EXECUTIVE SUMMARY EXECUTIVE SUMMARY OF PROGRESS

Size: px
Start display at page:

Download "EXECUTIVE SUMMARY EXECUTIVE SUMMARY OF PROGRESS"

Transcription

1 ES-1 EXECUTIVE SUMMARY OF PROGRESS The following is the executive summary of progress and/or presentations at the E/CRC meeting. Research Approach: Dr. Siamack A. Shirazi E/CRC has developed Erosion and Erosion-Corrosion computer programs that are available at the E/CRC web sites for E/CRC members. Sand Production Pipe Saver (SPPS) that is the E/CRC erosion prediction model (computer program) is being updated and evaluated. Current work at the E/CRC is to incorporate modifications that allow SPPS to handle multiphase flow more accurately. Experiments are being conducted in slug flow, low liquid loading gas flows and annular flows. Experiments are conducted varying particle size and liquid viscosity to model effects of particle size and viscosity more accurately. Current erosion models are being extended to fines (<50 microns particles) and viscous liquids. A 2-D version of SPPS has been developed that extend SPPS capabilities. The SPPS 2-D is also being extended to handle multiphase flow. E/CRC has developed a capability of predicting erosion in complex geometries utilizing a CFD based erosion model. The CFD based erosion model is also being validated for situations involving small particles and different fluid viscosities. The CO 2 corrosion model is available with MS Excel interface and has been extended to multiphase flow and is also available at the E/CRC website. Also, E/CRC has done significant research on erosion-corrosion of corrosion resistance alloys and guidelines and test results are available to the members of E/CRC. A computer program that was previously developed to predict erosion-corrosion of carbon steels is currently being updated in Excel with VBA to include current version of SPPS and SPPS-CO 2 for multiphase flow. Experiments under multiphase flow conditions will be conducted to verify and refine the model. Petrobras has sponsored a project at E/CRC to examine effects of sand and an oil phase on an inhibitor performance. The project is developing equations that can be used to determine inhibitor effectiveness as erosivity and corrosivity are varied. Petrobras is allowing the results to be incorporated to the Erosion-Corrosion computer program that is being developed at the E/CRC.

2 ES-2 EROSION/CORROSION RESEARCH CENTER Status of SPPS and User Manual: Dr. Brenton S. McLaury SPPS v4.2 is the latest version of SPPS, which also has an accompanying updated user s manual. This version contains a variety of models to calculate thickness loss rate (penetration rate) in several geometries. SPPS utilizes particle tracking to determine particle impact velocities that are then used in erosion equations to determine erosion. The traditional approach in SPPS applies a one-dimensional (1D) particle routine; however, this approach is deficient for small particles and high density flows. So, a twodimensional (2D) approach is now also available that comes closer to replicating computational fluid dynamic (CFD) simulation results. The 2D models also have the added features of an updated erosion equation and turbulent particle dispersion. For multiphase flows, the 1D model has the options of flow regime independent and flow regime dependent models. The flow regime independent models use mixture properties for the fluid properties and utilize an expression that is a function of superficial gas and liquid velocities to represent the velocity of the flow. The flow regime dependent models are specific to a given flow regime (flow pattern). For the 1D approach, the following flow regimes are available: mist (very low liquid high gas), annular, slug, churn and bubble flows. In the upcoming version (SPPS v4.3 beta), only the flow regime independent approach will be available for the 2D model. There were many modifications in the coding for SPPS v4.2. This work was done to make SPPS more reliable and more uniform for future updates. Most of this work does not affect the use of the program. However, there is one modification that affects use. SPPS is no longer one Excel file. A.zip file must be downloaded from the website and extracted. Since flow solutions stored for the 2D geometries are very large, it became necessary to separate them into another file. Current work is also being performed to use the updated erosion equation in the 1D model. The previous erosion equation provides erosion predictions that are often overly conservative. Since previous models developed for specific flow regimes were based on the previous erosion equation, simultaneous development of these flow regime specific models is being performed. Erosion in Slug Flow: Netaji Ravikiran Kesana, PhD Student Erosion is a common problem faced by oil and gas industries, and the repair of pipeline fittings damaged by erosion is extremely costly. Therefore measuring erosion under different flow conditions and in different flow geometries is important to help better understand the effect of various parameters on erosion and to provide information to develop protective guidelines for the oil and gas producers. 0

3 ES-3 To better understand the location of maximum erosion inside the 3 inch bend we implemented a new technology called Multipoint Thickness Measurement Using Ultrasonic Transducers. The ultrasonic transducers are mounted at 16 locations on the outside bend of the elbow which allows the measurement of erosion pattern under different operating conditions. Specifically, erosion experiments have been conducted for single-phase (gas) and multiphase flow patterns (slug and mist flows) in the horizontal orientation. The experiments were performed with air and water as the fluids and using 150 and 300 micron particle sizes with 1 % concentration by weight. Results demonstrate the location of the higher erosion on the elbow under considered flow patterns. Interestingly, the location of highest erosion that we are measuring for horizontal slug flow is on the top surface of the bend (12:00 O clock position) and for the other flow patterns the location of maximum erosion is on the outer radius of the bend near the 45 degree position. In order to find out the reason behind observing higher metal loss at the top of the bend in the slug flow regime, we have conducted the sand sampling experiments inside the bend using the probes flush mounted to the inside wall of the pipe. We found that from the sand distribution results, there is more sand at the top of the bend. Also, the liquid distribution profile in the cross section of the bend shows that there is a little liquid present at the top of the bend. More sand and little liquid at the top of the bend is causing more metal loss. To improve the slug flow erosion model incorporated into the SPPS, we are also planning to study slug characteristics, such as slug body length, liquid-hold up in the slug body and slug frequency by analyzing the vast amount of data collected using Wire Mesh Sensor (WMS). Previous investigators suggested that steady state slug body will not have a constant length and it follows a log-normal distribution. Earlier experiments conducted were at lower superficial gas velocities and there is a lack of experimental data on slug characteristics under which we performed our erosion measurements. Flow Loop Study for Developing an Erosion-Corrosion Rate Prediction Model in Presence of Inhibitor and Oil Dr. Shokrollah Hassani (Project supported by Petrobras) Corrosion has an important impact on the total cost of oil and gas production. From the diversity of corrosion related problems, CO 2 corrosion (sweet corrosion) is probably the material degradation mechanism most extensively assessed in this industry for the last 30 years. Chemical inhibition is one of the most effective and popular techniques in controlling corrosion in oil and gas production and distribution. Different mechanistic and empirical models are available to predict the CO 2 corrosion as a function of different parameters including CO 2 pressure, temperature, ph, chloride content, and etc. However, sand production during oil and gas production affects the chemical inhibition efficiency. Previous research at the E/CRC on inhibited erosion-corrosion has shown that low corrosion rates in inhibited systems can increase to unacceptable levels when sand production starts. Therefore, available models for prediction of CO 2 corrosion have

4 ES-4 EROSION/CORROSION RESEARCH CENTER to be modified for the effect of sand production on CO 2 corrosion especially in the presence of chemical inhibition. In a recent erosion-corrosion research for PETROBRAS, research was directed towards quantifying the effect that erosivity has on inhibitor efficiency under selected environmental conditions. Data accumulated in this research was used to develop a framework for prediction of inhibitor efficiency in erosive flows that will allow one to predict, for selected environmental conditions, inhibitor efficiency as a function of erosivity and inhibitor concentration. PETROBRAS has agreed to make the results of this work available to improve E/CRC erosion and erosion-corrosion prediction programs, SPPS and SPPS:E-C. Corrosion and erosion-corrosion rates as baseline data for this study were produced in flow loop testing using EIS, LPR, Long-term weight loss, Potentiodynamic polarization, and 3D profilometer methods over a wide range of inhibitor concentrations (i.e. 0 ppm, 10 ppm, 25 ppm, 50 ppm, 100 ppm, 150 ppm, and 250 ppm) in four different sets of ph, two sets of temperature, two different water cut, and three different erosivities. After producing the baseline data, inhibitor surface coverage was calculated based on corrosion rate information. Relations between inhibitor concentration and inhibitor surface coverage were fitted to different inhibitor adsorption isotherms (i.e. Langmuir, Frumkin, Temkin, and Flory-Huggins) and the best fit was selected to describe inhibitor adsorption behavior in flows containing sand. Inhibitor adsorption isotherm was integrated into the E/CRC mechanistic model for prediction of CO 2 corrosion rate. Experimental erosion-corrosion test results in the presence of inhibitor, the existing E/CRC erosion model and erosion-corrosion model, and inhibitor adsorption isotherms were used to predict erosion-corrosion rate as a function of inhibitor concentration. A framework and also a model for prediction of erosion-corrosion in the presence of inhibitor and sand were developed in this research. A computer program has also developed for PETROBRAS Company for prediction of inhibited erosion-corrosion rate as a function of different corrosivity and erosivity variables. For future work, a new test section has been designed for erosion-corrosion study at low erosivity and low water cut conditions which enable us to monitor total erosioncorrosion, pure erosion, and also corrosion part of erosion-corrosion during the experiment. This new design will be used to examine, improve and validate the proposed model. Effects of Viscosity and Particle Size on Erosion Measurement and Prediction: Sai Abhishek Nidasanametla and Amir Mansouri (New PhD Student) When oil and gas are removed from reservoirs, they usually contain impurities such as small sand particles. These particles impinge the wall of the pipes that gas and oil are carried in and damage the wall. This damage is called erosion. In order to prevent erosion damage, many industries are using erosion models to predict when the pipeline 0

5 ES-5 and fittings are going to fail due to erosion. The Erosion/Corrosion Research Center (E/CRC) at the University of Tulsa has conducted research on erosion and corrosion occurring under a range of conditions and pipe geometries. One of the main goals of E/CRC is to develop the software called Sand Production Pipe Saver (SPPS) which can predict erosion for a certain geometry and set of conditions. This software can be used as a guideline by the oil and gas industries. Erosion rates have been measured for 50, 150 and 350 µm spherical glass beads in air. The target material is Aluminum T6. The particle velocities tested are 24 and 42 m/s. The results showed that erosion is not significantly affected by particle size as long as the particles have the same impact speeds. A new erosion equation has been generated based on these results and implemented into a commercially available Computational Fluid Dynamics (CFD) code to predict erosion rates for a variety of flow conditions, flow geometries, and particle sizes. Concurrently, the erosion rate of the same material with a direct impingement geometry using 50, 150 and 350 µm glass beads are measured in liquid of various viscosities. The nozzle average liquid exit velocity was maintained at 10 m/s and carrier of viscosities 1, 10 and 30 cp are used. CFD analyses are performed in order to predict erosion rate in a same geometry. The erosion results showed that for the range of viscosities considered, larger particles produced higher erosion rates than smaller particles. CFD results showed that CFD tends to under-predict erosion rates for 150 and 350 µm particles while it tends to over-predict erosion rates for 50 µm. Comparison of sand and glass beads erosion results revealed that the shape of the particle only affects the erosion rate by magnitude but not the trend respect to change in viscosity. Therefore, it was proved that the discrepancy between CFD calculation and measurement is not due to the shape of particles. The effects of grid size, dimensions and turbulence models on the accuracy of CFD calculations have been studied. It was found that two-dimensional and threedimensional meshes yield the same erosion rates, the grid size affects CFD predictions for smaller particle sizes, and the turbulence models affect erosion rates for higher viscosities. Particle behavior near the wall was studied and it explains the differences in predictions are due to the number of particle impacts and average particle velocity. Future work will be conducted for additional CFD assessment to make sure CFD results are accurate. Small Particle Erosion: Fardis Najafi Fard The effect of the particle size on erosion has been investigated by researchers at the E/CRC, but in most cases, erosion from relatively small particles has not been consider nearly often as erosion from larger particles. However, recent experimental studies by the E/CRC show small, sharp particles can cause severe erosion in both gas and liquid systems. These small sands pass through gravel packs and cause erosion without

6 ES-6 EROSION/CORROSION RESEARCH CENTER being detected by acoustic sand monitors. It has been seen that usually erosion form small particles occurs in geometries with high turbulence or recalculating regions. These types of geometries are found in piping systems, chokes and valves. New experimental facilities at E/CRC allow researchers to conduct small particle erosion in gas. Direct impingement geometry was chosen due to its simplicity. Erosion from small particles is comparable with relatively larger particles in this geometry. Erosion results from these experiments were used by E/CRC researchers to develop a more accurate erosion model for small particles. Previous erosion equations over predicts the magnitude of small particles erosion in sudden contraction/expansion geometry by factor of 20 to 40 in liquid dominated system. Using new E/CRC erosion equation for small particles eliminates this over prediction at throat and reduces it to the factor of 4-6 after sudden expansion. This over prediction is due to the unphysical multiple impacts which occurs in liquid dominated systems. Currently commercial CFD code (FLUENT 6.3) is used at E/CRC for flow simulation and particle tracking. In CFD code eddy size is limited by cell size. So having larger cells (coarser mesh) results in having larger eddies. Due to the fact that in sudden contraction expansion geometries, eddies have a huge effect on particle behavior, Having larger eddies changes particles behavior and results in changing erosion prediction. Also CFD predicts that small particles which enter viscose sub-layer, tend to stay and hit the wall over and over in a really small area with almost constant impact velocity. This nonphysical behavior results in over prediction of erosion magnitude. Erosion sensitivity study on sudden expansion geometry shows initial particles boundary conditions and particles size playing an important role in CFD erosion prediction in gas. By changing initial particles boundary conditions, CFD prediction changes from not predicting any erosion to predicting erosion close to experimental data in this geometry. To overcome commercial CFD code problems, a separate particle tracking code is being developed. Since FLUENT correctly predict flow solution so flow solution is obtained in FLUENT and exported to E/CRC particle tracking code. Using E/CRC particle tracking code allows us to predict particle trajectories and resulting erosion. Since the current E/CRC particle tracking code is preliminary, more study is needed to examine the current particle tracking code. Due to the fact that small particles cause severe erosion in geometries with high turbulence and re-circulation area, developing an accurate erosion model is necessary. Eventually, new developments in CFD-based erosion modeling will be used to improve SPPS 2-D. 0

7 ES-7 Erosion-Corrosion Prediction Modeling: Faisal Al-Mutahar, PhD Candidate In the oil and gas production industry, carbon steel tubing and piping are susceptible to erosion-corrosion due to the erosive and corrosive nature of the flow. The combined effect of sand erosion and corrosion can be very significant. In this research, the effects of erosion-corrosion of carbon steel, due to sand and CO 2, are being studied for multiphase flow. Two different Erosion-corrosion mechanisms are being considered. The first is erosion-corrosion mechanism for non scale-forming (FeCO 3 ) conditions, and the second for scale-forming conditions. Existing E/CRC models for erosion and CO 2 corrosion have provided the foundation for the new Erosion-Corrosion model. The main contribution of this research can be summarized in three points: 1) Developing a mechanistic model of the competition between FeCO 3 scale growth by precipitation and scale removal by erosion, 2) Developing a procedure for prediction of erosion-corrosion in oil and gas production and transportation systems, and 3) Developing a computer program for predicting the erosion-corrosion penetration rate. The erosion-corrosion model has been developed by building on the E/CRC models SPPS:CO 2 and SPPS, drawing upon the technical literature on FeCO 3 scale formation where available, and conducting experiments on scale properties relevant to scale structure and erosion resistance. FeCO 3 scales, produced under a range of environmental conditions, have been characterized with respect to scale structure, thickness and erosion resistance. Models from the literature have been evaluated for quantifying iron carbonate scale precipitation and growth rates and for diffusion through the scale. Single phase flow erosion-corrosion data has been obtained from laboratory flow loops for evaluating and validating the model. For the scale characterization experiments, the effect of geometry, temperature, and ph on scale formation were examined. Iron carbonate scales were formed in single-phase flow loops at a range of environmental conditions. Specifically, scales were formed in jet impingement and channel flow geometries, at ph range of , temperature range of o F, 2% by weight NaCl, and 34 psia CO 2 pressure. The experimental results showed a pronounce effect of flow geometry in the scale structure. The scales formed in jet flow were thicker and less protective i.e. more porous than the scales formed in channel flow. The test results showed also that scales formed at lower temperatures and higher ph values had higher scale thickness and higher porosity. These observations can be attributed to the change in the supersaturation values resulting from the change in these parameters. Lower temperatures, lower ph values, and higher velocities decrease the supersturation which consequently led to formation of thicker and more porous scale. An extensive work was done in this research for characterizing the erosion resistance of iron carbonate scale. This was given a priority because scale erosion is a main

8 ES-8 EROSION/CORROSION RESEARCH CENTER component of the erosion-corrosion process of carbon steel in scale forming conditions. Characterization of the erosion resistance of iron carbonate scale was done by addressing the following questions: 1) Does the erosion behavior of the scale follow typical behavior of brittle, ductile or other material, 2) Does the erosion resistance of scale change by wetting, and 3) What is the ratio between average erosion ratios of FeCO3 scale to mild steel. To address these questions, erosion ratios for dry, wet, and submerged FeCO 3 scale were measured by direct impingement tests. Two forms of scales were pre-developed in single phase flow loop and then used for erosion tests. The first form has a scale thickness of 4-6 microns and the second form has a scale thickness of microns. The erosion ratio results have shown that the erosion behavior of the scale does not follow the typical behavior of brittle or ductile materials. It seems that iron carbonate scale has its own erosion behavior that changes with scale thickness. Collected data was used to calculate an Erosion Ratio Factor (ERF) that divides the erosion ratio for the scale by the erosion ratio for steel. Then the ERF for wetted surfaces (scale and bare steel) was compared to the ERF for dry surfaces (scale and bare steel). Pooling Erosion Ratio Factors for all data over all gas velocities and all impingement angles provided a body of data for ERF-dry surface having a mean value of 42.62, and a body of data for ERF-wetted surface having a mean value of A t-test with hypothesis that the true means are the same was conducted at significance level 0.05 yielding the result that the data collected so far does not provide strong evidence that the two means are different. If the Erosion Ratio Factor mean for wetted surfaces is not different from the Erosion Ratio Factor mean for the dry surfaces, then it follows that the erosion resistance mean for wetted scales is not different from the erosion resistance mean for the dry scales. A research version computer program has been developed for predicting erosioncorrosion penetration rate. Model predictions are being compared to limited experimental data. The comparison showed encouraging results. The model will be validated with larger body of single-phase and multiphase flow erosion-corrosion data for scale forming and non-scale forming conditions. Erosion Prediction Under Low Liquid Loading and Annular Flow Conditions: Ronald Vieira, PhD Student Low-liquid loading and annular gas-liquid flow conditions are commonly encountered in gas transportation pipelines. They may also occur in other production facilities as gas/condensate production systems. Experience gained from production of hydrocarbons has shown that severe degradation of production equipment may occur. Prediction of erosion in multiphase flow is a complex problem due to lack of accurate models for calculating particle impact velocities that cause erosion. The particle impact velocity is affected by the pipe geometry, carrying fluid velocity, flow pattern, particle size and distribution in the flow. The complexity of erosion prediction increases 0

9 ES-9 significantly for two-phase flow in elbows because of complicated flow patterns that occur when both liquid and gas are present in the flow. Among different flow patterns in horizontal and vertical flows, erosion is most severe when particles are transported in gas dominant systems such as low liquid loading gas and annular flows. Recent experiments have shown that for annular flows erosion does not consistently decreases with an increase in liquid rate for a given gas rate. In order to examine the location of maximum erosion for annular flows in 76.2 mm (3") bends, an ultrasonic technique is being used. Sixteen ultrasonic transducers are mounted at sixteen locations on the outside radius of a stainless steel elbow which allows the measurement of erosion pattern under different operating conditions. Erosion experiments have been conducted for annular flows in vertical and horizontal orientations. The experiments were performed with air and water as the fluids and using 300 micron particle sizes with 1 % concentration (weight of solids/weight of carrier liquid). Results show that the location of the higher erosion on the elbow under annular flows is on the outer radius of the bend near the 45 degree position. In order to confirm the results obtained, a new transducer configuration is proposed on the elbow. In addition, in order to better model the impacting sand rates and particle velocities in annular flows, new sand concentration samples have been collected in annular gasliquid flows for horizontal orientation in two different locations: at the upstream position of the bend and at 45 degrees on the elbow. Eight ports were used for collecting liquid and sand samples at each location. Results show considerable differences in sand concentration values and liquid film distributions for each sampling location. Also, wire mesh sensors were used to measure void fraction in horizontal annular flow. Future work also includes analyzing the data to validate and improve liquid film characteristics in the elbow. Accurate modeling of the liquid film is important to predict erosion in this flow regime. Liquid Impingement Erosion: Hadi Arabnejad, PhD Student In production and transportation of hydrocarbons pipe size and material is determined so that the flow velocity is below the erosional velocity and above the transport threshold velocity. The erosional velocity is defined as a flow velocity below which is safe to operate and beyond that erosion damage may occur. From economical aspect, this threshold applies a limit on the production rate, and reliable and accurate prediction of this value is of great importance. The American Petroleum Institute Recommended Practice 14E (API RP 14E) proposed an equation for determining gas-liquid mixture erosional flow velocity. Some authors believe that API equation is very simple and could be applied to predict complicated process of two-phase flow that is a function of different parameters. Also, some experimental results show that the predicted erosional velocities are very conservative.

10 ES-10 EROSION/CORROSION RESEARCH CENTER In order to recognize the liquid impingement erosion, a literature survey is being conducted which shows that some experimental studies has been done in other fields. In aerospace engineering, rain erosion is a similar phenomenon and also in power plant industries, turbine blades and steam pipeline are exposed to liquid droplet impingement erosion. There are two major types of experimental method to evaluate the material behavior in liquid droplet impact. In the first type, specimen is mounted on a rotating disk or arm and cut liquid jet or liquid droplet stream. In the second type, liquid jet or droplets are accelerated to hit a fixed specimen. Experimental results show that, there is a significant difference between the results provided by these two types of experiments. Moreover, in each type liquid droplets or continuous jet could be implemented to cause erosion and the results from these investigations are different. More survey is on the way to investigate which of these types of experiments are applicable to oil and gas industries and also to consider removal of corrosion products by means of liquid impact since they are normally more brittle than base materials. Erosion Equations for Oilfield Materials: Predicting erosion by solid particles is of great importance to the oil and gas industries. Currently, erosion prediction models such as CFD based erosion models and E/CRC SPPS rely on empirical erosion equations, particularly for engineering materials. Previously, simple erosion equations were obtained and were implemented into SPPS. These equations were based on average and/or maximum values of erosion based on wet impact testing. This research work focuses on development of erosion equations for several oilfield materials, such as 22 Chromium, Chrome Duplex, 1018 Carbon Steel, 4130 Carbon Steel, Inconel 625 and 316 SS. Experimental data will be used to develop new erosion equations that account for impact angles, and these equations will be used in SPPS and CFD to optimize erosion prediction. Several hundreds of direct impingement tests were performed with these materials metal coupons for three different gas velocities, including 287 ft/s, 192 ft/s, and 96 ft/s. Particle velocity measurement with LDV were conducted to calculate actual particle impact velocities for these experiments. Experiments were conducted with 150 micron sand and constant sand rate of approximately 20 grams/min, impact angles range from 15 degrees to 30, 45, and 90 degrees. The weight of metal coupons were measured before and after each single test to determine weight losses, and the erosion ratio has been determined by plotting the weight loss against sand throughput. Then, erosion ratios for different test conditions were plotted for each material to determine the beast angle function that is used in the erosion equation. A new form of angle function was proposed based on Oka s work. The erosion equations predicted erosion ratios show a good agreement with the experimental data. 0

11 ES-11 In summary, erosion equations were developed from extensive experimental data and can be implemented into SPPS and CFD for more accurate prediction of erosion. Limited further tests will be conducted for larger (300 µm) or smaller (50 µm) particles. Also, erosion testing may be conducted with different types of particles and effects of particle hardness on erosion ratio equations will be investigated. Development and Validation of 2-D SPPS: (Recruiting a new PhD student for this project) Two dimensional particle tracking was introduced into SPPS to improve its accuracy in erosion prediction. It was reported that the overall performance of SPPS 2-D is much better than SPPS 1-D for cases with single carrier phase (sand/gas or sand/liquid flows) The primary goal of the current work is to extend its application to multiphase flows, i.e., sand/gas/liquid flows. The idea is to combine some multiphase flow models and the original SPPS 2-D for single phase flow. The multiphase flow models are utilized to determine flow regime and related flow parameters, such as annular film thickness, liquid holdup, slug flow characteristics, and so on. The problem is then simplified to single phase flow for the purpose of erosion prediction. The 2-D particle tracking for single phase flow is then applied to calculate particle trajectory and impact information. Erosion value can then be calculated using erosion equation. The presentation in May 2011 showed how SPPS 2-D is applied to predicting erosion in slug flow and annular flow. By comparing with experimental data found in the literature and collected at E/CRC and TUSMP, it is seen that the overall performance of SPPS 2- D is much better than SPPS 1-D. In the past one year, a lot effort has been put to optimize and re-organize the source code of SPPS. The flow field information database is now separated from the main program, making it easy to be distributed and upgraded. A progress bar showing the progress of the calculation is added so that the user can tell whether SPPS is working or freezes. One of the future works is to examine the capability of SPPS 2-D in predicting erosion for other flow regimes. Currently for annular flow, SPPS 2-D simply applies a liquid film to the geometry wall of interest, and conducts 2-D particle tracking in both gas core and the liquid film. Its performance has to be further examined and validated against more experimental data. For mist flow, it is correlated to the corresponding gas flow and annular flow. The model is discussed in another presentation. Applying SPPS 2-D along with this model is also one of the future works. For all other flow regimes, SPPS 2-D assumes it is single phase flow but uses mixture fluid properties in particle tracking. Again, experimental data is required to validate its performance.

SPPS USER Manual 1 SPPS USER GUIDE DRAFT VERSION 6/20/2011. Please send comments to

SPPS USER Manual 1 SPPS USER GUIDE DRAFT VERSION 6/20/2011. Please send comments to SPPS USER Manual 1 SPPS USER GUIDE DRAFT VERSION 6/20/2011 Please send comments to Brenton S. McLaury or Siamack A. Shirazi brenton-mclaury@utulsa.edu, siamack-shirazi@utulsa.edu THE EROSION/CORROSION

More information

VALIDATION AND IMPROVEMENT OF SPPS IN LOW LIQUID LOADING AND ANNULAR FLOW

VALIDATION AND IMPROVEMENT OF SPPS IN LOW LIQUID LOADING AND ANNULAR FLOW VIII-1 VIII. VALIDATION AND IMPROVEMENT OF SPPS IN LOW LIQUID LOADING AND ANNULAR FLOW Introduction Solid particle erosion of piping and fittings is caused as a result of entrained sand particles in the

More information

Solid Particle Erosion in Slug Flow. Introduction

Solid Particle Erosion in Slug Flow. Introduction EROSION IN SLUG FLOW Solid Particle Erosion in Slug Flow Introduction Sand produced by oil and gas producers creates many problems such as accumulation of the sand in perforation tunnels, lines and pumps;

More information

Proceedings of the ASME th Joint US-European Fluids Engineering Division Summer Meeting FEDSM2014 August 3-7, 2014, Chicago, Illinois, USA

Proceedings of the ASME th Joint US-European Fluids Engineering Division Summer Meeting FEDSM2014 August 3-7, 2014, Chicago, Illinois, USA Proceedings of the ASME 2014 4th Joint US-European Fluids Engineering Division Summer Meeting FEDSM2014 August 3-7, 2014, Chicago, Illinois, USA FEDSM2014-21613 EXPERIMENTAL AND NUMERICAL INVESTIGATION

More information

PARTICLE TRACKING VELOCIMETRY (PTV) MEASUREMENT OF ABRASIVE MICROPARTICLE IMPACT SPEED AND ANGLE IN BOTH AIR-SAND AND SLURRY EROSION TESTERS

PARTICLE TRACKING VELOCIMETRY (PTV) MEASUREMENT OF ABRASIVE MICROPARTICLE IMPACT SPEED AND ANGLE IN BOTH AIR-SAND AND SLURRY EROSION TESTERS Proceedings of the ASME 2016 Fluids Engineering Division Summer Meeting FEDSM2016 July 10-14, 2016, Washington, DC, USA FEDSM2016-7768 PARTICLE TRACKING VELOCIMETRY (PTV) MEASUREMENT OF ABRASIVE MICROPARTICLE

More information

THE UNIVERSITY OF TULSA THE GRADUATE SCHOOL APPLICATION OF COMPUTATIONAL FLUID DYNAMICS (CFD) TO FLOW

THE UNIVERSITY OF TULSA THE GRADUATE SCHOOL APPLICATION OF COMPUTATIONAL FLUID DYNAMICS (CFD) TO FLOW THE UNIVERSITY OF TULSA THE GRADUATE SCHOOL APPLICATION OF COMPUTATIONAL FLUID DYNAMICS (CFD) TO FLOW SIMULATION AND EROSION PREDICTION IN SINGLE-PHASE AND MULTIPHASE FLOW by Xianghui Chen A dissertation

More information

T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL A COMBINED CFD-EXPERIMENTAL METHOD FOR DEVELOPING AN

T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL A COMBINED CFD-EXPERIMENTAL METHOD FOR DEVELOPING AN T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL A COMBINED CFD-EXPERIMENTAL METHOD FOR DEVELOPING AN EROSION EQUATION FOR BOTH GAS-SAND AND LIQUID-SAND FLOWS by Amir Mansouri A dissertation

More information

THE EFFECT OF TWO PHASE (AIR-WATER) FLOW CHARACTERISTICS ON MOMENTUM FLUX DUE TO FLOW TURNING ELEMENTS AT ATMOSPHERIC CONDITIONS

THE EFFECT OF TWO PHASE (AIR-WATER) FLOW CHARACTERISTICS ON MOMENTUM FLUX DUE TO FLOW TURNING ELEMENTS AT ATMOSPHERIC CONDITIONS International Journal of Latest Trends in Engineering and Technology Vol.(8)Issue(1), pp.319-328 DOI: http://dx.doi.org/10.21172/1.81.041 e-issn:2278-621x AN EXPERIMENTAL STUDY OF THE EFFECT OF TWO PHASE

More information

6th European Sand Management Forum, March 2014, Aberdeen

6th European Sand Management Forum, March 2014, Aberdeen 6th European Sand Management Forum, 26-27 March 2014, Aberdeen Erosion Management- Using Erosion Testing Combined with Erosion Modelling John Peters, NEL, UK NEL Holds UK National Standards for fluid flow

More information

EROSION IN SLUG FLOW X-1 EROSION IN SLUG FLOW

EROSION IN SLUG FLOW X-1 EROSION IN SLUG FLOW EROSION IN SLUG FLOW X-1 EROSION IN SLUG FLOW Introduction Oil and natural gas providers supply a large percentage of energy that is used to fuel our civilization s growth and prosperity. Foremost, petroleum

More information

Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock

Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock Development of a one-dimensional boiling model: Part I A two-phase flow pattern map for a heavy hydrocarbon feedstock Pieter Verhees, Abdul Akhras Rahman, Kevin M. Van Geem, Geraldine J. Heynderickx Laboratory

More information

T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL AND PREDICTIONS. by Risa Okita. A thesis submitted in partial fulfillment of

T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL AND PREDICTIONS. by Risa Okita. A thesis submitted in partial fulfillment of T H E U N I V E R S I T Y O F T U L S A THE GRADUATE SCHOOL EFFECTS OF VISCOSITY AND PARTICLE SIZE ON EROSION MEASUREMENTS AND PREDICTIONS by Risa Okita A thesis submitted in partial fulfillment of the

More information

Piping Systems and Flow Analysis (Chapter 3)

Piping Systems and Flow Analysis (Chapter 3) Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution

More information

OMAE FLUID-STRUCTURE INTERACTION MODELING OF SUBSEA JUMPER PIPE

OMAE FLUID-STRUCTURE INTERACTION MODELING OF SUBSEA JUMPER PIPE Proceedings of the ASME 2014 33 rd International Conference on Ocean, Offshore and Arctic Engineering OMAE2014 June 8-13, 2014, San Francisco, CA USA OMAE2014-24070 FLUID-STRUCTURE INTERACTION MODELING

More information

If there is convective heat transfer from outer surface to fluid maintained at T W.

If there is convective heat transfer from outer surface to fluid maintained at T W. Heat Transfer 1. What are the different modes of heat transfer? Explain with examples. 2. State Fourier s Law of heat conduction? Write some of their applications. 3. State the effect of variation of temperature

More information

Analysis of the Cooling Design in Electrical Transformer

Analysis of the Cooling Design in Electrical Transformer Analysis of the Cooling Design in Electrical Transformer Joel de Almeida Mendes E-mail: joeldealmeidamendes@hotmail.com Abstract This work presents the application of a CFD code Fluent to simulate the

More information

CFD Simulation of Turbulent Flow Structure in Stratified Gas/Liquid Flow and Validation with Experimental Data

CFD Simulation of Turbulent Flow Structure in Stratified Gas/Liquid Flow and Validation with Experimental Data SPE-174964-MS CFD Simulation of Turbulent Flow Structure in Stratified Gas/Liquid Flow and Validation with Experimental Data Ramin Dabirian, Amir Mansouri, Ram Mohan, and Ovadia Shoham, The University

More information

Erosion Testing & CFD Erosion Modelling. John Peters, NEL, 29 January 2014

Erosion Testing & CFD Erosion Modelling. John Peters, NEL, 29 January 2014 Erosion Testing & CFD Erosion Modelling John Peters, NEL, 29 January 2014 National Measurement System (NMS) NMS is a network of laboratories and processes Maintains national measurement infrastructure

More information

Literature review relevant to particle erosion in complex geometries

Literature review relevant to particle erosion in complex geometries Journal of Physics: Conference Series PAPER OPEN ACCESS Literature review relevant to particle erosion in complex geometries To cite this article: Eirik Volent and Ole Gunnar Dahlhaug 2018 J. Phys.: Conf.

More information

CFD STUDIES IN THE PREDICTION OF THERMAL STRIPING IN AN LMFBR

CFD STUDIES IN THE PREDICTION OF THERMAL STRIPING IN AN LMFBR CFD STUDIES IN THE PREDICTION OF THERMAL STRIPING IN AN LMFBR K. Velusamy, K. Natesan, P. Selvaraj, P. Chellapandi, S. C. Chetal, T. Sundararajan* and S. Suyambazhahan* Nuclear Engineering Group Indira

More information

MODELLING PARTICLE DEPOSITION ON GAS TURBINE BLADE SURFACES

MODELLING PARTICLE DEPOSITION ON GAS TURBINE BLADE SURFACES MODELLING PARTICLE DEPOSITION ON GAS TURBINE BLADE SURFACES MS. Hesham El-Batsh Institute of Thermal Turbomachines and Power Plants Vienna University of Technology Getreidemarkt 9/313, A-1060 Wien Tel:

More information

SIMULATION OF THE FILM FORMATION AT A HIGH-SPEED ROTARY BELL ATOMIZER USED IN AUTOMOTIVE SPRAY PAINTING PROCESSES

SIMULATION OF THE FILM FORMATION AT A HIGH-SPEED ROTARY BELL ATOMIZER USED IN AUTOMOTIVE SPRAY PAINTING PROCESSES Paper ID ILASS08-A009 ILASS08-2-14 ILASS 2008 Sep. 8-10, 2008, Como Lake, Italy SIMULATION OF THE FILM FORMATION AT A HIGH-SPEED ROTARY BELL ATOMIZER USED IN AUTOMOTIVE SPRAY PAINTING PROCESSES J. Domnick*,

More information

Investigation into Sand Deposition and Transportation in Multiphase Pipelines Phase 2

Investigation into Sand Deposition and Transportation in Multiphase Pipelines Phase 2 Investigation into Sand Deposition and Transportation in Multiphase Pipelines Phase 2 Matthew Avent Dr Jeremy Leggoe School of Mechanical and Chemical Engineering CEED Client: Woodside Energy Ltd. Abstract

More information

CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE

CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE CHAPTER 7 NUMERICAL MODELLING OF A SPIRAL HEAT EXCHANGER USING CFD TECHNIQUE In this chapter, the governing equations for the proposed numerical model with discretisation methods are presented. Spiral

More information

Experiment (4): Flow measurement

Experiment (4): Flow measurement Experiment (4): Flow measurement Introduction: The flow measuring apparatus is used to familiarize the students with typical methods of flow measurement of an incompressible fluid and, at the same time

More information

SONAR-BASED VOLUMETRIC FLOW METER FOR CHEMICAL AND PETROCHEMICAL APPLICATIONS

SONAR-BASED VOLUMETRIC FLOW METER FOR CHEMICAL AND PETROCHEMICAL APPLICATIONS SONAR-BASED VOLUMETRIC FLOW METER FOR CHEMICAL AND PETROCHEMICAL APPLICATIONS Daniel L. Gysling and Douglas H. Loose CiDRA Corporation 50 Barnes Park North Wallingford, CT 06492 USA Abstract A sonar-based

More information

NORTH SEA FLOW MEASUREMENT WORKSHOP 2004 In. St Andrews, Scotland

NORTH SEA FLOW MEASUREMENT WORKSHOP 2004 In. St Andrews, Scotland NORTH SEA FLOW MEASUREMENT WORKSHOP 2004 In St Andrews, Scotland From the 26 th to 28 th October, 2004 Tests of the V-Cone Flow Meter at Southwest Research Institute and Utah State University in Accordance

More information

Experimental and Numerical Investigation of Two- Phase Flow through Enlarging Singularity

Experimental and Numerical Investigation of Two- Phase Flow through Enlarging Singularity Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 212 Experimental and Numerical Investigation of Two- Phase Flow through Enlarging

More information

Multiphase Flow and Heat Transfer

Multiphase Flow and Heat Transfer Multiphase Flow and Heat Transfer ME546 -Sudheer Siddapureddy sudheer@iitp.ac.in Two Phase Flow Reference: S. Mostafa Ghiaasiaan, Two-Phase Flow, Boiling and Condensation, Cambridge University Press. http://dx.doi.org/10.1017/cbo9780511619410

More information

Experimental and numerical study of the initial stages in the interaction process between a planar shock wave and a water column

Experimental and numerical study of the initial stages in the interaction process between a planar shock wave and a water column Experimental and numerical study of the initial stages in the interaction process between a planar shock wave and a water column Dan Igra and Kazuyoshi Takayama Shock Wave Research Center, Institute of

More information

Water Circuit Lab. The pressure drop along a straight pipe segment can be calculated using the following set of equations:

Water Circuit Lab. The pressure drop along a straight pipe segment can be calculated using the following set of equations: Water Circuit Lab When a fluid flows in a conduit, there is friction between the flowing fluid and the pipe walls. The result of this friction is a net loss of energy in the flowing fluid. The fluid pressure

More information

Making Decisions with Insulation

Making Decisions with Insulation More on Heat Transfer from Cheresources.com: FREE Resources Making Decisions with Insulation Article: Basics of Vaporization Questions and Answers: Heat Transfer Experienced-Based Rules for Heat Exchangers

More information

Application of an ultrasonic velocity profile monitor in a hydraulic laboratory

Application of an ultrasonic velocity profile monitor in a hydraulic laboratory Application of an ultrasonic velocity profile monitor in a hydraulic laboratory Abstract Helmut Knoblauch 1, Roman Klasinc 1, Thomas Geisler 1 Velocity profile measurement using the ultrasound-pulse-doppler

More information

Estimation of Flow Accelerated Corrosion (FAC) in Feeder Pipes using CFDd Software Fluent

Estimation of Flow Accelerated Corrosion (FAC) in Feeder Pipes using CFDd Software Fluent Estimation of Flow Accelerated Corrosion (FAC) in Feeder Pipes using CFDd Software Fluent Dheya Al-Othmany Department of Nuclear Engineering, King Abdulaziz University, Jeddah 21589, Saudi Arabia Email

More information

EXPERIMENTAL ANALYSIS OF R-134a FLOW CONDENSATION IN A SMOOTH TUBE

EXPERIMENTAL ANALYSIS OF R-134a FLOW CONDENSATION IN A SMOOTH TUBE HEFAT2012 9 th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics 16 18 July 2012 Malta EXPERIMENTAL ANALYSIS OF R-134a FLOW CONDENSATION IN A SMOOTH TUBE Bastos S., Fernández-Seara

More information

Applied Fluid Mechanics

Applied Fluid Mechanics Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and

More information

Viscous Flow in Ducts

Viscous Flow in Ducts Dr. M. Siavashi Iran University of Science and Technology Spring 2014 Objectives 1. Have a deeper understanding of laminar and turbulent flow in pipes and the analysis of fully developed flow 2. Calculate

More information

Annubar Primary Element Flow Calculations

Annubar Primary Element Flow Calculations Rosemount 485 Annubar Annubar Primary Element Flow Calculations ANNUBAR PRIMARY ELEMENT FLOW EQUATIONS The Annubar primary element flow equations are all derived from the hydraulic equations which are

More information

A New Correlation for Predicting the Free Convection Loss from Solar Dish Concentrating Receivers

A New Correlation for Predicting the Free Convection Loss from Solar Dish Concentrating Receivers A New Correlation for Predicting the Free Convection Loss from Solar Dish Concentrating Receivers Abstract S. Paitoonsurikarn and K. Lovegrove Centre for Sustainable Energy Systems, Department of Engineering,

More information

INTERNAL FLOW IN A Y-JET ATOMISER ---NUMERICAL MODELLING---

INTERNAL FLOW IN A Y-JET ATOMISER ---NUMERICAL MODELLING--- ILASS-Europe 2002 Zaragoza 9 11 September 2002 INTERNAL FLOW IN A Y-JET ATOMISER ---NUMERICAL MODELLING--- Z. Tapia, A. Chávez e-mail: ztapia@imp.mx Instituto Mexicano del Petróleo Blvd. Adolfo Ruiz Cortines

More information

D.R. Rector, M.L. Stewart and A.P. Poloski Pacific Northwest National Laboratory P.O. Box 999, Richland, WA

D.R. Rector, M.L. Stewart and A.P. Poloski Pacific Northwest National Laboratory P.O. Box 999, Richland, WA Modeling of Sediment Bed Behavior for Critical Velocity in Horizontal Piping 9263 D.R. Rector, M.L. Stewart and A.P. Poloski Pacific Northwest National Laboratory P.O. Box 999, Richland, WA ABSTRACT A

More information

Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline

Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline Journal of Scientific & Industrial Research Vol. 74, March 2015, pp. 180-184 Analysis of Frictional Pressure Drop based on Flow Regimes of Oil-water Flow in Pipeline K R Naidu 1, T K Mandal 2 and S K Majumder

More information

ALASTAIR MCLACHLAN Applications Cameron

ALASTAIR MCLACHLAN Applications Cameron ALASTAIR MCLACHLAN Applications Cameron Have worked in the oil and gas flow measurement industry for 27 years primarily in custody transfer measurement using ultrasonic meters. Joined Cameron Caldon Ultrasonics

More information

White Paper FINAL REPORT AN EVALUATION OF THE HYDRODYNAMICS MECHANISMS WHICH DRIVE THE PERFORMANCE OF THE WESTFALL STATIC MIXER.

White Paper FINAL REPORT AN EVALUATION OF THE HYDRODYNAMICS MECHANISMS WHICH DRIVE THE PERFORMANCE OF THE WESTFALL STATIC MIXER. White Paper FINAL REPORT AN EVALUATION OF THE HYDRODYNAMICS MECHANISMS WHICH DRIVE THE PERFORMANCE OF THE WESTFALL STATIC MIXER Prepared by: Dr. Thomas J. Gieseke NUWCDIVNPT - Code 8233 March 29, 1999

More information

EROSION ANALYSIS FOR THE MISALIGNED U2 NOZZLE AND ITS CONNECTOR BLOCK

EROSION ANALYSIS FOR THE MISALIGNED U2 NOZZLE AND ITS CONNECTOR BLOCK WSRC-TR-2002-00352 EROSION ANALYSIS FOR THE MISALIGNED U2 NOZZLE AND ITS CONNECTOR BLOCK Si Young Lee and Richard A. Dimenna Westinghouse Savannah River Company Savannah River Site Aiken, SC 29808 Prepared

More information

Applied Fluid Mechanics

Applied Fluid Mechanics Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and

More information

Pipe Flow. Lecture 17

Pipe Flow. Lecture 17 Pipe Flow Lecture 7 Pipe Flow and the Energy Equation For pipe flow, the Bernoulli equation alone is not sufficient. Friction loss along the pipe, and momentum loss through diameter changes and corners

More information

CHAM Case Study CFD Modelling of Gas Dispersion from a Ruptured Supercritical CO 2 Pipeline

CHAM Case Study CFD Modelling of Gas Dispersion from a Ruptured Supercritical CO 2 Pipeline CHAM Limited Pioneering CFD Software for Education & Industry CHAM Case Study CFD Modelling of Gas Dispersion from a Ruptured Supercritical CO 2 Pipeline 1. INTRODUCTION This demonstration calculation

More information

Hydraulic Design Of Polyethylene Pipes

Hydraulic Design Of Polyethylene Pipes Hydraulic Design Of Polyethylene Pipes Waters & Farr polyethylene pipes offer a hydraulically smooth bore that provides excellent flow characteristics. Other advantages of Waters & Farr polyethylene pipes,

More information

1. Starting of a project and entering of basic initial data.

1. Starting of a project and entering of basic initial data. PROGRAM VISIMIX TURBULENT SV. Example 1. Contents. 1. Starting of a project and entering of basic initial data. 1.1. Opening a Project. 1.2. Entering dimensions of the tank. 1.3. Entering baffles. 1.4.

More information

INTRODUCTION TO MULTIPHASE FLOW. Mekanika Fluida II -Haryo Tomo-

INTRODUCTION TO MULTIPHASE FLOW. Mekanika Fluida II -Haryo Tomo- 1 INTRODUCTION TO MULTIPHASE FLOW Mekanika Fluida II -Haryo Tomo- 2 Definitions Multiphase flow is simultaneous flow of Matters with different phases( i.e. gas, liquid or solid). Matters with different

More information

SIMULATION OF FLOW IN A RADIAL FLOW FIXED BED REACTOR (RFBR)

SIMULATION OF FLOW IN A RADIAL FLOW FIXED BED REACTOR (RFBR) SIMULATION OF FLOW IN A RADIAL FLOW FIXED BED REACTOR (RFBR) Aqeel A. KAREERI, Habib H. ZUGHBI, *, and Habib H. AL-ALI * Ras Tanura Refinery, SAUDI ARAMCO, Saudi Arabia * Department of Chemical Engineering,

More information

CFD in COMSOL Multiphysics

CFD in COMSOL Multiphysics CFD in COMSOL Multiphysics Mats Nigam Copyright 2016 COMSOL. Any of the images, text, and equations here may be copied and modified for your own internal use. All trademarks are the property of their respective

More information

405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Data Book and Flow Handbook

405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Data Book and Flow Handbook Reference Manual 405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Book and Flow Handbook www.rosemount.com Reference Manual 405 and 1595 405 Compact Orifice Series and 1595 Conditioning

More information

What is a short circuit?

What is a short circuit? What is a short circuit? A short circuit is an electrical circuit that allows a current to travel along an unintended path, often where essentially no (or a very low) electrical impedance is encountered.

More information

Chemistry Instrumental Analysis Lecture 31. Chem 4631

Chemistry Instrumental Analysis Lecture 31. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 31 High Performance Liquid Chromatography (HPLC) High Performance Liquid Chromatography (HPLC) High Performance Liquid Chromatography (HPLC) Solvent Delivery

More information

Vertical Mantle Heat Exchangers for Solar Water Heaters

Vertical Mantle Heat Exchangers for Solar Water Heaters for Solar Water Heaters Y.C., G.L. Morrison and M. Behnia School of Mechanical and Manufacturing Engineering The University of New South Wales Sydney 2052 AUSTRALIA E-mail: yens@student.unsw.edu.au Abstract

More information

FIELD TEST OF WATER-STEAM SEPARATORS FOR THE DSG PROCESS

FIELD TEST OF WATER-STEAM SEPARATORS FOR THE DSG PROCESS FIELD TEST OF WATER-STEAM SEPARATORS FOR THE DSG PROCESS Markus Eck 1, Holger Schmidt 2, Martin Eickhoff 3, Tobias Hirsch 1 1 German Aerospace Center (DLR), Institute of Technical Thermodynamics, Pfaffenwaldring

More information

Experiment- To determine the coefficient of impact for vanes. Experiment To determine the coefficient of discharge of an orifice meter.

Experiment- To determine the coefficient of impact for vanes. Experiment To determine the coefficient of discharge of an orifice meter. SUBJECT: FLUID MECHANICS VIVA QUESTIONS (M.E 4 th SEM) Experiment- To determine the coefficient of impact for vanes. Q1. Explain impulse momentum principal. Ans1. Momentum equation is based on Newton s

More information

LOSSES DUE TO PIPE FITTINGS

LOSSES DUE TO PIPE FITTINGS LOSSES DUE TO PIPE FITTINGS Aim: To determine the losses across the fittings in a pipe network Theory: The resistance to flow in a pipe network causes loss in the pressure head along the flow. The overall

More information

[Prasanna m a*et al., 5(6): July, 2016] ISSN: IC Value: 3.00 Impact Factor: 4.116

[Prasanna m a*et al., 5(6): July, 2016] ISSN: IC Value: 3.00 Impact Factor: 4.116 IJESRT INTERNATIONAL JOURNAL OF ENGINEERING SCIENCES & RESEARCH TECHNOLOGY NUMERICAL ANALYSIS OF COMPRESSIBLE EFFECT IN THE FLOW METERING BY CLASSICAL VENTURIMETER Prasanna M A *, Dr V Seshadri, Yogesh

More information

Optimization of the nozzles structure in gas well

Optimization of the nozzles structure in gas well International Forum on Energy, Environment Science and Materials (IFEESM 2017) Optimization of the nozzles structure in gas well Zuwen WANG1, a, Shasha WANG2,b Yihua DOU3,c and Zhiguo WANG4,d 1 CNPC Chuanqing

More information

27. Running Water I (p ; )

27. Running Water I (p ; ) 27. Running Water I (p. 424-436; 440-444) Hydrosphere How much of the Earth s surface is covered by water? Earth's water is collectively called the and is stored in a number of so-called as follows: 1.

More information

FLOW MEASUREMENT. INC 102 Fundamental of Instrumentation and Process Control 2/2560

FLOW MEASUREMENT. INC 102 Fundamental of Instrumentation and Process Control 2/2560 FLOW MEASUREMENT INC 102 Fundamental of Instrumentation and Process Control 2/2560 TABLE OF CONTENTS A. INTRODUCTION B. LOCAL FLOW MEASUREMENT B.1 Particle Image Velocimetry (PIV) B.2 Laser doppler anemometry

More information

Comparison between Numerical and Experimental for UVP Measurement in Double Bent Pipe with Out-of-Plane Angle

Comparison between Numerical and Experimental for UVP Measurement in Double Bent Pipe with Out-of-Plane Angle Journal of Flow Control, Measurement & Visualization, 24, 2, 54-64 Published Online October 24 in SciRes. http://www.scirp.org/journal/jfcmv http://dx.doi.org/.4236/jfcmv.24.247 Comparison between Numerical

More information

Modeling Complex Flows! Direct Numerical Simulations! Computational Fluid Dynamics!

Modeling Complex Flows! Direct Numerical Simulations! Computational Fluid Dynamics! http://www.nd.edu/~gtryggva/cfd-course/! Modeling Complex Flows! Grétar Tryggvason! Spring 2011! Direct Numerical Simulations! In direct numerical simulations the full unsteady Navier-Stokes equations

More information

Studies on flow through and around a porous permeable sphere: II. Heat Transfer

Studies on flow through and around a porous permeable sphere: II. Heat Transfer Studies on flow through and around a porous permeable sphere: II. Heat Transfer A. K. Jain and S. Basu 1 Department of Chemical Engineering Indian Institute of Technology Delhi New Delhi 110016, India

More information

Investigation of Flow Profile in Open Channels using CFD

Investigation of Flow Profile in Open Channels using CFD Investigation of Flow Profile in Open Channels using CFD B. K. Gandhi 1, H.K. Verma 2 and Boby Abraham 3 Abstract Accuracy of the efficiency measurement of a hydro-electric generating unit depends on the

More information

HEAT TRANSFER PROFILES OF AN IMPINGING ATOMIZING WATER-AIR MIST JET

HEAT TRANSFER PROFILES OF AN IMPINGING ATOMIZING WATER-AIR MIST JET 8th World Conference on Experimental Heat Transfer, Fluid Mechanics, and Thermodynamics June 16-2, 213, Lisbon, Portugal HEAT TRANSFER PROFILES OF AN IMPINGING ATOMIZING WATER-AIR MIST JET ABSTRACT Cian

More information

Title: Max-Buchner Research Assistantship Award

Title: Max-Buchner Research Assistantship Award Title: Max-Buchner Research Assistantship Award Research Topic: Hydrodynamic Performance of Gas Oil-Sand Multiphase Production and Pipeline Transport Systems Type of Report: Final (Annual) Report Reporting

More information

A Numerical Estimate of Flexible Short-Tube Flow and Deformation with R-134a and R-410a

A Numerical Estimate of Flexible Short-Tube Flow and Deformation with R-134a and R-410a For personal use only. Additional reproduction, distribution, or transmission SL-08-043 A Numerical Estimate of Flexible Short-Tube Flow and Deformation with R-134a and R-410a Ramadan Bassiouny, PhD Dennis

More information

Experimental Investigations on the Local Distribution of wall static pressure coefficient Due To an Impinging Slot Air Jet on a Confined Rough Surface

Experimental Investigations on the Local Distribution of wall static pressure coefficient Due To an Impinging Slot Air Jet on a Confined Rough Surface Experimental Investigations on the Local Distribution of wall static pressure coefficient Due To an Impinging Slot Air Jet on a Confined Rough Surface 1 Adimurthy. M 1 BLDEA s VP DR. P G Halakatti college

More information

Deicing Chemicals - State of Practice

Deicing Chemicals - State of Practice Methods of Operation Deicing Chemicals - State of Practice Ron Wright Chemist Supervisor Idaho Transportation Department Traditional Methods Plow and antiskid Anti-icing Deicing Pre-wetting Anti-icing

More information

A STUDY ON SLUG INDUCED STRESSES USING FILE-BASED COUPLING TECHNIQUE

A STUDY ON SLUG INDUCED STRESSES USING FILE-BASED COUPLING TECHNIQUE A STUDY ON SLUG INDUCED STRESSES USING FILE-BASED COUPLING TECHNIQUE Abdalellah O. Mohmmed, Mohammad S. Nasif and Hussain H. Al-Kayiem Department of Mechanical Engineering, Universiti Teknologi Petronas,

More information

Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System

Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System Computational Fluid Dynamic (CFD) Analysis of Gas and Liquid Flow Through a Modular Sample System Tony Y. Bougebrayel, PE, PhD John J. Wawrowski Swagelok Solon, Ohio IFPAC 2003 Scottsdale, Az January 21-24,

More information

CONVECTION HEAT TRANSFER

CONVECTION HEAT TRANSFER CONVECTION HEAT TRANSFER SECOND EDITION Adrian Bejan J. A. Jones Professor of Mechanical Engineering Duke University Durham, North Carolina A WILEY-INTERSCIENCE PUBUCATION JOHN WILEY & SONS, INC. New York

More information

1D-3D COUPLED SIMULATION OF THE FUEL INJECTION INSIDE A HIGH PERFORMANCE ENGINE FOR MOTORSPORT APPLICATION: SPRAY TARGETING AND INJECTION TIMING

1D-3D COUPLED SIMULATION OF THE FUEL INJECTION INSIDE A HIGH PERFORMANCE ENGINE FOR MOTORSPORT APPLICATION: SPRAY TARGETING AND INJECTION TIMING 1D-3D COUPLED SIMULATION OF THE FUEL INJECTION INSIDE A HIGH PERFORMANCE ENGINE FOR MOTORSPORT APPLICATION: SPRAY TARGETING AND INJECTION TIMING M. Fiocco, D. Borghesi- Mahindra Racing S.P.A. Outline Introduction

More information

Sudden Expansion Exercise

Sudden Expansion Exercise Sudden Expansion Exercise EAS 361, Fall 2009 Before coming to the lab, read sections 1 through 4 of this document. Engineering of Everyday Things Gerald Recktenwald Portland State University gerry@me.pdx.edu

More information

Coflore Agitated Cell Reactor

Coflore Agitated Cell Reactor Coflore Agitated Cell Reactor Coflore ACR The Coflore ACR is a lab flow reactor developed by AM Technology for studying chemistry in flow and developing scalable continuous processes. Its flexible design

More information

STEADY FLOW THROUGH PIPES DARCY WEISBACH EQUATION FOR FLOW IN PIPES. HAZEN WILLIAM S FORMULA, LOSSES IN PIPELINES, HYDRAULIC GRADE LINES AND ENERGY

STEADY FLOW THROUGH PIPES DARCY WEISBACH EQUATION FOR FLOW IN PIPES. HAZEN WILLIAM S FORMULA, LOSSES IN PIPELINES, HYDRAULIC GRADE LINES AND ENERGY STEADY FLOW THROUGH PIPES DARCY WEISBACH EQUATION FOR FLOW IN PIPES. HAZEN WILLIAM S FORMULA, LOSSES IN PIPELINES, HYDRAULIC GRADE LINES AND ENERGY LINES 1 SIGNIFICANCE OF CONDUITS In considering the convenience

More information

NUMERICAL METHODOLOGY TO DETERMINE FLUID FLOW PATTERN WITH CORROSION IN PIPE BENDS USING COMPUTATIONAL FLUID DYNAMICS SOFTWARE

NUMERICAL METHODOLOGY TO DETERMINE FLUID FLOW PATTERN WITH CORROSION IN PIPE BENDS USING COMPUTATIONAL FLUID DYNAMICS SOFTWARE NUMERICAL METHODOLOGY TO DETERMINE FLUID FLOW PATTERN WITH CORROSION IN PIPE BENDS USING COMPUTATIONAL FLUID DYNAMICS SOFTWARE Muhammadu Masin Muhammadu 1, Kahar Osman 2 and Esah Hamzah 3 1 Department

More information

Topics in Other Lectures Droplet Groups and Array Instability of Injected Liquid Liquid Fuel-Films

Topics in Other Lectures Droplet Groups and Array Instability of Injected Liquid Liquid Fuel-Films Lecture Topics Transient Droplet Vaporization Convective Vaporization Liquid Circulation Transcritical Thermodynamics Droplet Drag and Motion Spray Computations Turbulence Effects Topics in Other Lectures

More information

Modelling multiphase flows in the Chemical and Process Industry

Modelling multiphase flows in the Chemical and Process Industry Modelling multiphase flows in the Chemical and Process Industry Simon Lo 9/11/09 Contents Breakup and coalescence in bubbly flows Particle flows with the Discrete Element Modelling approach Multiphase

More information

FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4)

FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4) FACULTY OF CHEMICAL & ENERGY ENGINEERING FLUID MECHANICS LABORATORY TITLE OF EXPERIMENT: MINOR LOSSES IN PIPE (E4) 1 1.0 Objectives The objective of this experiment is to calculate loss coefficient (K

More information

405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Data Book and Flow Handbook

405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Data Book and Flow Handbook 405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Book and Flow Handbook www.rosemount.com 405 Compact Orifice Series and 1595 Conditioning Orifice Plate Flow Test Book NOTICE Read

More information

NUMERICAL INVESTIGATION ON THE EFFECT OF COOLING WATER SPRAY ON HOT SUPERSONIC JET

NUMERICAL INVESTIGATION ON THE EFFECT OF COOLING WATER SPRAY ON HOT SUPERSONIC JET Volume 119 No. 12 2018, 59-63 ISSN: 1314-3395 (on-line version) url: http://www.ijpam.eu ijpam.eu NUMERICAL INVESTIGATION ON THE EFFECT OF COOLING WATER SPRAY ON HOT SUPERSONIC JET Ramprasad T and Jayakumar

More information

Predictionof discharge coefficient of Venturimeter at low Reynolds numbers by analytical and CFD Method

Predictionof discharge coefficient of Venturimeter at low Reynolds numbers by analytical and CFD Method International Journal of Engineering and Technical Research (IJETR) ISSN: 2321-0869, Volume-3, Issue-5, May 2015 Predictionof discharge coefficient of Venturimeter at low Reynolds numbers by analytical

More information

CONVECTION HEAT TRANSFER

CONVECTION HEAT TRANSFER CONVECTION HEAT TRANSFER THIRD EDITION Adrian Bejan J. A. Jones Professor of Mechanical Engineering Duke University Durham, North Carolina WILEY JOHN WILEY & SONS, INC. CONTENTS Preface Preface to the

More information

Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment:

Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment: 7 STEADY FLOW IN PIPES 7.1 Reynolds Number Reynolds, an engineering professor in early 1880 demonstrated two different types of flow through an experiment: Laminar flow Turbulent flow Reynolds apparatus

More information

Experimental Study of Steam Flow in a Convergent-Divergent Nozzle

Experimental Study of Steam Flow in a Convergent-Divergent Nozzle Experimental Study of Steam Flow in a Convergent-Divergent Nozzle 1 Marwa H. Athab, 2 Arkan Al-Taie, 3 Hussein W. Mashi 1 M.SC Student, 2 Professor, 3 Lecturer, Mechanical Engineering Department, UOT Abstract:

More information

Simultaneous heat and mass transfer studies in drying ammonium chloride in a batch-fluidized bed dryer

Simultaneous heat and mass transfer studies in drying ammonium chloride in a batch-fluidized bed dryer Indian Journal of Chemical Technology Vol. 13, September 006, pp. 440-447 Simultaneous heat and mass transfer studies in drying ammonium chloride in a batch-fluidized bed dryer R Kumaresan a & T Viruthagiri

More information

Laboratory of Thermal Hydraulics. General Overview

Laboratory of Thermal Hydraulics. General Overview Visit of Nuclear Master Students Laboratory of Thermal Hydraulics General Overview Horst-Michael Prasser December 04, 2009 Paul Scherrer Institut Main Goals Development of analytical and experimental methods

More information

Modeling of dispersed phase by Lagrangian approach in Fluent

Modeling of dispersed phase by Lagrangian approach in Fluent Lappeenranta University of Technology From the SelectedWorks of Kari Myöhänen 2008 Modeling of dispersed phase by Lagrangian approach in Fluent Kari Myöhänen Available at: https://works.bepress.com/kari_myohanen/5/

More information

Oil Retention and Pressure Drop of R134a, R1234yf and R410A with POE 100 in Suction Lines

Oil Retention and Pressure Drop of R134a, R1234yf and R410A with POE 100 in Suction Lines Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2012 Oil Retention and Pressure Drop of R134a, R1234yf and R410A with POE 100

More information

EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER

EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER THERMAL SCIENCE: Year 2014, Vol. 18, No. 4, pp. 1355-1360 1355 EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER by Rangasamy RAJAVEL Department of Mechanical Engineering, AMET University,

More information

Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes

Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes Computational Methods in Multiphase Flow VIII 335 Mechanistic model for four-phase sand/water/oil/gas stratified flow in horizontal pipes B. Moradi, M. Hossain & G. Oluyemi School of Engineering, Robert

More information

CFD modeling of Air-Water Two-phase Annular Flow before a 90 elbow

CFD modeling of Air-Water Two-phase Annular Flow before a 90 elbow 6 SECCIÓN TÉCNICA CFD modeling of Air-Water Two-phase Annular Flow before a 9 elbow Modelamiento en CFD de flujo anular bifásico aire-agua en una tubería antes de un codo de 9 Andrés Felipe Melo Zambrano

More information

Review of pipe flow: Friction & Minor Losses

Review of pipe flow: Friction & Minor Losses ENVE 204 Lecture -1 Review of pipe flow: Friction & Minor Losses Assist. Prof. Neslihan SEMERCİ Marmara University Department of Environmental Engineering Important Definitions Pressure Pipe Flow: Refers

More information

Conclusion Evaluating Methods for 3D CFD Models in Sediment Transport Computations

Conclusion Evaluating Methods for 3D CFD Models in Sediment Transport Computations Conclusion Evaluating Methods for 3D CFD Models in Sediment Transport Computations Hamid Reza Madihi* 1, Bagher Keshtgar 2, Sina Hosseini Fard 3 1, 2, 3 M.Sc. Coastal Environmental Engineering, Graduate

More information

INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW

INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW INFLUENCE OF JOULE THOMPSON EFFECT ON THE TEMPERATURE DISTRIBUTION IN VERTICAL TWO PHASE FLOW Daniel Merino Gabriel S. Bassani, Luiz Eduardo A. P. Duarte Deibi E. Garcia Angela O. Nieckele Two-phase Flow

More information