Table 2.
Prediction of the Absorption Maximum of the GFP S65T R96M T203Y Mutant at Room Temperature, Comparing the Assumption That Either the Driving Force or the Transition Energy Is Additivea
driving force (cm−1) | transition energy (cm−1) | |
---|---|---|
ihmat(65T)·ih:loop:GFP R96M | 10270 | 21645 |
s10:loop:GFP S65T | 8080 | 20695 |
s10:loop:GFP S65T T203Y | 4870 | 19666 |
ihmat(65T)·ih:loop:GFP R96M T203Y | ||
assumption | driving force is additive | transition energy is additive |
prediction | 10270 − 8080 + 4870 = 7060 | 21645 – 20695 + 19666 = 20616 |
predicted transition energy (absorption maximum) | (70602 + 190602)1/2 = 20330 cm−1 (492 nm) | 20616 cm−1 (485 nm) |
observed transition energy (absorption maximum) | 20240 cm−1 (494 nm) |
To account for the minor differences between absorption maxima of circular permutants, we use the ih circular permutant as the basal value. The driving forces and transition energies are extracted from Tables S13 and S12, respectively. The conversion between transition energy and driving force is performed via eq S13 using V0 = 9530 cm−1 (Figure 8).