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For totally charged PSSNa, at cp, 0.34 M. passing from c s, 0 to cs, 0.68 M corresponds to a variation of I, 1/2 (fcp, 2cs) by a factor 5. Since for these solutions lp ∼ I1/3, this gives a factor 51/3 ∼ 1.7 for lp. This is of the order of magnitude of the increase in height of the very short flat part (corresponding to the usual q 2S1(q) plateau of a Gaussian chain) observed in Figure 8; this increase is more visible under the form an intensity increase in the straight region of log-log plot of Figure 9. Thus, it agrees with a plateau height varying as 1/lp
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