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. 2010 Jul 12;365(1549):2137–2149. doi: 10.1098/rstb.2010.0045

Table 1.

Summary of the equation parameters for the effect of the temperature (1/kT) on BP and on GB (µgC ml−1 h−1, prior to Ln transformation) in space-for-time measurements and perturbation experiments. Ln (PB) or Ln (GB) = ab (1/kT); (n.s., not significant; c.i., 95% CI; CL, confidence level). References: (1), Vaqué et al. (1994) and references therein, Vaqué et al. (2002, 2001, 2008), Vázquez-Domínguez et al. (2005), Unrein et al. (2007), Boras et al. (2009); (2), J. M. Gasol (1998 unpublished data); (3), Pedrós-Alió et al. (2002); (4), Vaqué et al. (2009).

a b [c.i.] critical CL of the [c.i.] p-value n r2 references
space-for-time measurements BP 17.413 0.667 [0.569–0.765] <70% F1,189 = 50.1, p < 0.0001 190 0.21 (1)
GB 9.770 0.456 [0.329–0.584]a 95%a F1,127 = 50.0, p < 0.0001 128 0.28 (1)
perturbation experiments BP 7.204 0.385 [0.116–0.653] 95% F1,11 = 10.2, p < 0.001 12 0.50 (2)
26.034 0.823 [0.594–1.053] <70% F1,5 = 18.2, p < 0.01 6 0.82 (2)
1.762 0.256 n.s. 7 (2)
7.904 0.387 [0.060–0.714] 99% F1,5 = 29.6, p < 0.001 6 0.88 (2)
10.149 0.419 n.s. 6 (2)
1.683 0.213 n.s. 8 (2)
22.095 0.766 [0.595–0.936] <70% F1,5 = 28.5, p < 0.001 6 0.88 (3)
43.281 1.274 [0.175–2.724]a 95%a F1,4 = 7.8, p < 0.05 5 0.72 (3)
0.056 0.241 n.s. 6 (3)
22.474 0.799 [0.575–1.023] <70% F1,4 = 19.9, p < 0.01 5 0.87 (3)
−10.969 0.008 n.s. 5 (3)
9.804 0.483 [0.289–0.676] <70% F1,5 = 8.8, p < 0.01 6 0.69 (3)
6.681 0.411 n.s. 6 (3)
average of significant 19.828 0.702
GB −7.344 0.040 n.s. 5 (4)
19.803 0.672 [0.343–1.000] <70% F1,4 = 6.5, p < 0.05 5 0.68 (4)
28.403 0.898 [0.600–1.196] <70% F1,4 = 14.2, p < 0.01 5 0.82 (4)
21.635 0.766 n.s. 5 (4)
−4.555 0.107 n.s. 5 (4)
29.258 0.925 n.s. 5 (4)
20.813 0.728 [0.646–0.811] <70% F1,3 = 148.7, p < 0.001 4 0.99 (4)
7.444 0.424 n.s. 5 (4)
average of significant 23.006 0.766

aTheoretical prediction slope values (0.65 for BP and 0.75 for GB) do not lie on the [c.i.] of the slopes for the field observations.