Fig. 3

ST increases after a 50 s heating period by 42.25 GHz source (PD = 208 mW/cm²) in comparison with Alekseev’s [32] computational broad beam results. Alekseev BFR = 0.0006 s⁻¹. Computational results from this study given for 0.5,1,2 \(\times\omega\) where \(\omega =0.00055\) s.⁻¹