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# A bedform phase diagram for dense granular currents

## Abstract

Pyroclastic density currents (PDCs) are a life-threatening volcanic hazard. Our understanding and hazard assessments of these flows rely on interpretations of their deposits. The occurrence of stratified layers, cross-stratification, and bedforms in these deposits has been assumed as indicative of dilute, turbulent, supercritical flows causing traction-dominated deposition. Here we show, through analogue experiments, that a variety of bedforms can be produced by denser, aerated, granular currents, including backset bedforms that are formed in waning flows by an upstream-propagating granular bore. We are able to, for the first time, define phase fields for the formation of bedforms in PDC deposits. We examine how our findings impact the understanding of bedform features in outcrop, using the example of the Pozzolane Rosse ignimbrite of the Colli Albani volcano, Italy, and thus highlight that interpretations of the formative mechanisms of these features observed in the field must be reconsidered.

## Introduction

Particulate density currents are the largest mass transporters of sediment on the Earth’s surface. Deep-sea turbidity currents deposit the largest sediment accumulations on the Earth1, density currents emplace ejecta blankets around bolide impact craters2 and pyroclastic density currents (PDCs) can transport thousands of cubic kilometres of volcanic material during a single event3. These flows also pose a major geohazard, with deep-sea turbidity currents threatening seafloor infrastructure and PDCs being responsible for over 90,000 deaths since 1600 CE4,5. Understanding the behaviour of these particle-laden, fast-moving currents is fundamental to decreasing the risks they pose to society.

The dynamics and depositional processes of PDCs are difficult to analyse due to their destructiveness, and the concealment of the internal dynamics by an accompanying ash cloud. Understanding of PDC behaviour, therefore, is primarily based on interpretation of the geological record preserved in sedimentary deposits6,7,8,9,10, complemented by analogue and numerical modelling11,12,13,14.

The presence and morphology of sedimentary structures, such as bedforms, in a deposit can be interpreted to tell us about the internal behaviour of the density current that formed them15,16,17,18,19. Various types of cross-stratified bedforms occur in PDC strata and are assumed to be formed by dilute, high-velocity (surge) PDCs8,18,20,21,22,23,24, where tractional processes dominate in the flow-boundary zone due to the predominance of fluid turbulence as a particle support mechanism9,11,25,26. Denser, granular fluid-based PDCs are usually thought to be responsible for the creation of massive deposits, lacking in sedimentary structures6,9,27,28.

Bedform-related sedimentary structures in PDC deposits include backset features (i.e., upstream-dipping beds) formed by stoss-side aggradation, similar to chute-and-pool structures and antidunes found in fluvial systems (Fig. 1a, f and Fig. 1b, d), which are generally thought to be formed under supercritical flow conditions16,19,29,30. Early work on such structures in PDC deposits interpreted them similarly as the result of supercritical flows31,32,33,34. These backset bedforms have commonly been referred to as regressive, for example by Allen18, who interpreted them as sandwaves deposited by wet and cool pyroclastic surges. Since then regressive has been commonly used to describe stoss-aggrading features in PDC deposits, although linking this to flow conditions, rather than temperature and moisture content21,35,36,37. However, there have been attempts to introduce new terminology which does not hold the genetic connotations of antidune, chute-and-pool or sandwave. For example, Brown and Branney38 use the term regressive bedform for a giant set of sigmoidal, upstream-dipping lenses. Douillet et al.22 introduce the term regressive climbing dunes for bedforms which show upstream crest migration (Fig. 1c). Brand et al.39 adopt similar terminology, using regressive dune bedforms (Fig. 1e). In this paper, we avoid using such terms, in the interests of being purely descriptive, opting instead to use backset bedforms to refer to stoss-aggrading features, which have both asymmetrical (much steeper stoss sides; Fig. 1g) or roughly symmetrical lee and stoss slopes (Fig. 1h).

Analogue modelling of dense PDCs has advanced considerably over recent years, including work focusing on the influence of pore pressure13,40,41,42,43,44,45. High gas pore pressure created by various mechanisms within PDCs6,9,46,47,48 has been shown to be responsible for their unusually high mobility49,50,51, but only recently has physical modelling reflected the sustained and variable nature of such pore pressures with distance from source44,52.

Here, we examine the conditions which promote the growth of bedforms in aerated dense granular flows, as analogues for PDCs and their deposits. This work describes laboratory experiments, in which we use partially fluidised (aerated) fine-grained particles in a 3-m long flume (see ‘Methods'). These experiments are able to simulate many behaviours of PDCs13,43,44,52. As the deposit aggrades from the quasi-steady currents, the growth of bedforms is recorded using a high-speed camera. We study how backset bedform features form within the dense granular currents. Deposition is triggered in the experiments as the sustained aerated flow passes into a section of the flume with a reduced or absent basal gas flux, resulting in rapid deaeration and a consequent increase in frictional forces between particles. This is not intended to represent a specific natural process but rather simulate the rapid deaeration hypothesised to occur in natural PDCs as a result of various processes, such as loss of fines, temperature drops, thinning and/or the entrainment of coarser material45,48,53. The initial deaeration would be accelerated by the slowing current (decreasing shear rates), and increasing inter-particle frictional forces. We are able to, for the first time, define phase fields for the formation of types of bedforms in PDC deposits using current velocity, current thickness, Froude number and Friction number. We examine how our interpretations impact on the understanding of similar features in outcrop, using the example of the Pozzolane Rosse ignimbrite of the Colli Albani volcano, Italy.

## Results

### Bedform morphology

A range of bedforms were observed growing under a variety of flow conditions within the suite of experimental runs (see ‘Methods'). We categorise these bedforms into three types (Fig. 2): planar/very shallow backset (<2°) bedsets, backset bedforms with shallow stoss sides less than the dynamic angle of repose (<θDyn), and backset bedforms with steep (>θDyn) stoss sides. Planar bedsets, shallow backset bedforms and steep backset bedforms are present in each deposit except one (Fig. 2e), which does not show steep backset bedforms. Both steep and shallow backset bedforms comprise a bedset of multiple (3–4) stoss-side lamina dipping at varying angles, converging into a single corresponding lee-side lamina (Table 1). No progressive (prograding) bedforms were observed in any of the experimental runs because our experiments are run with waning, not waxing currents.

### Bedform deposition

The experiments began when the particles were released into the flume via trapdoor and impinged on the basal porous mesh, forming an aerated current. The leading edges of the currents were travelling at ~2 ms−1 as they passed into the lesser/unaerated second chamber of the flume (Fig. 3a; see Supplementary Movie 1). The sustained currents rapidly deaerate as they pass over the second chamber of the flume, promoting deposition. Small spontaneously generated variations in the current mass flux result in minor unsteadiness in the flow over timescales in the order of 0.05 s and flow thickness variations in the order of +/−10%, hence their quasi or nearly steady nature44. The currents initially deposit planar or very shallow backset bedsets after the break in aeration (Fig. 3b), at velocities of ~1–1.5 ms−1. Within 0.4–0.8 s of deposition beginning, stoss-side aggrading shallow backset bedforms are deposited above and upstream of the planar bedsets as the current velocities decrease (Fig. 3c–d). Within 1.1–1.6 s of deposition beginning, with the current velocities below ~0.5 ms−1, the upstream edge of the deposit steepens and collapses, with very steep backset bedsets deposited just prior to this, forming the stoss sides of steep backset bedforms (Fig. 3e–f). Current velocity and thickness data during deposition of the bedforms may be found in Supplementary Table 1.

### Velocity and thickness control on bedform formation

Planar, shallow and steep features fall into well-defined fields on a current velocity vs. current thickness plot, suggesting that current velocity and thickness controls the sedimentary structures in the deposit (Fig. 4a). For a given current thickness, planar bedsets are deposited at higher velocities (above 0.8 ms−1 in these experiments). Shallow backset bedforms are deposited at lower velocities, and steep backset bedforms are deposited at the lowest velocities (between 0.3 and 0.6 ms−1 in these experiments). With increasing current thickness, higher current velocities are required to remain in the shallow bedform and planar bedform stability fields. As a result of thickening within a steady current, bedform-induced deposits of different character can be formed without a requirement for a change in flow velocity. It is important to note that the deposit formed over the smallest aeration drop (0.66 Umf to 0.53 Umf) does not show steep backset bedforms, and only poorly developed shallow backset bedforms, suggesting the magnitude of the aeration drop and consequent velocity changes may also have some control.

### Phase fields

We define phase fields for the three types of bedforms using the Froude number (Fr) and the Friction Number (NF). The Froude number (Fr) represents the ratio of kinetic to potential energy (Eq. (1)).

$$Fr = U/\left( {gH} \right)^{1/2}$$
(1)

Where U = current velocity, g = gravity and H = current thickness. The Friction number (NF) is the ratio of frictional to viscous stresses and is defined as Bagnold number/Savage number54,55. The Savage number (NS, Eq. (2)) is the ratio of collisional stress to frictional stress55,56, and the Bagnold number (NB, Eq. (3)) is the ratio of collisional stress to viscous fluid stress55,57.

$$N_S = \frac{{\left( {\frac{U}{H}} \right)^2\delta ^2\rho _s}}{{\left( {\rho _s - \rho _f} \right)gH\tan \theta }}$$
(2)
$$N_B = \frac{{\left( {\frac{U}{H}} \right)\delta ^2\rho _{\mathrm{s}}\varphi }}{{\left( {1 - \varphi } \right)\mu }}$$
(3)

where ρs = particle density, ρf = fluid density, δ = particle diameter, θ = internal friction angle, φ = solid volume fraction and μ = fluid viscosity.

NS in these experiments range from 0.00003 to 0.03, and NB from 15 to 269. In natural PDCs, NS has been estimated to range from 10−8 to 10−9 13, which similar to our experiments is in the frictional regime56 despite the difference of several orders of magnitude. Our NB values overlap with those estimated for natural PDCs (100–102)13.

Froude numbers were calculated for each tracked sediment package during its deposition. Different types of bedforms are formed under different ranges of Fr, with greater overlap between the planar bedset and shallow backset bedform fields than between the shallow and steep backset bedform fields (Fig. 4b–c). As anticipated, there is a good correlation (R = 0.843) between Fr and velocity (Fig. 4c), but with a noticeably greater data spread at higher (>0.8 ms−1) velocities, whereas H exerts much less of a control on Fr (Fig. 4b).

Planar bedsets are mostly deposited at high Fr and low NF, shallow backset bedforms at moderate Fr and NF and steep backset bedforms at low Fr and high NF (Fig. 4d). The planar-shallow-steep sequence of bedform formation can therefore be seen as recording the transition of a fast, supercritical current dominated by viscous stresses to a slower current increasingly dominated by frictional stresses.

### Similar bedforms in the field

The Pozzolane Rosse (PR) ignimbrite covers an area of more than 1600 km2 around the Colli Albani volcano, Italy58, and has been dated (40Ar/39Ar) at 456 ± 3 ka59. It surmounts topography of 250 m to reach altitudes of 440 m60. The ignimbrite is generally massive, matrix-supported and poorly sorted, with a noticeable paucity in fine ash. Emplacement temperatures have been estimated to be between 630 °C and 710 °C61.

Six samples were taken for this study from three localities (within 18–24 km of the vent; Fig. 5a) and two facies (massive, and undulated bedding as described by Giordano and Doronzo62). Grains are dominantly poorly vesicular scoria with compositions plotting in the tephrite/basanite field63. The grain-size distribution of all samples is dominated by lapilli-sized grains and poor in the <63-µm fraction (Fig. 5b; Supplementary Table 2), which is consistent with samples from other studies (Fig. 5c), plotting in the fines-depleted flow field of Walker25. Therefore, we consider the parent PDC of the PR ignimbrite to be a good natural example of an analogue dense, granular current.

Rotating drum tests on the six samples taken from the PR (excluding grains >0.0056 m) gave static minimum (θSmin), maximum (θSmax) and dynamic (θDyn) angles of repose of 35.3°, 51.7° and 45.2°, respectively (Supplementary Fig. 1). Although these values are considerably higher than those obtained for the particles used in the experiments (Supplementary Fig. 2) (likely due to the variable grain size and angularity of the ignimbrite grains), the scaling remains reasonable due to the larger particle sizes in the natural materials (see Eq. (2)).

Backset bedforms are found in the undulated bedding facies in the NE sector of the PR ignimbrite, where the depositing current left the radial plain and ran up into the Apennine mountains62. The undulated facies transitions laterally into the massive facies of the PR on scales of hundreds of metres, and both facies have the same grain size and compositional characteristics (Fig. 5b–c), thus we interpret them to be from the same parent PDC. The bedforms in the PR share similarities with our experimental deposits (c.f. Figs. 6a and  2a–c, Figs. 6c and  2d); and measured stoss angles for both natural and experimental bedforms span the same range (Fig. 6b). The stoss layers seen in the PR backset bedforms are never overturned upstream like some of the experimental deposits. Preservation of overturned beds in natural deposits may be difficult—upstream avalanching of material from this unstable bedform may be reincorporated into a sustained current, or they may be cryptic and not easily visible in natural material. Shallow stoss-sided bedforms are found in this facies (Fig. 6d), although they tend to have greater lee (due to the greater repose angles of the material) and stoss angles than experimental examples, where both are <10° (Fig. 6b).

## Discussion

Our experimental deposits consist of planar bedsets and shallow and steep backset bedforms. The existing widespread interpretation of backset features in PDC deposits is that they are a product of upper flow regime/Froude supercritical flow within dilute PDCs31,32,33,34,35,64, or that relatively steep backset bedforms are specifically a record of the formation and propagation of Froude jumps, where flow transforms from Froude supercritical (>1) to Froude subcritical, similar to fluvial chute-and-pool structures20,31,35,37,39,64,65,66 (Fig. 1a/e, f). Our experimental currents show rapidly evolving Froude numbers (Fig. 4). Within the current body, planar beds are deposited at Fr 3–5, shallow backset bedforms at Fr 2–3 and steep backset bedforms at Fr 0.59–2. We show that an apparent Froude jump within the flow forms in the current during deposition of the steep backset bedforms (Fig. 7). As the experimental current is granular, we adopt the term granular jump67,68,69, which shares many characteristics with its hydraulic counterpart. However, the outgoing current only briefly has Fr < 1, due to thickening of the current directly prior to its being blocked, meaning that a granular jump, strictly defined as a flow transitioning from Fr > 1 to Fr < 1, exists here for only 0.1–0.2 s.

As the sediment deposit grows in thickness, a critical point is reached where the incoming flow cannot surpass the positive slope, and the pseudo-jump propagates upstream as a granular bore68, which travels at 0.14 ms−1 between 96 cm and 90 cm along the flume length. Here, we use granular bore to describe the upstream propagation of the depositional front of the granular material, regardless of flow conditions. This process appears to be similar to the stoss-side blocking or granular jamming invoked to explain stoss-aggrading bedforms at Tungurahua22,70, where the granular current is simply blocked by topography with no particular fluid conditions necessary.

An interesting feature seen in the granular jump of Boudet et al.67 and our own currents is the steepening of stoss faces well beyond the repose angle at the front of the granular bore, and its collapse by avalanching (Fig. 7d). This is likely caused by rapid deposition from the incoming flow countering the effects of gravity sliding, and allowing the bedforms to steepen well beyond repose angle. Again, a similar phenomenon of very high sedimentation rates is used to explain near-vertical bedding at Tungurahua70. The particles deposited by the current as the deposit front steepens form our steep backset bedforms, with stoss angles up to 90°. This may explain why the smallest aeration drop in our experiments (0.66 Umf to 0.53 Umf) did not form steep backset bedforms—the drop was too small to promote the levels of deaeration and deceleration necessary for such rapid sedimentation. Our experimental data therefore call the widespread interpretation of backset bedforms recording Froude jumps within dilute PDCs into question, as we show that similar features can form in dense granular flows in relation to an extremely transient Froude jump, and more clearly related to stoss-side blocking.

Calculated NS and NB numbers indicate that planar bedsets are deposited under conditions closer to a collision-dominated flow regime (NS > 0.1 and NB > 45071) than the backset bedforms (Supplementary Table 1). The planar bedset deposition occurs beyond the transition to the unfluidised section of flume, and therefore they are deposited by a current which is experiencing more collisions between particles due to the loss of gas pore pressure. The backset bedforms are deposited closer to this transition point, where the current has a higher gas pore pressure and grain collisions are not as prevalent. A ratio of NB to NS (NF) shows that frictional stresses are considerably higher than viscous shear stresses in the area of the currents depositing steep backset bedforms (Fig. 4d). As the current is waning at this point and relatively thick, this could result in sustained contacts between particles despite relatively high gas pore pressures.

The PR ignimbrite is generally massive and fines poor, which suggests that the flow-boundary zone conditions of the parent PDC were highly concentrated, likely close to the fluid escape-dominated and granular flow-dominated end-members of Branney and Kokelaar9. In addition, the dense nature of the clasts, lack of fines and the lack of widespread stratification all suggest that the ignimbrite is the deposit of a dense, granular PDC. The presence of backset bedforms within the deposit, which are typically indicative of dilute, turbulent flow (pyroclastic surges), is therefore paradoxical. Rather, the backset bedforms must have been produced by some other process than turbulence within a dilute current.

The similarities between the structures in the PR ignimbrite and our experimental deposits formed by a dense granular current suggest that the depositional processes involved in both cases could be related. We interpret the undulated bedding facies—which includes the backset bedforms—to have been deposited by the same PDC as the rest of the PR ignimbrite. This is due to the traceable lateral transition between facies, the similarity between the grain-size curves over a range of localities, and because the tephra is compositionally identical in the two lithofacies. Instead, the change in facies could be due to the onset of rapid deposition and stoss-side blocking related to the run-up of the PDC into the Apennine mountains (Fig. 5a). Giordano and Doronzo62 interpret the undulated bedding to the east of the volcano as the result of rapid sedimentation and a reduction in the lateral mass discharge rate caused by a palaeovalley perpendicular to flow. Our experimental steep stoss-sided bedforms are created in a waning flow regime after the cessation of basal gas injection and the resulting decrease in pore pressure results in rapid sedimentation, so these interpretations are consistent.

We propose a depositional model whereby shallow backset bedforms are deposited by supercritical flow, forming a topographic irregularity which slows the incoming current (Fig. 8a–b), causing stoss-side blocking, forming a granular bore and promoting rapid deposition (Fig. 8c). Continued deposition steepens the front of the bore until it collapses upstream through avalanching (Fig. 8d–e). Our work provides direct evidence that bedforms can be created by dense granular PDCs, and supports the stoss-side blocking process first suggested by Douillet22,70 based on field deposits.

The upstream propagation of a granular bore, which is caused by the blocking of the current by the aggrading deposit, is a process which in nature could be exacerbated or triggered by pre-existing topography69. The waning nature of the incoming flow at this point, and its relatively low Froude number, suggests that while most of these steep backset bedforms are technically recording the transition from supercritical to subcritical flow, both the shallow backset bedforms and planar beds are formed under increasingly supercritical conditions. It follows that shallow backset bedforms and planar bedsets may then be better indicators of supercritical flow conditions when interpreting dense PDC deposits. The proposed phase diagrams presented here are a major step towards quantitative links between PDC processes and their deposits.

Bedforms can be the product of a dense granular flow and can form without any interference (e.g., tractional shear) from an overlying dilute turbulent layer. As the presence of bedforms (e.g., cross-stratification and backsets) has been commonly used as diagnostic evidence for dilute, turbulent currents, our findings have important implications for field interpretation—as different types of PDCs can react differently to topography the correct classification is necessary for hazard assessment. Other sedimentary characteristics such as field relations, grain size and sorting must be used in order to distinguish between the two PDC end-members. This challenge to the interpretation of the deposits of particulate granular currents is particularly relevant to other free-surface granular mass flows, including landslides, snow avalanches and debris flows. Our experiments demonstrate that formation of different bedforms may by controlled by current thickness and current velocity which has important implications for hazard mapping, and the potential for further investigation to (a) expand the bedform stability criteria identified here, and (b) define palaeoflow conditions from recorded bedforms.

## Methods

### Flume set-up

We use the experimental flume of Smith et al.52, modified so that release of the particulate density current is controlled by a trapdoor instead of a horizontal lock gate (Fig. 9), such that colour stratification in the starting charge transmits to the flow and deposit. The base of the flume comprises 1-m-long sections that can provide independently controlled gas fluxes through a porous baseplate in each section in order to fluidise any overpassing material. The flume was kept at an angle of 2°, to promote flow away from the impingement surface while maintaining a sub-horizontal surface.

The air-supply plumbing allows a gas flux to be fed through the base of the flume, producing sustained aeration of the current. In such thin (<0.03 m), rapidly degassing laboratory currents, this enables us to simulate the long-lived high gas pore pressures that characterise thicker PDCs44,52. The gas flux supplied through the base in each of the three sections of the channel was controlled to vary the aeration state of the currents, all of which were below minimum fluidisation velocity (Umf), as complete fluidisation would result in non-deposition44.

Various aeration states were used to trigger different flow behaviours. The first chamber (0.66–0.93 Umf) always had higher gas flux than the second chamber (0–0.66 Umf) to trigger deposition in the target area of the flume. The experiments were recorded using a high-speed camera at 200 frames per second. This video recorded a side-wall area of the channel at 1-m runout (across the contact between the first and second gas-supply chambers), allowing for measurement of the flow conditions. From the opening of the trapdoor to the cessation of deposition, each experimental run lasted approximately 4 s.

### Experimental material and deposits

The experiments were performed using particles of spherical soda lime ballotini with grain sizes of 45–90 μm (average D32 = 63.4 μm calculated from six samples across the material batch) similar to the particles used in previous experimental granular currents40,42,44. These ballotini belong to the Group A classification of Geldart72, comprising particles 45–90 μm, which expand homogenously above Umf until bubbles form, and which are non-cohesive. As PDCs contain dominantly Group A particles, this allows dynamic similarity between the natural and experimental currents13. Detailed mechanical properties of the ballotini are presented in Supplementary Table 3, derived from rotating drum73 and shearbox (BS 1377-7:1990) testing. These give cohesion values of 0 kPa, and an internal friction angle of 25.3° (Supplementary Fig. 3). Static minimum (θSmin), maximum (θSmax) and dynamic (θDyn) angles of repose are found to be of 11.7°, 31.9° and 20.9°, respectively (Supplementary Fig. 2).

Due to the monodisperse nature of the materials, any internal structure is easily masked by lack of contrast between packages of sediment74. To this end, the charge for each experiment was built up of layers of dyed beads so that flow packages could be tracked throughout flow and deposition, as used in Rowley et al.44. Reported velocities are calculated by tracking these coloured sediment packages in the body of the current immediately prior to their deposition.

When reporting the length of a bedform, the distance from the onset of the stoss-side lamina to the termination of the lee slope on the depositional surface was measured. Thickness refers to the distance between the lowest point of a lamina in the bedform to the highest point of a lamina in that same bedform (Fig. 1g, h). Bedform lengths and thicknesses are reported, as opposed to wavelengths and amplitudes, as we do not produce repetitive trains of bedforms. This is because of the short nature of the experiments—the current is not sustained for long enough, and doing so would require an unfeasible amount of material under the current set-up.

### Error measurements

Errors (2 s.d.) for various measurements are as follows: current thickness: ±0.0013 m. Current velocity: ±0.055 ms−1. Fr: ±0.17. NF: ±67,000.

## Data availability

Data supporting the graphs in Fig. 4 are derived from raw video files, and are available in Supplementary Table 1. One experimental run is available as Supplementary Movie 1. Four other videos are available upon reasonable request.

## References

1. 1.

Bouma, A. H, Normark, W. R. & Barnes, N. E. Submarine Fans and Related Turbidite Systems (Springer, New York, NY, 1985).

2. 2.

Siegert, S., Branney, M. J. & Hecht, L. Density current origin of a melt-bearing impact ejecta blanket. Geology 45, 855–858 (2017).

3. 3.

Self, S. The effects and consequences of very large explosive volcanic eruptions. Philos. T. R. Soc. A 364, 2073–2097 (2006).

4. 4.

Auker, M. R., Sparks, R. S. J., Siebert, L., Crossweller, H. S. & Ewert, J. A statistical analysis of the global historical volcanic fatalities record. J. Appl. Volcanol. 2, https://doi.org/10.1186/2191-5040-2-2 (2013).

5. 5.

Tanguy, J.-C., Ribière, C. H., Scarth, A. & Tjetjep, W. Victims from volcanic eruptions: a revised database. Bull. Volcanol. 60, 137–144 (1998).

6. 6.

Sparks, R. S. J. Grain size variations in ignimbrites and implications for the transport of pyroclastic flows. Sedimentology 23, 147–188 (1976).

7. 7.

Wilson, C. J. N. The Taupo eruption, New Zealand: II. The Taupo Ignimbrite. Philos. T. R. Soc. A 314, 229–310 (1985).

8. 8.

Cas, R. A. F. & Wright, J. V. Volcanic Successions: Modern and Ancient (Allen and Unwin, London, 1987).

9. 9.

Branney, M. J. & Kokelaar, P. Pyroclastic density currents and the sedimentation of ignimbrites. Geol. Soc. Lond. Memoir. 27, 1–143 (2002).

10. 10.

Pollock, N. M., Brand, B. D., Rowley, P. J., Sarocchi, D. & Sulpizio, R. Inferring pyroclastic density current flow conditions using syn-depositional sedimentary structures. Bull. Volcanol. 81, 46 (2019).

11. 11.

Valentine, G. A. Stratified flow in pyroclastic surges. Bull. Volcanol. 49, 616–630 (1987).

12. 12.

Dobran, F., Neri, A. & Macedonio, G. Numerical simulation of collapsing volcanic columns. J. Geophys. Res. 98, 4231–4259 (1993).

13. 13.

Roche, O. Depositional processes and gas pore pressure in pyroclastic flows: an experimental perspective. Bull. Volcanol. 74, 1807–1820 (2012).

14. 14.

Dufek, J. The fluid mechanics of pyroclastic density currents. Annu. Rev. Fluid Mech. 48, 459–485 (2016).

15. 15.

Bouma, A. H. Sedimentology of Some Flysch Deposits (Elsevier, Amsterdam, 1962).

16. 16.

Jopling, A. V. & Richardson, E. V. Backset bedding developed in shooting flow in laboratory experiments. J. Sed. Petrol. 36, 821–825 (1966).

17. 17.

Normark, W. R., Hess, G. R., Stow, D. A. V. & Bowen, A. J. Sediment waves on the Monterey Fan levee: a preliminary physical interpretation. Mar. Geol. 37, 1–18 (1980).

18. 18.

Allen, J. Sedimentary Structures: Their Character and Physical Basis, Vol. 2 (Elsevier, Amsterdam, 1982).

19. 19.

Alexander, J., Bridge, J. S., Cheel, R. J. & Leclair, S. F. Bedforms and associated sedimentary structures formed under water flows over aggrading sand beds. Sedimentology 48, 133–152 (2001).

20. 20.

Schmincke, H.-U., Fisher, R. V. & Waters, A. C. Antidune and chute and pool structures in the base surge deposits of the Laacher See area, Germany. Sedimentology 20, 553–574 (1973).

21. 21.

Cole, P. Migration direction of sand-wave structures in pyroclastic-surge deposits: implications for depositional processes. Geology 19, 1108–1111 (1991).

22. 22.

Douillet, G. A. et al. Dune bedforms produced by dilute pyroclastic density currents from the August 2006 eruption of Tungurahua volcano, Ecuador. Bull. Volcanol. 75, 762 (2013).

23. 23.

Wohletz, K. H. & Sheridan, M. F. A model of pyroclastic surge. Geol. Soc. Am. Sp. Pap. 180, 177–194 (1979).

24. 24.

Walker, G. P. L. Characteristics of dune-bedded pyroclastic surge bedsets. J. Volcanol. Geotherm. Res. 20, 281–296 (1984).

25. 25.

Walker, G. P. L. Ignimbrite types and ignimbrite problems. J. Volcano Geotherm. Res. 17, 65–88 (1983).

26. 26.

Dellino, P., Mele, D., Sulpizio, R., La Volpe, L. & Braia, G. A method for the calculation of the impact parameters of dilute pyroclastic density currents based on deposit particle characteristics. J. Geophys. Res. A-Sol. Ea. 113, https://doi.org/10.1029/2007JB005365 (2008).

27. 27.

Fisher, R. V., Schmincke, H.-U. & Van Bogaard, P. Origin and emplacement of a pyroclastic flow and surge unit at Laacher See, Germany. J. Volcanol. Geotherm. Res. 17, 375–392 (1983).

28. 28.

Cas, R. A. F. et al. The flow dynamics of an extremely large volume pyroclastic flow, the 2.08-Ma Cerro Galán ignimbrite, NW Argentina, and comparison with other flow types. Bull. Volcanol. 73, 1583–1609 (2011).

29. 29.

Middleton, G. V. Antidune cross-bedding in a large flume. J. Sed. Petrol. 35, 922–927 (1965).

30. 30.

Cartigny, M. J. B., Ventra, D., Postma, G. & Van Den Berg, J. H. Morphodynamics and sedimentary structures of bedforms under supercritical-flow conditions: new insights from flume experiments. Sedimentology 21, 712–748 (2014).

31. 31.

Fisher, R. & Waters, A. Bed forms in Base-Surge deposits: Lunar implications. Science 26, 1349–1352 (1969).

32. 32.

Fisher, R. & Waters, A. Base surge bed forms in maar volcanoes. Am. J. Sci. 268, 157–180 (1970).

33. 33.

Waters, A. C. & Fisher, R. V. Base surges and their deposits: Capelinhos and Taal volcanoes. J. Geophys. Res. 76, 5596–5614 (1971).

34. 34.

Crowe, B. & Fisher, R. Sedimentary structures in base-surge deposits with special reference to cross-bedding, ubehebe craters, death valley, California. Bull. Geol. Soc. Am. 84, 663–682 (1973).

35. 35.

Cole, P. & Scarpati, C. A facies interpretation of the eruption and emplacement mechanisms of the upper part of the Neapolitan Yellow Tuff, Campi Flegrei, southern Italy. Bull. Volcanol. 55, 311–326 (1993).

36. 36.

Druitt, T. H. Emplacement of the 18 May 1980 lateral blast deposit ENE of Mount St. Helens, Washington. Bull. Volcanol. 54, 554–572 (1992).

37. 37.

Gençalioğlu-Kuşcu, C., Atilla, C., Cas, R. A. F. & Kuşcu, I. Base surge deposits, eruption history, and depositional processes of a wet phreatomagmatic volcano in Central Anatolia (Cora Maar). J. Volcano Geotherm. Res. 159, 198–209 (2007).

38. 38.

Brown, R. & Branney, M. Bypassing and diachronous deposition from density currents: evidence from a giant regressive bed form in the Poris ignimbrite, Tenerife, Canary Islands. Geology 32, 445–448 (2004).

39. 39.

Brand, B., Bendaña, S., Self, S. & Pollock, N. Topographic controls on pyroclastic density current dynamics: insight from 18 May 1980 deposits at Mount St. Helens, Washington (USA). J. Volcano Geotherm. Res. 321, 1–17 (2016).

40. 40.

Roche, O., Gilbertson, M. A., Phillips, J. C. & Sparks, R. S. J. Experimental study of gas-fluidized granular flows with implications for pyroclastic flow emplacement. J. Geophys. Res. A-Sol. Ea. 109, https://doi.org/10.1029/2003JB002916 (2004).

41. 41.

Girolami, L., Roche, O., Druitt, T. & Corpetti, T. Particle velocity fields and depositional processes in laboratory ash flows, with implications for the sedimentation of dense pyroclastic flows. Bull. Volcanol. 72, 747–759 (2010).

42. 42.

Montserrat, S., Tamburrino, A., Roche, O. & Niño, Y. Pore fluid pressure diffusion in defluidizing granular columns. J. Geophys. Res. F–Earth Surf. 117, https://doi.org/10.1029/2011JF002164 (2012).

43. 43.

Chédeville, C. & Roche, O. Autofluidization of pyroclastic flows propagating on rough substrates as shown by laboratory experiments. J. Geophys. Res. A-Sol. Ea. 119, 1764–1776 (2014).

44. 44.

Rowley, P. J., Roche, O., Druitt, T. H. & Cas, R. Experimental study of dense pyroclastic density currents using sustained, gas-fluidized granular flows. Bull. Volcanol. 76, 855 (2014).

45. 45.

Gueugneau, V., Kelfoun, K., Roche, O. & Chupin, L. Effects of pore pressure in pyroclastic flows: numerical simulation and experimental validation. Geophys. Res. Lett. 44, 2194–2202 (2017).

46. 46.

Wilson, C. J. N. The role of fluidization in the emplacement of pyroclastic flows: an experimental approach. J. Volcano Geotherm. Res. 8, 231–249 (1980).

47. 47.

Giordano, G. The effect of paleotopography on lithic distribution and facies associations of small volume ignimbrites: the WTT Cupa (Roccamonfina volcano, Italy). J. Volcanol. Geotherm. Res. 87, 255–273 (1998).

48. 48.

Druitt, T. H., Avard, G., Bruni, G., Lettieri, P. & Maez, F. Gas retention in fine-grained pyroclastic flow materials at high temperatures. Bull. Volcanol. 69, 881–901 (2007).

49. 49.

Hayashi, J. & Self, S. A comparison of pyroclastic flow and debris avalanche mobility. J. Geophys. Res. 97, 9063–9071 (1992).

50. 50.

Calder, E. et al. Mobility of pyroclastic flows and surges at the Soufriere Hills Volcano, Montserrat. Geophys. Res. Lett. 26, 534–540 (1999).

51. 51.

Lube, G. et al. Generation of air lubrication within pyroclastic density currents. Nat. Geosci. 12, 381–386 (2019).

52. 52.

Smith, G., Williams, R., Rowley, P. & Parsons, D. Investigation of variable aeration of monodisperse mixtures: implications for pyroclastic density currents. Bull. Volcanol. 80, 67 (2018).

53. 53.

Bareschino, P. et al. Fluidization and de-aeration of pyroclastic mixtures: the influence of fines content, polydispersity and shear flow. J. Volcanol. Geotherm. Res. 164, 284–292 (2007).

54. 54.

Iverson, R. M. & LaHusen, R. G. Friction in debris flows: inferences from large-scale flume experiments. Hydraulic Eng. 93, 1604–1609 (1993).

55. 55.

Iverson, R. M. The physic of debris flows. Rev. Geophys. 35, 245–296 (1997).

56. 56.

Savage, S. B. & Hutter, K. The motion of a finite mass of granular material down a rough incline. J. Fluid Mech. 199, 177–215 (1989).

57. 57.

Bagnold, R. A. Experiments on a gravity-free dispersion of large solid spheres in a Newtonian fluid under shear. Proc. R. Soc. Lond., Ser. A 225, 49–63 (1954).

58. 58.

Giordano, G. & Dobran, F. Computer simulations of the Tuscolano Artemisio’s second pyroclastic flow unit (Alban Hills, Latium, Italy). J. Volcanol. Geoth. Res. 61, 69–94 (1994).

59. 59.

Marra, F., Karner, D. B., Freda, C., Gaeta, M. & Renne, P. Large mafic eruptions at Alban Hills Volcanic District (Central Italy): chronostratigraphy, petrography and eruptive behavior. J. Volcanol. Geotherm. Res. 179, 217–232 (2009).

60. 60.

Giordano, G. et al. Stratigraphy, volcano tectonics and evolution of the Colli Albani volcanic field. In The Colli Albani Volcano Special Publications of IAVCEI 3 (eds. Funiciello, R. & Giordano, G.) 43–98 (The Geological Society, London, 2010).

61. 61.

Trolese, M., Giordano, G., Cifelli, F., Winkler, A. & Mattei, M. Forced transport of thermal energy in magmatic and phreatomagmatic large volume ignimbrites: paleomagnetic evidence from the Colli Albani volcano, Italy. Earth. Planet. Sc. Lett. 478, 179–191 (2017).

62. 62.

Giordano, G. & Doronzo, D. M. Sedimentation and mobility of PDCs: a reappraisal of ignimbrites’ aspect ratio. Sci. Rep. 7, 1–7 (2017).

63. 63.

Conticelli, S. et al. Geochemistry, isotopes and mineral chemistry of the Colli Albani volcanic rocks: constraints on magma genesis and evolution. In The Colli Albani Volcano Special Publications of IAVCEI 3 (eds. Funiciello, R. & Giordano, G.) 107–139 (The Geological Society, London, 2010).

64. 64.

Brand, B. & Clarke, A. An unusually energetic basaltic phreatomagmatic eruption: Using deposit characteristics to constrain dilute pyroclastic density current dynamics. J. Volcanol. Geotherm. Res. 243–244, 81–90 (2012).

65. 65.

Rowley, P., MacLeod, N., Kuntz, M. & Kaplan, A. Proximal bedding deposits related to pyroclastic flows of May 18, 1980, Mount St. Helens, Washington. Bull. Geol. Soc. Am. 96, 1373–1383 (1985).

66. 66.

Fisher, R. V. & Schmincke, H.-U. Pyroclastic Rocks (Springer-Verlag, Berlin, 1984).

67. 67.

Boudet, J. F., Amarouchene, Y., Bonnier, B. & Kellay, H. The granular jump. J. Fluid Mech. 572, 413–431 (2007).

68. 68.

Faug, T. Depth-averaged analytic solutions for free-surface granular flows impacting rigid walls down inclines. Phys. Rev. E 92, https://doi.org/10.1103/PhysRevE.92.062310 (2015).

69. 69.

Faug, T., Childs, P., Wyburn, E. & Einav, I. Standing jumps in shallow granular flows down smooth inclines. Phys. Fluids. 27, https://doi.org/10.1063/1.4927447 (2015).

70. 70.

Douillet, G. et al. Pyroclastic dune bedforms: macroscale structures and lateral variations. Examples from the 2006 pyroclastic currents at Tungurahua (Ecuador). Sedimentology 66, 1531–1559 (2018).

71. 71.

Iverson, R. M. & Denlinger, R. P. Flow of variably fluidized granular masses across three-dimensional terrain: 1. Coulomb mixture theory. J. Geophys. Res. 106, 537–552 (2001).

72. 72.

Geldart, D. Types of gas fluidization. Powder Technol. 7, 285–292 (1973).

73. 73.

Carrigy, M. A. Experiments on the angles of repose of granular materials. Sedimentology 14, 147–158 (1970).

74. 74.

Rowley, P. J., Kokelaar, P., Menzies, M. & Waltham, D. Shear-derived mixing in dense granular flows. J. Sediment. Res. 81, 874–884 (2011).

75. 75.

Fielding, C. R. Upper flow regime sheets, lenses and scour fills: extending the range of architectural elements for fluvial sediment bodies. Sediment. Geol. 190, 227–240 (2006).

## Acknowledgements

This work was carried out as part of a PhD project funded by a University of Hull PhD scholarship in the Catastrophic Flows Research Cluster. Experiments were performed in the Geohazards Lab at the University of Portsmouth, using equipment funded by a British Society for Geomorphology Early Career Researcher Grant held by P.R. D.P. was supported through funding from the European Research Council (ERC) under the European Union’s Horizon 2020 Research and Innovation Programme (Grant Agreement no. 72955). G.G., M.T. and A.S. gratefully acknowledge The Grant of Excellence Departments, MIUR-Italy.

## Author information

Authors

### Contributions

G.S. carried out experimental work and drafted the paper. G.S., P.R., G.G., M.T. and A.S. carried out fieldwork. G.S., P.R. and R.W. analysed the experimental data. G.S., P.R., R.W., G.G., M.T., A.S. and D.P. discussed results and edited/commented on the paper. Characterisation of the experimental materials was led by S.C.

### Corresponding author

Correspondence to Gregory Smith.

## Ethics declarations

### Competing interests

The authors declare no competing interests.

Peer review information Nature Communications thanks Guilhem Douillet and Benjamin Andrews for their contribution to the peer review of this work. Peer review reports are available.

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Smith, G., Rowley, P., Williams, R. et al. A bedform phase diagram for dense granular currents. Nat Commun 11, 2873 (2020). https://doi.org/10.1038/s41467-020-16657-z

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