# Volcano inflation prior to an eruption: Numerical simulations based on a 1-D magma flow model in an open conduit

- Ryohei Kawaguchi
^{1}Email author, - Takeshi Nishimura
^{1}and - Haruo Sato
^{1}

**65**:6501201477

https://doi.org/10.5047/eps.2013.05.005

© The Society of Geomagnetism and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; The Geodetic Society of Japan; The Japanese Society for Planetary Sciences; TERRAPUB. 2013

**Received: **30 July 2012

**Accepted: **3 May 2013

**Published: **6 December 2013

## Abstract

We numerically simulate volcanic inflation caused by magma ascent in a shallow conduit at volcanoes which repeatedly erupt, in order to understand the effect of volatile behavior on magma from geodetic data. Considering magma in which the relative velocities between melt and gas bubbles are negligible, we model magma flow in a one-dimensional open conduit with diffusive gas bubble growth. We calculate the ground displacements and tilts caused by spatio-temporal changes of magma pressure in the conduit. Our simulations show that magma without volatiles causes decelerated changes in volcanic inflation. Magma with gas bubble growth inflates the volcano with a constant, or accelerated, rate. Temporal changes of volcanic deformation are also affected by the magma pressure at the bottom of the conduit. When the pressure is small, the displacements and tilts increase in proportion to the 1.5th power of time. This time rate is similar to that predicted from a basic gas bubble growth model. When the pressure equals the lithostatic pressure, the effects of gas bubble growth relatively decrease and the displacements and tilts increase linearly with time.

## Key words

## 1. Introduction

Volatile behavior in magma plays an important role in eruption styles and intensities. To understand the physical processes in magma that control magma ascent and eruption styles, many studies have been conducted on the basis of laboratory experiments, numerical calculations and theoretical considerations. Theoretical and numerical models have examined bubble growth processes at micro scales, and clarified that the bubble growth rate mainly depends upon the amount of volatiles saturated in the melt and the physical properties of the melt such as the viscosity and diffusion coefficients of the volatiles in the melt (e.g., Sparks, 1978; Proussevitch et al., 1993; Proussevitch and Sahagian, 1996; Lensky et al., 2004). Laboratory experiments have clarified the volatile behavior and the physical properties of magma (e.g., Lyakhovsky et al., 1996; Okumura et al., 2008). For example, Lyakhovsky et al. (1996) performed a gas bubble growth experiment under high pressure and high temperature conditions, and measured the bubble radius and the number density of bubbles for a rhyolitic hydrated melt. Their experimental results are well explained by the theoretical bubble growth model presented by Proussevitch et al. (1993). They also showed that the bubble radius growth rate is proportional to the square root of time when the bubble growth process is subjected to the diffusion of volatiles.

Numerical simulations have investigated the macro-scale magma ascent processes in magmatic conduits to elucidate the mechanism of volcanic eruptions. For sustained Plinian type eruptions, steady-state magma flow models have revealed the importance of magma properties and conduit shape on the dynamics of magma flow and volcanic eruption styles (e.g., Wilson et al., 1980; Woods and Koyaguchi, 1994; Yoshida and Koyaguchi, 1999; De Michieli Vitturi et al., 2008). Non-sustained Vulcanian eruptions have also been studied by using time-dependent magma flow models (e.g., Barmin et al., 2002; Melnik and Sparks, 2002; Costa et al., 2007; Mason et al., 2006; Ida, 2007; Nakanishi and Koyaguchi, 2008; Anderson and Segall, 2011). Melnik and Sparks (2002) and Mason et al. (2006) showed that the substantivity of explosive eruptions is significantly affected by the volatile behavior in magma: when volatiles can diffuse fast enough in the magma, the eruption becomes a sustained Plinian eruption, while magma with a slow diffusion of volatiles turns an eruption into a short-lived Vulcanian explosion.

In addition to these laboratory and theoretical studies, analyses of geophysical data obtained at active volcanoes have been intensively conducted to capture â€˜in situ' mag-matic motion. For example, geodetic data analyses are useful for determining the locations and sizes of volcanic pressure sources by applying pressure source models (Mogi, 1958; Okada, 1985; Davis, 1986). Recent observations conducted at active craters have succeeded in detecting tiny inflation and deflation signals associated with small Vulca-nian or Strombolian explosions with high resolution. For example, at the Stromboli volcano, small inflations that accelerate with time are observed for repetitive explosions (Ripepe and Harris, 2008). At the Semeru volcano in Indonesia, accelerating inflations are also observed 200–300 s before small Vulcanian eruptions, while gas burst events follow the inflations for about 20 s with a constant rate (Nishi et al., 2007; Iguchi et al., 2008; Nishimura et al., 2012). Inflations prior to small Vulcanian eruptions are also observed at the Suwanosejima volcano, Japan (Iguchi et al., 2008). These inflations are thought to result from pressur-ization processes associated with magma ascent and/or gas flow in the shallow conduit.

It is quite important to quantitatively relate the geodetic data that capture macro-scale magma behavior with micro-scale phenomena in the magma to elucidate the magma dynamics and eruption mechanisms. Simple models, including the interaction between gas bubbles in the magma and the surrounding elastic rock, are presented by, for example, Nishimura (2004) and Shimomura et al. (2006). These results are used to understand the inflation processes, or oscillating crack motions, detected by geodetic and seismic observations (Chouet et al., 2006; Voight et al., 2006). Relationships between geodetic data and magma ascent, including macro-scale phenomena, have also been theoretically examined. Nishimura (2006) showed that magma ascent without out-gassing causes accelerated volcanic inflation that may lead to explosive eruptions. Magma ascent with out-gassing gradually inflates the volcano and causes non-explosive eruptions. His results suggest that geodetic measurements are useful in capturing micro-scale phenomena in magma that may control eruption styles.

The present study focuses on repetitive eruptions, such as Vulcanian type, to understand the relationship between micro-scale phenomena in magma and inflation processes prior to eruptions. These eruptions occur over a relatively short time interval, and the conduit system is considered to be open so that magma ascent is not significantly affected by the surrounding rocks. Nishimura (2009) recently studied volcanic inflation associated with such repetitive eruptions, and separately examined the inflations for three basic processes of magma ascent: Poiseuille flow, gas bubble growth due to diffusive gas flow, and rising gas bubble. However, the real magma ascent process in a volcanic conduit is a composite phenomenon consisting of these basic processes. Hence, it is necessary to examine magma flow that includes the expansion of gas phases in an open conduit. At a shallow depth in the conduit, there are two primary mechanisms that can expand the volume of gas phases: diffusive flow of water molecules from saturated melt to gas bubbles, and pressure differences between the gas and the surrounding melt. The present study examines magma flow mainly including the former mechanism, which may occur at volcanoes characterized by a viscous magma (e.g. andesitic magma) in which the relative velocity between the gas bubbles and the melt is taken to be negligibly small. We formulate the basic equations of two-phase magma flow to represent the magma ascent, including the Poiseuille flow and diffusive bubble growth processes, to study the temporal changes of volcanic inflation prior to eruptions. Since the melt and gas bubbles are supposed to ascend at the same speed, our model does not target the eruptions of low-viscous magma. First, we present a two-phase magma flow model in a one-dimensional open conduit using the basic equations of magma flow. Sub-sequently, we calculate temporal changes of volcanic deformation using the spatio-temporal distribution of magma pressure in the conduit that is calculated by the magma flow model. Simulating the magma ascent for different parameters of magma properties related to the bubble growth process, we discuss the relationship between the magma properties in the conduit to volcanic deformation.

## 2. Model

### 2.1 Magma ascent process in repetitive eruptions

Magma motions in a conduit have often been studied by one-dimensional non-steady two-phase magma flow models (Melnik and Sparks, 2002; Mason et al., 2006; Ida, 2007). These models suppose that diffusive gas flow is the dominant process that expands the volume of the gas phase, and that the relative velocities between the gas phase and the melt is negligibly small. The present study also assumes these conditions. For instance, the gas bubbles need to be characterized with a radius of less than about 10^{-1} m, for a magma with a viscosity of 10^{4}–10^{5} Pa s, because relative velocities between the gas bubbles and the melt are estimated to be less than 10^{–5}–10^{–4} m/s from Stokes' law. We further neglect nucleation and the coalescence of gas bubbles, and out-gassing processes from the magma into the surrounding medium, in our model. These are important basic processes for magma dynamics at a shallow depth; however, this paper is a first attempt to formulate relationships between magma flow models and ground deformation. Hence, we do not take into account these processes in the present study.

We simulate an open conduit and changes in the conduit radius caused by magma pressure. In the shallow part of the conduit (< 1 km), magma pressure variations are predicted to be less than tens of MPa from the lithostatic pressure. Assuming a rigidity of surrounding rocks of 1–10 GPa at a depth of 1 km, we estimate the changes of the circular conduit radius to be 0.025–0.25%. Even when the conduit shape is elliptical, with an aspect ratio of 10, the radius change is 2.5%. These values are negligibly small compared with changes in the magma flow within the conduit, so that we may reasonably assume a conduit with a constant radius.

### 2.2 Governing equations of magma flow in an open conduit

*ρ*is the density of two-phase magma,

*ρ*

_{ e }is the density of gas in the bubbles,

*J*is the mass flux of volatile from supersaturated melt to gas bubbles per unit volume of magma,

*v*is the magma ascent velocity,

*t*is the time measured from the eruption, and

*z*is the vertical coordinate with

*z*= 0 corresponding to the ground surface. The vertical coordinate is positive in the downward direction. Since gas and melt phases are assumed to have the same ascent velocity, the equation of motion of two-phase magma is expressed by that of a one-phase viscous fluid. Inertial terms in the equation of motion are assumed to be negligibly small because of the high viscosity of magma in our model, so we obtain:where

*a*is the conduit radius,

*η*

_{ f }is the melt viscosity,

*p*is the melt pressure, and

*g*is the gravitational acceleration. The density of two-phase magma is expressed by the densities of the gas and melt phases and the gas volume fraction

*ψ*:where

*ρ*

_{ l }is the density of the melt. Assuming that the gas phase in the bubbles is represented as a perfect gas and the melt is compressible viscous fluid, we obtain the equations of state of the gas and liquid melt phases:where

*p*

_{ r }and

*ρ*

_{ r }are the pressure and density of the melt at a reference depth (we may assume the bottom of the conduit), respectively,

*p*

_{ g }is the pressure of the gas phase in the gas bubbles,

*K*

_{ l }is the bulk modulus of the melt,

*B*is the universal gas constant divided by the molecular weight of a gas molecule, and

*T*is the absolute temperature of the magma. Here, we suppose a constant temperature of the magma independent of depth and time.

Notations used in this study.

| Bulk magma density |

| Melt density |

| Ex-solved volatile density |

| Melt pressure |

| Gas pressure |

| Melt viscosity |

| Magma ascent velocity |

| Void ratio |

| Conduit radius |

| Gravity acceleration |

| Mass flux of volatile |

| Universal gas constant |

| Magma temperature |

| Bulk modulus of melt |

| Bubble radius |

| Cell radius |

| Volatile concentration |

| Bubble number density |

| Diffusivity of volatile in melt |

| Time |

| Vertical coordinate |

### 2.3 Governing equations of gas bubble growth process in magma

*R*

_{ g }is the gas bubble radius and

*S*is the elementary cell radius. In this equation, the surface tension term is neglected, because the effect of surface tension is small for gas bubbles at a shallow depth where the gas bubble radius is considered to be large (> 10

^{–5}m).

*c*is the concentration of volatiles in the melt,

*D*is the diffusive coefficient of the volatiles in the melt, D/D

*t*is the total derivative, and

*r*is the radial coordinate. The mass change of volatiles in the gas bubble is related to the diffusive mass flux of volatiles into the gas bubble, which depends on the concentration gradient of volatiles on the bubble melt interface:The total mass flux of volatile

*J*is expressed by using the number density of the gas bubbles:where

*n*is the number density of the gas bubbles.

*Pe*, which is the ratio of the characteristic time for diffusion of volatiles to viscous deformation, is small. In this case, the unsteady term in the diffusion equation (Eq. (7)) can be neglected, because diffusion is fast enough to establish a steady-state concentration distribution of volatiles in the melt. Thus, the diffusion equation can be rewritten as:This approximation enables us to obtain an analytical solution of volatile concentration distribution in the melt, which is expressed as (Lyakhovsky et al., 1996):where

*C*

_{1}and

*C*

_{2}are integration constants. Using the mass conservation law and Henry's law,

*c*(

*R*

_{g}) = (

*K*

_{ h }

*p*

_{ g }) , where

*K*

_{ h }is Henry's constant, we can determine C1 and

*C*

_{2}as follows (Mason et al., 2006):where

*c*

_{0}is the volatile concentration in the melt when the gas bubble radius is negligibly small. By substituting Eqs. (11)–(12b) into Eq. (9), the mass flux of volatiles into the melt is rewritten as:

*R*

_{g}, the cell radius

*S*, the number density of the gas bubbles

*n*, and the gas volume fraction

*ψ*:where the subscript * represents the value when the gas bubble radius is small enough to neglect its volume at the deeper portion of the conduit. By using the above relationships, the bubble number density is related to the void ratio:The bubble number density per unit volume of magma changes with the expansion of the magma cell due to de-pressurization. In Eqs. (14) and (15), we suppose that the melt volume is constant. This is because pressure variations are less than tens of MPa in our simulation range, while the bulk modulus of the melt is on the order of tens of GPa. Hence, the melt volume change is negligibly small (< 0.1%). Although we assume a compressible melt in Eq. (5), the relationships in Eq. (14) can be useful. Substituting Eq. (14) into Eqs. (6) and (13), we obtain:The magma ascent process, including the gas bubble growth process, in the cylindrical conduit is calculated using the above two equations (Eqs. (16) and (17)) and the governing equations of magma flow (Eqs. (1)–(5)) as a function of depth

*z*and time

*t*.

### 2.4 Initial and boundary conditions

Pressure waves, caused by a withdrawal of magma at the top of the conduit due to an eruption, do not reach the deeper portion of the conduit when the magma viscosity is high and the bulk modulus of the magma is small (Nishimura, 2009). Hence, we suppose that the pressure at the bottom of the conduit *p*_{0} is constant. The pressure above the magma head depth in the open conduit is also set to be constant *p*_{h}. The melt pressure linearly increases with depth.

*c*

_{0}), the magma head depth in the conduit (

*z*

_{m0}), and the initial pressure difference between the gas bubbles and the melt (Δ

*p*). Note that the volatile concentration,

*c*

_{0}, is defined for a magma without gas bubbles and that the initial volatile concentration in the melt changes with depth, due to the pressure dependence of the solubility of volatiles in the melt. The initial gas pressure (

*p*

_{g0}(

*z*)) is set to be higher than the melt pressure, because the surrounding viscous melt prevents the expansion of gas bubbles from being subjected to a sudden depressurization. The pressure difference between the gas bubbles and the melt is set to change with depth. In the present study, we set the initial gas pressure as shown in Fig. 3, so that the amount of melt decompression decreases with depth. The initial pressure difference also decreases with depth into the deeper portion of the conduit. The pressure difference at the top of the conduit is set to be zero, and linearly increases with depth at the shallowest part. This is because the top of the magma is subjected to depressurization for a longer time. The pressure difference has a maximum, Δ

*p*, at

*z*=

*h*– 0.9 × (

*h*–

*z*

_{m0}), where

*h*is the conduit length, and linearly decreases with depth.

*c*(

*p*

_{g0}(

*z*)) is the volatile concentration at the initial gas pressure.

### 2.5 Normalization of the governing equations

*ρ*

_{ r }, the conduit length

*h*, and the degree of viscous drag

*η*

*f*/

*a*

^{2}. The dimensionless variables and constants are:We further introduce three characteristic time-scale parameters: (1) the Poiseuille flow time scale

*τ*

_{ p }, which is determined from the size of the conduit and the density and viscosity of the melt; (2) the viscous deformation time scale

*τ*

_{ v }, which is determined from the initial pressure difference between the gas bubble and the melt; and (3) the diffusion time scale

*τ*

_{ d }, which is determined from the number density of gas bubbles and the diffusion coefficient of the volatile in the melt. These are expressed as (Navon and Lyakhovsky, 1998; Mason et al., 2006):The Poiseuille flow time scale represents the time scale of macro-scale magma ascent processes due to pressure gradients in the conduit. The viscous deformation time scale and diffusion time scale represent the time scales of micro-scale gas bubble growth processes. When the Poiseuille flow time scale is smaller than the viscous deformation time scale and the diffusion time scale, the magma ascent velocity is faster than the bubble growth speed so that magma reaches the ground surface until the gas bubbles have grown sufficiently. When the viscous deformation time scale is smaller than the diffusion time scale, the bubble growth process is governed by the viscous resistance of the melt. When the diffusion time scale is smaller than the viscous deformation time scale, the bubble growth process is governed by the diffusive volatile flow from melt to gas bubbles. These characteristic time-scale parameters have often been used in previous magma flow models, although the coefficients on the normalized parameters are sometimes different (Lensky et al., 2004). Then, we obtain the dimensionless equations:

Scale units used in this study.

Physical quantity | Scale unit | Typical value |
---|---|---|

Density |
| 2500 kg/m |

Length |
| 1000 m |

Time |
| 320 s |

Pressure |
| 25 MPa |

Velocity |
| 3 m/s |

We solve these dimensionless equations by using the finite difference method. For the numerical calculation, the dimensionless coordinate is divided into equally spaced grid points. The number of grid points covering the whole conduit is always set to be 100. The discrete variables at each grid point are calculated as a function of time by integrating the dimensionless differential equations (22)–(24) with the fourth-order Runge-Kutta method. The magma head depth, which moves upward with time, is not always located at a grid point. The grid point just below the magma head depth is used for the calculation, and the dimension-less variables at the top grid point are determined by linearly interpolating the values at the boundary of the magma head and the values at the grid just beneath the highest grid. The magma head depth is calculated by using the magma velocity at the top grid point, which is determined from Eq. (25). When the magma head reaches the ground surface, the calculation is stopped.

### 2.6 Calculation of volcanic deformation

*u*

_{ r }and the vertical displacement

*u*

_{ z }, on the flat ground surface of a homogeneous elastic half-space, are obtained by using the analytical solutions of the displacement field by a pressurized open conduit (Bonaccorso and Davis, 1999):whereand

*r*is the horizontal distance from the vent to a station on the flat surface,

*v*is the Poisson's ratio of the surrounding elastic medium, d

*p*(

*z, t*) is the excess magma pressure from the initial condition (

*t*= 0),

*μ*is the rigidity of the surrounding elastic medium,

*a*is the conduit radius, and (Fig. 4). Herein,

*u*

_{ z }and

*u*

_{ r }are positive when the displacements are upward and outward from the vent, respectively. The tilt

*γ*is expressed as:where

*γ*is positive when the ground is lifted up toward the vent.

*h*:In the following sections, the calculation results are shown using these dimensionless displacements.

## 3. Simulation Results

### 3.1 Model parameters

*p*

_{0}and

*p*

_{ h }), the initial magma head depth (

*z*

_{m0}), the pressure difference between gas bubble and melt (Δ

*p*), the volatile concentration (

*c*

_{0}) and the ratios of characteristic time scales (

*τ*p/

*τ*

_{ d }and

*τ*

_{ p }/

*τ*

_{ v }) which appear in the dimensionless equations. In consideration of our assumption that the relative velocities between the gas bubbles and the melt is negligibly small, we use the physical parameters shown in Table 3, in which their typical values and variation ranges are given. The characteristic time scales,

*τ*

_{ p },

*τ*

_{ v }and

*τ*

_{ d }, are estimated to be 320 s, 1 s and 0.1 s, respectively, for the typical values shown in Table 3. We assume

*μ*= 10 GPa and

*v*= 0.25 for the surrounding elastic medium.

Typical values and variations of magma properties and conduit sizes used in this study.

Property | Symbol | Typical value | Variation range |
---|---|---|---|

Melt density |
| 2.5×10 | |

Bulk modulus of melt |
| 1.2×10 | |

Gas constant |
| 8.31 J K | |

Magma temperature |
| 1100 K | |

Melt viscosity |
| 10 | 10 |

Gas bubble number density |
| 10 | 10 |

Diffusivity |
| 10 | 10 |

Initial pressure difference | Δ | 0.1 MPa | 0.1–1 MPa |

Conduit radius |
| 10 m | 3–10 m |

### 3.2 General characteristics of magma ascent and volcano deformation

*h*. The displacements, as well as tilts, increase with the distance

*r*′, reach peaks at

*r*′ = 0.1–0.4, and gradually decrease with distance. As the magma head ascends in the conduit from

*t*′ = 0 to

*t*′ = 0.24, the amplitudes of the displacements and tilts increase, and the peaks of the displacements and tilts appear at distances close to the vent. The locations where the tilts show peak values are farther away than those of displacements. These results suggest that the spatio-temporal distribution of volcanic deformation may be used to estimate the depth of the magma head and its temporal changes. Figure 7 shows the temporal changes of volcanic deformation at stations located at different distances from the vent. The figure shows that the deformation rates at locations close to the vent (

*r*′ < 1) greatly increase with time, despite an almost constant magma ascent speed. This is because the displacements and tilts at a station close to the vent are more affected by the depth change of the magma head in the conduit. For example, a tilt at

*r*′ = 0.2 shows a downlift toward the vent after the start of magma ascent, and then changes to an uplift. Whereas the deformation rates at larger distances (

*r*′ ≥1) change little with time. Thus, the displacements and tilts at a station far from the vent increase, being proportional to the magma head depth.

### 3.3 Effects of the model parameters

To examine the effects of the model parameters on the deformation, we simulate the magma ascent by changing one parameter and fixing the others. The temporal changes of the volcanic deformation at *r*′ = 1.0 are examined to omit the effect of depth change of the magma head.

*t*′

^{1.5}. This accelerated change is the same as that predicted by the diffusive gas bubble growth model of Nishimura (2009). This indicates that a decreasing decreases the pressure gradient, so that a volume expansion due to the gas bubble growth process becomes the dominant driving force. These results suggest that the rate of volcanic deformation is affected by the initial pressure gradient built up in the conduit just after eruption.

*r*′ = 1.0 for different time-scale ratios,

*τ*

_{ p }/

*τ*

_{ v }and

*τ*

_{ p }/

*τ*

_{ d }. In the range of the model parameters shown in Table 3,

*τ*

_{ v }and

*τ*

_{ d }are always smaller than

*τ*

_{ p }. This condition represents a bubble growth process that proceeds faster than the Poiseuille magma flow. When (Figs. 9(a, b)), the characteristic time-scale parameters do not affect the temporal changes in the deformation because the effect of the pressure gradient in the conduit is large enough to decrease the effect of gas bubble growth. When (Figs. 9(c, d)), the radial displacements increase with time, being proportional to in the range of the model parameters shown in the Table 3 (

*τ*

_{ p }/

*τ*

_{ v }= 320–1280). These results are the same as those shown in Fig. 8. For the case of a smaller value (

*τ*

_{ p }/

*τ*

_{ v }= 0.1), the radial displacement linearly increases with time. The small

*τ*

_{ p }represents the condition where the conduit radius is sufficiently large and/or magma viscosity is low. In this case, a small viscous resistance in the Poiseuille flow results in magma moving upward before gas bubble growth, which decreases the effect of the driving force by the volume expansion of the gas bubbles. A difference in

*τ*

_{ p }/

*τ*

_{ d }, does not change temporal changes in the deformation, even for . We use the analytical solution of the diffusive mass flux of volatiles for the bubble growth process, assuming that the diffusion of volatiles in the melt is fast. Therefore, to investigate the effect of diffusion time-scales in detail, it is necessary to solve the diffusion equation accurately. These simulations indicate that the time scale parameter

*τ*

_{ p }/

*τ*

_{ v }affects the temporal changes of deformation when the pressure gradient in the conduit is small.

*r*′ = 1.0 for a magma with, and without, volatiles. When the magma has no volatiles (

*c*

_{0}= 0.0%), the driving force of the magma is just the pressure gradient in the conduit. In this case, as the magma ascends, the ascent velocity decreases with time and becomes almost zero near the ground surface, since the pressure gradient in the magma approaches that caused by the gravitational force. As a result, the time rates of the radial displacement and tilt decrease with time. On the other hand, the radial displacement and tilt almost constantly increase with time when the magma includes volatiles (

*c*

_{0}= 1.0%). This is because the magma pressure gradient in the conduit is small due to a low magma density and does not change much with time. In addition, the driving force for the magma with volatiles include the pressure gradient in the conduit and the volume expansion due to gas bubble growth. Therefore, the rate of volcanic deformation does not decrease as does the magma without volatiles. The amplitudes of volcanic deformation due to magma without volatiles are larger than those when the magma contains gas bubbles, when the magma reaches the ground surface because the magma density is large.

*r*′ = 1.0 for different initial pressure differences between the gas bubbles and the melt Δ

*p*′. The parameter Δ

*p*′ changes from 0.004 to 0.04, which corresponds to a pressure of 0.1–1.0 MPa. Since Δ

*p*′ increases the initial volatile supersaturation in the melt, the mass flux of volatiles from the saturated melt to the gas bubbles for large Δ

*p*′ is faster at the beginning of the magma ascent than that for small Δ

*p*′. This is recognized in the differences of the power of the lapse time of the temporal changes in the radial displacement, while the magma ascending time and the final amplitudes of the deformation are little affected by Δ

*p*′. Figure 11(b) shows the temporal changes in the radial displacements for magma pressure at the top of the conduit , which may be related to the weight or viscous resistance of cap rocks. The large magma head pressure hinders the magma ascent; hence, the amplitude of the volcanic deformation decreases with increasing . The magma head pressure does not affect the magma ascent process as much as does the pressure at the bottom of the conduit. Figure 11(c) shows the temporal changes in the radial displacements for different initial magma head depths , which may be related to the volume of volcanic products from a previous eruption. As increases, the magma ascending time to reach the ground surface becomes longer and the amplitudes of the displacement increase. has little effect on the rate of volcanic deformation.

## 4. Discussion

We have presented a magma ascent model in an open conduit and examined the basic behavior of volcanic deformations for various model parameters. First, we examine whether or not our model can explain the geodetic and seismic data observed at active volcanoes. Interval times of eruptions and tilt amplitudes observed at the Semeru volcano, Indonesia, are about 3 to 30 minutes, and about 1–10 nanoradian at a distance of 500 m away from the active vent (figure 5 of Iguchi et al., 2008). At the Suwanose-jima volcano, Japan, uplifts start about 120 s before explosions and about 30 × 10^{–6} m vertical uplifts are observed at a distance of 500 m (station SWC-UD, in Iguchi et al., 2008, Fig. 4). These volcanoes erupt basaltic-andesitic magma which has a viscosity of about 10^{4}–10^{5} Pa s. Also, an analysis of the explosion earthquakes uses a conduit radius of 10 m (Nishimura, 1998), but recent activities of Suwanose-jima are small, so we assume a conduit radius, *a*, of 5 m. The eruption size of the Semeru volcano is also similar to that of Suwanosejima. Tameguri et al. (2004) determined the initial phase of the explosion earthquakes at about 500 m, so we tentatively set the conduit length to be 1000 m. The pressure at the bottom, *p*_{0}, is set to be 20 MPa, which is obtained from the magma static pressure at that depth. Thus, using typical model parameters of the magma properties shown in Table 3, we estimate the magma ascent time to be 13.5 minutes and the maximum amplitude of tilt to be 3 nanoradian at *r* = 500 m for *c*_{0} = 0.5%. Also, assuming *z*_{m0} = 400 m, and *η*_{
f
} = 8 × 10^{4} Pa s, the duration time of the magma ascent and the vertical displacement are estimated to be 120 s and 30 × 10^{–6} m, respectively, at *r* = 500 m. These estimated values are reasonably matched with the observations. However, as indicated in Eqs. (27) and (28), the amplitude of deformation is proportional to the square of the conduit radius and increases with the conduit length. Also, the magma ascending time depends on the Poiseuille flow time, *τ*_{
p
}, that is mainly affected by conduit radius, magma viscosity and the length of the conduit. We may be able to assume a reasonable conduit length for the volcanic eruptions, where dense geodetic observation data are available, and determine the viscosity by analyzing the volcanic samples. Such data enable us to discuss in more detail the magma ascent process of a volcanic eruption by carrying out these kinds of observation. Also, considering the characteristics of temporal changes of volcano deformation, such as acceleration or non-acceleration, we may further discuss the magma ascent processes at active volcanoes and estimate the physical magma parameters.

Our model has simplified the magma process in the conduit by using mathematical representations for bubble growth and fluid motions that are often used in previous studies. The model mainly includes the main driving forces of magma ascent: the volume expansions of gas bubbles and the pressure gradient in the fluid. However, we did not consider, for example, out-gassing from the magma in the conduit (Ida, 2007), or fragmentations of the magma (e.g., Melnik, 2000; Koyaguchi et al., 2008), because these processes are complex and are still under investigation. Also, several studies based on geophysical observation data present a model consisting of a gas pocket at a very shallow depth just beneath a lava dome, or cap rocks, for Vulcanian eruptions (e.g., Ishihara, 1990). These processes require to be modeled to further examine various kinds of volcano inflations at active volcanoes. We have calculated the volcano deformation assuming that the displacements of the conduit wall due to magma pressure is much smaller than the conduit radius. But, when the conduit is like a thin dike, it is necessary to include the interaction of magma flow and conduit deformation. In addition, finite element methods, or boundary element methods, are useful for calculating the deformation of volcanoes with a steep topography.

## 5. Conclusion

- (1)
The magma pressure at the bottom of the conduit strongly affects the rate of the temporal changes in volcanic deformation. When the pressure at the bottom of the conduit is small, the pressure gradient decreases, and the volume expansion due to the gas bubble growth becomes dominant in the magma ascent process. As a result, the displacements and tilt increase, are proportional to the 1.5th power of time. On the other hand, when the pressure at the bottom of the conduit is large, the displacements and tilt increase linearly proportional to the lapse time. This is probably because the magma ascent process is dominated by the mag-matic pressure gradient in the conduit.

- (2)
The ratio of the characteristic time-scale parameter (

*τ*_{ p }/*τ*_{ v }) affects the temporal changes of volcanic deformation, when the pressure gradient of the magma in the conduit is small. When*τ*_{ p }/*τ*_{ v }< 1, the effect of gas bubble growth processes decreases due to the viscous resistance of the melt, and displacements and tilt increase and are proportional to the lapse time. - (3)
When volatiles are not included in the magma, the magma ascent velocity decreases with time and the deformation decelerates, since the driving force, which is the pressure gradient, becomes weak with the magma ascent.

- (4)
The initial conditions regarding the pressure difference between the gas bubble and the melt, and the magma head depth, change the magma ascent time and the amplitude of the volcanic deformation with little affect on the time rate of displacements and tilt.

## Declarations

### Acknowledgments

Careful comments from an anonymous reviewer and Phil Dawson improved this manuscript. We appreciate Nobuo Geshi for editorial efforts. This study is supported by the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan (No. 21540427). R. Kawaguchi was partly supported by the International Advanced Research and the Education Organization (IAREO) and Global COE program of Tohoku University.

## Authors’ Affiliations

## References

- Anderson, K. and P. Segall, Physics based models of ground deformation and extrusion rate at effusively erupting volcanoes,
*J. Geophys. Res*.,**116**, B07204, doi:10.1029/2010JB007939, 2011.Google Scholar - Arefmanesh, A. and S. G. Advani, Diffusion-induced growth of a gas bubble in a viscoelastic fluid,
*Rheol. Acta*,**30**, 274–283, 1991.View ArticleGoogle Scholar - Barmin, A., O. Melnik, and R. S. J. Sparks, Periodic behavior in lava dome eruptions,
*Earth Planet. Sci. Lett*.,**199**, 173–184, 2002.View ArticleGoogle Scholar - Bonaccorso, A. and P. M. Davis, Models of ground deformation from vertical volcanic conduits with application to eruptions of Mount St. Helens and Mount Etna,
*J. Volcanol. Geotherm. Res*.,**104**, 10,531–10,542, 1999.Google Scholar - Chouet, B., P. Dawson, and M. Nakano, Dynamics of diffusive bubble growth and pressure recovery in bubbly rhyolitic melt embedded in an elastic solid,
*J. Geophys. Res*.,**111**, B07310, doi:10.1029/2005JB004174, 2006.Google Scholar - Costa, A., O. Melnik, and R. S. J. Spaeks, Controls of conduit geometry and wallrock elasticity on lava dome eruptions,
*Earth Planet. Sci. Lett*.,**260**(1–2), 137–151, doi:10.1016/j.epsl.2007.05.024, 2007.View ArticleGoogle Scholar - Davis, P. M., Surface deformation due to inflation of an arbitrarily oriented triaxial ellipsoidal cavity in an elastic half-space, with reference to Ki-lauea Volcano, Hawaii,
*J. Geophys. Res*.,**91**, 7429–7438, 1986.View ArticleGoogle Scholar - De Michieli Vitturi, M., A. B. Clarke, A. Neri, and B. Voight, Effects of conduit geometry on magma ascent dynamics in dome-forming eruptions,
*Earth Planet. Sci. Lett*.,**272**(3–4), 567–578, doi:10.1016/j.epsl.2008.05.025, 2008.View ArticleGoogle Scholar - Ida, Y., Driving force of lateral permeable gas flow in magma and the criterion of explosive and effusive eruptions,
*J. Volcanol. Geotherm. Res*.,**162**(3–4), 172–184, doi:10.1016/j.jvolgeores.2007.03.005, 2007.View ArticleGoogle Scholar - Iguchi, M., H. Yakiwara, T. Tameguri, M. Hendrasto, and J. Hirabayashi, Mechanism of explosive eruption revealed by geophysical observations at the Sakurajima, Suwanosejima and Semeru volcanoes,
*J. Volcanol. Geotherm. Res*.,**178**(1), 1–9, doi:10.1016/j.jvolgeores.2007.10.010, 2008.View ArticleGoogle Scholar - Ishihara, K., Pressure source and induced ground deformation associated with explosive eruptions at an andesitic volcano: Sakurajima volcano, Japan, in Magma Transport and Storage, edited by Ryan, M. P., 335–356, John Wiley & Sons, 1990.Google Scholar
- Koyaguchi, T., B Scheu, N. Mitani, and O. Melnik, A fragmentation criterion for highly viscous bubbly magmas estimated from shock tube experiments,
*J. Volcanol. Geotherm. Res*.,**178**(1), 58–71, doi:10.1016/j.jvolgeores.2008.02.008, 2008.View ArticleGoogle Scholar - Lensky, N. G., O. Navon, and V. Lyakhovsky, Bubble growth during decompression of magma: experimental and theoretical investigation,
*J. Volcanol. Geotherm. Res*.,**129**(1–3), 7–22, doi:10.1016/S0377-0273(03)00229-4, 2004.View ArticleGoogle Scholar - Lyakhovsky, V., S. Hurwitz, and O. Navon, Bubble growth in rhyolitic melts: experimental and numerical investigation,
*Bull. Volcanol*.,**58**, 19–32, 1996.View ArticleGoogle Scholar - Mason, R., A. Starostin, O. Melnik, and R. S. J. Sparks, From Vulcanian explosions to sustained explosive eruptions: The role of diffusive mass transfer in conduit flow dynamics,
*J. Volcanol. Geotherm. Res*.,**153**(1–2), 148–165, doi:10.1016/j.jvolgeores.2005.08.011, 2006.View ArticleGoogle Scholar - Melnik, O., Dynamics of two-phase conduit flow of high-viscosity gas-saturated magma: large variations of sustained explosive eruption intensity,
*Bull. Volcanol*.,**62**, 153–170, 2000.View ArticleGoogle Scholar - Melnik, O. and R. S. J. Sparks, Modelling of conduit flow dynamics during explosive activity at Soufriere Hills Volcano, Monserrat, in The eruption of Soufriere Hills Volcano, Monserrat, from 1995 to 1999, edited by Druitt, T. H. and Kokelaar, B. P., Memoirs of Geol. Soc., London, 307–317, 2002.Google Scholar
- Mogi, K., Relations between the eruptions of various volcanoes and the deformations of the ground surface around them,
*Bull. Earthq. Res. Inst. Univ. Tokyo*,**36**, 99–134, 1958.Google Scholar - Nakanishi, M. and T. Koyaguchi, A stability analysis of a conduit flow model for lava dome eruptions,
*J. Volcanol. Geotherm. Res*.,**178**, 46–57, doi:10.1016/j.jvolgeores.2008.01.011, 2008.View ArticleGoogle Scholar - Navon, O. and V. Lyakhovsky, Vesiculation process in silicic magmas, in Physics of Explosive Eruption, edited by Gilbert, G. S. and Sparks, R. S. J., Geological Society of London, 27–50, 1998.Google Scholar
- Nishi, K., M. Hendrasto, I. Mulyana, U. Rosadi, and M. A. Purbawinata, Micro-tilt changes preceding summit explosions at Semeru volcano, Indonesia,
*Earth Planets Space*,**59**, 151–156, 2007.View ArticleGoogle Scholar - Nishimura, T., Source mechanisms of volcanic explosion earthquakes: single force and implosive sources,
*J. Volcanol. Geotherm. Res*.,**86**, 97–106, 1998.View ArticleGoogle Scholar - Nishimura, T., Pressure recovery in magma due to bubble growth,
*Geo-phys. Res. Lett*.,,**31**, L12613, doi:10.1029/2004GL019810, 2004.View ArticleGoogle Scholar - Nishimura, T., Ground deformation due to magma ascent with and without degassing,
*Geophys. Res. Lett*.,**33**, L23309, doi:10.1029/2006GL028101, 2006.View ArticleGoogle Scholar - Nishimura, T., Ground deformation caused by magma ascent in an open conduit,
*J. Volcanol. Geotherm. Res*.,**187**(3–4), 178–192, doi:10.1016/j.jvolgeores.2009.09.001, 2009.View ArticleGoogle Scholar - Nishimura, T., M. Iguchi, R. Kawaguchi, Surono, M. Hendrasto, and U. Rosadi, Inflations prior to Vulcanian eruptions and gas bursts detected by tilt observations at Semeru Volcano, Indonesia,
*Bull. Volcanol*.,**74**, 903–911, 2012.View ArticleGoogle Scholar - Okada, Y., Surface deformation due to shear and tensile faults in a halfspace,
*Bull. Seismol. Soc. Am*.,**75**, 1135–1154, 1985.Google Scholar - Okumura, S., M. Nakamura, A. Tsuchiyama, T. Nakano, and K. Uesugi, Evolution of bubble microstructure in sheared rhyolite: Formation of a channel-like bubble network,
*J. Geophys. Res*.,**113**(B7), B07208, doi:10.1029/2007JB005362, 2008.Google Scholar - Proussevitch, A. A. and D. L. Sahagian, Dynamics of coupled diffusive and decompressive bubble growth in magmatic systems,
*J. Geophys. Res*.,**101**, 17,447–17,517, 1996.View ArticleGoogle Scholar - Proussevitch, A. A., D. L. Sahagian, and A. T. Anderson, Dynamics of diffusive bubble growth in magmas: isothermal case,
*J. Geophys. Res*.,**98**, 283–307, 1993.Google Scholar - Ripepe, M. and A. J. L. Harris, Dynamics of the 5 April 2003 explosive paroxysm observed at Stromboli by near-vent thermal, seismic and inflasonic array,
*Geophys. Res. Lett*.,**35**, L07306, doi:10.1029/2007GL032533, 2008.View ArticleGoogle Scholar - Scriven, L. E., On the dynamics of phase growth,
*Chem. Eng. Sci*.,**10**, 1–13, 1959.View ArticleGoogle Scholar - Shimomura, Y., T. Nishimura, and H. Sato, Bubble growth processes in magma surrounded by elastic medium,
*J. Volcanol. Geotherm. Res*.,**155**, 307–322, doi:10.1016/j.jvolgeores.2006.04.003, 2006.View ArticleGoogle Scholar - Sparks, R. S. J., The dynamics of bubble formation and growth in magmas: a review and analysis,
*J. Volcanol. Geotherm. Res*.,**3**, 1–37, 1978.View ArticleGoogle Scholar - Tameguri, T., M. Iguchi, and H. Yakiwara, Analysis of eruption earthquakes accompanied with small-scale eruptions at Suwanosejima volcano in November, 2003,
*Ann. Disast. Prev. Inst., Kyoto Univ*.,**47 B**, 773–777, 2004 (in Japanese with English abstract).Google Scholar - Voight, B., A. T. Linde, I. S. Sacks, G. S. Mattioli, R. S. J. Sparks, D. Elsworth, D. Hidayat, P. E. Malin, E. Shalev, C. Widiwijayanti, S. R. Young, V. Bass, A. Clarke, P. Dunkley, W. Johnston, N. McWhorter, J. Neuberg, and P. Williams, Unprecedented pressure increase in deep magma reservoir triggered by lava-dome collapse,
*Geophys. Res. Lett*.,**33**(3), L03312, doi:10.1029/2005GL024870, 2006.View ArticleGoogle Scholar - Wilson, L., R. S. J. Sparks, and G. P. L. Walker, Explosive volcanic eruption-IV. The control of magma properties and conduit geometry on eruption columm behaviour,
*Geophys. J. R. Astron. Soc*.,**63**, 117–148, 1980.View ArticleGoogle Scholar - Woods, A. W. and T. Koyaguchi, Transitions between explosive and effusive eruptions of silicic magmas,
*Nature*,**370**, 641–644, 1994.View ArticleGoogle Scholar - Yoshida, S. and T. Koyaguchi, A new regime of volcanic eruption due to the relative motion between liquid and gas,
*J. Volcanol. Geotherm. Res*.,**89**, 303–315, 1999.View ArticleGoogle Scholar