Skip to main content

Table 1 Film thickness h (standard deviation \(\delta h\)) calculated by fitting \(R_{\mathrm{a}}(t)\) (\(\phi = 0.4\) suspension) to inviscid and viscous models. HF : high-frequency wave; H : Helmholtz resonance; AF : air flow; N: number of runs used; r : correlation coefficient (standard deviation \(\delta r\)); \(\Delta t\) : Time span used for the fit. In terms of N, the inviscid model gives a higher r for 69 % of the runs

From: Excitation of airwaves by bubble bursting in suspensions : regime transitions and implications for basaltic volcanic eruptions

Case

N

Inviscid \(h (\delta h) (\mu\)m)

Viscous \(h (\delta h)(\mu\)m)

3 (HF)

35

5 (4)

26 (21)

5 (H)

16

69 (93)

44 (36)

6a (AF\(+\)H)

4

65 (60)

36 (25)

6b (AF)

3

4 (4)

22 (12)

Total, r (\(\delta r\))

58

0.984 (0.002)

0.969 (0.003)

Total, \(\Delta t\) (ms)

58

\(2.4 \pm 2.4\)

\(1.2 \pm 1.0\)