Figure 2.

N306D/E channels present a clear O1O2 phenotype. (A) A representative single-channel recording of N306D in the WT background shows the characteristic O1O2 phenotype, supporting the idea that it is the negative charge introduced at position 306 that accounts for the O1O2 phenotype displayed in N306D and in MTSES-modified N306C/Cysless. Single-channel amplitudes of O1 (0.18 ± 0.01, n = 3) and O2 (0.24 ± 0.01, n = 3) states can be measured in the all-points histogram on the right. (B) Expanded opening bursts show details of each opening events as marked in A. (C) A representative single-channel recording of N306E in the WT background further confirms the role of a negative charge at position 306 in conferring the O1O2 phenotype. The all-points histogram shows distinct single-channel amplitudes of the O1 (0.19 ± 0.01, n = 3) and O2 states (0.27 ± 0.01, n = 3).

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