) and various TEA fraction in the counter cations, φ TEA = 0 − 1, and the spherical FOS micelles therein were connected into threads and further organized into dendritic networks. For φ TEA ≥ 0.5, the FOS threads/networks exhibited the Maxwell-type terminal relaxation reflecting their thermal scission. In this range of φ TEA , the terminal relaxation time τ increased with decreasing φ TEA while the steady state compliance J e was insensitive to φ TEA . On a further decrease of φ TEA below 0.3, τ became insensitive to φ TEA and J e gradually increased possibly because the motion of the threads in the unscissored form became faster than the thermal scission to govern the terminal relaxation.These rheological features were discussed in relation to the effects of TEA and TMA on the thermal scission of the FOS threads/networks: Since the charge was the same for TMA and TEA but the bare radius was smaller for TMA, the TMA cations should be preferentially bound on the FOS thread. The thermal scission of the FOS thread, occurring through an exchange of the bound and non-bound TEA cations (Watanabe et al., Rheol Acta, 28, 110 (2000)), appeared to be strongly suppressed by the preferentially bound TMA cations that effectively blocked the exchanging sites. Indeed, in a range of φ TEA ≥ 0.5 where the thermal scission governed the relaxation of the system, the rheological data were well described by a simple model considering this blocking effect.