We study the conductivities of (i) the equilibrium isochoric state (), (ii) the equilibrium isobaric state (), and also the (iii) non-equilibrium ultrafast matter (UFM) state ($\sigma_{\rm uf}T_iT_e$. Aluminum, lithium and carbon are considered, being increasingly complex warm dense matter (WDM) systems, with carbon having transient covalent bonds. First-principles calculations, i.e., neutral-pseudoatom (NPA) calculations and density-functional theory (DFT) with molecular-dynamics (MD) simulations, are compared where possible with experimental data to characterize $\sigma_{\rm ic}, \sigma_{\rm ib}\sigma_{\rm uf}\sigma_{\rm ib}$ are closest to the available experimental data when compared to results from DFT+MD, where simulations of about 64-125 atoms are typically used. The published conductivities for Li are reviewed and the value at a temperature of 4.5 eV is examined using supporting X-ray Thomson scattering calculations. A physical picture of the variations of with temperature and density applicable to these materials is given. The insensitivity of to below 10 eV for carbon, compared to Al and Li, is clarified.

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