Overpressure

About: Overpressure is a research topic. Over the lifetime, 3236 publications have been published within this topic receiving 34648 citations.

Numerical simulations of volcanic jets: Importance of vent overpressure

Abstract: JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 113, B02204, doi:10.1029/2007JB005133, 2008 Numerical simulations of volcanic jets: Importance of vent overpressure Darcy E. Ogden, 1 Kenneth H. Wohletz, 2 Gary A. Glatzmaier, 1 and Emily E. Brodsky 1 Received 24 April 2007; revised 5 October 2007; accepted 5 November 2007; published 29 February 2008. [ 1 ] Explosive volcanic eruption columns are generally subdivided into a gas-thrust region and a convection-dominated plume. Where vents have greater than atmospheric pressure, the gas-thrust region is overpressured and develops a jet-like structure of standing shock waves. Using a pseudogas approximation for a mixture of tephra and gas, we numerically simulate the effects of shock waves on the gas-thrust region. These simulations are of free-jet decompression of a steady state high-pressure vent in the absence of gravity or a crater. Our results show that the strength and position of standing shock waves are strongly dependent on the vent pressure and vent radius. These factors control the gas-thrust region’s dimensions and the character of vertical heat flux into the convective plume. With increased overpressure, the gas-thrust region becomes wider and develops an outer sheath in which the erupted mixture moves at higher speeds than it does near the column center. The radius of this sheath is linearly dependent on the vent radius and the square root of the overpressure. The sheath structure results in an annular vertical heat flux profile at the base of the convective plume, which is in stark contrast to the generally applied Gaussian or top-hat profile. We show that the magnitude of expansion is larger than that predicted from previous 1D analyses, resulting in much slower average vertical velocities after expansion. These new relationships between vent pressure and plume expansion may be used with observations of plume diameter to constrain the pressure at the vent. Citation: Ogden, D. E., K. H. Wohletz, G. A. Glatzmaier, and E. E. Brodsky (2008), Numerical simulations of volcanic jets: Importance of vent overpressure, J. Geophys. Res., 113, B02204, doi:10.1029/2007JB005133. 1. Introduction [ 2 ] In large, explosive volcanic eruptions, the eruptive fluid issues from the vent as a high speed, compressible gas with entrained solid particulates. It is important to quantify the behavior of this gas-thrust region because it provides a connection between the fluid dynamics in the conduit and that of the buoyant column. If the eruptive fluid velocity is at or greater than sonic and vent pressure is higher than atmospheric pressure, the dynamics will be complicated by the presence of standing shock waves that can drastically alter the distribution of the vertical heat flux necessary for eruption column stability. The fluid dynamics and structure of a compressible jet issuing from a sonic nozzle into an ambient atmosphere of lower pressure are well known from experimental, analytical and computational studies [e.g., Crist et al., 1966; Young, 1975; Norman et al., 1982; Figure 1]. Although application of compressible jet dynamics to explosive volcanic eruptions was first sug- gested over 25 years ago by Kieffer [1981], the concept has Earth & Planetary Sciences Department, University of California at Santa Cruz, Santa Cruz, California, USA. Los Alamos National Laboratory, Los Alamos, New Mexico, USA. Copyright 2008 by the American Geophysical Union. 0148-0227/08/2007JB005133$09.00 yet to be widely applied in modeling and analysis of explosive eruption columns. [ 3 ] In this paper, we present computational results that quantify the important effects of vent pressure on the fluid dynamics of volcanic jets and show that overpressured jets produce vertical heat flux profiles that are drastically different than those of pressure-balanced jets. (Note: to avoid confusion, here we use the physics convention and consider ‘‘heat flux’’ the thermal energy transfer per area per unit time (J m 2 s 1 ) and ‘‘heat flow’’ the thermal energy transfer integrated over an entire area per time (J s 1 ). In volcanology literature, the term ‘‘heat flux’’ is often used to mean either of these things [e.g., Woods, 1988; Mastin, 2007]). The simulations shown here are time-dependent, though they assume a steady vent condition. Through these simulations, we quantify the effects of vent pressure and radius on plume radius and heat flux distribution after expansion of the jet. This may allow the prediction of major features of the eruptive structure. We do not consider the effects of variations in conduit dynamics, buoyancy, or the presence of a crater in order to focus only on the effects of vent pressure and radius alone. This study is not a complete picture of the complicated flow dynamics of a volcanic eruption. Rather, the results presented here could be consid- ered the ‘‘simplest case’’ to which one could compare the dynamics resulting from more complicated simulations and observations of high-pressure volcanic jets. B02204 1 of 18

The Effect of Obstacle Arrays on the Combustion of Large Premixed Gas/Air Clouds

Abstract: A series of large-scale combustion tests has been conducted in which - 4000 m3 of premixed natural gas/air and propane/air was ignited in a wedge-shaped enclosure representing a segment of a large pancake-shaped cloud. Whereas an unobstructed natural gas/air cloud produced only a few millibars overpressure when ignited by a low-energy ignition source an obstacle array consisting of six grids of horizontal pipes, representing a segment of industrial plant, accelerated the flame to a speed in excess of 100 m/s and produced an overpressure of ∼200 mbars. A number of different obstacle configurations were investigated to demonstrate the effects of changing the obstacle parameters (height, blockage and grid spacing) on the flame speed and overpressure. The results of these tests clearly show that obstacle arrays typical of those encountered in industrial plant can lead to the production of damaging overpressures.

Simplified vent sizing equations for emergency relief requirements in reactors and storage vessels

Abstract: Simplified vent sizing equations for emergency relief requirements in reaction kettles and storage vessels are obtained from analytical consideration. Venting modes include homogeneous-vessel venting, all-vacor venting, and all-liquid venting; energy sources due to runaway chemical reactions and external heating are treated separately. The resulting equations have been shown via numerical examples to yield good agreement with detailed computer simulations, both in terms of temperature and pressure histories during venting and in vent size predictions. These equations are generally applicable over a wide range of overpressure situations and reduce to the correct limit at no overpressure. The relative merit of allowing for overpressure in various venting modes can be demonstrated using these equations. Because of their simple forms, requiring only pertinent physical property and thermal data, these equations readily lend themselves to quick but accurate vent sizing predictions.