The ability of various alkanes to be intercalated into the second-stage ces
ium graphitide, CsC24, was investigated using the two-bulb technique. The s
tructural changes occurring during intercalation were studied by real-time
neutron diffraction. At moderate pressure, the intercalation of large molec
ules such as n-butane, n-pentane and n-hexane simultaneously leads to a mix
ture of a second-stage ternary phase and a first-stage binary phase "CsC8".
Under increased pressure a pure first-stage ternary phase is finally forme
d. The intercalation of cyclopentane occurs in two steps: a pure second-sta
ge ternary phase is first observed, whereas CsC8 only appears at about half
filling. For the smallest alkane, CH4, complete ternarization leads to a s
econd-stage ternary phase together with a small amount of an enriched secon
d-stage binary derivative. Owing to the formation of binary domains rich in
alkali metal during the ternarization, the cesium density is smaller in th
e second-stage ternary phase than in the starling binary compound. The in-p
lane cesium concentration of the ternary phase strongly depends on the proj
ected surface area of the alkane molecule. During invasion of the interlame
llar space, large molecules induce a decrease of the average distance betwe
en cesium ions. Electrostatic repulsive energy between cations is minimized
through expulsion of cesium in binary domains. A pleated-layer model with
canted fronts is presented, in order to account both for the various phases
existing within each grain, and for the structural transformations caused
by the intercalation reaction. (C) 1998 Elsevier Science Ltd. All rights re
served.