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. 2013 Dec;79(23):7249–7255. doi: 10.1128/AEM.02439-13

Table 1.

Models of AIV persistence associated with water incubated with live Daphnia and water without Daphnia through timea

Model Functional form Kb Adjusted R2 Log σ̂2d ΔAICc wi
By treatment
    Modified exponential decay AIV = {aCW × exp[(bCW/(X + cCW)]} + {aDW × exp[bDW/(X + cDW)]} 6 0.76 9.91 0.00c 0.93
    Exponential decay AIV = [aCW + bCW × exp(−cCW × X)] + [aDW + bDW × exp(−cDW × X)] 6 0.75 9.99 5.26 0.07
AIV = [aCW × exp(−bCW × X)] + [aDW × exp(−bDW × X)] 4 0.70 10.17 13.11 0.00
    Linear AIV = (aCW + bCW × X) + (aDW + bDW × X) 4 0.37 10.92 64.08 0.00
Pooled
    Modified exponential decay AIV = a × exp[b/(X + c)] 3 0.42 10.99 66.51 0.00
    Exponential decay AIV = a + b × exp(−c × X) 3 0.42 10.99 66.66 0.00
AIV = a × exp(−b × X) 2 0.26 11.26 82.83 0.00
    Linear AIV = a + b × X 2 0.16 11.38 90.72 0.00
a

Shown are models of AIV persistence associated with water incubated with live Daphnia (DW) and water without Daphnia (CW) through time (X, in minutes). Strength of support for each model is inferred by AICc model weight (wi). We considered linear (2-parameter) relationships, exponential decay functions (2 and 3 parameters), and a modified exponential decay function (3 parameters) fitted to pooled data and data separated by treatment.

b

Number of parameters.

c

AICc = 687.17.

d

Log of the estimated variance.