15 Corrosion Testing under Moderate and High
Transcription
15 Corrosion Testing under Moderate and High
Laboratory Test Methods for Corrosion Testing Under Moderate and High Shear Conditions Hunter Thomson, Matthew McCall, Deborah Bowering, Gordon Graham Scaled Solutions Limited, 6 Nettlehill Road, Livingston, EH54 5DL, United Kingdom Paper for Presentation at the 26th International Oilfield Chemistry Symposium 2015, Geilo, Norway, 22–25 March 2015 Abstract In both materials selection and in the application of corrosion inhibitors for the protection of oil and gas infrastructure, conditions can arise where fast flowing fluids result in very high shear, turbulent conditions (e.g. at constrictions such as valves and in-flow control devices). Effectively preventing corrosion under these high shear conditions is therefore of critical importance. A range of laboratory test methods exists for generating moderate and high shear environments in which to assess chemicals and materials for field application. Common test methods such as rotating cylinder electrode (RCE) and rotating cage autoclave (RCA) tests can provide useful data at moderate shear stresses (up to 100 Pa), while more complex methods such as jet impingement (JI) can be used to generate significantly higher shear stresses. Recently we have developed a range of more advanced laboratory test methods for the assessment of materials and production chemicals, including corrosion and scale inhibitors, at very high shear stresses up to 10,000 Pa using both weight loss and electrochemical (LPR) approaches. Conducting these tests in conjunction with more common moderate shear RCE and RCA tests allows us to build-up a picture of how different materials and chemicals perform with increasing shear stress. The development of electrochemical LPR approaches under the high shear conditions (JI-LPR) and under HP/HT autoclave conditions allows results to be generated more rapidly, while allowing more detailed evaluation of the film forming process to be evaluated than would otherwise be achievable by more conventional weight loss approaches. In this work the higher shear electrochemical JI has been compared with the more conventional weight loss JI, and also other techniques to validate the approach. The application of these advanced laboratory methods to assess materials performance and the effect of corrosion inhibitors under increasingly higher shear conditions is currently playing a vital role in evaluating the performance of materials and production chemicals for very challenging conditions, prior to field application. Furthermore, the ability to conduct these tests under increasingly higher pressures and temperatures is also of importance to enable field conditions to be matched in the laboratory. Introduction The corrosion rate of a metal is not purely dependant on electro-chemical processes but can also be significantly affected by the force exerted by fluid flowing at its surface [1]. It is well known that corrosion tends to be more severe around bends than in straight sections due to the change in fluid velocity leading to an increase in shear stress [2]. The use of in-flow control valves (ICVs) and in-flow control devices (ICDs) to improve production has become increasingly common in recent years. The small apertures combined with the high flow in these systems can result in very high shear regimes and increased turbulence. This accelerated fluid flow can lead to enhanced corrosion rates due to removal of protective corrosion by-products from the metal surface, whilst also bringing corrosive species into contact with the unprotected surface. If a corrosion inhibitor is similarly affected this can lead to catastrophic failure in an otherwise well controlled system [1]. As a result of this risk of accelerated corrosion rates, various laboratory tests have been developed to study the effects of increasing shear on corrosion [3]. A schematic of three available techniques is shown in Figure 1, illustrating the location and shape of a typical test specimen or specimens, and the direction of fluid flow within the system. Digital images displaying the main aspects of the different techniques being considered here are also provided in Figure 2 (a)-(e). -1- Figure 1: Schematic representation of the techniques used Rotating Cylinder Electrode Rotating Cage Jet Impingement Key Test specimen Direction of fluid flow Figure 2: Digital images of the techniques used 2(a) LPR Bubble Test 2(b) Rotating Cage 0 Pa 90°C, 1 bar LPR 2(c) Rotating Cylinder Electrode (RCE) Up to 80 Pa 90°C, 1 bar LPR, Pitting Up to 80 Pa 200°C, 300 bar Weight Loss, Pitting 2(d) Jet Impingement (Standard Set-up) 2(e) Jet Impingement (Autoclave Set-up) Inlet line from Inlet line from reservoir via reservoir via pump pump Outlet line to PRV Inlet line from reservoir via pump JetJet Nozzle Coupon Coupon Electrical connections for LPR 0 – 400 Pa 90°C, 1 bar LPR, Weight Loss, Pitting Up to 10,000 Pa 100°C, 200 bar LPR, Weight Loss, Pitting -2- Rotating cage tests can readily achieve shear stresses up to ca. 100 Pa but are prone to vortex formation with irregular flow dynamics which can lead to variability within the test – i.e. formation of pits on some test pieces [4] and uneven shear stresses across the surface’s leading to uneven corrosion. Rotating cylinder electrode (RCE) tests allow for more easily modelled flow dynamics but are again limited to a single shear stress up to ca. 100 Pa. The need to evaluate higher shear systems in a laboratory setting led to the development of the jet impingement (JI) test methodology [5]. This technique allows for testing at much higher shear stresses (e.g. up to ca. 10000 Pa in our laboratories). The flow regime caused by a jet impinging on a flat plate placed perpendicular to the jet can be divided into three regions; A stagnation region where the velocity is largely perpendicular to the plate surface, a wall jet region where the velocity is largely parallel to the plate, and the hydrodynamic boundary region where the flow rate and turbulence decrease rapidly. These three regions can provide good analogues for a variety of systems. The flow rate, jet nozzle size and test piece can all be readily altered to tailor the shear stresses or flow regime desired. A plot displaying the variation in shear stress with radial distance across the coupon surface in a typical jet impingement test is displayed in Figure 3 below. Figure 3: Plot displaying variation in shear stress with radial distance in a typical jet impingement test. Note: Plot displays only the stagnation and wall jet region. The hydrodynamic boundary region is omitted. High shear regimes such as those experienced in and around ICDs and ICVs can also dramatically affect scale formation, since it is a kinetically controlled process. This can include a theoretically “non-scaling” brine composition becoming problematic at restrictions within the system where shear stress and turbulence increase. The JI technique described here has also been shown to be effective in the assessment of scale formation, and investigations using the technique have shown both increases in scaling tendency and a change in scale composition at increased shear stress [6]. Method Development Initial works examined conventional weight loss JI analysis and compared results against other weight loss approaches. At this time the general consensus was that due to a combination of the uneven flow dynamics and difficulties in maintaining electrical connections within the JI set up that simple electrochemical LPR measurements were less reliable. This work therefore set out to develop reliable electrochemical JI measurements utilising both two and three electrode set-ups, initially for moderate shear LPR tests and limited to ambient pressure (maximum temperature ~ 90°C). These tests were conducted using conventional glass cells, similar to that used in conventional bubble tests (see Figure 2(d)). Alongside this work higher shear techniques were being developed at shear stresses up to 10,000 Pa and at elevated temperatures and pressures using newly designed HP/HT JI autoclaves (see Figure 2(e)). These served a number of purposes; firstly by enabling tests to be conducted at elevated temperatures and pressures, and also served to overcome a potential uncertainty in the lower pressure -3- set-up, whereby gas bubbles and cavitation could potentially occur due to the differential pressures across the injection nozzle itself when testing at higher shears. The final stage then came to introduce the electrochemical LPR measurements into the JI Autoclaves by utilising HP electrical connectors. This proved the most challenging with various prototypes being required both under the lower pressure “bubble cell” approach and also for the higher pressure / higher shear autoclave approach. Results described in this paper only show results for the final design and serve to demonstrate the increased amount of information relating to the kinetics of the corrosion process and the impact of either protective films and / or film forming inhibitors that is generally achieved with electrochemical processes, and also demonstrates that even at extremely high shears of ~ 10,000 Pa electrochemical approaches can still be used to provide accurate corrosion measurements / corrosion inhibitor performance measurements over short timeframes (typically ~ 24 hour test runs), which represents a considerable advantage over longer term weight loss measurements. Experimental Methods Test conditions The corrosion rates of two metallurgies (C1018 and L80-13Cr Steel, see Table 2) were measured at a range of shear stresses. The performance of a generic corrosion inhibitor was also assessed for its ability to mediate the corrosion of C1018 steel. Three test techniques were used in this project; 2electrode LPR bubble tests, 3-electrode RCE-LPR tests and 3-electrode JI-LPR tests for the ambient pressure “bubble cell” moderate shear JI conditions (up to 400Pa) and a 2-electrode cell for the higher shear (10,000 Pa) HP/HT Autoclave JI conditions . The test conditions are summarised below. Brine Chemistry Representative of a typical 50:50 formation water:sea water mix from the Gulf region. Note: brine prepared with sulphate anions omitted to prevent scale formation. Table 1: Brine Chemistry Ion mg/l Na+ 32000 Ca2+ 5750 Mg2+ 1500 Sr2+ 400 [HCO3]100 Temperature Pressure Brine Gas Metallurgy Techniques Test Duration: Shear Stress Analysis pH 80°C Ambient See Table 1 1bar 100% CO2 C1018, L80-13Cr – see Table 2 Bubble test, RCE, JI 18 hours (bubble tests and RCE tests), 48 hours (JI tests) 0, 40, 80, 200 and 400 Pa & 10,000 Pa Linear Polarisation Resistance (LPR) Weight-loss unadjusted, measured as 5.1-5.3 under test conditions Table 2: Compositions of the Metals Used in this Project Element C1018 L80-13Cr Composition (%) Composition (%) Aluminium 0.024 Carbon 0.016 0.21 Cobalt 0.016 Chromium 13.03 Copper 0.087 Manganese 0.74 0.53 Molybdenum 0.025 -4- Nitrogen Neodymium Nickel Phosphorus Sulphur Silicon Vanadium 0.013 0.01 0.22 - 0.0308 0.026 0.169 0.015 0.003 0.31 0.019 Analysis LPR measurements were conducted using a two or three electrode setup with a scanning range from – 10 to +10 mV (with respect to the open circuit potential) and a scanning rate of 30 mV/ min with readings taken every 30 minutes over an 18 hour period. Coupon weight loss analysis was carried out on the electrodes used for RCE-LPR and JI-LPR tests following the ASTM standard [7]. JI Shear Stress Calculation The JI test method used is based upon ASTM Standard G208 [5]. This describes how the velocity of the test fluid changes as it radiates out along the test coupon. Near to the jet the flow is largely axial changing rapidly to become parallel to the surface of the test coupon, this region is of little use for correlation to pipe flow conditions so for standard corrosion tests this section is removed (hole of radius 1.5 x the jet radius) and plugged with an inert plastic (PEEK) or epoxy resin flush to the coupon surface. From the point of maximum velocity and minimum jet thickness at approximately 2 radial distances to 4 radial distances the shear stress exerted is mathematically defined as: w 0.1788 U Re 2 0 0.182 r r0 2.0 Where: Re τw ρ U0 r r0 Re υ = = = = = = = 2r0 U 0 wall shear stress (N/m2), density (kg/m3), velocity (m/s) of the flow at the position of leaving the nozzle, distance from stagnation point (m), jet nozzle radius (m), Reynold’s number, and kinematic viscosity (viscosity/density) of the testing liquid (m2/s) The shear stress quoted throughout this report for JI tests is that found at r = 2r0; the point of maximum flow and minimum jet thickness. Results and Discussion 1) C1018 Testing The results for all test conducted with C1018 are summarised in Table 3, below. The corrosion rates (CR) obtained by LPR analysis are given as those measured at the end of the 18 hour test and also averaged over the full duration of the test (Note: test duration ranged from 18 – 48 hours). While the corrosion rate observed after 18 hours is typically used to assess the performance of a corrosion inhibitor in electrochemical corrosion tests, for the purpose of this discussion the average corrosion rate over the entire test duration provides a more direct comparison to that obtained by weight-loss analysis. Shear stresses for the different techniques were selected to provide a direct comparison between test methods in the shear stress region in which they overlap, while also looking at the higher shear stresses capable with jet impingement. -5- Table 3: Summary of Results of C1018 Testing Test Method Shear Stress (Pa) Bubble Test 0 RCE JI Autoclave JI 40 40 80 80 40 40 80 80 200 400 CI Concentration (ppmv) 0 10 30 50 0 30 0 30 0 30 0 30 0 0 10000 0 Corrosion Rate (CR) LPR Weight Loss * 18h Average 5.63 5.06 0.15 0.90 0.05 0.71 0.04 0.64 9.10 8.51 7.41 0.39 1.28 1.32 7.65 8.05 6.15 0.33 1.30 1.30 2.99 3.75 3.12 0.96 1.53 1.37 2.11 3.82 2.55 0.94 1.57 1.52 7.50 7.79 7.50 7.49 7.35 8.16 10.43 9.37 - * Note due to the change in corrosion profiles observed with time the weight loss corrosion rates are compared with the “average” LPR measurements observed throughout the test time. (i) C1018 – LPR Bubble Tests To provide an initial baseline under pseudo-static conditions, LPR bubble tests were conducted with a generic corrosion inhibitor (CI) at a range of concentrations in order to obtain the minimum effective dose (MED) for C1018 steel. The concentrations tested were chosen to be representative of those typically used in practise under these types of conditions. A corrosion rate of ≤ 0.1mm/y was selected as the pass criterion to be achieved at the MED as this is commonly used in laboratory assessments of CI performance, and as a typical acceptable corrosion rate in field applications. The results of these tests are plotted in Figure 4, below, with corrosion rate plotted on a logarithmic scale on the y-axis, against time in hours on the x-axis. -6- A blank test with no CI added gave a final corrosion rate of ca. 5.63 mm/y; the corrosion rate did not vary a great deal over the test with an average corrosion rate of ca. 5.06 mm/y. The CI was then tested at three concentrations; 10, 30 and 50 ppmv. The MED for this chemical was determined to be 30 ppmv, achieving a corrosion rate of ca. 0.05 mm/y at the end of the 18 hour test, corresponding to a ca. 99% reduction in corrosion rate relative to the blank test. It is worth noting that this chemical took approximately 3 hours to achieve a corrosion rate ≤ 0.1 mm/y following addition, indicative of slow formation of the protective layer. (ii) C1018 – RCE Tests Using the MED determined in Part (i) the performance of the corrosion inhibitor was further assessed in RCE tests conducted at 40 and 80 Pa. Blank tests with no CI added were also performed at these shear stresses. The results of these tests are displayed graphically in Figure 5, below. The corrosion rates obtained from the blank tests were very similar at both 40 and 80 Pa with an average corrosion rate of ca. 8.5 and 8.0 mm/y respectively, over the course of the 18 hour test. Comparing the blank RCE tests to that from the bubble tests shows an increase in corrosion rate with increased shear stress under the test conditions; ca. 8 mm/y at increased shear (40 – 80 Pa) vs. 5 mm/y at 0 Pa. However, when comparing the blank RCE tests at 40 and 80 Pa there is very little difference in the corrosion rates observed, suggesting that there is a non-linear relationship between corrosion rate and shear under these conditions. When the CI was employed in the RCE tests at the MED determined in the bubble tests (30 ppmv), final corrosion rates of ca 0.39 and 0.33 mm/y were observed at shear stresses of 40 Pa and 80 Pa, respectively. The concentration tested did not meet the pass criterion under either shear stress, indicating a reduction in CI performance at these moderate shear stresses. As discussed in Part (i), in the static bubble tests the chemical displayed an initial sharp drop in corrosion rate followed by a relatively slow improvement in inhibition at this concentration over the duration of the test. This gradual improvement in performance could be due to numerous factors including the dispersion of the chemical, and the persistency of the film formed. However, in the RCE tests the corrosion rate also displayed a sharp drop 30 minutes after CI addition, but displayed no further reduction over the remainder of these higher shear tests. These results suggest that dispersibility is not the critical factor for the performance of this chemical, but that the increased shear prevents this chemical from building up a more protective layer on the metal surface over time; therefore shear is affecting film formation ability of the tested CI under these conditions. -7- (iii) C1018 - JI Tests Similarly to the RCE tests, JI tests were performed at 40 and 80 Pa in the absence of CI and at the previously determined MED of the CI. Additional tests with no CI present were also performed at 200, 400 and 10000 Pa. Results are displayed graphically in Figure 6, below. At 40 and 80 Pa average corrosion rates of ca. 3.8 mm/y were observed in the blank tests with no chemical present. This is a lower corrosion rate than observed in the RCE tests (8-8.5 mm/y). However, when the tests conducted in the presence of CI are compared then the converse is true; the corrosion rates observed at the end of the 18 hour tests are ca. 0.96 and 0.94 mm/y for the 40 and 80 Pa JI-LPR tests respectively, significantly higher than the equivalents in the RCE tests. This is thought to relate to poorer film adherence under the flow dynamics of the JI system. When higher shear stresses are tested (200 and 400 Pa), the corrosion rate in the absence of any inhibitor increases to ca. 7.5-8.2 mm/y, in the region of those measured in lower shear RCE tests. There is some evidence, both from the electrochemical trends and also post treatment microscopic analysis of the coupons, to suggest that a partially protective corrosion product film may be forming on the C1018 metal surface under the jet impingement flow regime, with initially higher corrosion rates dropping off particularly over the first 2 hours of the tests. This was not apparent in the bubble tests or RCE tests. The difference in flow regimes for the RCE and JI tests may also account for the reduction in performance of the CI when employed in the JI tests. Moving to the extremely high shear 10000 Pa conditions, a further increase in corrosion rate to ca. 9-10 mm/y is observed. The main conclusion is that the electrochemical approaches and the weight loss approaches for the JI set up are internally consistent. The JI data also shows a clear trend of increasing shear leading to increased corrosion but with a generally non-linear approach. The results in terms of corrosion rate appear to plateau at moderate shears, with only a relatively small change observed when moving from approximately 200-400 Pa up to the ultra-high shear 10,000 Pa tests. -8- 2) L80-13Cr Testing The results for all L80-13Cr testing are summarised in Table 4, below. Table 4: Summary of Results of L80-13Cr Testing LPR Corrosion Rate Shear Stress Test Method (Pa) 18h Average Bubble Test 0 0.017 0.014 40 0.021 0.022 RCE 80 0.032 0.031 40 0.12 0.12 JI 80 0.13 0.13 400 0.14 0.17 Autoclave JI 10000 - - Weight Loss CR <0.1 <0.1 0.24 0.08 0.15 0.40 (i) L80-13Cr – Bubble Tests and RCE Tests Bubble tests were initially performed to obtain a pseudo-static baseline corrosion rate. RCE tests were performed at 40 and 80 Pa. The results of these tests are displayed graphically in Figure 6, below, with corrosion rate plotted on a logarithmic scale on the y-axis, against time in hours on the x-axis. As would be expected for a corrosion resistant alloy such as L80-13Cr, these results indicate relatively low corrosion rates for this metal composition at shear stresses up to 80 Pa, significantly less than 0.1 mm/y in all cases. (ii) L80-13Cr – JI Tests JI-LPR tests were performed at 40, 80 and 400 Pa, with the results for these tests displayed graphically in Figure 8, below. -9- JI test results indicate significantly higher corrosion rates for L80-13Cr compared with the RCE testing at equivalent wall shear stresses (40-80 Pa), with average corrosion rates in the region of 0.1-0.2 mm/y compared with ~ 0.02-0.03 mm/y for the RCE approaches. These results could again be attributed to differences of the flow regimes from the two different test methodologies, whereby the JI methodology creates a more severe environment due to the gradient in shear stress across the high shear transition zone caused by the impinging fluid. We consider that for the JI approach the protective films may be damaged due to different flow regimes close to the surface. Moving to the higher shear 400 Pa JI-LPR tests there is no indication of a relationship of increasing corrosion rate with increasing wall shear stress under these conditions, with corrosion rates of 0.1-0.2 mm/y observed, which are still consistent with those observed at 40 and 80 Pa. However, under the extremely high shear 10000 Pa conditions, an increase in corrosion rate to ca. 0.4 mm/y is observed. Summary and Conclusions Due to the need to assess corrosion in challenging environments in oil and gas field applications, a range of techniques have been used and developed to investigate the impact of wall shear stress at a metal surface on corrosion rate. These laboratory tests can provide useful information on the performance of both materials of construction and production chemicals such as corrosion inhibitors, in locations of higher wall shear such as fast flowing fluids in pipelines, particularly at bends and restrictions, and through small orifices such as ICDs and ICVs. Work in this paper has focussed on the development of high shear (200 – 400 Pa) and ultra-high shear (up to 10,000 Pa) JI approaches under both “bubble cell” conditions (ambient pressure, 90°C) and also under HP/HT conditions using specially designed autoclaves. The main aim was to enable high shear measurements to be made under representative flow conditions and to study the effect of shear on corrosion rates and corrosion inhibition for areas of the production system (such as ICD’s and ICV’s) where significantly higher shear regimes exist. In conjunction with this, further developments have been progressed to allow accurate electrochemical measurements to be made under JI conditions allowing more rapid throughput of corrosion measurement, but more critically to obtain information on the kinetic processes relating to corrosion and film formation / film persistence. The results described in this paper illustrate therefore the developments made in the high shear JI and LPT JI methodologies developed in our laboratories. - 10 - For the techniques tested, LPR and weight loss data show good correlation in all test methods, including the high shear JI approaches indicating that both electrochemical and weight loss methods can be applied, providing increased confidence and validation of the accuracy of the electrochemical measurements. This represents a significant benefit due to reduced test durations (typical LPR measurements conducted over a 24 hour time frame compared with 7-28 days for long term weight loss measurements). The JI method appears to be more severe than RCE where equivalent maximum wall shear stresses are examined. This is evidenced by the order of magnitude increase in corrosion rate at equivalent wall shear stresses for L80-13Cr, the initially higher corrosion rates at equivalent wall shear stress for C1018 (subsequently masked by corrosion product film formation), and the poorer CI performance on C1018 under JI test conditions. The increased corrosion rates for the L80-13Cr is suspected to be due to damage to the protective film caused by the fluid dynamics in the JI system whereas the lower corrosion rates initially observed for the C1018 (at lower shears) appears to relate to increased formation of protective carbonate surface films – which again may relate to the fluid dynamics. These aspects are currently being investigated, although it is known from related works that surface scaling can be exacerbated due to the fluid flow regimes within JI approaches [6]. In general the results conclude that although increased shear has a dramatic effect on surface corrosion, the effect is non-linear and is also dependant on the materials. For C1018, maximum corrosion rates plateau at relatively low shear (i.e. increasing surface shear from 200 to 10,000 Pa appears to result in relatively minimal impact on the coverall corrosion rates). For other materials such as L80-13Cr increasing the corrosion rate is still non-linear, but elevated corrosion rates are observed at higher shears (e.g. ~ 0.15 mm/y at 400 Pa increasing to ~ 0.4 mm/y at 10,000 Pa) which is suspected to relate to damage of the protective films. However, when examining corrosion inhibitor performance more dramatic effects are recorded for the cases examined here, with reduced corrosion inhibitor performance recorded at elevated shear. For conventional film forming corrosion inhibitors this is expected, however understanding the corrosion inhibition and film persistency under very high shear regimes remains of considerable interest. Further work is therefore ongoing examining inhibitor performance at increased shear to determine the limits of different classes of film forming inhibitors. Finally this work concludes that laboratory technique selection and an understanding of the flow regimes in the field and laboratory is therefore of critical importance in selecting the test method most applicable to a particular application. In rotating cylinder testing, it is the metal specimen that is rotating at a constant rate relative to the test fluid, proving a uniform flow around the circumference of the test metal, as would be experienced at moderate shears in pipeline flow. In jet impingement the fluid flows through a nozzle and across the face of the test piece, making it more applicable to studies of flow through orifices such as ICDs and ICVs and other very higher shear stresses experienced in and around these devices. The differences recorded between different techniques can be explained both by a combination of localised (surface) fluid flow dynamics and by the effect on surface film formation. Further works are underway to simulate the fluid flow regimes under the different approaches and compare these with a range of field conditions and is expected to be the subject of a forthcoming paper. - 11 - References 1. Palmer, J., Hedges, W. and Dawson, J. eds. A Working Party Report on the Use of Corrosion Inhibitors in Oil and Gas Production. Maney; published for the European Federation of Corrosion on behalf of the Institute of Materials, Minerals and Mining. London, UK, 2004. 2. Kennely, K.J., Hausler, R.H., and Silverman, D.C., eds., Flow-Induced Corrosion: Fundamental Studies and Industry Experience. NACE International, Houston, TX, USA, 1992. 3. ASTM G170-06, Standard Guide for Evaluating and Qualifying Oilfield and Refinery Corrosion Inhibitors in the Laboratory. ASTM International, PA, USA. 4. Demoz, A., Dabros, T., Michaelian, K., Papavinasam, S., and Revie, W., A New Impinging Jet Device for Corrosion Studies. Corrosion: May 2004, Vol. 60, No. 5, pp. 455-464. 5. ASTM G208-12, Standard Practise for Evaluating and Qualifying Oilfield and Refinery Corrosion Inhibitors Using Jet Impingement Apparatus. ASTM International, PA, USA. 6. Graham, G. M., Thomson, H., Bowering, D. and Stalker, R., Correlation of Shear and Turbulence on Scale Formation and Inhibition. SPE 169761 presented at the SPE International Oilfield Scale Conference, Aberdeen, UK, 14-15 May 2014. 7. ASTM G1-03(2011), Standard Practice for Preparing, Cleaning, and Evaluating Corrosion Test Specimens. ASTM International, PA, USA. - 12 -