“…If we assume 1-D fuel-pusher assembly, without mixing, from mass conservation, continuity of pressure, and temperature at the D-T-glass interface, the fuel compression is given by (Storm et al 1980) M DT and M p are, respectively, the fuel and pusher masses, (pAR) the pusher areal density, p m and pj the fuel densities, the index / corresponds to initial condition and m to the measured value at the burn time, Z p is the average pusher ionization, and a is approximate to 2. It can also be more simply evaluated from the pusher areal density by using a simple model.…”