class='wp-smiley' /> </p>
<p>The points which I had raised and you further commented on were not to say that charge-pairing does not occur. Rather that, although such a concept was proposed in the mid 1980s (or may be even earlier), even after 25yrs our understanding of such a basic proposition remains fraught with equal amounts of uncertainties!</p>
<p>Anyhow, the Pless et. al. paper &#8211; initially the paper actually does seem to be very exciting. But honestly after you&#8217;ve actually seen the supplementary materials as well, I just can&#8217;t help being left bewildered. Here&#8217;s why:<br />
E293 neutralization with Nha: no effect GV. But kinetics of GV and FV are slowed down. Through some funny/unexplained calculations, the authors concluded that the pronounced deceleration of the kinetics (which by some weird way corresponded to a 3-fold change in the activation/deactivation kinetics) suggests its role as a &#8220;modest catalyst&#8221;. The way the paper is written it is worded in such a way so as to suggest that E to Nha substitution does not apart from change the charge, but E to Q makes a H-bond donor, a H-bond acceptor, thereby suggesting that solvation at the site plays an important role.<br />
Dougherty&#8217;s group have clearly shown that the H-bonding capacity of Nha, relative to E, is ~2-3 kcal/mol weaker. If the effects observed on perturbation of the site are largely via solvation, then Nha would&#8217;ve had more of an effect (this is just speculation on my part).<br />
The next point in this regard is that, E293 when mutated to Q produces steady-state GV, QV and FV curves which aren&#8217;t signficantly different from WT. The effect of E to Q mutation is large seen in the limiting slope analysis (Seoh et. al. Neuron 1996), where it was seen that this negative charge neutralization reduces Qmax from 13 to ~9. So my point is a similar experiment needs to be done with E293 to Nha to actually say whatever Pless et. al. want to say about this site.<br />
Finally, about the role of this E293 in reducing Qmax &#8211; if you compare Aggarwal and Mackinnon&#8217;s values to Seoh et. al.&#8217;s values, there is a consistent discrepancy of 2-3 charge units for almost all the charge neutralizations. (The charge add back experiments by Ahern and Horn in JGP actually support Aggarwal and Mackinnon and are not in agreement with Seoh et al). Is the reduction of Qmax due to E293Q, real to begin with? Also it must be mentioned that the comparable site in the BK channels is a Tyr. Ma and Horrigan (JGP 2006) found that mutating this site to E does not have any effect on Qmax.<br />
So, where are we about really understanding the role of E293 in the functional cycle of the VSDs &#8211; for me, actually nowhere!!!</p>
<p>Next for E283, Pless at. al.&#8217;s data and analysis is more palatable (but only slightly so). If you see the crystal structure of 2R9R, there are water molecules everywhere around the E283 site. How can charge pairing occur if there is water all around? </p>
<p>About the D316 site, I wouldn&#8217;t know what to make of it, if you consider the data in the supplementary information. </p>
<p>The other thing which I just want to mention that while stabilizing the charge is important. Keeping it a bit unstable is also as important, so that things can happen at the millisecond time scale. It is almost reminiscent of Dr. Mackinnon&#8217;s Nobel Lecture Video, where he talks about the paradox between flux of ions and the high selectivity of K ions. While the charges need some stabilization, I firmly believe that it is necessary to have forces attenuating such stabilizations as well, so that the energy barriers for the transitions are relatively smaller such that the charges can move up and down quickly as the voltage-changes.</p>
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		<title>Comment on The importance of charge compensation in the membrane by lettsscience</title>
		<link>http://lettsscience.com/2012/09/15/the-importance-of-charge-compensation-in-the-membrane/#comment-366</link>
		<dc:creator><![CDATA[lettsscience]]></dc:creator>
		<pubDate>Wed, 19 Sep 2012 16:40:27 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=1196#comment-366</guid>
		<description><![CDATA[Thank you for the awesome comments! I really enjoyed reading them and have spent the last few days pondering them. This is exactly the kind of discussion that I was hoping to generate when I started the blog. Below I have tried to respond to each of your points. Please let me know what you think. Also I would love to hear from any anyone else.  

It is clear that other channels don’t have the exact same pattern of charge compensation. I imagine that altering the distributions of charges within the membrane would be an excellent way for evolution to alter the gating behavior of the channel. Moving or removing counter charges in the membrane would affect the relative stabilities of the different channel states. More work certainly needs to be done to fully understand this potential mechanism. Also these different channels don’t all have the same number of gating charges so until we have more structures it is difficult to compare them directly. 

Thank you for bringing up the very interesting work of &lt;a href=&quot;http://www.nature.com/nchembio/journal/vaop/ncurrent/full/nchembio.622.html?annotation=1&quot; target=&quot;_blank&quot; rel=&quot;nofollow&quot;&gt;Pless et al.&lt;/a&gt; I really should have included this paper in my discussion but somehow it slipped my mind. What they show is not that these residues have no role in stabilizing the different conformations of the VSD but that their role may not be mediated by direct electrostatic interaction with S4. Instead, their role may be more about, as you say, generating a charge stabilizing hydrophilic environment proximal to the gating charges by attracting water into the VSD structure. Perhaps the way my post is written it emphasizes electrostatics too much and doesn’t emphasize hydrophilicity and water penetration enough. Clearly both are important and related. Additionally, it is very clear from their data the most buried external charge-compensation site (the outer S2 acid) is clearly electrostatic, which completely supports the arguments present in this post. 

There are certainly potential caveats to the work of &lt;a href=&quot;http://www.pnas.org/content/109/31/12800.short&quot; target=&quot;_blank&quot; rel=&quot;nofollow&quot;&gt;Hoshi and Armstrong&lt;/a&gt; and you very nicely point them out. To be devils advocate, the effects they see are from adding 50 μM La3+ - which of course comes along with 150 μM Cl- - to solutions which already contained over 140 mM Na+ and 150 mM Cl-. This is not really comparable to the 10-fold changes in ionic strength done by &lt;a href=&quot;http://jgp.rupress.org/content/117/1/69&quot; target=&quot;_blank&quot; rel=&quot;nofollow&quot;&gt;Islas and Sigworth&lt;/a&gt;. Therefore, I would imagine that the ionic strength effects of Debye-screening would be minimal.  However, it is certainly possible that strong interactions of La3+ with the phosphate head groups of the lipids could be partially (or wholly) responsible for the changes in gating seen.

In the 2005 Science paper from the von Heijne lab &lt;a href=&quot;http://www.sciencemag.org/content/307/5714/1427.short&quot; target=&quot;_blank&quot; rel=&quot;nofollow&quot;&gt;Hessa et al.&lt;/a&gt; “conclude that the S4 helix is poised near the threshold of efficient bilayer insertion” and even calculate a positive apparent free energy of translocon-mediated integration. To me this does not indicate that the S4 “readily inserts” or that it can “happily sit in the membrane.” Can it insert, yes, with low efficiency. The fact that, as you say, the membrane likely distorts to accommodate the inserted S4 indicates to me that it is pretty unhappy. Also the fact that Hessa et al. observe that a significant proportion of the S4 helices do not insert into the membrane is also telling. Finally they conclude that, “If one or two of the Arg residues in S4 are partially shielded from direct lipid contact in the intact channel structure, as has been proposed, ΔG&lt;sub&gt;app&lt;/sub&gt; might be further reduced.” As I demonstrate in this post, the structure shows us how this stabilization is achieved.

You are completely correct in saying that structures do not provide interaction energies and that existing problems with force fields prevent accurate computational deduction of interaction energies. However, the structures do clearly show us which interactions exist and it is now up to us to figure out the experiments that need to be done to determine the specific energies to truly understand their relative importance. 

I agree that scientist should avoid becoming attached to their assumptions. There certainly is still a lot of uncertainty and plenty of room for argument ☺ 

It is well known by anyone who studies these channels that a significant proportion of point mutations results in either no expression or non-functional channels, so clearly a single point mutation can disrupt the entire channel structure. This can also be true for soluble proteins. I am certainly not saying that people shouldn’t do or publish mutagenesis studies, only that we have to be careful when we interpret them. This can be difficult in modern publishing, which encourages and even insists that scientists over sell their findings giving the impression of close-mindedness and being married to assumptions. However, with very few exceptions, most scientists in the field that I have met don’t actually believe their own hype. This problem with scientific publishing is part of the reason I felt the need to start this blog. As per always, the best way to combat close-mindedness in science is to perform more carefully designed well thought out experiments. Anyone who loves science loves being proven wrong. The tricky part is in the proving.]]></description>
		<content:encoded><![CDATA[<p>Thank you for the awesome comments! I really enjoyed reading them and have spent the last few days pondering them. This is exactly the kind of discussion that I was hoping to generate when I started the blog. Below I have tried to respond to each of your points. Please let me know what you think. Also I would love to hear from any anyone else.  </p>
<p>It is clear that other channels don’t have the exact same pattern of charge compensation. I imagine that altering the distributions of charges within the membrane would be an excellent way for evolution to alter the gating behavior of the channel. Moving or removing counter charges in the membrane would affect the relative stabilities of the different channel states. More work certainly needs to be done to fully understand this potential mechanism. Also these different channels don’t all have the same number of gating charges so until we have more structures it is difficult to compare them directly. </p>
<p>Thank you for bringing up the very interesting work of <a href="http://www.nature.com/nchembio/journal/vaop/ncurrent/full/nchembio.622.html?annotation=1" target="_blank" rel="nofollow">Pless et al.</a> I really should have included this paper in my discussion but somehow it slipped my mind. What they show is not that these residues have no role in stabilizing the different conformations of the VSD but that their role may not be mediated by direct electrostatic interaction with S4. Instead, their role may be more about, as you say, generating a charge stabilizing hydrophilic environment proximal to the gating charges by attracting water into the VSD structure. Perhaps the way my post is written it emphasizes electrostatics too much and doesn’t emphasize hydrophilicity and water penetration enough. Clearly both are important and related. Additionally, it is very clear from their data the most buried external charge-compensation site (the outer S2 acid) is clearly electrostatic, which completely supports the arguments present in this post. </p>
<p>There are certainly potential caveats to the work of <a href="http://www.pnas.org/content/109/31/12800.short" target="_blank" rel="nofollow">Hoshi and Armstrong</a> and you very nicely point them out. To be devils advocate, the effects they see are from adding 50 μM La3+ &#8211; which of course comes along with 150 μM Cl- &#8211; to solutions which already contained over 140 mM Na+ and 150 mM Cl-. This is not really comparable to the 10-fold changes in ionic strength done by <a href="http://jgp.rupress.org/content/117/1/69" target="_blank" rel="nofollow">Islas and Sigworth</a>. Therefore, I would imagine that the ionic strength effects of Debye-screening would be minimal.  However, it is certainly possible that strong interactions of La3+ with the phosphate head groups of the lipids could be partially (or wholly) responsible for the changes in gating seen.</p>
<p>In the 2005 Science paper from the von Heijne lab <a href="http://www.sciencemag.org/content/307/5714/1427.short" target="_blank" rel="nofollow">Hessa et al.</a> “conclude that the S4 helix is poised near the threshold of efficient bilayer insertion” and even calculate a positive apparent free energy of translocon-mediated integration. To me this does not indicate that the S4 “readily inserts” or that it can “happily sit in the membrane.” Can it insert, yes, with low efficiency. The fact that, as you say, the membrane likely distorts to accommodate the inserted S4 indicates to me that it is pretty unhappy. Also the fact that Hessa et al. observe that a significant proportion of the S4 helices do not insert into the membrane is also telling. Finally they conclude that, “If one or two of the Arg residues in S4 are partially shielded from direct lipid contact in the intact channel structure, as has been proposed, ΔG<sub>app</sub> might be further reduced.” As I demonstrate in this post, the structure shows us how this stabilization is achieved.</p>
<p>You are completely correct in saying that structures do not provide interaction energies and that existing problems with force fields prevent accurate computational deduction of interaction energies. However, the structures do clearly show us which interactions exist and it is now up to us to figure out the experiments that need to be done to determine the specific energies to truly understand their relative importance. </p>
<p>I agree that scientist should avoid becoming attached to their assumptions. There certainly is still a lot of uncertainty and plenty of room for argument ☺ </p>
<p>It is well known by anyone who studies these channels that a significant proportion of point mutations results in either no expression or non-functional channels, so clearly a single point mutation can disrupt the entire channel structure. This can also be true for soluble proteins. I am certainly not saying that people shouldn’t do or publish mutagenesis studies, only that we have to be careful when we interpret them. This can be difficult in modern publishing, which encourages and even insists that scientists over sell their findings giving the impression of close-mindedness and being married to assumptions. However, with very few exceptions, most scientists in the field that I have met don’t actually believe their own hype. This problem with scientific publishing is part of the reason I felt the need to start this blog. As per always, the best way to combat close-mindedness in science is to perform more carefully designed well thought out experiments. Anyone who loves science loves being proven wrong. The tricky part is in the proving.</p>
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		<title>Comment on The importance of charge compensation in the membrane by Sandipan Chowdhury</title>
		<link>http://lettsscience.com/2012/09/15/the-importance-of-charge-compensation-in-the-membrane/#comment-362</link>
		<dc:creator><![CDATA[Sandipan Chowdhury]]></dc:creator>
		<pubDate>Tue, 18 Sep 2012 05:15:16 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=1196#comment-362</guid>
		<description><![CDATA[Nice post yet again...but I do have some comments, especially about the role of the negative charges:
The strong conservation of the negative charges and their positions as revealed in structure seem to strongly support the notion that charge-pairing is a potential mechanism whereby the putatively large energy barrier associated with translocation of the Args have been suppressed during the functional cycle of the voltage-sensors. However, E283 (external S2) which is potentially interacting with multiple positive charges on S2 is not conserved in several several VSDs such as those in the Nav, Cav and other Kv channel families. What forces stabilize the VSDs in such systems? A recent paper by Pless et. al. (Nature Chemical Biology, 2011) seems to suggest that the countercharges in the charge transfer center are also not involved in any electrostatic interaction, which stabilizes conformations. All the negative charges occur in a region bathed in water - the crystallographic waters in the 2R9R structure are strongly nestled around E283 (external S2) while the internal negative charges are in a deep broad crevice which in all likelihood is also water filled. Electrostatic interactions between the Args on S4 and the negative charges would be severely attenuated under such conditions. In fact in many soluble proteins it has been convincingly demonstrated that the desolvation penalty associated with a salt-bridge interaction is counter-intuitively, destabilizing. The paper by Hoshi and Armstrong have neglected to consider a crucial effect of La3+ - the 3+ charge! La3+ has strong surface charge effects (shields the phospholipid head groups and thus could potentially decelerate activation by interfering with the interactions of R1 with the lipid groups). (Mg2+ has been shown to exert such an effect by Diane Papazian&#039;s group). Additionally, Islas and Sigworth (2001, JGP) had shown that increasing ionic strengths of the bulk medium could have large effects on the shape of electric field, simply by virtue of Debye-screening - La3+ (and its negative ions in the salt) would significantly enhance the ionic strength and thereby could also be potentially responsible for the effects described by Hoshi and Armstrong. Additionally, Hessaa-Von-Heijne have demonstrated that the S4 helix, despite the preponderance of positive charges can readily insert itself in the membrane. FTIR measurements of the S4 peptide also have shown the transmembrane orientation of the helix. Thus inspite of being decorated with all these charges, the S4 helix can, quite unfathomably, happily sit inside the membrane! If one goes into the detailed physics of the issue, probably the only way this could happen is if, upon incorporation, the S4 helix alters the shape of the membrane (say thins it out). Such thinning has been observed by Kenton Swartz&#039;s group through the use of neutron diffraction and solid state NMR measurements. However, the extent of thinning reported (~5A by the full VSD of KvAP) is far too small to explain the large energy cost of housing so many positive charges in the membrane. May be the water in the crevices help pacify the otherwise belligerent Args...who knows??? Of course all of this is largely speculative and the only way out of this conundrum can be by calculating energies of interaction. Structures are useful, but they provide no proof of interaction (strength/attractive/repulsive); computational evaluation of interactions are fraught with uncertainties about the force-fields; functional measurements are limited by accuracy of data collection and to what extent are the details considered. 
A common trait of scientists in the ion channel community (and may be all of science) is that - each have their own favorite assumption which they most of often cling on to with all their might - but who is to say which assumption is valid and which one is not? For example, water in crevices seems to be &quot;so big a deal&quot; for the proponents of small scale VSD motion - the assumption is that water in the crevices has the same properties as in the bulk. On absolute scale, such an assumption can be only partially correct, at best (and at worst, completely wrong!!!) since several experimental physical chemists have strongly argued and demonstrated that water within crevices have vastly different properties (the list not limited just to dielectric constant) than bulk water. However, we chose not to deal with such an assumption largely because of absence of methods to show its significance/insignificance. The major thrust in the study of ion channels is mutation and analysis of mutations - now if one begins to consider that even a single point mutation could disrupt the structure, it might become impossible to publish even a single paper! Hence we chose to, most often, neglect that assumption and barge ahead with our scanning mutagenesis studies. I am deeply passionate and interested about the physics of charge transfer dynamics in the voltage-sensors. Unfortunately, the close-mindedness of our community, which is upheld under a facade of scientific skepticism, is just too overbearing at times :(. 
(P.S.: Sorry for the negativity)
Keep the posts coming.]]></description>
		<content:encoded><![CDATA[<p>Nice post yet again&#8230;but I do have some comments, especially about the role of the negative charges:<br />
The strong conservation of the negative charges and their positions as revealed in structure seem to strongly support the notion that charge-pairing is a potential mechanism whereby the putatively large energy barrier associated with translocation of the Args have been suppressed during the functional cycle of the voltage-sensors. However, E283 (external S2) which is potentially interacting with multiple positive charges on S2 is not conserved in several several VSDs such as those in the Nav, Cav and other Kv channel families. What forces stabilize the VSDs in such systems? A recent paper by Pless et. al. (Nature Chemical Biology, 2011) seems to suggest that the countercharges in the charge transfer center are also not involved in any electrostatic interaction, which stabilizes conformations. All the negative charges occur in a region bathed in water &#8211; the crystallographic waters in the 2R9R structure are strongly nestled around E283 (external S2) while the internal negative charges are in a deep broad crevice which in all likelihood is also water filled. Electrostatic interactions between the Args on S4 and the negative charges would be severely attenuated under such conditions. In fact in many soluble proteins it has been convincingly demonstrated that the desolvation penalty associated with a salt-bridge interaction is counter-intuitively, destabilizing. The paper by Hoshi and Armstrong have neglected to consider a crucial effect of La3+ &#8211; the 3+ charge! La3+ has strong surface charge effects (shields the phospholipid head groups and thus could potentially decelerate activation by interfering with the interactions of R1 with the lipid groups). (Mg2+ has been shown to exert such an effect by Diane Papazian&#8217;s group). Additionally, Islas and Sigworth (2001, JGP) had shown that increasing ionic strengths of the bulk medium could have large effects on the shape of electric field, simply by virtue of Debye-screening &#8211; La3+ (and its negative ions in the salt) would significantly enhance the ionic strength and thereby could also be potentially responsible for the effects described by Hoshi and Armstrong. Additionally, Hessaa-Von-Heijne have demonstrated that the S4 helix, despite the preponderance of positive charges can readily insert itself in the membrane. FTIR measurements of the S4 peptide also have shown the transmembrane orientation of the helix. Thus inspite of being decorated with all these charges, the S4 helix can, quite unfathomably, happily sit inside the membrane! If one goes into the detailed physics of the issue, probably the only way this could happen is if, upon incorporation, the S4 helix alters the shape of the membrane (say thins it out). Such thinning has been observed by Kenton Swartz&#8217;s group through the use of neutron diffraction and solid state NMR measurements. However, the extent of thinning reported (~5A by the full VSD of KvAP) is far too small to explain the large energy cost of housing so many positive charges in the membrane. May be the water in the crevices help pacify the otherwise belligerent Args&#8230;who knows??? Of course all of this is largely speculative and the only way out of this conundrum can be by calculating energies of interaction. Structures are useful, but they provide no proof of interaction (strength/attractive/repulsive); computational evaluation of interactions are fraught with uncertainties about the force-fields; functional measurements are limited by accuracy of data collection and to what extent are the details considered.<br />
A common trait of scientists in the ion channel community (and may be all of science) is that &#8211; each have their own favorite assumption which they most of often cling on to with all their might &#8211; but who is to say which assumption is valid and which one is not? For example, water in crevices seems to be &#8220;so big a deal&#8221; for the proponents of small scale VSD motion &#8211; the assumption is that water in the crevices has the same properties as in the bulk. On absolute scale, such an assumption can be only partially correct, at best (and at worst, completely wrong!!!) since several experimental physical chemists have strongly argued and demonstrated that water within crevices have vastly different properties (the list not limited just to dielectric constant) than bulk water. However, we chose not to deal with such an assumption largely because of absence of methods to show its significance/insignificance. The major thrust in the study of ion channels is mutation and analysis of mutations &#8211; now if one begins to consider that even a single point mutation could disrupt the structure, it might become impossible to publish even a single paper! Hence we chose to, most often, neglect that assumption and barge ahead with our scanning mutagenesis studies. I am deeply passionate and interested about the physics of charge transfer dynamics in the voltage-sensors. Unfortunately, the close-mindedness of our community, which is upheld under a facade of scientific skepticism, is just too overbearing at times <img src='http://s0.wp.com/wp-includes/images/smilies/icon_sad.gif' alt=':(' class='wp-smiley' /> .<br />
(P.S.: Sorry for the negativity)<br />
Keep the posts coming.</p>
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	<item>
		<title>Comment on The Omega Current by The importance of charge compensation in the membrane &#171; LettsScience</title>
		<link>http://lettsscience.com/2012/07/24/the-omega-current/#comment-361</link>
		<dc:creator><![CDATA[The importance of charge compensation in the membrane &#171; LettsScience]]></dc:creator>
		<pubDate>Tue, 18 Sep 2012 00:49:05 +0000</pubDate>
		<guid isPermaLink="false">http://lettsscience.com/?p=987#comment-361</guid>
		<description><![CDATA[[...] it is thought that R2 or even R1 (in the potential deeply hyperpolarized conformation, see my previous post) would occupy the charge transfer center. This would leave the external charge compensation sites [...]]]></description>
		<content:encoded><![CDATA[<p>[...] it is thought that R2 or even R1 (in the potential deeply hyperpolarized conformation, see my previous post) would occupy the charge transfer center. This would leave the external charge compensation sites [...]</p>
]]></content:encoded>
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