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Recovery from
Slow Inactivation
in K+ Channels
Is Controlled by
Buried Water
Molecules
Jared L. Ostmeyer1, Sudha
Chakrapani2, Eduardo
Perozo1, Benoît Roux1
1University of Chicago, 2Case Western Reserve University
Activation Gate Open
Conductive
Filter Inactive Filter
Activation Gate Closed
Conductive Filter
Inactive Filter
Entry into
Inactivation
Recovery
from
Inactivation
time(sec)
Ext [K+] mM
Conformational transitions underlying
recovery from slow inactivation
10-20 seconds
1K4D 1K4C
Subtle differences between the two
conformations of the selectivity filter.
1K4D 1K4C
Pinched Conductive
Pinched Conformation Is Stable
Hydrogen Bond Network Binds Waters
HOH:2006
HOH:2007
HOH:2010
79:N
81:O
80:OD
71:O
‡Cross subunit interaction with 76:O not shown
‡
1K4C1K4D
Waters Appear to Block Recovery
Free Energy Landscape of the Recovery
Process
Markov Model Predicts Long Recovery
Time
1/kb = 79 ns
1/kf = 11 μs
1/ka = 8.3(150/[K+]) ns
Experimental Model
Experimental Results
τcontrol = 12.2±3.0 sec τsucrose= 7.7±5.5 sec
Conclusion
Water molecules act as ligands that trap the selectivity filter
in an inactive confirmation when present. This explains the
long timescales of slow-inactivation.
Wild Type Y82A Mutant
Luis Cuello
Acknowledgements
Eduardo Perozo
Albert Pan
Sudha Chakrapani
Benoît Roux
NIH Grants:
• R01-GM062342 (B.R)
• R01-GM57846 (E.P.)
NRBSC (Anton Allocation):
• RC2GM093307
INCITE:
• Supercomputing time provided at
Oak Ridge National Laboratories

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recovery_talk_0.7

Editor's Notes

  1. Hello, my name is Jared Ostmeyer. Today I am going to talk about recovery from slow-inactivation in K+ channels. It is our conclusion that this process is controlled by water molecules buried inside the protein.
  2. In all K+ channels that exhibit slow-inactivation, current passing through the channel will taper off over time. It is well known that the loss of current is mediated by some conformation transition taking place in the selectivity filter (LEFT) . In other words, if we open the activation gate to allow current to pass through, and we wait long enough, we should expect to see the selectivity filter an inactivated state. We can summarize this process with a simple hypothetical free-energy landscape where the inactive filter is the more stable state. The process is reversed once the activation gate is closed. Closing the activation gate promotes recovery from inactivation, returning the selectivity filter back to its original conductive state, so the channel is primed and ready to go again. The recovery process is extremely slow. In KcsA, a potassium channel, recovery from slow inactivation takes up to 8 seconds even in the presence of 1M extracellular K+ solution. Now we can again summarize recovery from inactivation with another hypothetical free-energy landscape. But this time our hypothetical free-energy landscape for the recovery process is essentially opposite what is was before. Now I’ve drawn a sizeable free-energy barrier that acts to impede recovery from slow-inactivation because we know this process takes a long time.
  3. Like the title of my talk suggests, we want to study slow-inactivation. It just so happens that we have X-ray crystal structures of the two endpoints of the recovery process for KCSA. Here is the selectivity filter from the crystal structure 1K4D. It features a pinched filter that looks just a little to narrow in the middle for K+ ions to pass through. Presumably this is a non-conductive state of the selectivity filter. There was debate over whether or not the pinched filter represented slow inactivated state of the filter. Just because the conformation looks non-conductive doesn’t mean it actually represents the long lasting inactivated state. Recently, Luis Cuello obtained X-ray crystal structures of KcsA with open activation gates. We just saw that when the activation gate is open, the selectivity filter should reach its slow-inactivated state. It just so happens that the selectivity filter in the open structures is in the same pinched conformation. Here, I have just superimposed the filter from an open channel on top of the pinched state. You can see that they are essentially the same. Thus, the end-stage conformation of the selectivity filter of an open channel matches that of the initial state of the closed channel. This reinforces the viewpoint that the pinched filter models the structure of the inactivated filter. Here is the selectivity filter from the crystal structure 1K4C. It features an obviously conductive filter. Binding sites for K+ ions line the permeation pathway throughout the entire filter.
  4. There is just one problem. Here I am again showing you the pinched and conductive filter. If we superimposed these two structures on top of each other… we see that the difference between the coordinates of the two conformation is subtle. The largest difference through the permeation pathway of the filter is where the filter pinches shut. Here, the Cα glycine residues have moved in by an 1Å. This is an absurdly subtle change. If we knew nothing about K+ channels other than these two crystal structures of KcsA, we might expect the recovery process could occur spontaneously simply due to thermal fluctuations alone. It is hard to image why it takes so long for the channel to recover. To put the timescales in perspective, bacteria can synthesize entire subunits of the channel on the same timescale as the recovery process.
  5. To elucidate what is going on we began by running a 17μs long simulation of the pinched selectivity filter. We setup the simulation to promote recovery from inactivation in everyway we could. The activation gate was in a closed conformation, & we bathed the channel in the simulation in 1M KCl solution. We honestly expected to observe the selectivity filter fluctuate to the width of a conductive filter. However, over the course of our 17μs long simulation nothing interesting happened. In the top trace I am showing you the width of the selectivity filter measured as the distance between the Cα atoms on the glycine residues. As you can see the width of the filter remained at 5.5Å, which is the width of the pinched filter. The width of the filter never deviated to 8.1Å. This told us the pinched conformation was stable, at least over the timescale of 17μs. The bottom trace shows the position of K+ ions along the height of the selectivity filter. As you can see, K+ ions were never able to reach positions in the center of the selectivity filter. This told us the pinched filter was indeed non-conductive. Over on the right I showing you the selectivity filter at the end of the simulation. We noticed that water molecules had remained behind the selectivity filter throughout the entire simulation. We then asked the question what was it that was keeping water molecules present behind the filter.
  6. Already, you can see that the traces of the inactivating currents look very different under the applied osmotic stress.
  7. This work was supported by the National Institute of Health through grant R01-GM062342 (J.O. and B.R) and R01-GM57846 (S.C. and E.P.). The authors acknowledge supercomputer time provided by the Oak Ridge National Laboratory via the INCITE program of the Department of Energy. Anton computer time was provided by the National Resource for Biomedical Supercomputing and the Pittsburgh Supercomputing Center through Grant RC2GM093307 from the National Institutes of Health. The Anton machine had been donated generously by David E. Shaw; we are most grateful for the opportunity to use Anton.