For POTEntial=3DPO, a restraining function for 3D NOE-NOE
experiments is used.
The intensity of a 3D NOE-NOE crosspeak,
![$I_{ijk}(\tau_{m1},\tau_{m2})$](img662.png)
,
between spins
![$i,j$](img663.png)
, and
![$k$](img71.png)
, is
proportional to the product of the individual NOE transfer
efficiencies of each mixing time:
![\begin{displaymath}
I_{ijk}(\tau_{m1},\tau_{m2}) = c[exp(-{\bf R}\tau_{m2})]_{ij}
[\exp(-{\bf R} \tau_{m1})]_{jk}A_{kk}(0),
\end{displaymath}](img664.png) |
(20.14) |
where
![$\tau_{m1}$](img665.png)
is the first and
![$\tau_{m2}$](img666.png)
the second mixing time,
R the cross-relaxation matrix,
![$A_{kk}(0)$](img667.png)
the
equilibrium magnetization of spins
![$k$](img71.png)
, and
![$c$](img443.png)
a constant.
The 3D NOE-NOE intensity can be approximated by
![\begin{displaymath}
I_{ijk}^{calc} = r_{ij}^{-6} r_{jk}^{-6}.
\end{displaymath}](img668.png) |
(20.15) |
where
![$r_{ij}$](img669.png)
and
![$r_{jk}$](img670.png)
are the distances between spins
![$i,j$](img663.png)
and
![$j,
k$](img671.png)
,
respectively, and the proportionality constant is set equal to one.
The 3D NOE-NOE function is given by
![\begin{displaymath}
E_{NOE}^{class} = S \times
\end{displaymath}](img672.png) |
(20.16) |
where
![$S$](img264.png)
is the energy constant specified
by the SCALe statement,
![$I_{ijk}^{obs}$](img674.png)
is the
observed NOE-NOE intensities,
![$\Delta_{l}$](img675.png)
and
![$\Delta_{u}$](img676.png)
are error bounds, and
![$K$](img677.png)
is a scale factor specified by
the RSWITch statement. The NOE-NOE connectivity
![$i \rightarrow j \rightarrow k$](img678.png)
and the
intensity and error-bound information are provided by
a pair of ASSIgn statements:
The first ASSIgn statement specifies spins
![$i$](img120.png)
and
![$j$](img488.png)
, along
with the observed intensity
![$I_{ijk}^{obs}$](img674.png)
and the
error bounds
![$\Delta_{l}$](img675.png)
and
![$\Delta_{u}$](img676.png)
. The second ASSIgn
statement specifies spins
![$j$](img488.png)
and
![$k$](img71.png)
; the three real numbers
following the second selection are irrelevant and can be set
to arbitrary values.
Note: the 3D NOE-NOE function can be used in combination with
R-6 or center averaging. For further details, the reader is referred
to
Habazettl et al.
(
1992b,
a)
and
Bernstein et al. (1993).
Xplor-NIH 2024-09-13