We present a series of numerical and analytical computations on heat conduc
tion for a strongly chaotic system-the Lorentz gas. Heat conduction is char
acterized by nontrivial features: While the heat conductivity is well defin
ed in the thermodynamic limit, a linear gradient appears only for quite sma
ll temperature differences. The key dynamical feature inducing such a behav
ior is recognized as deterministic diffusion (along transport direction) wh
ich is usually associated to full hyperbolicity. [S0031-9007(99)08614-7].