Figure 3.
The dependence of the rate of change of blast wave radius with respect to observer time, $\mathrm{ d}R/\mathrm{ d}t$, on Lorentz factor $\Gamma$ and viewing angle $\theta$, for ejecta approaching the observer. The coloured lines show the full equation (11), compared with the on-axis limit from equation (6) shown with a dot-dashed line. The pink and blue shaded regions show approximate initial Lorentz factor ranges for XRBs and GRBs. At $\theta =0^\circ$, the solution agrees with the $2 \Gamma ^2$ asymptote for high $\Gamma$. At small angles to the line of sight, the curves also agree with this curve for intermediate $\Gamma$ before flattening off as the $\cos \theta$ term becomes important.

The dependence of the rate of change of blast wave radius with respect to observer time, |$\mathrm{ d}R/\mathrm{ d}t$|⁠, on Lorentz factor |$\Gamma$| and viewing angle |$\theta$|⁠, for ejecta approaching the observer. The coloured lines show the full equation (11), compared with the on-axis limit from equation (6) shown with a dot-dashed line. The pink and blue shaded regions show approximate initial Lorentz factor ranges for XRBs and GRBs. At |$\theta =0^\circ$|⁠, the solution agrees with the |$2 \Gamma ^2$| asymptote for high |$\Gamma$|⁠. At small angles to the line of sight, the curves also agree with this curve for intermediate |$\Gamma$| before flattening off as the |$\cos \theta$| term becomes important.

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