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. 2014 Jul 7;111(30):11205–11210. doi: 10.1073/pnas.1407327111

Table 1.

The rates of CO2 uptake in whole filaments and O2 exchange in whole filaments and isolated heterocysts of the WT and the flv mutant strains

Strain and inhibitors Filaments Heterocysts
CO2 uptake O2 uptake Gross O2 evolution Net O2 evolution O2 uptake
Dark Light Light-induced Dark Light Light-induced
WT 7.0 ± 0.3 20.3 ± 1.1 69.5 ± 0.8 49.1 ± 0.8 187.5 ± 5.5 118.0 ± 5.9 3.4 ± 0.5 5.6 ± 0.5 2.2 ± 0.7
 + KCN 1.3 ± 0.4** 5.5 ± 0.8 4.2 ± 0.4**
 + KCN, SHAM 0.7 ± 0.3** 7.5 ± 0.5** 6.8 ± 0.2**
 + Antimycin A 1.4 ± 0.6** 5.7 ± 0.7 4.4 ± 0.1**
flv1B 7.5 ± 2.1 21.1 ± 1.6 58.5 ± 0.5** 37.4 ± 2.1** 181.5 ± 5.8 123.0 ± 5.0 4.9 ± 0.8* 6.7 ± 0.5* 1.8 ± 0.3
flv3B 5.2 ± 0.3** 32.4 ± 3.15* 54.3 ± 2.1** 21.8 ± 5.3** 142.8 ± 6.8** 88.5 ± 4.6* 7.4 ± 0.7** 6.5 ± 0.1* Nd
flv1B/3B 5.1 ± 0.4** 30.4 ± 1.4** 55.8 ± 1.7** 25.4 ± 3.1** 145.5 ± 5.6** 89.7 ± 7.2* 6.5 ± 0.6** 6.4 ± 0.1* Nd

Gas exchange rates are presented as micromoles per milligram of Chl a per hour. Filaments were grown in N2-fixing conditions. Light-induced O2 uptake was calculated by subtracting the O2 uptake rate in darkness from the O2 uptake rate in the light. Net O2 evolution was deducted as a residual rate of gross O2 evolution after subtraction of the light O2 uptake rate. Mean ± SD, n = 3, asterisks indicate statistically significant differences with the WT (*P < 0.05; **P < 0.01). Nd, not detected.