0.003 s, i.e. about 1% for a RE
cycle. Given that I only attempt an exchange every 1000 cycles, I took
this to be negligible.
The only odd thing I saw was that on a RE cycle it appears to spend 0.6s
in do_force() which is twice the average MD step time. I didn't print
this out for
to see qualitative similarities.
Note also that you are comparing the molecule in solution with the
molecule in the crystal, and there will certainly be differences near
crystal contacts.
There is no B factor for NMR structures. The closest equivalent is to
look at the variation between MODE
Ah yes, of course. I keep forgetting these strange units ;-)
m
On Wed, 2009-02-04 at 11:16 +0100, David van der Spoel wrote:
> Martyn Winn wrote:
> > The factor is 8 * pi^2
>
> The 100 comes from nm to Angstrom.
>
> > The factor 1/3 arises when you take the
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so.6 => /usr/lib/libXdmcp.so.6 (0x7f071fa37000)
Cheers
Martyn
On Tue, 2008-12-02 at 13:52 +0100, Florian Haberl wrote:
> Hi,
>
> On Tuesday, 2. December 2008, Martyn Winn wrote:
> > Hi all,
> >
> > I've compiled 4.0.2 from source on an EM64T machine runn
ogies if I missed it.
Cheers
Martyn
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