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On converging shock waves of spherical and polyhedral form

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380 D. W. Schwendeman<br />

(a) Time = 0.2921 Average radius = 0.2378 (b) Time = 0.3021 Average radius = 0.2020<br />

7<br />

7<br />

6<br />

6<br />

Shock Mach number<br />

5<br />

4<br />

Shock Mach number<br />

5<br />

4<br />

3<br />

3<br />

(c) Time = 0.3069 Average radius = 0.1842 (d) Time = 0.3110 Average radius = 0.1679<br />

7<br />

7<br />

6<br />

6<br />

Shock Mach number<br />

5<br />

4<br />

Shock Mach number<br />

5<br />

4<br />

3<br />

3<br />

(e) Time = 0.3147 Average radius = 0.1527 ( f ) Time = 0.3183 Average radius = 0.1376<br />

7<br />

7<br />

6<br />

6<br />

Shock Mach number<br />

5<br />

4<br />

Shock Mach number<br />

5<br />

4<br />

3<br />

3<br />

Figure 9 (a–f ). For caption see facing page.<br />

with the behaviour <strong>of</strong> the local extrema in Mach number along the ray from V . If we<br />

label the Mach number <strong>and</strong> radius at local maxima, say, as M p <strong>and</strong> r p , respectively,<br />

then it is evident from the plots that<br />

M p ∝ r −2/n<br />

p<br />

so that the increase in Mach number for each step <strong>of</strong> the repeating sequence follows

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