Potassium channel seen from the side (two of four identical subunits are shown) and from above (all four subunits are shown.) The selectivity filter loops at the center prevent other ions such as sodium from passing through the pore.
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More than a static image

Just four years ago, the world got its first view of what a potassium channel looks like. An X-ray crystallographic image taken in 1998 by Rod MacKinnon and collaborators at Rockefeller University revealed the channel's three-dimensional form. Its mouth was perfectly sized to admit a potassium ion stripped of its surrounding cloud of water molecules but would not let in a dehydrated sodium ion. The channel was long enough to hold several ions at once, suggesting how it could transport ions so quickly. And the channel's negatively charged interior, which resembled the environment of water, suggested it could entice a potassium ion to shed its water molecules and slip inside as easily as if it remained in solution. That, however, was where the insights ended.

"The X-ray images gave us the essential elements that are needed to understand the channel's operation. But these are static, so one cannot see the forces that come into play when the ions and the water molecules are moving," Roux says. To understand how the channel ushers potassium ions along, and why the ions don't repel one another more strongly, scientists needed to create and animate a virtual version of the entire system using molecular dynamics. This was done using supercomputers, including the SGI Origin2000 at NCSA at the University of Illinois at Urbana-Champaign.

Berneche and Roux used a program known as CHARMM (Chemistry at Harvard Molecular Mechanics), which is designed specifically to run molecular dynamics simulations, to build a potassium channel, cell membrane molecules, water molecules and potassium ions. "Our calculations are a way to exploit the fantastic information obtained recently from the X-ray images so that we can really connect them to the most fundamental physical laws," Roux says. All in all, the program tracked the activities of about 40,000 atoms--a hefty computational burden.

But even with today's most powerful supercomputers, it would be impossible to track the movements of every atom in the system while simulating a single potassium ion arriving at, entering, and completely traversing the channel. So Berneche and Roux adopted a more practical strategy and mapped the energetic topography of the journey instead. The technique can be likened to measuring the hills and valleys a rolling ball might encounter. The places within the channel where repulsive atomic forces encourage ions to roll away would be the hills. Sites within the channel where energy barriers are low tend to slow the travel of ions like valleys. With this topography mapped out, they were able to calculate the average energetic environment a traveling potassium ion would be likely to see.