We have recorded the high resolution (150 MHz) excitation spectra of NO2 molecules cooled in a supersonic jet in two energy ranges : 16 000-19 362 cm(-1) ["yellow" range, see R. Georges, A. Delon, and R. Jest, J. Chem. Phys. 103, 1732 (1995), hereafter referred to as paper I] and 23 326-23 945 cm(-1) ("blue" range). In this paper we are interested mainly in the rovibronic properties of about 1500 rotational levels (N=1, K=0, J=1/2, and J=3/2) observed in these two ranges. Among these levels about 480 are observed via the so-called extra lines, i.e., the lines which are observable because of rovibronic couplings between bright levels (N=1, K=0, B-2(2) vibronic character) and nearby dark levels. These rovibronic couplings result mainly from second order spin-orbit and orbit-rotation interactions which have been evidenced previously by Zeeman effect and anticrossing experiments [A. Delon, P. Dupre, and R. Jest, J. Chem. Phys. 99, 9482 (1993)]. By comparing the average matrix element of rovibronic interactions occuring for N=1, K=0 (J=1/2 and J=3/2), and for N=3, K=0 (J=5/2 and J=7/2) we can exclude a significant contribution from Coriolis interactions. A model of small random matrices constructed by using the properties of the above mentioned rovibronic Hamiltonian (density of states, selection rules, and matrix elements) allowed us to reproduce the observed statistical properties of the rovibronic states : average number of extra lines per vibronic band, distribution of intensities, Fourier transform analysis, next-neighbor spacing distribution, hierarchical tree analysis, and intensity and energy correlations between J=1/2 and J=3/2 lines. All these properties confirm that the second-order spin-orbit interaction is responsible for most of the observed extra lines for low rotational levels N=1 and N=3, K=0. As a result, the average reduced rovibronic matrix element is 0.6-/+0.1 cm(-1) and 0.72-/+0.1 cm(-1) for the yellow and blue ranges, respectively. The yellow range result is in reasonable agreement with the results obtained previously under magnetic field experiments. We also derive analytical formulas applicable for the weak interaction regime and discuss the relation between the observed distribution of matrix elements and the true distribution.