Table 4.

Fitting linear versus cyclic models to single-channel currents from AChRs activated by low [ACh]

Model kon koff f0 b0 jon joff f1 b1 LL nfp 
 398 ± 39 5,457 ± 513 297 ± 3 8,883 ± 64 – – 299 ± 7 234 ± 3 365,875 
 – – 303 ± 2 8,435 ± 63 470 ± 8 371 ± 6 2,911 ± 350 29 ± 2 366,151 
 10 ± 1 5,086 ± 790 290 ± 12 8,404 ± 348 395 ± 19 272 ± 12 2,032 ± 182 78 ± 4 366,306 
Model kon koff f0 b0 jon joff f1 b1 LL nfp 
 398 ± 39 5,457 ± 513 297 ± 3 8,883 ± 64 – – 299 ± 7 234 ± 3 365,875 
 – – 303 ± 2 8,435 ± 63 470 ± 8 371 ± 6 2,911 ± 350 29 ± 2 366,151 
 10 ± 1 5,086 ± 790 290 ± 12 8,404 ± 348 395 ± 19 272 ± 12 2,032 ± 182 78 ± 4 366,306 

In the full cycle (Fig. 5 B, inset), the agonist (A) could bind to both the C (low affinity) and O (high affinity) conformations. Rate constants (mean ± SD) were from the global cross-concentration fit (n = 64,790 intervals; s−1 or µM−1s−1). kon, low affinity association rate constant; koff, low affinity dissociation rate constant; jon, high affinity association rate constant; joff, high affinity dissociation rate constant; LL, loglikelihood; nfp, number of free parameters. fn and bn are the opening and closing rate constants with n-bound agonists. From the gating rate constants of the cyclic model, E1 = 26 and E0 = 0.035 (E1/E0 = 742).

or Create an Account

Close Modal
Close Modal