Figure 9
Evolution of the apparent velocity as a function of the observation angle for a constant intensity profile (thick solid line) or an angular-dependent (Gaussian in the present case) intensity profile (thick dashed line). We use a Gaussian profile (D3) for the Lorenz factor. For comparison, the case of a conical profile (D1) and constant intensity is plotted in the thin line. The jet opening angle θj = 15° and γ0 = 5.

Evolution of the apparent velocity as a function of the observation angle for a constant intensity profile (thick solid line) or an angular-dependent (Gaussian in the present case) intensity profile (thick dashed line). We use a Gaussian profile (D3) for the Lorenz factor. For comparison, the case of a conical profile (D1) and constant intensity is plotted in the thin line. The jet opening angle θj = 15° and γ0 = 5.

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