Electron thermalization distance distributions and thermal electron mobilities in dense liquid isobutane
Free ion yields [Formula: see text], were measured at electric field strengths E up to 6.7 MV m−1 in liquid isobutane at 556 ≤ d/kg m−3 ≤ 739 (294.4–114.6 K). The yields decreased with decreasing temperature and increasing density up to 677 kg m−3; further increases in density led to little change in [Formula: see text]. The thermalization distance distribution F(y) was estimated by fitting the field dependence of [Formula: see text] using the extended On sager model. At lower densities F(y) = YGP (three-dimensional Gaussian body with power tail) provided an adequate fit to the results, while at higher densities F(y) = YE (one-dimensional exponential distribution) was better. Thus the electron-scattering properties of liquid isobutane change somewhat with density. The thermalizing ability of liquid isobutane increased with increasing density up to ~660 kg m−3, then decreased at densities > 690 kg m−3. By comparison, the Arrhenius temperature coefficient of mobility of thermal electrons changed in the same density region: Eμ ≈ 7 kJ mol−1 at d < 660 kg m−3, and ≈ 16 kJ mol−1 at d > 690 kg m−3. Keywords: isobutane, electron thermalization distance, free ion yield, liquid, electron mobility, radiolysis.