Skip to main content
. Author manuscript; available in PMC: 2014 Aug 11.
Published in final edited form as: J Mol Model. 2010 Jul 3;17(4):899–911. doi: 10.1007/s00894-010-0784-7

Table 3. Results from the energy optimization of T- and R-state models of the FBPase averaged over four subunits (kcal mol−1).

Total final energy (all subunits)
FBPase (tetramer)a ATCase (dodecamer)b
No ligand Ligand (AMP) No ligand Ligand (PALA)
T state -45523 -46870 -111070 -114270
R state -45549 -46809 -111340 -114850
Difference 26 -61 270 580
The energy of the β-sheet of relevant domainsc
No ligand Ligand (AMP) No ligand Ligand (PALA)
Intra Inter Intra Inter Intra Inter Intra Inter
T state -499.15 -1251.68 -494.36 -1364.52 -406.95 -1122.4 -404.85 -1475.49
(SD)e (3.04) (3.61) (3.82) (18.5) (1.24) (10.03) (0.72) (7.16)
R state -478.75 -1279.15 -466.97 -1425.31 -413.35 -1146.12 -409.00 -1496.53
(SD)e (0.01) (0.01) (0.01) (0.06) (3.46) (2.96) (4.11) (0.74)
Difference -20.4 27.79 -29.25 60.79 6.4 23.72 4.15 21.04
Diff of relevant statesd -15.61 -85.37 2.05 374.13
Diff of total (Intra+Inter) -100.98 376.18
a

In the FBPase calculations, the AMP was present as a ligand that stabilizes the T state

b

In the ATCase calculations, PALA was present as a ligand that stabilizes the R state

c

In FBPase, the β-sheet of the AMP-binding domain was selected for computation; in ATCase, the ASP domain was selected

d

For FBPase (T + AMP) − R, for ATCase T − (R + PALA)

e

Standard deviation calculated over the subunits participating in an assembly: 4 in FBPase and 6 in ATCase