Table 1.
Density*, μm−2 | Diameter†, nm | a/b Ratio | Area‡, nm2 | Number of helices§ | |
---|---|---|---|---|---|
Opsin | 1444 ± 43 | (a) 4.4 ± 0.4 | 1.3 | 11 ± 2 | 8 ± 1 |
(b) 3.3 ± 0.5 | |||||
Cx50 | 1415 ± 81 | 6.5 ± 0.5 | 1 | 34 ± 4 | 24 ± 3 |
APQ1 | 825 ± 63 | 6.5 ± 0.5 | 1 | 33 ± 4 | 24 ± 3 |
MIP | 3288 ± 136 | 6.6 ± 0.5 | 1 | 34 ± 4 | 24 ± 3 |
SGLT1 | 2070 ± 130 | (a) 5.8 ± 0.6 | 1.2 | 21 ± 3 | 15 ± 2 |
(b) 4.7 ± 0.5 | |||||
CFTR | 678 ± 27 | 6.6 ± 0.4 | 1 | 34 ± 3 | 25 ± 2 |
Total density of P face particles. Density of the endogenous P face particles was 355 ± 21/μm2.
Diameters were corrected for the thickness of the platinum-carbon film by subtracting 2.4 ± 0.4 nm from the mean diameters obtained from the frequency histograms (see Experimental Procedures).
Cross-sectional area was obtained by assuming a circular geometry for Cx50, AQP1 and MIP , and CFTR and an elliptical geometry for opsin and SGLT1.
Predicted number of helices was calculated by using 1.40 ± 0.03 nm2/helix (see Fig. 3B). Values are means ± SEM.