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. 2013 Aug 22;288(41):29281–29293. doi: 10.1074/jbc.M113.500975

TABLE 3.

Biophysical parameters of CaV3.2 wild-type and double mutant channels were estimated from recordings obtained with the cut-open oocyte technique in the presence of 10 mm Ba2+

Double mutants are shown with the IIS4-S5 mutant always to the left of the pair. Most double mutants were made between IIS4-S5 and IIS6. Double mutants with Asn-1548 in IIIS6 and Asn-1853 in IVS6 are shown below and are separated by a line. Activation properties (E0.5,act and z) were estimated from the mean I-V relationships and fitted to a Boltzmann equation where z is the slope factor. Activation and inactivation energies were calculated as follows: ΔGact = z · F · E0.5,act; ΔΔGact = ΔGact,mut − ΔGact,wt; ΔGinact = z · F · E0.5,inact; and ΔΔGinact = ΔGinact,mut − ΔGinact,wt. The voltage dependence of inactivation was determined from the peak currents after 2-s depolarizing pulses from a holding potential of −120 mV. The data are shown with the mean ± S.E. of the individual experiments and the number of experiments appears in parentheses.

V0.5, act ΔGact ΔΔGact Ipeak V0.5, inact ΔGinact τact, −20 mV τinact, −20 mV ΔΔGinter (act) ΔΔGinteract
mV kcal mol1 nA mV kcal mol1 ms kcal mol1
CaV3.2 WT −47 ± 1 (37) −4.3 ± 0.2 NAa −1300 ± 200 −65 ± 1 (10) −8.6 ± 0.5 3.2 ± 0.1 (18) 11.6 ± 0.2 NA NA
V906G/I1013G −54 ± 2 (5) −6.1 ± 0.7b −1.8 ± 0.9 −300 ± 100 −69.1 ± 0.6 (4) −7.9 ± 0.6 4.2 ± 0.3c (5) 48 ± 2b −0.8 ± 1.8 −2.1 ± 2.5
V907G/I1013G −55 ± 1 (6) −4.1 ± 0.2 0.2 ± 0.4 −190 ± 40 −78.2 ± 0.2 (3) −7.8 ± 0.5 2.9 ± 0.3 (6) 40 ± 1b 4.6 ± 1.3 0.3 ± 2.1
L908G/N1008G −50 ± 3 (5) −5.0 ± 0.7 −0.7 ± 0.9 −80 ± 20 −76 ± 1 (4) −6.9 ± 0.3 2.8 ± 0.3 (5) 11 ± 1 −1.3 ± 1.9 −0.5 ± 1.9
L908A/I1013A −52 ± 1 (5) −5.4 ± 0.3 −1.1 ± 0.5 −160 ± 40 −67 ± 1 (5) −5.8 ± 0.6c 3.4 ± 0.3 (5) 72 ± 2b −1.3 ± 1.2 2.4 ± 2.5
L908G/I1013G −48 ± 1 (6) −3.9 ± 0.3 0.4 ± 0.5 −120 ± 20 −72 ± 1 (4) −7.2 ± 0.4 3.7 ± 0.5 (6) 25.0 ± 0.8b 2.1 ± 1.1 0.6 ± 2.5
V909G/I1013G −48 ± 1 (4) −4.9 ± 0.9 −0.6 ± 1.1 −170 ± 40 −65 ± 2 (3) −6.9 ± 0.8 5.0 ± 0.5b (4) 53 ± 3b 0.4 ± 1.8 1.1 ± 2.6
K910G/I1013G −46.7 ± 0.6 (5) −3.9 ± 0.2 0.4 ± 0.4 −150 ± 30 −65 ± 1 (4) −6.2 ± 0.2 3.6 ± 0.2 (5) 47 ± 4b 0.2 ± 0.9 1.1 ± 2.3
T911A/I1013A −46 ± 2 (6) −4.4 ± 0.4 −0.1 ± 0.6 −340 ± 80 −60.5 ± 0.8 (6) −6.9 ± 0.5 6.1 ± 0.5b (6) 71 ± 5b −1.6 ± 1.2 NDd
T911G/I1013G −43.4 ± 0.8 (6) −3.6 ± 0.2 0.7 ± 0.4 −260 ± 30 −66 ± 1 (6) −6.0 ± 0.5c 6.7 ± 0.5b (6) 41 ± 2b 1.8 ± 0.9 2.9 ± 2.6
T911G/L1014G −47 ± 2 (6) −3.8 ± 0.4 0.5 ± 0.6 −200 ± 100 −75 ± 1 (4) −8 ± 1 8 ± 1b (6) 26 ± 1b −0.8 ± 1 1.8 ± 2.8
M912G/I1013G −48.6 ± 0.7 (6) −4.7 ± 0.1 −0.4 ± 0.3 −180 ± 60 −68 ± 1 (6) −7.5 ± 0.4 5.0 ± 0.6b (6) 42 ± 1b 1.1 ± 1.1 2.3 ± 2.8
N914G/E1016G −36.5 ± 0.9 (6) −2.8 ± 0.2b 1.5 ± 0.4 −90 ± 10 −61.0 ± 0.7 (6) −7.0 ± 0.4 3.9 ± 0.2c (6) 15.0 ± 0.3b −0.8 ± 1.2 ND
V915G/L1010G −27 ± 3 (6) −1.6 ± 0.3b 2.7 ± 0.5 −110 ± 30 −58 ± 1 (3) −8.6 ± 0.6 5.1 ± 0.6b (6) 14.9 ± 0.9b −0.3 ± 0.6 ND
V907A/N1548A −43 ± 3 (4) −3.4 ± 0.6 0.9 ± 0.8 −50 ± 10 −90 ± 2 (2) −6 ± 2 3.1 ± 0.2 (4) 12 ± 2 1 ± 1.2 −1.4 ± 3.1
V907G/N1548G −47 ± 1 (10) −3.8 ± 0.2 0.5 ± 0.4 −110 ± 17 −82 ± 2 (6) −5.7 ± 0.6c 2.6 ± 0.1 (10) 15 ± 1b 3.4 ± 1.2 1.6 ± 1.6
L908A/N1548A −39 ± 2 (6) −3.6 ± 0.3 0.7 ± 0.5 −180 ± 30 −74.6 ± 0.9 (6) −7.3 ± 0.2 4.0 ± 0.3c (6) 9.9 ± 0.3c 0.8 ± 1.0 −0.8 ± 1.7
L908G/N1548G −35 ± 1 (11) −3.3 ± 0.4c 1.0 ± 0.6 −220 ± 60 −74 ± 1 (9) −7.2 ± 0.5 3.5 ± 0.2 (11) 16.5 ± 0.4b 1.2 ± 1.1 −0.3 ± 2.0
T911A/N1548A −36 ± 2 (7) −2.9 ± 0.4b 1.4 ± 0.6 −240 ± 70 −73 ± 2 (6) −8.4 ± 0.5 4.0 ± 0.2c (7) 10.0 ± 0.7c 0.2 ± 1.0 ND
T911G/N1548G −37 ± 2 (7) −2.6 ± 0.2b 1.7 ± 0.4 −100 ± 20 −74 ± 2 (4) −7.6 ± 0.4 3.4 ± 0.4 (7) 13 ± 1 1.3 ± 0.8 0.4 ± 1.9
L908G/N1853G −43.4 ± 0.9 (9) −3.8 ± 0.2 0.5 ± 0.4 −180 ± 30 −70 ± 2 (5) −7.9 ± 0.6 3.5 ± 0.2 (9) 17.2 ± 0.4b −1 ± 1 ND

a NA, not applicable.

b p < 0.01 as compared with CaV3.2 WT.

c p < 0.001 as compared with CaV3.2 WT.

d ND, not determined.