Table 2.
Fold-change |
||||||||||
---|---|---|---|---|---|---|---|---|---|---|
Construct | Agonist | f | SE | b | SE | E | Observed | Predicted | ΔΔG | n |
A96Y+Y127A | Cho | 2690 | 400 | 3530 | 850 | 0.76 | 16.5 | 169 | 1.4 | 3 |
A96K+Y127E | Cho | 4680 | 190 | 5510 | 480 | 0.85 | 18.5 | 0.118 | −3.0 | 3 |
A96C+Y127C | Cho | 7760 | 460 | 793 | 98 | 9.79 | 213 | 0.589 | −3.5 | 3 |
I49A+A96L | Cho | 1980 | 290 | 6360 | 430 | 0.31 | 6.77 | 18 | 0.6 | 5 |
I49Y+A96L | Cho | 8110 | 1000 | 925 | 140 | 8.77 | 191 | 468 | 0.5 | 5 |
I49K+A96D | Cho | 3640 | 15 | 1230 | 19 | 2.97 | 64.6 | 65,600 | 4.1 | 3 |
I49C+A96C | ACh | 2690 | 320 | 3340 | 410 | 0.80 | 0.029 | 673 | 5.9 | 3 |
I49D+Y127K | ACh | 3620 | 99 | 8590 | 1100 | 0.42 | 0.015 | 0.013 | −0.1 | 3 |
I49Y+Y127I | ACh | 3700 | 270 | 9460 | 180 | 0.39 | 0.014 | 0.009 | −0.2 | 4 |
I49K+Y127D | ACh | 321 | 34 | 7830 | 60 | 0.041 | 0.001 | 0.001 | −0.0 | 3 |
I49C+Y127C | ACh | 5570 | 250 | 9930 | 1000 | 0.56 | 0.020 | 0.029 | 0.2 | 3 |
Y93H+A96H | None | 203 | 44 | 8420 | 1900 | 0.024 | 36,500 | 48,200 | 0.1 | 3 |
Y93R+A96H | None | 124 | 15 | 12,200 | 140 | 0.010 | 15,400 | 8950 | −0.32 | 3 |
A96N+W149S | None | 411 | 5 | 9380 | 800 | 0.044 | 66,400 | 73,300 | 0.06 | 3 |
N95W+Y127F | ACh | 12200 | 1400 | 2510 | 22 | 4.88 | 0.173 | 0.132 | −0.16 | 3 |
I49Y+N95W | ACh | 1810 | 380 | 4990 | 590 | 0.36 | 0.013 | 0.021 | 0.30 | 5 |
Column definitions are given in Table 1. Fold-change (observed) is Emutant-pair/Ewt and fold-change (predicted) is the product of the fold-changes in E measured for each mutant of the pair alone. Rate constants for αY127, αY93, and αW149 mutants can be found in Purohit and Auerbach (21,41). The coupling energy, ΔΔG (kcal/mol), is calculated as described in Materials and Methods. The range-coupling-energy is the difference between the largest and smallest ΔΔG values (kcal/mol): 96-127 (Y/A-C/C) = 4.9; 96-49 (C/C-Y/L) = 5.4; 49-127 (C/C-D/K) = 0.3.