Table I.
Residue | 0°C | 10°C | 20°C |
---|---|---|---|
48 | 1456 ± 370 | ||
55 | 1159 ± 150 | 1176 ± 200 | 1584 ± 340 |
56 | 1070 ± 160 | 1239 ± 400 | |
57 | 1511 ± 360 | ||
61 | 1354 ± 350 | ||
62 | 1534 ± 180 | 1542 ± 300 | |
63 | 1456 ± 340 | 2417 ± 460 | 1957 ± 310 |
65 | 811 ± 200 | 2129 ± 400 | 5114 ± 1000 |
66 | 559 ± 180 | 2849 ± 230 | 5452 ± 1000 |
67 | 189 ± 260 | 3628 ± 450 | 4193 ± 1000 |
68 | 934 ± 350 | ||
69 | 725 ± 400 | ||
72 | 1200 ± 300 | 5794 ± 2800 | |
73 | |||
74 | 3666 ± 350 | ||
75 | 748 ± 170 | ||
76 | 956 ± 100 | 2578 ± 120 | 5326 ± 1000 |
77 | 562 ± 150 | 2558 ± 160 | 5490 ± 1000 |
82 | 1070 ± 120 | O.L. | 2240 ± 250 |
83 | 633 ± 100 | 2610 ± 280 | 5201 ± 1000 |
84 | 1200 ± 400 | ||
91 | kA = 0.54 ± 0.07a | kA = 0.85 ± 0.18a | 960 ± 200 |
92 | kA = 1.64 ± 0.15a | kA = 2.15 ± 0.11a | 1072 ± 200 |
96 | kA = 1.01 ± 0.11a | kA = 0.9 ± 0.15a | 1351 ± 250 |
98 | 1159 ± 200 | 2130 ± 400 | 1031 ± 300 |
99 | 460 ± 100 | 400 ± 100 | 1320 ± 100 |
102 | 1511 ± 150 | 1524 ± 400 | 1750 ± 100 |
109 | 1269 ± 150 | 3041 ± 1000 | 1700 ± 600 |
110 | 684 ± 120 | 3142 ± 500 | 5800 ± 1000 |
111 | 1008 ± 100 | 2737 ± 200 | 4864 ± 1500 |
113 | 950 ± 100 | 1400 ± 200 | 1400 ± 100 |
119 | kA = 1.84 ± 0.14a | kA = 1.41 ± 0.08a | 1588 ± 200 |
120 | kA = 1.85 ± 0.12a | kA = 2.74 ± 0.13a | 1366 ± 100 |
122 | kA = 1.84 ± 0.11a | kA = 2.33 ± 0.13a | 1408 ± 200 |
126 | 1453 ± 160 | ||
128 | 1038 ± 240 |
Only the forward rate constant, kA, could be extracted due to slow exchange (see text). Both kA and the respective uncertainties were calculated using the “slow exchange equation” described in Materials and Methods.