TABLE 1.
Residue* | ΔRex* (s−1) | ΔΔRex†(s−1) | Rex* (s−1) | (μs)* | (ppm)* | f† |
---|---|---|---|---|---|---|
14 | <0.7 | −2.3 | 4.5 | <33 | 1.5 | <0.5 |
19 | 3.4 | −3.6 | 12.0 | 55 | 2.8 | 0.6 |
27 | 1.6 | 0.0 | 8.6 | 40 | 2.8 | 0.8 |
28 | 2.0 | 1.1 | 7.2 | 55 | 2.2 | 0.9 |
36 | 2.2 | 1.6 | 1 | >220 | <0.8 | – |
39 | 4.7 | 1.5 | 23.8 | 40 | 4.6 | 0.9 |
42 | 4.2 | −1.0 | 1.7 | >210 | <0.9 | – |
51 | 0.5 | −1.5 | 2.8 | 37 | 1.2 | 0.5 |
55 | 6.2 | −7.8 | 28.0 | 45 | 4.6 | 0.6 |
57 | 2.9 | 1.45 | 1 | >230 | <0.8 | – |
60 | 3.3 | −0.1 | 5.8 | 90 | 1.7 | 0.8 |
72 | 2.3 | −0.0 | 10.0 | 20 | 2.8 | 0.8 |
73 | 2.2 | 0.4 | 7.9 | 62 | 2.3 | 0.9 |
75 | 1.6 | −0.3 | 6.5 | 50 | 2.2 | 0.8 |
76 | 0.6 | −8.9 | 11.0 | 15 | 5.0 | 0.4 |
77 | 1.9 | 0.7 | 8.5 | 45 | 2.6 | 0.8 |
92 | 2.2 | −1.1 | 8.3 | 55 | 2.4 | 0.7 |
112 | 3.4 | 1.7 | 8.0 | 70 | 2.2 | 0.9 |
113 | 3.2 | 1.2 | 9.5 | 60 | 2.4 | 0.9 |
115 | 4.6 | 1.2 | 1 | >300 | <1.1 | – |
118 | <0.7 | −2.0 | 3.3 | <35 | 1.4 | <0.5 |
142 | – | – | 20.3 | – | – | – |
144 | 0.8 | 0.5 | 8.0 | 20 | 3.6 | 0.8 |
146 | 5.8 | –0.7 | 9.9 | 90 | 2.2 | 0.8 |
147 | 2.7 | 1.7 | 2.2 | 145 | 1 | 0.9 |
Selected residues (selection value underlined) with either Rex > 6.4 s−1 or ΔRex > 2.5 s−1 or ΔΔRex < −1.4 s−1. The fast exchange equations were used to derive from the correlation of ΔRex and Rex as explained in the Theory section. The error in is estimated to be ∼30 μs and ∼1 ppm in based on 1 s−1 errors in ΔRex and Rex; is calculated from with pA = pB = 0.5 and represents the minimum value of Δex, because pApB reaches a maximum at pA = 0.5. The ΔRex showed a systematic offset of ∼−2 s−1. The values given and used in the derivation of and have been corrected for this offset. Residues 36, 42, 57, and 115 have small Rex; the is a lower limit and the an upper limit based on a maximum value of Rex of 1 s−1.
Residues 14, 19, 51, 55, 76, 92, 118, and 146 show a relatively high decrease in ΔRex (ΔΔRex < −0.5, italic) upon decrease in temperature, leading to relatively large fractional decrease in the exchange rate kex (f = kex,300/kex,308, italic; see Theory section for the equations used). Based on the error in ΔΔRex (1.4 s−1) and ΔRex (0.7 s−1), the error in f is estimated to be 0.15. For the four residues 36, 42, 57, and 115, no reliable estimate of f can be made, because of the uncertainty in the value of kex. For residues 14 and 118 the upper limit of f and is given as estimated from the lower limit of ΔRex.