TABLE 4.
VHH | ka | kd | KD | KD (calculated)a |
---|---|---|---|---|
1/ms | 1/s | m | ||
JJX21 | 2.0 × 105 | 7.4 × 10−6 | 3.84 × 10−11 | <7.5 × 10−11 |
JNA6 | 4.58 × 105 | 9.55 × 10−7 | 2.10 × 10−12 | <6.22 × 10−12 |
JNA2 | 1.34 × 106 | 1.69 × 10−5 | 1.26 × 10−11 | NAb |
JNA3 | 3.96 × 105 | 1.26 × 10−5 | 3.20 × 10−11 | NA |
JNA10 | 4.40 × 105 | 1.20 × 10−6 | 2.70 × 10−12 | <6.48 × 10−12 |
JNA11 | 5.77 × 105 | 9.66 × 10−7 | 1.67 × 10−12 | <4.94 × 10−12 |
JNA8 | 3.43 × 105 | 1.47 × 10−6 | 4.27 × 10−12 | <2.77 × 10−12 |
JNA14 | 7.67 × 105 | 7.96 × 10−7 | 1.04 × 10−12 | <3.10 × 10−12 |
a KD calculated was calculated using the kd limit and the ka measured for those VHHs that did not dissociate from ricin within the kd limit. In several instances little to no VHH dissociation was detected over a 6-h time course, suggesting that the dissociation rate constants were slower than 2 × 10−6 s−1 (37). It was therefore not possible to generate a true KD value. Instead, the KD was calculated based on the so-called 5% rule that compensates for the limitations of SPR (38). Actual SPR sensorgrams are provided in supplemental Fig. S2.
bNA, not applicable.