Technical Article – A Framework for Evaluation of Ultrasonic Corrosion Inspection and Monitoring Strategies for  Large Steel Structures Yifeng Zhang, PhD, and Frederic Cegla, PhD

Technical Article – A Framework for Evaluation of Ultrasonic Corrosion Inspection and Monitoring Strategies for Large Steel Structures Yifeng Zhang, PhD, and Frederic Cegla, PhD

MEET THE AUTHORS

Dr Yifeng Zhang is a Postdoctoral Research Associate in the Non-Destructive Evaluation (NDE) Group at Imperial College London. His work focuses on ultrasonic Structural Health Monitoring (SHM) and inspection technologies that enhance structural integrity and operational efficiency across the energy and petrochemical sectors.

Dr Frederic Cegla is a Reader/Associate Professor in the non-destructive evaluation (NDE) Group at Imperial College London. His research focuses on developing and applying advanced technologies for non-destructive evaluation NDE, SHM, and process monitoring — linking cutting-edge sensing and wave physics with practical solutions for industry.

Introduction: The Challenge of Corrosion Surveillance

Corrosion remains one of the most persistent challenges in managing industrial assets such as power plants, processing facilities, pipelines, and ships. Unlike sudden failures, it develops gradually, often across vast areas and over decades of service.

The result is a degradation process that is both spatially and temporally diverse. Non-destructive evaluation (NDE) techniques such as ultrasonic testing and thickness gauging are widely used to provide critical information that underpins the safety, reliability, and availability of various assets. In practice, it is rarely feasible to perform complete (100%) inspection coverage of large downstream or marine facilities. Instead, inspection areas are typically prioritised using risk-based assessment (RBA) programmes, which focus resources on regions with the highest likelihood or consequence of corrosion Because of these practical constraints, current ultrasonic methods have evolved along two main directions.

Figure 1: Ultrasonic Thickness Measurement Techniques, Trade-Offs Between Spatial Coverage and Temporal Resolution.

Scheduled one-off inspections — often combined with visual assessments and performed using scanning systems — can cover large areas but occur infrequently due to the need for plant shutdowns or limited access [1–2]. In contrast, permanently installed automated monitoring sensors offer improved measurement repeatability and high temporal resolution but are typically deployed only at a few selected locations [3–4] owing to cost and installation complexity.

Towards Hybrid Inspection and Monitoring

Recent advances in robotics and sensor technologies are creating powerful synergies that blur the line between traditional one-off inspection and continuous monitoring. It is envisaged that autonomous robotic platforms will in future manipulate ultrasonic probes across complex geometries, while monitoring sensors will be deployed in hard-to-reach areas that once required significant manual effort.

Prototypes of resident inspection robots — designed to remain on the asset and operate semi-independently — are moving from research labs towards field demonstrations [5-6].

Figure 2: Integration of EMAT With Robotic Platforms (Image Courtesy of The Offshore Robotics for The Certification of Assets (ORCA) Hub, From Research That Led To The Formation of Sonobotics Ltd).

These developments point towards a hybrid surveillance model that combines the strengths of both worlds as part of the agreed inspection programme. For example, resident robots could perform encoded ultrasonic scans across a structure, leaving behind monitoring sensors in critical regions for long-term trending. There, instead of choosing between wide but infrequent inspections and highly localised monitoring, a mixed approach could provide a more complete picture of corrosion progression in both time and space. The opportunities are clear, but so are the challenges. How many robots or sensors are needed to ensure sufficient reliability and compliance with the agreed overall inspection programme? How does the hybrid scheme align with existing approaches? What are the cost implications and likely return on investment? These questions must be addressed before hybrid inspection-monitoring schemes can achieve widespread adoption.

While current best practices for NDT in the energy sector follow established standards such as API 581 and guidance provided
by organisations such as ESR-HOIS, a forward-looking study funded by the UK Research Centre in NDE (RCNDE) explored new methodologies to systematically evaluate and optimise hybrid inspection–monitoring strategies. [7–8]. This article highlights the main findings of the study, introducing a generic framework applicable across diverse industries and corrosion scenarios.

A Framework for Evaluating Hybrid Inspection–Monitoring Schemes

The proposed framework comprises four essential steps, each of which plays a role in simulating how corrosion evolves, how it is measured, and how the acquired data are interpreted.

1.Corrosion Modelling: Capturing the Degradation Process

The framework begins by establishing a model that accurately captures corrosion damage progression. Corrosion manifests differently across industries—from uniform wall thinning in pipelines to localised pitting in offshore structures and complex mixed morphologies in chemical processing facilities. It is recognised that no single model would suffice for all applications, and different scenarios demand models of varying complexity and fidelity.

While corrosion mechanisms vary widely, ultrasonic NDE measurements share a common dependency: the corroded surface profile. Since wave reflection from the corroding surface dictates the characteristics of measured ultrasonic signals, a suitable corrosion model must capture both the relevant surface morphology and its temporal evolution.

This approach decouples electrochemical complexities from NDE simulation requirements, enabling the corrosion model to be readily updated or substituted for different scenarios.

2. Modelling the NDE Technique

The second stage involves accurately representing the NDE method itself. Like all measurement systems, NDE techniques inherently contain errors and uncertainties. For instance, as part of theHOIS Joint Industry Project [9-10], the measurement error and uncertainties of several manual and automated corrosion mapping methods were evaluated, and the findings were found to vary significantly depending on the choice of equipment.

For normal-incidence ultrasonic thickness measurements, the signal depends on multiple factors: transducer characteristics (e.g. size, shape, operating frequency) and surface conditions (e.g. roughness) [11-12]. Signal processing algorithms further influence measurement outputs, with algorithm selection typically based on the expected defect type. Understanding and quantifying these error sources is crucial, as they propagate through to all subsequent analyses and decision-making processes.

While finite-element simulations can accurately capture wave propagation phenomena, their computational demands make statistical analysis of stochastic corrosion processes challenging. Surrogate models — either physics-based or data-driven—offer a practical alternative by balancing computational efficiency with accuracy. These simplified models enable systematic evaluation of NDE techniques while maintaining sufficient fidelity to represent real-world performance.

In practice, multiple models may be required to represent different equipment types, and these can later be integrated and refined as field experience accumulates. Ultimately, the chosen NDE model must reflect the technique’s inherent limitations and uncertainties as encountered in field applications.

xFigure 3: An Overview Of The Proposed Evaluation Framework.

Figure 4: Illustration Of The Ultrasonic Scanning Measurement: Comparison Between The True Underlying Surface And The Thickness Measurement Map Predicted By A Surrogate Model.

 3. Simulation of Data Acquisition Processes

The third stage models the data acquisition process, addressing real-world constraints such as operational access, spatial scanning resolution, limited probe availability, and restricted temporal measurement frequency. By focusing on data subsampling in time and space, the framework accounts for the incomplete nature of field measurements caused by sparse grids, irregular intervals, and missed data points. These constraints ensure a realistic representation of field deployment scenarios, enabling accurate assessments under practical conditions.

4.Defining Metrics of Reliability and Risk

Once simulated data are available, the next step is to establish performance assessment criteria. This involves defining a clear corrosion assessment objective, such as detecting defects above
a specified threshold or tracking the location and extent of the minimum remaining thickness. Ideally this data collection should be combined and reported along with prevailing operating parameters / modes e.g. cyclic operation to provide added value.

Quantitative metrics, such as the probability of detection (POD) or receiver operating characteristic (ROC) analysis, are then applied. These metrics are evaluated on an ensemble of representative surfaces using Monte Carlo-style simulations to assess the effectiveness of various NDE data acquisition techniques and procedures. A proof-of-concept demonstration is detailed in Reference [7], where the objective was set to tracking the minimum remaining thickness within a defined tolerance. The study introduces a metric called the unreliability function (URF) to quantify the reliability of inspection and monitoring schemes. Using an ensemble of realisations that mimic field measurement characteristics, the study evaluates the reliability of three strategies: surface scanning, monitoring with permanently installed sensors, and a hybrid approach combining surface scanning with movable monitoring sensors. For the given scenario, the findings reveal that partial surface scanning followed by sensor repositioning/optimisation creates a hybrid strategy that substantially improves performance despite reduced operational demands: fewer sensors per location, limited coverage, and longer inspection cycles.

Conclusion and Outlook

Although manual inspection will continue to play an essential role in ensuring the structural integrity of critical infrastructure, advances in automation and robotics now make it feasible for an increasing proportion of inspection and monitoring activities to be performed automatically. In practice, adopting a hybrid inspection–monitoring strategy provides a promising means of optimising data collection and enhancing overall asset integrity.

The framework presented here outlines a structured approach
for evaluating hybrid inspection-monitoring schemes that
leverage recent advances in robotics, sensing, and modelling.
By clearly defining the interfaces between corrosion modelling, data acquisition, and performance evaluation, it supports the development of more flexible surveillance methods for industrial assets. Successful implementation requires coordinated efforts among corrosion engineers/scientists, NDE engineers, asset owners, and regulators. Key priorities include adapting models to specific industrial settings, validating performance through field studies, and developing accessible tools for practitioners. This progression from theoretical framework to practical implementation will enhance operational safety, asset availability, and economic efficiency.

References

1. J. Turcotte et al., “Comparison corrosion mapping solutions using phased array, conventional UT and 3D scanners,” 19th World Conference on Non-Destructive Testing (WCNDT 2016), 13-17 June 2016 in Munich, Germany. e-Journal of Nondestructive Testing Vol. 21(7). https://www.ndt.net/?id=19236.

2. V. P. Nikhil et al., “Flaw detection and monitoring over corroded surface through ultrasonic c-scan imaging,” Engineering Research Express, vol. 2 no.1, pp. 015010, jan 2020.
https://doi.org/10.1088/2631-8695/ab618d.

3. F. B. Cegla et al., “High-temperature (>500°c) wall thickness monitoring using dry coupled ultrasonic waveguide transducers,” IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, vol. 58, no. 1, pp. 156–167, 2011. https://doi.org/10.1109/TUFFC.2011.1782.

4. C. H. Zhong et al., “Investigation of Inductively Coupled Ultrasonic Transducer System for NDE”. IEEE Transactions
on Ultrasonics, Ferroelectrics, and Frequency Control, vol.
60, no. 6, pp. 1115–1125, 2013. https://doi.org/10.1109/TUFFC.2013.2674.

5. V. Ivan et al., “Autonomous non-destructive remote robotic inspection of offshore assets,” In Proc. OTC Offshore Technology Conference, May 2020, pp. D011S006R003. https://doi.
org/10.4043/30754-MS.

6. M. D. Silva et al., “Using External Automated Ultrasonic Inspection (C-Scan) for Mapping Internal Corrosion on Offshore Caissons,” In Proc. Offshore Technology Conference Brasil, 2023, pp. D031S033R001. https://doi.org/10.4043/32907-MS.

7. Y. Zhang and F. Cegla, “Quantitative evaluation of the reliability of hybrid corrosion inspection and monitoring approaches,” NDT & E Int., 2025, pp. 103527. https://doi.org/10.1016/j. ndteint.2025.103527.

8. Y. Zhang and F. Cegla, “Mon ami – monitoring and inspection strategy assessment investigation tool”. Accessed: July 18, 2025. https://www.pogo.software/monami/index.html.

9. S. F. Burch, “Precision thickness measurements for corrosion monitoring: initial recommendations and trial results”, HOIS, vol. 11, R3, no. 1, 2011.

10. S. Mark, “HOIS recommended practice for statistical analysis of inspection data – issue 1”, HOIS, 2013.

11. R. Howard and F. Cegla, “The effect of pits of different sizes
on ultrasonic shear wave signals,” in Proc. AIP Conference Proceedings, Aug. 2018, https://doi.org/10.1063/1.5031544.

12. D. Benstock et al., “The influence of surface roughness on ultrasonic thickness measurements”. The Journal of the Acoustical Society of America, 2014, vol. 136, no. 6, pp.3028–3039. https://doi.org/10.1121/1.4900565.

 

Epoxy Passive Fire Protection Over Galvanised Steel

Epoxy Passive Fire Protection Over Galvanised Steel

MEET THE AUTHOR

Chris Fyfe, an ICorr Fellow member, is a senior field auditor and coach at International Paint (a division within AkzoNobel) with over 40 years of experience in protective coatings and corrosion control. He has a strong background in passive fire protection (PFP). He has provided on-site technical support and managed complex fabric maintenance projects within the oil and gas sector. He is a strong advocate for professional development and has championed the training and upskilling of many Epoxy PFP applicators.

1. Introduction

Epoxy Passive Fire Protection (EPFP) systems are safety-critical coatings that are installed in high-hazard process facilities and sometimes also in public buildings. Their requirement is often driven by legislation and are considered of life-safety importance.

Epoxy Passive Fire Protection (EPFP) is designed to insulate critical steel structures from the temperature rise (heat) in a fire event. This safety-critical insulation function slows the temperature rise to maintain structural or pressure retaining integrity, giving time for emergency shutdown, inventory blowdown, and/or safe abandonment. Therefore, correct quality control activities during the whole installation process are critical; this is because the entire system holds a function but ultimately is only as strong as its foundation. For example, when the EPFP is applied to a galvanised surface, the galvanising itself becomes that foundation, and therefore, it’s critical that confidence (quality assurance) is demonstrated.  If the galvanising fails, then the EPFP may become compromised.

Hot-dip galvanising creates a metallurgical bond between zinc and steel. When executed correctly on a properly prepared surface, this bond is incredibly robust. However, several factors in the galvanising process can create a weak and unreliable substrate that may be unsuitable for supporting a safety-critical EPFP system. It is crucial to understand that these issues are not restricted to EPFP alone; they are a fundamental concern for all high-build coating systems that rely on a strong foundation to function. An example of galvanised steel section with EPFP applied is shown below in Photo 1.

This article will explore:

1. The inherent risks associated with galvanising including excessive thickness, metallurgical defects, and inadequate repair methods that can compromise the bond and ultimately could detract from the overall durability of the system.

2. This article will argue that the best practice is the direct application of EPFP paint systems to properly prepared steel substrates as a correctly installed EPFP system can give a comparable durability range. Therefore, galvanising should only be considered as a substrate for EPFP when there are no other design options available, and even then, only with additional (stringent) quality control measures that may go beyond typical industry/project expectations. This article will explore the inherent risks associated with galvanising including excessive thickness, metallurgical defects, and inadequate repair methods that can compromise the bond and ultimately could detract from the overall durability of the system.

2. The Challenge with Galvanising

The ability of a galvanised coating to support an EPFP system can be severely impaired by several influencing factors:

Excessive galvanising thickness: The primary source of impairment.

Metallurgical defects: Inclusions and weak layers that may form during the galvanising process.

Poor bonding: Initial or Inadequate surface preparation leading to a weak bond.

Surface passivation: Post-galvanising treatments that can impair adhesion.

The “Thicker is Better” Concept

Standard galvanising specifications like ISO 1461 and ASTM A123 are written with no consideration that EPFP system may also get specified and are typically for corrosion protection, they do not consider any additional thick film coating such a EPFP system.

They often imply that exceeding the minimum with no consideration to maximum thickness is not a cause for concern. However, for EPFP applications, this is a dangerous misleading understanding. Experience has shown that as a galvanised coating thickness increases, its cohesive strength may decrease. The primary drivers for this excessive growth are the chemical composition of the steel—typically its silicon (Si) and phosphorus (P) content—and the thermal mass of the steel section [2].

High Silicon and Phosphorus Content: Steel with high levels of silicon (particularly in the range of 0.04% to 0.14%, known as the “Sandelin range”) and phosphorus accelerates the growth of the zinc-iron alloy layers (eta, zeta, and delta).

Uncontrolled Growth: Rapid growth results in a thick, brittle, and often friable zeta layer. Instead of a dense, tightly bonded coating, there is an increasing likelihood that a coarse crystalline structure which is inherently weak may result.

Therefore, a galvanised coating that is too thick—for example, exceeding 250 µm (microns)—may not be robust when coated with thick EPFP coatings. It may have micro-cracks and a high degree of internal stress resulting in voids and weak layers. When the EPFP is applied over this type of surface, the galvanised layer itself can delaminate due to stress imparted by the EPFP.

3.Setting Strict Limits

Therefore, a robust, well-written project specification should consider the standard galvanising process and procedure but, in addition, set its own quality control and quality assurance requirements. The following limits should be considered important:

Upper Galvanising Limit: The galvanising thickness must be strictly controlled. Any measurements exceeding 250 µm should trigger a formal integrity assessment. Sections with thicknesses greater than 250-400 µm should be quarantined until additional quality control testing can give assurance of acceptability. This includes but is not limited to. Adhesion testing using both internationally recognised standards and EPFP manufacturers’ recommended procedures.

Mill Test Certificates: Engineers and specifiers should always review the steel’s Mill Test Certificate (MTC) at the design stage. An MTC (specifically a Type 3.1 certificate as per ISO 10474) provides a detailed chemical breakdown. If the silicon and phosphorus levels are high, excessive galvanising growth could be considered predictable, and the required additional inspection protocols can then be implemented by the engineer early at the galvaniser’s facility.

4.Defects Which Could Impair Performance

Defects within the galvanising layer that may create points of failure.

• Ash and Dross Inclusions: Ash (zinc oxide from the zinc bath surface) and dross (iron-zinc particles from the bath bottom) can become entrapped in the coating. These inclusions can be poorly bonded, creating an area of instant non-adhesion for the primer and EPFP [3].


5.Process Factors which Could Impair Performance

Properties at the surface of the galvanising layer that may create immediate points of failure.

Passivation and Quenching: Post-treatment of galvanised surfaces with chromates or water quenching is common. Water quenching creates a thin, weak layer of zinc oxides and hydroxides on the surface. Chromate treatments are often used for aesthetics.This layer is completely unsuitable for coating adhesion and should be prohibited in the project specification. Any steel that has been water-quenched should be rejected before an EPFP application.

Use of Cold Spray Repair Compounds: Where surface defects are observed by the galvaniser, cold spray repair compounds may be used to improve the aesthetic appearance of the galvanising.

Note. These repair compounds are not compatible with EPFP systems and may lead to coating system delamination. Any items where cold spray repair compounds have been used should be rejected prior to EPFP system application.

6.High Film Builds: A Closer Look at the Implications

When a thick-film material like EPFP is applied over a cohesively weak galvanised layer, several critical issues could materialise.

1. Adhesion Failure: The primer for the EPFP system cannot achieve a proper bond to a galvanised surface which is contaminated with weak oxide layers or has incompatible treatments applied. The failure point is within the incompatible treatment in the case of cold spray repair compounds or between the primer and the galvanised steel.

2. Internal Stress: The EPFP can induce stress during cure, and a brittle or weak, over-thick layer may crack or delaminate.

7. Remedial Actions: No Half Measures

When non-conformances are found, the remedial actions need to be appropriate to the EPFP system application. The goal is not to “repair” the galvanising in the traditional sense but to create a sound substrate for the EPFP.

1. Quarantined: For issues like water quenching or thickness exceeding 250 µm to 400 µm, the section should be quarantined. Until quality assurance can be demonstrated.

2. Thorough blasting with appropriate media: For sections with excessive thickness (250 µm – 400 µm) or surface defects like ash, the only acceptable method of repair is to aggressively abrasive blast. The goal of a “sweep blast” is not merely to create a profile; it is to remove the defective and friable outer layers of the galvanising until a sound adherent zinc layer is exposed. If this means blasting through to harder alloy layers in localised areas, then the justification can be presented: “Lifetime expectation is met by the application of the EPFP system.” However, this must be brought to the client’s attention as a technical or engineering query, as it fundamentally changes the specification requirement.

3. Stop Inadequate Repairs: Standard galvanising repair methods, such as cold spray repair compounds detailed in standards like ASTM A780, or the use of zinc-based solders (“zinc sticks”), should not be accepted for surfaces receiving EPFP. These repairs do not possess the cohesive strength or compatibility with the EPFP system and could create a point of failure.

All galvanised steel specified for EPFP application should always be sweep blasted to remove surface contaminants and any weak oxide layer, providing an angular profile of 50-75 µm for the EPFP system to anchor against. This should be stated clearly in the specification.

8. Conclusion: A Call for Best Practice

The industry must shift its mindset. Applying EPFP over hot-dip galvanising introduces significant, unnecessary risk to a facility’s most critical safety infrastructure. The default specification should always be EPFP applied directly to appropriately primed steel prepared to the EPFP manufacturer’s requirements.

When galvanising is unavoidable, it must not be treated as a finished product but as a substrate in need of quality control and further preparation for the EPFP system.

To achieve a safe and reliable outcome, the following actions should be considered essential.

Early Intervention: Review mill test certificates at the project’s outset to identify reactive steels and plan for heightened inspection.

Specify Correctly: Write a detailed coating specification that explicitly prohibits water quenching and surface treatments and defines strict lower and upper thickness limits for the galvanising coating.

Mandatory Surface Preparation: Mandate that all galvanised surfaces receive an aggressive sweep blast to remove weak layers and create a suitable surface profile before priming.

Consult the Experts: Engage the EPFP manufacturer at the design stage to assist with specifications and inspection test plans (ITPs).

By prioritising the integrity of the substrate, we can ensure that these vital safety systems perform as designed, protecting assets, the environment, and, most importantly, lives.

References

1. https://www.glorysteelwork.com/2024/05/07/causes-and-control-methods-of-hot-dip-galvanizing-surface defects/#:~:text=If%20there%20are%20more%20active,layer%20grow%20rapidly%20and%20push.

2. Kestler., C. E. (n.d.). The Galvalume Sheet Manufacturing Process. In C. E. Kestler., The Galvalume Sheet Manufacturing Process.

3. https://steelprogroup.com/galvanized-steel/finish/defects-and-treatment/#:~:text=Ash%20staining%20is%20caused%20by,dipping%2C%20leaving%20a%20grayish%20stain.

A Critical Assessment of The Half-Life  Ageing Term and Failure to Predict  Future Galvanic Anode Behaviour

A Critical Assessment of The Half-Life Ageing Term and Failure to Predict Future Galvanic Anode Behaviour

Meet The Authors

Christian Stone, M.S., M.Phys., is a corrosion scientist and technical expert at Concrete Preservation Technologies (CPT) who specialises in the development of next-generation corrosion management systems, supports the use of cathodic protection worldwide, and is a leading expert in corrosion in RAAC concrete. Christian sits on a number of professional organisations, is a member of the Loughborough University RAAC Research Team and is currently undertaking further research on RAAC with Loughborough University.

Gareth Glass is a Director at Concrete Preservation Technologies (CPT), a position he has held since the inception of the company in 2005.  He has extensive experience in materials technology, durability and rehabilitation of structures with over 100 publications to his name in the area of corrosion protection. He obtained his PhD from the Corrosion and Protection Centre, University of Manchester.

Introduction

The term ‘ageing factor’ (sometimes referred to as ‘ageing constant’) for galvanic Anodes, was first coined by Sergi et al in ‘Monitoring results of galvanic anodes in steel reinforced concrete over 20 years’ in Construction and Building Materials, 2020 [1]. The principle behind this idea is that discrete measurements of galvanic current data from precast anode systems, when plotted on a logarithmic graph, could be fitted with a straight line. Therefore, they claim that their anodes exhibit a ‘half-life’ model with the current trending to zero, halving over set time intervals, the ‘ageing factor’. They further claim that when the anodic current density falls below a threshold, the anodes no longer adequately protect the steel reinforcement.

Modelling – Apparent Discrepancies

The first site analysed by Sergi et al. was a bridge in Leicester; current was measured. approximately 26 times for 12 individual patch-anodes from a single patch over 20 years. The initial description of the anodic current describes three distinct stages of relatively stable current output, each below the prior level: 0-6 years, 7-14 years and 15-20 years. This was described, at least in part, due to a drop in pH of the pore solution of the electrolyte. A half-life ageing constant of approximately 7 years over which the current would half was then generated by the plotting of the current readings on a logarithmic scale and a straight line being fit to the data [1]. The reason for the choice of a logarithmic scale is not fully explained, with decreases in surface area and depletion of lithium hydroxide being cited.

This concept was furthered in the next year in the Journal of Building Engineering (June 2021) [3], at the Corrosion Conference (November 2021) [4], Structural Faults and Repair Conference (2022), an ICRI webinar, ’Design Considerations for Galvanic Anodes’ (December 2022) [5], in the book Life-Cycle of Structures and Infrastructure Systems [6], and 3rd Conference & Expo Genoa (2024) [7]. Throughout these publications, ‘ageing factors’ were published for approximately 12 elements using precast Vector Corrosion Technologies (VCT) anodes and their precast precursors, and included both site and laboratory data. Of particular note was the ICRI webinar and the AMPP Italy Corrosion Conference white paper, where the half-life style ‘ageing-factor’ hypothesis was applied to non-precast anodes manufactured by other companies, including Concrete Preservation Technologies (CPT) and an ‘ageing factor’ was published for CPT’s hybrid anode, one that is initially powered externally before being wired galvanically, the DuoGuardTM anode system [5,7]. The predicted ‘ageing constant’ published for these anodes was 2.9 years, and was compared unfavourably to the 11 year ‘ageing factor’ for their own products.

There were however, some significant changes made to use of this empirical model. Rather than being a model for some precast patch anodes manufactured by a single company and their precursor anodes the hypothesis was now being applied to anode arrays cast with a different geometry, embedded in a different cementitious material, located in the host concrete rather than a patch, and very importantly not activated using the same chemistry that was cited as a major cause of the exponential decay in the original paper [1]. DuoGuardTM is activated chemically in such a way that the activator is not depleted but recycled, continually drawn back to the anode. Therefore, the theoretical underpinnings cited by the authors do not appear to hold for these anodes. This has led to the need for a closer look at this model and whether it can tell us anything about the behaviour of these anode systems or whether the model can reliably predict the behaviour of CPT anodes.

In order to understand this model, it is important to first explore the stated and hidden axioms behind the hypothesis and how these lead Sergi, Whitmore and others to interpret their data in such a way. In this section, we will place to one side the fact that there is no stated theoretical underpinning to the choice of a logarithmic scale and allow for the strength of the predicted current data to judge
its veracity.

Half-Life Theory Axiom – There is A Set, Minimum Current Threshold For the Protection of Steel In Concrete

The corrosion risk of steel is due to its environment. This should be a relatively uncontroversial statement, as it is known that steel in fresh concrete is passive and requires no cathodic protection, and steel in carbonated concrete has a lower corrosion rate on average than steel in chloride-rich environments [8]. Furthermore, corrosion rates can vary due to the exposure to moisture, availability of oxygen and be changed by coatings applied to the steel. It is therefore reasonable to assume that the amount of protection steel in concrete requires for protection is a product of its environment.

Although the authors do acknowledge the importance of chloride in the amount of current needed to protect steel in concrete [7], they ignore many of the other factors. This inherent complexity is why it is often much easier to measure changes in the steel due to protection rather than purely the current output of the system. Such measurements are common with impressed current cathodic protection (ICCP) systems that use ISO 12696:2021 [9], which gives steel potentials in the immune region and polarisation held in the steel. originating from Mixed Potential Theory [10,11], as criteria for protection. Within galvanic cathodic protection (GCP), it is  common to track the depolarised steel potentials [12] to measure changes in corrosion risk, polarisation [13] and corrosion rates [14,15]. These measure the effect of the anodes on the steel rather than the output alone to determine the level of protection achieved.

Comparison of Anode Systems

This is further complicated by the fact that some anode systems are installed in different ways, leading to varied current spread. It matters very little how much current an anode produces if it is not reaching the at-risk steel it is installed to protect. To explain this concept more clearly, two anode systems for patch repair will be compared: a precast anode designed to be tied onto the reinforcement in a patch and a patch anode that is installed into a putty in the periphery of the patch, away from a single steel rebar. Below CPTs precast anode RebaGuardTM and drilled anodes PatchGuardTM can be seen. RebaGuardTM is similar to the anodes installed in many of the author’s works.

The steel being protected by patch anodes is the steel outside of the patch, as the steel in the patch is in fresh, alkaline, contaminant-free concrete. The precast anodes are tied to the steel within the patch. It is not difficult to see that it is likely that a large portion of the current will take the easiest path between the zinc and the steel, to the reinforcement onto which it is tied. The current that does exit the patch must avoid taking the easiest path, passing through the interface between the patch and the host concrete, which will have a resistance and spread to the steel outside of the patch which is at some distance from the anodes. These anodes can and do work, but it is unlikely that all the current they produce is available to the steel they are protecting.

The PatchGuardTM anode is installed into the periphery of the patch, in the host concrete into a conductive putty, much closer to the steel it is designed to protect. Unlike the precast anodes, it is not tied to a single reinforcement, and the current will therefore more easily spread to the at-risk reinforcement. Furthermore, due to the increased resistivity of most patch materials and the resistive interface of the patch making current flow into the patch more difficult, it will favour passing current to the steel outside the patch rather than within the patch. It is therefore logical to think that the current from this PatchGuardTM anode will protect the rebar much more efficiently than the precast anode. Having the same current requirement for each of these anodes is illogical.

The validity of their threshold may be tested using the author’s data. The first work published in this series was the 20-year data from a ‘bridge in Leicester’ [1]. This site is a site which staff at CPT is quite familiar, and many senior members of staff were present at the installation of these anodes. Though the paper claims that after 20 years that the anodes are reaching the end of their life, with the current output dropping under their threshold for protection at approximately 14.5 years. In a statement to the Cathodic Protection Association (CPA) from March 2023 by CPT [16], it was shown that in 2015, ten years after the installation of the anodes, there was cracking in the element following the line of the reinforcement extending from the repairs. This is not a measure of success in a galvanic anode system and shows a flaw in their current threshold.

Potential Measurement Error – Taking Current Data From A Responsive System

One of the most important concepts with galvanic anodes is their responsive behaviour [17,18]. The driving voltage, as long as the anodes are activated, is due to the galvanic series and therefore can be approximated as constant; the current delivered to the steel is therefore largely dependent on the resistivity of the electrolyte in the circuit, the concrete. So, when the concrete is wet, full of ions, warm, etc, the circuit has a lower resistance and the cell between the zinc and the steel produces a higher current. This is a part of the draw of these anode systems as they give a level of protection which changes with the corrosion risk of the environment.

One of the issues that comes with this fluctuation in current is that when the anode currents are measured infrequently without other corresponding data, such as the weather. Steel polarisation or natural steel potentials – the data can be misleading. Currents taken on wet and warm days may be much larger than those taken on dry and cool days, which can make seeing trends in current output difficult, unless Adequate data is collected.

Furthermore, anodes installed into wet patches, or into slow-curing putties may have initial currents which are atypical due to the moisture surrounding the anode, decreasing the resistance between the zinc and the steel. In CPT’s anode systems, the putty may take many years to cure, a design feature to initially provide a larger current to aid in the passivation of the steel due to the reduction reactions at the steel surface producing hydroxide ions.

This ageing constant generated for CPT DuoGuard anodes was created from a few data points using anodic current data from
only the first nine years of the galvanic protection [7]. This was during the period when the putty was curing. This may have led
to some inaccuracies in predicting the long-term behaviour of these anodes.

Whiteadder Bridge – Duoguard Hybrid
Anode System CASE Study

The data used by Sergi et al to calculate the ageing factor for DuoGuardTM anodes was taken from data published from Whiteadder Bridge in the UK [17].Here, two zones of anodes
were installed within a proprietary putty in regularly spaced,
drilled holes, and wired together to form arrays which protect the upper and lower portions of the structural element supporting the span of the bridge over a river. The anodes were installed to counteract the corrosion issues caused by de-icing salts and moisture ingress, including tidal flooding of the river.

The anodes were initially powered until at least 50kC of charge had been passed for every square meter of steel surface area to realkalise the steel environment, utilising the zinc’s ability to pass much higher currents than MMO titanium anodes when powered, and then connected directly to the steel via a junction box. Reference electrodes were installed in the zones, and the current output of the anodes alongside the reference potentials were measured by a data logger installed in an enclosure. This gives a constant stream of data, far in excess of those sites of similar ages used in the work by Sergi and Whitmore.

The element has been protected for 18.5 years now without the need for any maintenance beyond the replacement of SIM cards in the enclosure which transmit the data wirelessly to our office, and has been monitored with over 100,000 data points collected over the first 17.5 years of protection in each zone and over 1,000,000 data points collected in sum. The data used for the predicted 2.9-year ageing factor found in the AMPP Italy white paper [7] was taken from the first 9 years of data [17], which was not the most recent publicly available data set at the time [18] and appears to include only a small number of data points. It is unclear how these data points were selected. Due to the initial charging of the anodes, the authors claim that it would be expected that such anodes would likely have a decreased life due to having to pass a large amount of current early in their design life [7].

Although this model is now used in specifications and design documents worldwide, this will be the first predictive test of their empirical model and, importantly, a test of whether this model can be applied to anodes other than their own, for which they likely have a greater abundance of data. The aim of the following section is to analyse the predictive power of this model using data from the CPT site used in their analysis using the most recent data collected which presumably they had little access to.

Site Data – Responsive Behaviour

Below are the current and the polarised steel potentials for the lower zone of anodes installed on Whiteadder Bridge above, the same data used in the author’s work [7,17], but now with an additional 8 years of data. The red line is the galvanic current data showing the characteristic responsive behaviour with currents rising and falling in yearly cycles due to temperature changes and peaking during periods of increased moisture due to rainfall or flooding. This supports the theory that current is being driven in these anodes due to changes in resistance in the concrete electrolyte. The blue line is the polarised steel potential. When the current increases, we see a corresponding peak in the steel potential as the current generates a polarisation in the steel. Polarisation is a sign of steel passivity, with more passive steel polarising more easily than corroding steel. A green line has been added to show that over time the steel potentials are trending less negative, an indication of increased steel passivity.

The first few years of the data do show an increased current output from the anodes. As was previously stated, this is likely due to the putty into which the anodes were installed curing. After this period, the current appears to become more stable and respond to changes in resistivity from a relatively stable baseline. Taking a closer look at the data from around 9 years after installation, we can see the current from both zones increases due to fluctuations in temperature during the day as well as throughout the year. This response to corrosion risk with increased protection is one of the hallmarks of a naturally smart corrosion management system that is driven by electrochemistry.

After flooding and rainfall, we can see that not only does the current increase due to the moisture ingress, but it also falls slowly as the moisture evaporates, leading to increased protection during the entire period of increased risk. Furthermore, some of the peaks in current seen during periods of increased moisture are larger than

the initial anode current, indicating that the current output is not being primarily driven by a build up of corrosion products or a depletion in activator for these systems but a reaction to the environment and the corrosion risk.

Testing he Predictive Power of The Half-Life ‘Ageing Factor’

In order to test the predictive power of the model, we must choose a null hypothesis against which it will be compared. The simplest null hypothesis would be that the median current the system was producing between 8 and 9 years, the last year of the data set utilised by the authors, stays constant. This appears to be a fair null hypothesis to test their predicted values against, as one predicts a decrease and the other predicts no decrease in current.

The authors published a half-life ‘ageing factor’ of 2.9 years, where the current halves every 2.9 year period. Here we have plotted the predicted values for each hypothesis against the data collected from the site during the period from year 8 to year 17, approximately 3 ageing factors or an expectation that the current, if the model is correct, will fall by more than 87.5%. A log current graph was chosen to transcribe the half-life model data into a straight line in a similar fashion to that employed by Sergi in
his work.

As can clearly be seen, the values predicted by the ‘ageing factor’ model (red) diverge from those measured on site over time, whereas the constant current model fits the data much more closely. This becomes evident when the mean squared error (MSE) of each predicted data set is measured; with the half-life hypothesis having an MSE of 0.237 mA2 and the MSE of a simple constant value
model being 0.0135 mA2, an order of magnitude smaller.

The error is likely due to a misunderstanding of how these anodes will behave differently over time due to their activation chemistry and presuming that the same methodology should be employed without testing other hypotheses, leading to the authors choosing to fit the same exponential decay that fit their own data. A simple change in their methodology to presume an exponential decay overlaying a more stable pattern can lead to a much better fit in the data and a lower MSE over the previously available data.

Below is an empirical model presuming a decay plus a constant current calculated using the first 9 years of data only. It should be noted that this is not a lifetime predictive model for these anodes, which will depend on many factors, as the anodes will not continue protecting the steel indefinitely and it is expected that when the volume of the anodes reduces beyond a threshold the ratio of zinc to steel surface areas will be insufficient to pass the same current. This fact in included in the design calculations of these anode systems. This is also not an endorsement of current being used as a benchmark for anode performance. However, as around 7% of the anodes on this site have currently been consumed, in the lifetime provided for this system it is unlikely to reach this threshold and this basic model may suffice, depending on environmental conditions. Therefore, over this limited time period, a relatively stable current may be used as changes in surface areas are relatively slow due to the anode geometry chosen by CPT and the activator should continue to keep the zinc active. An initial period of higher current due to the resistivity drop from the curing of the putty is also included in this limited model.

We believe that much of the error in the predicted value of the ageing term is due to the presumption that the overall behaviour would be similar. However, the difference in the activators used to keep the anodes active may lead to differing behaviour giving precast anodes an exponential decay of current to zero. This depletion in their activator, may lead to the amount of protection being in a large part dependent not on the amount of zinc but rather on the amount of activator utilised. Activators such as lithium hydroxide are consumed, may be leached away from the anodes, and carbonate after manufacture. Anodes activated in similar ways to PatchGuardTM and DuoGuardTM are likely to age very differently, as the availability of activator will not deplete in the same fashion and are therefore unlikely to show the same ageing characteristics. This can be seen clearly by calculating their hypothetical ageing constant using the data from years 8-17 using the same method as Sergi et al. Here we calculate the ageing constant over which the current is halved to be over 36,000 years. This is plainly absurd, as the zinc will be completely depleted after around 100-250 years. The underlying ageing of CPT anodes is therefore very unlikely to be exponential in nature.

Conclusions

It is clear from this data that the major factor driving the current output of CPT’s discrete anodes, is changes in the resistivity of the environment. After 17 years, the current was still responding strongly to changes in moisture, producing currents in excess of the median galvanic current from the first year of installation when moisture ingress reduces the resistivity of the environment. Precast anodes, such as the type used in the creation of the half-life model, may also be limited by a second factor, the depletion of their activator. This is concerning as these anode types are very popular worldwide and are often sold based on a mass of zinc, when, without sufficient activator, that mass of zinc will not be fully utilised. With lithium hydroxide as an activator, the mass of the activator would likely need to be much greater than the mass of zinc. It is likely, therefore, that only a portion of these anodes will be sufficiently activated before the current declines substantially.

Due to the depletion of activator, some form of ageing term may well apply to VCT style products as stated by their authors. However, due to this hypothesis failing to accurately predict the behaviour of other anode systems, it should be avoided in all specification documents as it may be unique to a certain set of products. It is important to ensure that clients are getting the same level of protection from anodes sold as equivalents in the market.

References

[1] G. Sergi, G. Seneviratne, D. Simpson, Monitoring results of galvanic anodes in steel reinforced concrete over 20 years, Construction and Building Materials, Volume 269, 2021, 121309, ISSN 0950- 618, https://doi.org/10.1016/j.conbuildmat.2020.121309.

[2] G. Sergi, Galvanic Corrosion Control of Reinforced Concrete: Lessons Learnt from 20 Years of Site Trials, ICorr presentation, Aberdeen, 30/03/2021, https://www.icorr.org/wp- content/uploads/2021/06/2021-03-30-ICorr-Aberdeen-Event-ICorr-Aberdeen-Presentation-30-03-21- Dr-George-Sergi-Vector-Corrosion.pdf 2021.

[3] G. Sergi, G. Seneviratne, D. Simpson, Monitoring results of galvanic anodes in steel reinforced concrete over 20 years, Construction & Building Materials, 269, 121309 2021.

[4] D. Whitmore, G. Sergi, Long-term monitoring provides data required to predict performance and perform intelligent design of galvanic corrosion control systems for reinforced concrete structures, Corrosion 2021, AMPP, Paper No. 16792, 2021.

[5] D. Whitmore, Design Considerations for Galvanic Anodes, ICRI webinar, December 2022.

6] G. Sergi, Life extension of existing steel reinforced structures by simple cathodic protection techniques for sustainable durability, Life-Cycle of Structures and Infrastructure Systems – Biondini & Frangopol (Eds), ISBN 978-1-003-32302-0 2023.

[7] G. Sergi, P. McCloskey, D. Simpson, Long-term performance of galvanic anodes for steel reinforced concrete, 3rd Conference & Expo Genoa 2024, AMPP Italy,https://www.vector- corrosion.com/assets/page_renderer/Sergi_George-Extended_Abstract.pdf, 2024.

[8] L. Bertolini, B. Elsener, P. Pedeferri, & R. Polder, Corrosion of Steel in Concrete: Prevention,Diagnosis, Repair. Corrosion of Steel in Concrete: Prevention, Diagnosis, Repair, 1–392. 2005 https://doi.org/10.1002/3527603379.

[9] ISO BS EN 12696:2022.

[10] G. K. Glass, A. M. Hassanein, N. R. Buenfeld, Monitoring the passivation of steel in concrete induced by cathodic protection, Corrosion Science, Vol. 39, No. 8, pp. 1451-1458, 1997.

[11] C. Stone, G. K. Glass, Assessment Criteria For The Electrochemical Protection Of Steel, Australasian Corrosion Association Conference, Cairns, November 2024.

[12] Standard Test Method for Corrosion Potentials of Uncoated Reinforcing Steel in Concrete, ASTM C876 22b, October 2022[11] National Highways 5700 Series.

[13] C. Christodoulou, C Goodier, S. A. Austin. Site performance of galvanic anodes in concrete repairs. Concrete Solutions-Proceedings of Concrete Solutions, 5th International Conference on Concrete Repair 2014 Aug 18 (pp. 167-172). 2014.

[14] Corrosion of steel in concrete: investigation and assessment, BRE Digest 444, 2000, ISBN 860813615.

[15] Electrochemical tests for reinforcement corrosion, Concrete Society Technical Report 60, 2024.

[16] G. K. Glass, Statement to the Cathodic Protection Association, SCA technical Meeting, March2023.

[17] D. Bewley, High-power, low-maintenance, hybrid corrosion protection, Bridge construction and repair, Concrete, Oct 2016, pp. 25-27 2016.

[18] D. Bewley, C. Stone, Long-term monitoring of innovative corrosion control system yields fascinating results, Concrete, Volume 57, Issue 5 June 2023.

Editor’s Note

This Journal provides a platform to all to present their investigations and research. It is not the intention to endorse particular products and readers must satisfy themselves in regard to their applicability and their particular needs.

200 Years On: Sir Humphry Davy and Cathodic Protection

200 Years On: Sir Humphry Davy and Cathodic Protection

Meet The Authors

Dr Bruce Ackland obtained a Bachelor of Science with Honours in Physics in 1979 and a Doctor of Philosophy in 1984 from Monash University, in the Department of Materials Engineering. Bruce has worked in the corrosion and cathodic protection industry since 1982, forming Bruce Ackland and Associates in 1985. Cathodic protection projects have involved work throughout Australia, New Zealand, Asia, SE Asia, the Middle East, North Africa and the USA. Bruce maintains an active role as a member and chairman in Australian Standards committees, participates in relevant ISO standards working groups, is the current chairman of the Australian Electrolysis Committee and is an accredited ACA Corrosion Technologist.

Dr Kathryn Dylejko is a corrosion engineer based in Australia at the Defence Science and Technology Group, specialising in minimising and controlling corrosion on Navy platforms. With roots as a mechanical engineer in armoured vehicles since 2006, she transitioned to corrosion 12 years ago, leveraging computational modelling to optimise cathodic protection systems for Navy vessels. Kate’s expertise spans various facets of corrosion, with a keen focus on cathodic protection systems for maritime platforms. Her research includes electrochemical studies on calcareous deposits and corrosion potential monitoring across Navy vessels and wharves. Actively contributing to the Victorian branch of the Australasian Corrosion Association, Kate recently achieved certification as an AMPP CP2 Cathodic Protection Technician, reinforcing her commitment to advancing the practice of corrosion control technologies.

Dr Markus Büchler FICorr, is Director of the Swiss Society for Corrosion Protection, President of the European Committee for the Study of Corrosion and Protection of Pipes and Pipelines Systems (CEOCOR), and convenor of ISO TC 156 WG10 on cathodic protection of buried and immersed metallic structures.

 

 

Introduction

The year 2024 marks the 200th anniversary of the first two of three remarkable papers [1-3] by Sir Humphry Davy describing the earliest scientific investigations into what we now call cathodic protection (CP). Although the word “cathode” was not in use until proposed by Michael Faraday in 1834 [4], this paper will keep using the modern abbreviation “CP” for convenience. Similarly, Faraday also proposed using the word “anode” in his 1834 paper and we will call the anodic metals used by Davy as anodes, rather than “protectors”. 

Davy presented three seminal papers to the Royal Society in London, beginning with his first on January 22, 1824 [1] giving the scientific reasons, background and laboratory research results for the application of CP to prevent corrosion of copper sheeting on timber ships in seawater. His second paper describing additional experiments and observations for copper sheeting on vessels in Chatham and Portsmouth Navy dockyards was presented on June 17, 1824 [2] and his third paper detailing full scale research and results for ships on the high seas was read on June 9, 1825 [3].

There was controversy then, as there is now, about some aspects of Davy’s work  [5, 6]. This paper discusses some of these issues and demonstrates that Davy was well aware of any shortcomings but importantly, he also suggested possible solutions to overcome the occasional problem of an increase in fouling of the copper sheet under specific circumstances [3, 7]. Notably, the application worked unambiguously to prevent corrosion of the copper in all cases, with fouling only occurring on some vessels and Davy was in the process of understanding the differences in operational circumstances. It will be shown that it was primarily a loss in funding and a wish by the British Admiralty (after pressure from some ship’s captains and the media) for quick solutions that cut short further investigatory work after just two years (i.e. 1823 to 1825). It was left to future scientists and engineers to show how CP could be used effectively and efficiently to protect any metal or alloy immersed in an electrolyte, including even reinforced concrete [8]. When reviewing his work, it must be seen in the context of the scientific understanding of electrochemical processes at the time. For instance, Davy was able to formulate the principles and application of CP decades before the electron was discovered by J.J. Thomson in 1897 and long before chemical and electrochemical reactions were written in the format used today. Judging his discoveries against modern principles is unfair at best and anyway, he was spot-on about plenty of technical points, as will be seen.

Previous Discoveries Leading to Davy’s Understanding of Electrochemical Processes and “Cathodic Protection”

Humphry Davy quickly adopted and contributed to the electrochemical technology developed by luminaries such as Luigi Galvani [9],  Alessandro Volta [10], Nicholson and Carlisle [11] and others. An example of the terrific electrical power he was able to produce can be seen in Figure 1 which shows the battery banks below a lecture theatre where he was demonstrating electric arc lighting. The portrait of Davy in Figure 2 includes a typical Voltaic pile (typically consisting of alternating stacks of brine-soaked cards sandwiched between pieces of copper and zinc or other combinations of dissimilar metals), a common feature in portraits of electrochemical scientists.

This background placed Davy in a perfect position to investigate a costly corrosion issue for the British Navy. In 1822, Davy was first approached by the British Navy Board to provide advice regarding the corrosion of copper sheeting on the Royal Navy’s timber ships [5]. The copper sheeting was effective at protecting the ships’ timber from worms and preventing the growth of “weeds” which otherwise had the effect of slowing the ships movement through the water. Davy read the board’s letter to the Council of the Royal Society of which Davy was President. The Council formed a committee (with Davy as President) to investigate the matter and decided to test copper specimens supplied by the Navy. Davy eventually dispensed with the committee and began working personally on the problem in 1823, reported directly to the Admiralty on 17th January 1824 and then read a groundbreaking paper to the Royal Society on 22th January 1824.

Davy’s Paper of January 22nd, 1824

This, Davy’s first paper on CP, proves the ability of CP to prevent corrosion. There may well be other consequences, but the beneficial effect upon corrosion was unambiguously proven and is not in dispute.

Let’s look at some of the key issues raised in this first paper:

Davy, along with his assistant Michael Faraday, proved incorrect the general supposition at the time that the “rapid decay” (i.e. corrosion) of copper was due to impurities, surmising that “pure” copper was acted upon more rapidly than the specimens which contained alloy (although the type of alloying was not provided) and that “changes” (corrosion) in various specimens of ships copper collected by the Navy Board “… must have depended upon other causes than the absolute quality of the metal”. The quality of the metal is important but other factors were also believed by Davy to play a critical role including “temperature, the relative saltness (sic.) of the sea, and perhaps the rapidity of the motion of the ship; circumstances in relation to which I am about to make decisive experiments” [2].

Davy described “the nature of chemical changes taking place in the constituents of sea water by the agency of copper” and especially the importance of oxygen in the process.

Davy repeats his hypothesis from 1807 [12] (read 20 November 1806) “that chemical and electrical changes may be identical”; a feature clarified and enumerated by his assistant Michael Faraday [4] several decades later with what is now popularly called Faraday’s Law of electrochemical equivalence [4]. Davy then describes how, by this hypothesis, “that chemical attractions may be exalted, modified or destroyed, by changes in the electrical states of bodies”. In other words, change the electrical state from its natural positive or negative state (i.e. change the potential, another word not yet in electrochemical use) and you will cause the chemistry to change. Davy then notes that it was the “application of this principle that, in 1807, I separated the bases of the alkalies from the oxygene with which they are combined and preserved them for examination; and decomposed other bodies formerly supposed to be simple”.

All of these past works by Davy led him “to the discovery which is the subject of this Paper”.

It is a testament to Davy’s scientific method that he supported his hypothesis by past research results, created an understanding of the processes involved and then went on to test it in the laboratory and with full scale trials, collecting and analysing the data for comparison with the predictions of the hypothesis.

Once he had established the basis of his hypothesis, he went on to suppose that if copper “could be rendered slightly negative, the corroding action of sea water upon it would be null; (i.e. polarise the copper negative) and whatever might be the differences of the kinds of copper sheeting and their electrical action upon each other (i.e. galvanic effects), still every effect of chemical action must be prevented, if the whole surface were rendered negative” He then astoundingly says “But how was this to be effected? I first thought of using a Voltaic battery; but this could be hardly applicable in practice”. So, Davy first thought of using an impressed current CP system! He could hardly know that future DC power supplies would make impressed current an easy and common means of cathodically polarising a structure. Davy then says “I next thought of the contact of zinc, tin, or iron”; i.e. galvanic anode CP.

Davy, assisted by “Mr Faraday” then conducted a series of experiments using these three metals to mitigate corrosion on copper. He then reports that although tin was initially effective, “it was found that the defensive action of the tin was injured, a coating of sub-muriate (chloride compound of tin) having formed, which preserved the tin from the action of the liquid”; the tin chloride deposits reduced the effectiveness of tin as an anode. “ With zinc or iron, whether malleable or cast, no such diminution of effect was produced”. Davy now knew for certain that he had effective anodes for the galvanic CP of copper.

Davy and Faraday then proceeded to conduct numerous experiments using zinc and iron in various shapes and sizes attached to copper, including small pieces “as large as a pea”, wires, nails, sheets connected directly by wires, filaments, soldering etc, and always with areas of zinc or iron much smaller than the copper being protected.

Near the end of the paper Davy notes “…. that small pieces of zinc, or which is much cheaper, of malleable or cast iron, placed in contact with the copper sheeting of ships, which is all in electrical connection, will entirely prevent its corrosion”. It is an important note by Davy that the iron anodes were much cheaper, and we will return to this issue when discussing the next two papers presented to the Royal Society.

Finally, Davy says that in future communications he might describe other applications that the principle can be used “to the preservation of iron, steel, tin, brass, and various useful metals”. He was definitely aware that
the principle is widely applicable to any metal or alloy, a feature we enjoy today [13].

Davy’s Paper of June 17th 1824, Additional Experiments and Observations

Davy reports the results of sheets of copper connected to zinc, malleable and cast iron for many weeks in Portsmouth Harbour. He notes that cast iron, which is the cheapest and most easily procured of the materials tested “is likewise most fitted for the protection of copper” and lasts longer than malleable iron or zinc. Davy later however, after further research, recommends a preference to use zinc anodes rather than iron [3].

Davy anticipated and observed “the deposition of alkaline substances” on the copper being “carbonated lime and carbonate and hydrate of magnesia”. Nicholson and Carlisle had discovered the decomposition of water using a voltaic pile [11] (described by Davy as a “capital fact” [7]) and included a description of “the separation of alkali on the negative plates of the apparatus”, hence Davy’s anticipation. These now familiar calcareous deposits of calcium carbonate and magnesium hydroxide are crucial to
the efficiency of CP systems in seawater. Davy was clearly aware of the increase in alkalinity at the cathode and acidification at the anode.
(Note: Even though the concept of pH and the quantification of acidity
and alkalinity was not formulated until 1909 [14], Davy talks extensively about the alkalinity and acidity produced during galvanic coupling of different metals).

Davy also understood and documented that when the calcareous deposit completely covered the copper sheets, it could result in “weeds” and “insects” collecting on them. Davy then considers the amounts of calcareous deposits generated by various quantities of anode material. He found that using zinc and iron anode to copper area ratios from 1/35 to 1/80, the copper became coated with calcareous deposits but “weeds” eventually adhered to the surface as well. He then reports that when the ratio was reduced to 1/150 “… the surface, though it has undergone a slight degree of solution, has remained perfectly clean; a circumstance of great importance as it points out the limits of protection; and makes the application of a very small quantity of the oxidable metal, more advantageous in fact than that of a larger one”. So, Davy here cautions about the excessive application of anodes for the specific protection of copper in seawater when fouling is unwanted and illustrated that fouling could also be mitigated if careful selection of the anode quantities was made for the specific circumstances in which they were used.

Davy’s Paper of June 9th 1825, Further Research

Davy’s full-scale trials were generally very successful, certainly he prevented the copper corrosion, and he makes the comment that the fouling was usually not an issue if the vessel is on the move. He notes that mooring stationary in harbour allows calcareous deposits to form more readily (surface pH will rise more than when in motion) and weeds etc can adhere. He also mentions the quality of the copper may be important and that the proportion of the anode: cathode area ratio affects deposits.

He observed that the marine growths are often initiated on the iron oxides deposited near the anodes (“protectors’’); he recommends here a preference to use zinc anodes rather than iron, “Zinc, in consequence of its forming little or no insoluble compound in brine or seawater, will be preferable to iron …”

Davy defends his work from page 341 onwards in his 1825 paper where he says “A false and entirely unfounded statement respecting this vessel (the 28-gun “Sammarang”) was published in most of the newspapers, that the bottom was covered in weeds and barnacles. I was present at Portsmouth soon after she was brought into dock: there was not the smallest weed or shell-fish upon the whole of the bottom from a few feet round the stern protectors to the lead on her bow.” He goes on to describe other instances of fouling and non-fouling when protected and at least attempts to understand the various circumstances.It appears that cast iron anodes were used in most of the field trials on ocean-going copper sheathed ships. For instance, Davy states in the Bakerian Lecture of 1826 (p. 420) [7], when discussing the field trials and operations “… in the only experiment in which zinc has been employed for this purpose in actual service, the ship returned … perfectly clean”. Davy wanted to conduct further experiments on ships in service, because the mitigation of corrosion was proven and fouling only occasional for reasons he thought could have been elucidated by further work.

It seems reasonable to expect the vessel captains, wanting the most from the protection system, to add iron anodes at possibly excessive rates since they were relatively cheap, easily procured and then complain that fouling was unacceptable. This is corroborated by Davy’s observation [3] when discussing several ships returned from the West Indies that “The proportion of protecting metal in all of them has been beyond what I have recommended, 1/90 to 1/70; yet two of them have been found perfectly clean, and with the copper untouched after voyages to Demarara; and another nearly in the same state, after two voyages to the same place. Two others have had their bottoms more or less covered with barnacles; but the preservation of the copper has been in all cases judged complete”. Davy was therefore not reluctant to report fouling on some ships but balanced this with positive reports. Clearly it was possible to obtain both corrosion protection and no fouling; it would just require continued methodical research (and with ship owners/captains installing the recommended quantities of anodes rather than excessive amounts).

On the issue of fouling, F. James’ otherwise excellent article on Davy [5] claims that “Davy does not seem to have appreciated the side effect, and he was certainly unable to overcome it”. This is incorrect on two points; Davy did appreciate the issue if one refers to the scientific articles as we have above where Davy addresses this specific issue and he was in the throes of trying to better establish the conditions in which corrosion mitigation and acceptable amounts of fouling could be achieved. Unfortunately, ongoing pressure finally led the Admiralty to issue orders to the Navy Board on 19 July 1825 to discontinue the project [5], thus ending further research just two years after first being initiated. The historian S. Ruston, in an essay discussing Davy as the philosopher [6], seems to draw heavily on James’ article where Ruston writes “Unfortunately, what had worked in the laboratory did not work at sea …”. This is incorrect since there was no disputing that the corrosion was fully mitigated; it worked perfectly well and was the original aim of the Admiralty’s directions, with only fouling being a troublesome and sometimes unacceptable side effect. On this Ruston goes on to write “…the electro-plating (sic.) had a chemical side effect, which stopped the poisonous copper salts from going into the sea and resulted in ships’ bottoms being fouled thus slowing them considerably”. Although Ruston mistakes electrochemical protection used by Davy as “electro-plating”, the essay ignores the actual scientific words of Davy within his papers to the Royal Society where, as discussed above, he understood the effect of calcareous deposits, the effect on fouling and the need to strike a practical balance between corrosion protection and fouling.

There was a lot riding on Davy’s work and competition from other inventors tied with the newspapers [5]. Plenty of “fake news” and “alternative truths” – not much has changed! If we study these works with our scientific, objective eyes we can establish a good understanding of the success or otherwise of Davy’s work. Davy makes so many great and insightful statements about his observations, many of which are equally valid today. Also don’t forget that he had the greatest assistant one could imagine in Michael Faraday in these works. The veracity of Davy’s publications is not in doubt, especially with Faraday on board.

Today’s Navy

The world’s navies to this day use cathodic protection on virtually every ship, submarine and marine vessel on the oceans and waterways across the globe to mitigate corrosion, both external to the hull and within internal water filled spaces [15-17]. Ships hulls are of course now predominantly coated steel, but Davy would surely have been pleased to know that zinc anodes are still used extensively as shown in Figure 3, using the same basic principles [17]. Impressed current systems are used for larger current demand applications on bigger vessels but even these are often supplemented with zinc anodes around high current demand areas and shielded locations such as sea chests, ballast tanks, propellers or shafts. Aluminium alloy anodes also provide excellent, cost-effective performance in seawater, but zinc is especially versatile when vessels experience waters of varying salinity such as estuaries and harbours with freshwater inflow.

Conclusions

Although the intent of this paper is to focus on Davy’s work, it is important to note that in the decades and now centuries following Davy’s work extraordinary advances were made in the understanding of the science that underpins CP [13, 18, 19], amongst other fields of science and engineering, this included:

•Michael Faraday’s discovery and experimental proof about the electrochemical equivalence between electric current and corrosion already mentioned.

•Josiah Gibbs’ development of the thermodynamics that lets us determine whether an electrochemical reaction can occur.

•Julius Tafel’s investigations and descriptions during the 1890’s and early 1900’s about how changes in the metal potential can regulate the anodic and cathodic reaction rates and

•Walther Nernst who showed how the potential of a metal could be calculated if the concentrations of reactants and products were known and in doing so, the stability of chemical species could be predicted if the potential and pH were known.

•Marcel Pourbaix summarised all of these features into his first beautiful Pourbaix diagrams [20, 21].

•Mears and Brown [22] also provided a clear kinetic description of CP in 1938 that is still valid today.

•R. J. Kuhn [23, 24] first suggested the earliest criterion for CP of polarising to -0.85 VCSE or more negative, which was shown to be suitable for steel, not only in seawater [25] but also in soils [26].

The increase in pH at the metal surface [27] and the subsequent development of passive oxide films during cathodic polarisation and their role in mitigating corrosion for steel, when considering both the kinetics and thermodynamics, is now well established for iron and steel alloys [28-30] and our deeper understanding continues to evolve, as good science always does.

Role of Calcareous Deposits

•It was recognised very early on [31] that the primary protective action of the calcareous deposits is to; (i) act as a barrier to oxygen or other depolarisers, (ii) increase the internal resistance of the local corrosion cells and (iii) increase the pH of the water film in contact with the metal surface above that of normal seawater. The benefits to marine cathodic protection systems are now well known, particularly in reducing the current density requirement for corrosion mitigation [31-35], a feature reflected in various industry standards for marine structures [36-38].

•The formation of calcareous deposits anticipated and observed by Davy is also still of special interest today and the circumstances of their formation continue to be investigated [17, 39]. R. J. Kuhn [24] also noted the formation of calcareous deposits that varied from “… practically nothing in neutral areas to an inch in thickness in heavily drained areas”, and hence in the degree of the protective or beneficial efficiency.

•The calcareous deposits formed by CP can also have detrimental effects such as accelerated bearing wear in water-lubricated propeller shafts and seizing of hull valves due to clogging [17], or in non-seawater applications such as limiting heat transfer of pumps causing overheating. Means of avoiding these adverse effects continue to be investigated [17], along with understanding the effects of CP upon biofouling [40].

Davy achieved remarkable success even though after 200 years, issues with the protection of metals and alloys using CP are still the subject of ongoing research and refinement. The future remains bright, with vigorous research continuing worldwide into CP, advancing the science and range of applications to an ever-widening array of structures. Science never sleeps and no doubt each new generation of scientists and engineers will, bit by bit, keep adding to our knowledge and advance Davy’s legacy.

References

1. Davy, H. (1824) OVI. On the Corrosion of Copper Sheeting by Sea Water, and on Methods of Preventing This Effect; and on Their Application to Ships of War and Other Ships. Philosophical Transactions of the Royal Society of London 114 January 22, 1824 151-158

2. Davy, H. (1824) XII. Additional Experiments and Observations on the Application of Electrical Combinations to the Preservation of the Copper Sheathing of Ships, and to Other Purposes. Philosophical Transactions of the Royal Society of London 114 June 17, 1824 242-246

3. Davy, H. (1825) XV. Further Researches on the Preservation of Metals by Electrochemical Means. Philosophical Transactions of the Royal Society of London 115 June 9, 1825 328-346

4. Faraday, M. (1834) On Electro-chemical Decomposition, continued (part of Experimental Researches in Electricity – Seventh Series). Philisophical Transactions of the Royal Society of London 124 77-122

5. James, F. A. J. L. (1992) Davy in the dockyard: Humphry Davy, The Royal Society and the electrochemical protection of the copper sheeting of His Majesty’s ships in the mid 1820s. Physis 29 205-225

6. Ruston, S. (2019) Humphry Davy: Analogy, Priority and the “true philosopher”. AMBIX 66 (2-3, May-August) 121-139

7. Davy, H. (1826) The Bakerian Lecture. On the relations of electrical and chemical changes. Philosophical Transactions of the Royal Society of London 116 383-422

8. Cherry, B. and Green, W. (2021) Corrosion and Protection of Reinforced Concrete, CRC Press

9. Galvani, L. (1791) De Viribus Electricitatis in Motu Musculari Commentarius (A Commentary on the Powers of Electricity in Muscular Motion). De bononiensi scientiarum et atrium instuto atque academia Commentarii 7 363-418

10. Volta, A. (1800) On the Electricity Excited by the Mere Contact of Conducting Substances of Different Kinds. Philosophical Transactions of the Royal Society of London 90 403-430

11. Nicholson, W. (1800) Account of the Electrical or Galvanic Apparatus of Sig. Alex.Volta and Experiments performed with the same. Nicholson’s Journal of Natural Philosophy, Chemistry and the Arts 4 (July) 179-191

12. Davy, H. (1807) The Bakerian Lecture, on some chemical agencies of electricity. Philisophical Transactions of the Royal Society of London 97 1-56

13. Ackland, B. G. (2012) Cathodic Protection – It Never Sleeps. In: Corrosion and Prevention 2012, Plenary no. 4, Melbourne: 11-14 November 2012, Australasian Corrosion Association

14. Sörensen, S. P. L. (1909) Enzymstudien. II. Mitteilung. Über die Messung und die Bedeutung der Wasserstoffionenkoncentration bei enzymatischen Prozessen [Enzyme studies. 2nd Report. On the measurement and the importance of hydrogen ion concentration during enzymatic processes]. Biochemische Zeitschrift (in German) 21 131-304

15. Morgan, J. (1987) Cathodic Protection. Second ed, National Association of Corrosion Engineers, Houston, Texas

16. von Baeckmann, W., Schwenk, W. and Prinz, W. (1997) Handbook of Cathodic Corrosion Protection, Gulf Professional Publishing

17. Dylejko, K., Neil, W. (2024) Plenary Lecture – Cathodic Protection and its Implications for Vessels in the Royal Australian Navy. In: Australasian Corrosion Association Conference 2024, Cairns, Australia

18. Ackland, B. G. (2005) P.F. Thomson Memorial Lecture – Cathodic Protection – Black Box Technology? In: Corrosion and Prevention 2005, paper no. 4, Brisbane, Australia, Australasian Corrosion Association

19. Martinelli-Orlando, F., Mundra, S. and Angst, U. M. (2024) Cathodic protection mechanism of iron and steel in porous media. Communications Materials 5 (1) 2024/02/16 15

20. Pourbaix, M. (1945) Thermodynamique des solutions aqueuses diluées. Représentation graphique du rôle du pH et du potentiel. Delft

21. Pourbaix, M. (1974) Atlas of Electrochemical Equilibria in Aqueous Solutions, National Association of Corrosion Engineers

22. Mears, R. B. and Brown, R. H. (1938) A Theory of Cathodic Protection. Transactions of The Electrochemical Society 74 (1) January 1, 1938 519-531

23. Kuhn, R. J. (1933) Cathodic Protection of Underground Pipe Lines from Soil Corrosion. API Proceedings 14 (Section 4) 153-167

24. Kuhn, R. J. (1928) Galvanic Current on Cast Iron Pipes – Their Causes and Effects – Methods of Measuring and Means of Prevention. In: Soil Corrosion Conference, Washington: December 10, Bureau of Standards

25. Schwerdtfeger, W. J. (1958) Current and Potential Relations for the Cathodic Protection of Steel in Salt Water. Journal of Research of the National Bureau of Standards 60 (3) March 1958 153-159

26. Schwerdtfeger, W. J. and McDorman, O. N. (1951) Potential and Current Requirements for the Cathodic Protection of Steel in Soils. Journal of Research of the National Bureau of Standards 47 (2) August 1951 104-112

27. Kobayashi, T. (1974) Effect of Environmental Factors on the Protective Potential of Steel. In: Proceedings of the 5th International Congress on Metallic Corrosion, Houston, Texas, NACE

28. Angst, U., et al. (2016) Cathodic Protection of Soil Buried Steel Pipelines – A Critical Discussion of Protection Criteria and Threshold Values. Werkstoffe und Korrosion 67 (11) 1135-1142

29. Angst, U. (2019) A Critical Review of the Science and Engineering of Cathodic Protection of Steel in Soil and Concrete. Corrosion 75 (12) 1420-1433

30. Freiman, L. I., Kuznetsova, E.G. (2001) Model Investigation of the Peculiarities of the Corrosion and Cathodic Protection of Steel in the Insulation Defects on Underground Steel Pipelines. Protection of Metals 37 (5) 484-490

31. Humble, R. A. (1948) Cathodic Protection of Steel in Sea Water With Magnesium Anodes. Corrosion 4 (July) 358-370

32. Wolfson, S. L. and Hartt, W. H. (1981) An Initial Investigation of Calcareous Depsoits Upon Cathodic Steel Surfaces in Sea Water. Corrosion 37 (2) 70-76

33. Ryan, L. T. (1954) Cathodic protection of steel-piled wharves. Journal of the Institute of Engineers, Australia 26 (7) 160-168

34. Humble, R. A. (1949) The Cathodic Protection of Steel Piling in Sea Water. Corrosion 5 (September) 292-302

35. Hartt, W. H., Culberson, C. H. and Smith, S. W. (1984) Calcareous Deposits on Metal Surfaces in Seawater – A Critical Review. Corrosion 40 (11) 609-618

36. ISO 15589-2 Oil and gas industries including lower carbon energy — Cathodic protection of pipeline transportation systems, Part 2: Offshore pipelines.  (2024).

37. DNV-RP-B401 Cathodic protection design.  (2021).

38. AS 2832.3 Cathodic Protection of Metals Part 3: Fixed Immersed Structures.  (2005).

39. Carre, C., Zanibellato, A., Jeannin, M., Sabot, R., Gunkel-Grillon. & Serres, A. (2020) Electrochemical calcareous deposition in seawater: A review. Environmental Chemistry Letters 18 1193-1208

40. Vuong, P., McKinley, A. & Kaur, P. (2023) Understanding biofouling and contaminant accretion on submerged marine structures. npj Materials Degradation 7 Article 50, https://doi.org/10.1038/s41529-023-00370-5

A New Approach to Explore Passivation Characteristics  of Type 316L Stainless Steel

A New Approach to Explore Passivation Characteristics of Type 316L Stainless Steel

Yosef Thio Widyawan, Dirk L Engelberg
Metallurgy and Corrosion, Department of Materials, School of Natural Sciences,
The University of Manchester, United Kingdom

Yosef Thio Widyawan, BEng, ST, MSc, is a recently graduated engineering professional with academic and practical expertise in naval architecture and corrosion control engineering.He holds a Master’s degree with Distinction in Corrosion Control Engineering from the University of Manchester and a joint Bachelor’s degree in Naval Architecture from Institut Teknologi Sepuluh Nopember, Indonesia and Mokpo National University, Korea. His experience spans roles in ship structural design, welding engineering, and protective organic zinc coating/painting site coordination at Hyundai Samho Heavy Industry, PaxOcean Shipyard, and PT. NOV Profab. Certified as an AMPP Coating Inspector and holding a Welding Engineering Diploma, Yosef demonstrates a strong commitment to integrity, sustainability, and professional development in the marine and offshore industries.

Dirk Engelberg is a professor in materials performance and corrosion at the University of Manchester. He obtained a Dipl.-Ing. (FH) in Surface Engineering and Materials Science from Aalen University (Germany) before moving to Manchester in 2000 for an M.Sc. in Corrosion Science & Engineering and a PhD in Metallurgy & Materials Science. He joined the Corrosion & Protection Centre as an academic lecturer in 2010, which is now part of Metallurgy & Corrosion (Corrosion@Manchester) in the Department of Materials.  Dirk’s research is centred on (i) understanding material degradation related to the storage, disposal, and decontamination of nuclear waste, (ii) applied electrochemistry and high-throughput screening techniques, (iii) development of innovative solutions for net-zero engineering, and (iv) localised corrosion, stress corrosion cracking and hydrogen embrittlement. Dirk is also an expert in microstructure engineering and leads several cross-disciplinary projects combining mechanical, civil, and chemical engineering with chemistry, physics and materials-based research.

(*The work reported here is based on Yosef’s dissertation for the MSc in Corrosion Control Engineering (CCE) at The University of Manchester).

1. Introduction

Austenitic stainless steels are commonly used for applications in the energy, medical and chemical process industries due to their enhanced corrosion resistance, ease of availability and beneficial physical properties [1]. However, the material is not immune to corrosion, which is frequently caused by chlorides and other halide ions that may be present in petrochemical refinery systems or marine atmospheres [2]. Such corrosion damage can lead to serious material loss, crevice or localised corrosion or even stress corrosion cracking (SCC). Thus, monitoring, inspecting, predicting and investigating the corrosion behaviour and its patterns are most important to avoid the risk of material failure and to ensure the materials are performing accordingly.

Passivation treatments are viable options to enhance the corrosion resistance of stainless steels, providing an additional layer of protection

via enhancing surface passive film properties. These treatments are either applied via exposure to citric or nitric acids [3,4,5] or via electrochemical treatments [6]. Passivation treatments strengthen the existing passive film of stainless steel surfaces, but there will likely often remain some residual issues at sites of jointing and particularly welding.

A novel method for screening materials for their corrosion resistance is bipolar electrochemistry. The technique has been used for high-throughput corrosion screening and to obtain information about microstructures that might provide enhanced protection against material degradation [7,8].

The idea of this dissertation is to explore bipolar electrochemistry for modifying passive film properties on type 316L stainless steel.

The set-up does not require a direct ohmic contact to the test sample, and the set-up is quite simple and easy to replicate. A bipolar electrode (BPE) is an electrically conductive substance that encourages electrochemical reactions at its extremities (poles) when exposed to an electrical field between two feeder electrodes [9]. Through bipolar electrochemistry [10], the material’s surface properties can be either modified or assessed.

Differing from the conventional three-electrode experimental corrosion test, the bipolar set-up can be used to conduct corrosion assessment across a far wider range of applied potentials and materials. Bipolar electrochemistry has even been used to screen 2707 Hyper-duplex stainless steels for their corrosion resistance [11]. This is possible through scan rate independent, directly acting potential gradients along the BPE. In addition, one of the studies related to the oil and gas industries is the employment of cathodic protection, where stray current can be further studied via bipolar electrochemistry utilisation or the formation of inhibitor films under anodic or cathodic polarisation control. These test set-ups are currently being further developed for corrosion screening.

2. Methodology

Material and Sample Preparation

Type 316L sheet samples with dimensions of 10 mm x 25 mm were mechanically prepared with SiC paper from 400 up to 2500 grit, then polished with diamond paste to a ¼ micrometre finish. The final mirror-finished surface is required for passivation and corrosion test experiments—the desired quality of sample finish is also needed for elemental depth profile analysis with Glow Discharge Optical Emission Spectroscopy (GDOES). Figure 1 gives a flow chart of the research methodology and analysis steps applied. The prepared samples were first passivated using a novel bipolar electrochemistry approach, followed by assessment of the passivated surfaces in HCl solutions using standard 3-electrode electrochemistry. The sample surfaces were then analysed after corrosion testing using optical microscopy. One additional sample was also prepared under bipolar passivation treatment (in citric acid and boric acid) in order to observe the GD-OES depth profiling effect of bipolar passivation treatment.

Bipolar Electrochemistry Passivation Treatment

The passivation treatment utilised citric acid (C6H8O7), and boric acid (H3BO3) as passivating agents in order to facilitate the formation of a gradient passivation layer along the BPE surface. Employing bipolar electrochemistry to induce passivation at the anodic side, with the cathodic side expected to weaken the passive film. The expected outcome here was to generate one sample surface containing the full spectrum, starting with a strong passive film at the anodic side, to surfaces experiencing OCP conditions close to the central region, to a cathodically cleaned surface at the cathodic end of the BPE. Figure 2 below shows the bipolar test set-up, with the sample exposed to the electric field between both feeder electrodes, but without any electrical connection to an outside power source. Here it was expected that the negative pole of the feeder electrode would induce a positive reaction at the one end of the BPE surface, with the positive feeder inducing a negative pole at the BPE. The set-up was similar to experiments to test stray current corrosion of different metals related to cathodic protection as well as buried power line corrosion [12,13].

The effect of cathodic polarisation on passive film stability has been demonstrated previously under different applied potentials on super duplex stainless steel [14].

The bipolar parameters used for the passivation treatment were 8V with 10-minute or 30-minute polarisation in 10% (wt.) citric acid or 1 M boric acid. A Keysight power source was was used for applying the voltage. For surface film characterisation GDOES depth profile measurements were carried out, and each experiment was conducted 3x for each parameter variable.

Corrosion Test

Directly after the bipolar passivation treatment, standard 3 electrode potentio-dynamic corrosion tests were carried out to assess the effect of the surface passivation treatment. An 0.01 M, 0.1 M and 1 M hydrochloric acid (HCl) solution was used with Ag/AgCl/saturated KCl reference electrode.

Open circuit potential (OCP) measurements were recorded for 180 minutes, to see whether changes occurred at the surface that might be reflected in a shift of the OCP. The assessed samples were then observed under an optical microscope to analyse the impact of the corrosion testing on the treated sample surfaces.

Glow Discharge Optical Emission Spectroscopy (GDOES)

The depth profiles of the sample surface were measured using a GD-OES instrument. The power output used was 30 W and 650 Pa. with the sample very flat and the backside of the sample parallel to the front side to enable the vacuum to work properly. GD-OES analysis was carried out at both ends and the centre of the sample after passivation.

3. Results and Discussion

Figure 3 below shows the OCP versus time for the untreated type 316L surface. The test in 0.01 M HCl shows a steady increase of OCP from -0.2 V at the start to about -0.05 V after 3 hours, with the 0.1 M HCl giving a final rest potential close to -0.1 V, and the 1 M HCl sample somehow stabilising at -0.3 V. These long OCP measurements were employed to understand whether the bipolar passivation treatment caused changes in the OCP response.

Figure 4 further summarises the OCP response of the citric and boric acid treated BPE surfaces, with the same trend apparent for all samples. The OCP test for citric acid passivation exposed to 0.1 M HCl started at -0.2 V and stabilised at -0.13 V, with the only marked difference observed for the boric acid treated surface giving an initial potential of +0.3 V. Although the final potential was slightly less positive than the 0.1 M HCl test of the untreated type 316L surface, it still showed the material’s resistance was in a similar OCP range.

Furthermore, the OCP test for both passivation treated surfaces exposed to 1 M HCl started at -0.35 V and gradually rose to about -0.28 V, then remained steady until the end of the test at 3 hours. Both passivation treatments showed a distinct OCP stabilisation hump after 1 hour of exposure. This shows the system reaches a stable state, but at a far more negative potential compared to the lower HCl concentration.

The bipolar passivation treatment was expected to enhance the passive layer at the anodic side of the bipolar electrode, leading to a more corrosion resistant surface, compared to the cathodic side. However, since the full sample was immersed in the passivating solutions, even the central part would be expected to be more resistant than the cathodic, with the later cathodic BPE side is expected to have a far weaker passive film [14].

Although all the results show a similar behaviour, when the corrosion test was deployed in 1 M HCl, the treated sample obtained a constant OCP far earlier than the reference sample test; this could be due to the effect of passivation treatment, which enabled the samples to obtain their equilibrium earlier than the reference sample without passivation treatment [15].

Comparing the results of the samples that have been treated with bipolar passivation in 10% citric acid and 1 M boric acid in Figure 4, the OCP data showed no particular difference between them. The application of bipolar electrochemistry on the citric acid and boric acid passivation showed a similar behaviour when immersed in the 0.1 M HCl and 1 M HCl.

Figure 5 above summarises the optical microscopy observations of both sample surfaces that underwent bipolar electrochemistry passivation treatment in 10% citric acid and 1 M boric acid, which were corrosion in both 0.1M and 1M HCl solutions. The optical assessment showed no significant corrosion attack variation between the anodic and the cathodic pole of the BPE sample. The difference in 0.1M to 1M HCl exposure clearly showed more general surface roughening, with the appearance changing into a “wrinkle-like” roughened contour after 1M HCl exposure. Type 316L is known to readily corrode in 1M HCl.

The idea of this OCP exposure test in HCl was to understand whether differences exist between the anodically and cathodically treated sides after the bipolar passivation treatment. No visual differences were actually observed along the sample surface after both 0.1M and
1M HCl exposure.

Characterisation

GD-OES application for surface chemical analysis is described in more detail in Ref. [16,17]. The plasma generated during the measurement will create a circular crater of 4 mm in diameter, as shown in Figure 6 below. The scan rate was 1 m/s to obtain the depth profiles with a sputter duration of 75 seconds, with measurements taken at different locations. The collision between the argon ions and the sputtered material excites atoms and releases the photon energy as a characteristic light spectrum. The data obtained from the measurements shows the emission intensity versus time (s). GD-OES is frequently used for the depth profiling of thin surface films and layers, such as passive surface films, galvanised materials, or PVD/CVD coatings [18].

All data obtained showed carbon contamination at the surface, which is expected with sample storage under standard ambient conditions in the laboratory. Figure 7 above shows the resulting GD-OES depth profile of the reference Type 316L sample, with carbonaceous surface contamination, followed by enriched chromium, with the iron (Fe) and nickel (Ni) then indicating the bulk composition. The oxygen signal was found slightly raised in the surface region, with the horizontal line then indicating a drop in this signal, indicative of the interface between surface oxide and the bulk.

Finally, Figure 8 below compares the GD-OES depth profiles of the specimens treated in 10% citric acid and 1 M boric acid. The application of the bipolar passivation treatment seemed to influence to some degree the formation of the passive film of the Type 316L sample. The passive film formation of the sample under passivation treatment in 10% citric acid showed some minor change in chromium signal between the middle region and both anodic and cathodic regions. The middle region shows the presence of iron on the outer surface, while chromium dominates both the anodic and cathodic poles [19].

Observation of the cathode side of the passivated sample (both in citric and boric acid – Figure 8) showed a higher intensity level of chromium at the very beginning of the time axis. This may indicate that the chromium exists at the very outer layer of the treated sample’s cathode side; therefore, the treated sample had higher chromium content on the passive layer than the untreated sample. This behaviour might be influenced by the application of bipolar passivation treatment on the sample, which strengthens the formation of a passive layer on the sample’s cathode side.

The chromium intensity of the sample treated in 10% citric acid fell before it reached the bulk interface. On the other hand, the sample treated in 1 M boric acid underwent a falling of chromium intensity before it went constant at the bulk layer. According to Ref. [36], the peak of the elements chromium and iron showed that the elements were the major cationic alloys in the redox reaction. Thus, it can be assumed that applying 1 M boric acid was a more susceptible, favourable environment for the passivation of stainless steel 316L compared to the treated sample in 10% citric acid.

Conclusion

The overall bipolar passivation treatment did not show the expected behavior regarding the formation of a gradient passive film, although some interesting response was observed conducting OCP measurements in 1 M HCl solution.

It seems though that the application of bipolar passivation treatments influences somehow local passive layer compositions. From GD-OES characterisation of the sample passivated in 10% citric acid, the anodic and cathodic regions seemed Cr enriched in the oxide layers, while the middle part of the surface remained covered with iron oxide. On the other hand, on the sample exposed to 1 M boric acid, the anodic and centre part of the sample have iron oxide at the outer film surface, while the cathodic region was enriched with chromium. More work is certainly needed to further investigate the successful application of bipolar passivating treatments.

References

[1] P Kangas and G C Chai, “Use of Advanced Austenitic and Duplex Stainless Steels for Applications in Oil & Gas and Process Industry,” AMR, vol. 794, pp. 645–669, Sep. 2013, doi: 10.4028/www.scientific.net/AMR.794.645.

[2] A H Al-Moubaraki and I B Obot, “Corrosion Challenges in Petroleum Refinery Operations: Sources, Mechanisms, Mitigation, And Future Outlook,” Journal of Saudi Chemical Society, vol. 25, no. 12, p. 101370, 2021, doi: https://doi.org/10.1016/j.jscs.2021.101370.

[3] ASTM A380-99E1  Standard Practice for Cleaning, Descaling, and Passivation of Stainless Steel Parts, Equipment, and Systems, 2017. doi: 10.1520/A0380_A0380M-17.

[4] ASTM A967-05E2  Standard Specification for Chemical Passivation Treatments for Stainless Steel Parts, 2013. doi: 10.1520/A0967-05E02.

[5] BS EN 2516:2023 Aerospace Series – Passivation of Corrosion Resisting Steels and Decontamination of Nickel or Cobalt Base Alloys, BS EN 2516:2023, Feb. 06, 2024. doi: 978 0 539 30425 1.

[6] ASTM B912-02(2018)  Standard Specification for Passivation of Stainless Steels Using Electropolishing, 2018. doi: 10.1520/B0912-02R18.

[7] Y  Zhou, J Qi, and D L Engelberg, “A Novel High Throughput Electrochemistry Corrosion Test Method: Bipolar Electrochemistry,” 2023.

[8] Y Zhou, J Qi, and D L Engelberg, “On The Application of Bipolar Electrochemistry For Simulating Galvanic Corrosion Behaviour of Dissimilar Stainless Steels,” Electrochemistry Communications, vol. 126, p. 107023, 2021, doi: 10.1016/j.elecom.2021.107023.

[9] S E  Fosdick et al., “Bipolar Electrochemistry,” Angew Chem Int Ed, vol. 52, no. 40, pp. 10438–10456, Sep. 2013, doi: 10.1002/anie.201300947.

[10] R M Crooks, “Principles of Bipolar Electrochemistry,” ChemElectroChem, vol. 3, no. 3, pp. 357–359, Mar. 2016, doi: 10.1002/celc.201500549.

[11] Y Zhou et al., “A Rapid Corrosion Screening Technique for Grade 2707 Hyper Duplex Stainless Steel At Ambient Temperature,” Materials and Corrosion, vol. 75, no. 2, pp. 227–234, 2023, doi: 10.1002/maco.202313943.

[12] T J Lennox and M H  Peterson, “Stray Current Corrosion of Steel, ”Naval Engineers Journal, vol. 88, no. 1, pp. 45–53, 1976, doi: 10.1111/j.1559-3584.1976.tb03795.x.

[13] J M K Nairn et al., P Wade, and S Thomas, “Cell-Within-Cell Study of Stray Current Copper Corrosion: Impact of Soil Conductivity and Source Distance,” Corrosion Engineering Science and Technology, The International Journal of Corrosion Processes and Corrosion Control, 2025, doi: 10.1177/1478422×241311671.

[14] C  Ornek et al., “Understanding Passive Film Degradation and Its Effect On Hydrogen Embrittlement of Super Duplex Stainless Steel – Synchrotron X-Ray And Electrochemical Measurements Combined With Calphad And Ab-Initio Computational Studies,” Applied Surface Science, vol. 628, p. 157364, 2023, doi: 10.1016/j.apsusc.2023.157364.

[15] S Mischler and A I Munoz, “Tribocorrosion,” in Encyclopedia of Interfacial Chemistry, Elsevier, 2018, pp. 504–514. doi: 10.1016/B978-0-12-409547-2.13424-9.

[16] R Payling and T Nelis, Glow Discharge Optical Emission Spectroscopy: A Practical Guide. Royal Society of Chemistry, 2007. Available:https://books.google.co.uk/books?id=7mwoDwAAQBAJ&dq=glow+discharge+optical+emission+spectroscopy+&lr=&source=gbs_navlinks_s

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[18] T Nelis and R  Payling, Surface Analysis Methods in Materials Science. Berlin, Heidelberg: Springer. [Online]. Available: https://link.springer.com/chapter/10.1007/978-3-662-05227-3_24

[19] M Uemura et al., “Depth Profile Analysis of Thin Passive Films on Stainless Steel By Glow Discharge Optical Emission Spectroscopy,” Corrosion Science, vol. 51, no. 7, pp. 1554–1559, Jul. 2009, doi: 10.1016/j.corsci.2008.11.017.

Improved Electrochemical Corrosion  Testing in Extreme Conditions:  Collaborative Advances in Autoclave Testing

Improved Electrochemical Corrosion Testing in Extreme Conditions: Collaborative Advances in Autoclave Testing

‘Amber Sykes¹, Danny Burkle², Robert Jacklin1,2 Joshua Owen¹, R Woollam¹, R Barker¹
¹School of Mechanical Engineering, University of Leeds, UK | ²LBBC Baskerville, UK

Amber Sykes is currently a PhD student at the University of Leeds, within the Institute of Functional Surfaces, where she is researching iron carbonate corrosion product formation in geothermal environments. Prior to her PhD research, Amber gained a Master of Engineering (MEng) degree in Mechanical Engineering at the University of Bath. During 2024 she received an EFC – European Federation of Corrosion Award for Best Oral Presentation by an Early Career Author.

 

]Dr Danny Burkle, is a Principal Engineer and corrosion testing specialist at LBBC Baskerville. He earned his Master’s Degree in Mechanical Engineering and a PhD in Corrosion from the University of Leeds. With over 10 years’ experience dedicated to the corrosion field, he is a professional member of the Institute of Corrosion (ICorr) and formerly the chair of Young ICorr, Danny now leads the ICorr Corrosion Engineering Division (CED). His contributions to corrosion research have included 6 published journal papers as the lead author and over 10 papers as a named author/contributor. He joined LBBC in 2017 through a KTP – Knowledge Transfer Partnership with the University of Leeds, Danny and has since progressed seamlessly from a Design Engineer to a Principal Engineer. His trajectory has a strong focus on business development and sales related to the research sector.

1. Introduction: Why Collaboration Matters

This article highlights a collaborative approach in developing a test method to obtain high-quality, reproducible electrochemical data within an autoclave operating at elevated pressure and temperature.

The evaluation and understanding of material corrosivity in high-pressure, high-temperature (HPHT) environments is critical to ensuring asset integrity in industries such as Oil and Gas, Carbon Capture and Storage (CCS) and Geothermal Energy to name a few. Carbon steel processing infrastructure in these systems is frequently exposed to carbon dioxide (CO2)-containing fluids, accelerating corrosion and threatening long-term integrity.

Under specific CO2 – containing conditions—particularly elevated temperature, pressure, and chemical saturation—the corrosion product iron carbonate (FeCO3) can precipitate onto the internal surfaces of carbon steel pipes. This layer can slow degradation by blocking active corrosion sites and impeding the diffusion of electrochemically active ions [1]. Understanding the formation, structure, and protective mechanisms of FeCO3 layers is therefore vital for accurate corrosion modelling and prediction, and hence asset integrity management.

Autoclave technology can facilitate experimental corrosion testing in HPHT environments, in which protective FeCO3 layers tend to form. In-situ electrochemical monitoring techniques, such as Linear Polarisation Resistance (LPR) and Electrochemical Impedance Spectroscopy (EIS), can provide real-time insight into the rate of FeCO3 layer formation, and the evolving mechanisms of corrosion protection offered by the layer. However, the application of these techniques in HPHT conditions remains exceptionally challenging. Issues such as reference electrode instability, electrical interference, and difficulty maintaining test equilibrium often lead to poor data reproducibility and limit the utility of these techniques for model development and material evaluation.

To address this gap, a collaborative project between LBBC Baskerville and the University of Leeds has advanced the reliability and precision of electrochemical testing in autoclaves. By combining industrial design expertise with academic electrochemical research, the team has developed a refined methodology capable of delivering high-quality, reproducible electrochemical data under extreme conditions.

This article presents two core outcomes of that collaboration:

1.How a refined testing methodology enables reproducible monitoring of corrosion product formation in autoclave conditions.

2.How this data supports advanced EIS modelling to quantify the layer’s physical properties in an autoclave.

Together, these insights offer a practical foundation for enhancing corrosion prediction in real-world HPHT systems.

2. Experimental Set-Up: Refining the Approach

The collaborative work began by identifying recurring limitations in electrochemical autoclave testing. Robert Jacklin’s PhD research project at University of Leeds played a key role in diagnosing failure points, including pressure instability, signal drift, and inconsistent electrode positioning [2].

The team developed a refined procedure using the LBBC Baskerville CTA-S1300 autoclave, incorporating:

•Improved sealing methods and sample insulation to prevent electrical interference,

•A low-pressure CO2 sparging method to pre-saturate the brine prior to solution transfer,

•Careful arrangement of working, counter, and reference electrodes to avoid electrical interference,

•Use of a back pressure regulator (BPR) to maintain consistent test pressure during heating.

Electrode Preparation and Assembly

A three-electrode set up was used to take in-situ electrochemical measurements, including an X65 carbon steel working electrode, a Hastelloy C-276 counter electrode and an externally pressure balanced silver/silver chloride (Ag/AgCl) reference electrode. The working and counter electrodes were prepared by wet grinding all surfaces to P600 grit and sealing the back and sides with high-pressure thermosetting resin. An additional X65 carbon steel coupon was prepared for each test to assess mass loss. The arrangement of the electrochemical samples and mass loss coupon in the autoclave is shown in Figure 1.

Brine Preparation and Autoclave Testing Procedure

A 3 wt.% sodium-chloride (NaCl) brine was prepared by dissolving >99 % purity NaCl in deionised water, followed by stirring and continuous CO2 sparging for a minimum of 12 hours to ensure oxygen removal and full saturation. The 1.3L LBBC Baskerville autoclave was also flushed through with CO2 for a minimum of 30 minutes before the brine solution was transferred into the autoclave by CO2 gas displacement.

The autoclave was pressurised to the desired operating pressure (5, 10 or 15 bar) using a high-pressure CO2 line at room temperature, followed by heating to 80 °C using a hot plate and temperature probe. A BPR maintained the test pressure during the heating phase. Upon reaching the target temperature, the outlet valve to the BPR was closed and the pressure in the autoclave was allowed to evolve naturally throughout the test. The working, counter and reference electrodes were connected to a Gamry Potentiostat to take electrochemical measurements. The autoclave vessel was grounded through a metal hot plate [2].  An image of the autoclave set up is shown in Figure 1.

Electrochemical testing followed a repeatable schedule: Open Circuit Potential (OCP), five cycles of LPR, and EIS scans. This setup significantly improved baseline stability and reduced variability across runs. These methods were carefully documented and refined through repeated testing, highlighting how hardware design, procedural control, and pressure regulation directly influence
data quality.

This approach was initially used to refine the procedure and ensure high-quality, reproducible measurements at 5 bar, before being applied in tests at 10 and 15 bar to evaluate reproducibility and environmental sensitivity.

3. Reproducibly Tracking FeCO2 Layer Formation in Autoclaves

The LPR results in Figure 2 were obtained using the refined autoclave testing set up and show how the average inverse polarisation resistance (Rp-1) varied throughout the 120-hours corrosion tests at 5, 10 and 15 bar. Rp-1 is directly proportional to the corrosion rate of the underlying carbon steel surface. The error bars represent the range in Rp-1 values across four repeats at 5 bar and two repeats at 10 and 15 bar.

The evolution of a protective FeCO3 layer was initially investigated at 80 °C and 5 bar.

At these conditions, a rapid decrease in corrosion rate occurred after the first 40 hours of exposure, aligning with the onset of FeCO3 precipitation. The EIS Nyquist plots also showed a change in shape from two distinct semi-circles to the formation of a low-frequency linear tail, shown in Figure 5, indicating the transition from active corrosion to a diffusion-limited processes. At this point, the mechanism of protection offered by the FeCO3 layer transitioned from predominantly surface blocking to effectively restricting the diffusion of ions [1]. This occurred alongside the ‘pseudo-passivation’ phenomenon, between 70 and 80 hours, marked by a sudden anodic shift in OCP, shown in Figure 3, and a plateau in polarisation resistance [4]. The cross-sectional scanning electron microscopy (SEM) images in Figure 4 confirm the evolution of a low-porosity FeCO3 layer, consistent with the formation of an effective diffusion barrier, supporting the electrochemical interpretations. These findings validated that the new autoclave methodology could reproducibly capture the entire corrosion-product evolution timeline, from initial exposure through to protective film formation.

The LPR results in Figure 2 also show that the refined autoclave testing methodology could capture repeatable electrochemical measurements in more demanding environments, and with accelerated corrosion kinetics. Increasing the operating pressure from 5 to 15 bar resulted in higher initial corrosion rates and a faster rate of formation of a protective FeCO3 layer [3]. These tests demonstrate the sensitivity of FeCO3 formation and corrosion characteristics to environmental changes and highlights the importance of experimental testing over a wide range of operating conditions.

4. Quantifying Layer Properties Using High-Precision EIS Modelling

The LPR responses in Figure 2 show that corrosion product formation significantly alters the corrosion rate of the underlying carbon steel and must be considered for the accurate prediction of corrosion rates in HPHT environments. However, the current incorporation of FeCO3 into CO2 corrosion models relies on numerous theoretical assumptions regarding the physical properties of the layer, and how these properties contribute towards the mechanisms of corrosion protection [5]. To quantify the protectiveness of corrosion products layers throughout their development, and extract physical properties of FeCO3, equivalent electrical circuit models can be fit to the experimental EIS data.

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High-precision EIS data is required to obtain useful and reliable information from equivalent circuit models. To assess the quality of the experimental EIS data, Kramers-Kronig analysis is used. The Kramers-Kronig transformation assesses the validity of the EIS response by testing for linearity, causality and stability [6].  This assessment is particularly important for the low frequency EIS data, used to characterise diffusion behaviour. The time scales required for low frequency measurements are increased, such that the stability condition may not be achieved. Once the EIS data has been validated, the quality of fit between the modelled and measured EIS data is calculated using chi-squared analysis normalised by the degrees of freedom (x2/v). The circuit models illustrated in Figure 5 both achieve an excellent quality of fit to the experimental EIS data, achieving x2/v values of less than 0.0002.

The quality of the electrochemical data in this study was sufficient to extract the full low-frequency EIS response, enabling the quantification of diffusion characteristics through the FeCO3 layer. This represents a significant advancement, as such measurements have rarely been achieved under comparable high-pressure, high-temperature conditions. The circuit models illustrated in Figure 5 were used to quantify the extent of surface coverage from FeCO3, and the diffusion coefficients of ions through the layer. This allows the respective contributions of surface blocking and diffusion restriction towards the overall reduction in corrosion rate to be identified, information that is critical to the advancement of corrosion prediction models.

The physical porosity of the FeCO3 layer was also estimated from in-situ EIS measurements, showing promising agreement with results from literature [7]. Validating the use of electrochemical techniques to evaluate the porosity of corrosion product layers in-situ would be a landmark finding for this research area.

In this study, the development of a robust autoclave testing methodology enabled the collection of high-precision and meaningful EIS data in HPHT environments. Equivalent electrical circuit models could then be utilized to extract physical properties of the layer, in-situ, throughout the layer’s development – information which no other technique can provide.

Standardisation of electrochemical set-ups and autoclave testing procedures will continue to improve EIS data quality and facilitate innovative EIS studies that can further the development of corrosion prediction models and advance the knowledge of the wider corrosion industry.

5. Conclusion: A Path Forward Through Partnership

This collaboration between LBBC Baskerville and the University of Leeds has delivered two critical advances in autoclave corrosion testing:

• A validated methodology for reproducibly tracking FeCO3 layer formation under HPHT conditions using LPR, OCP, and EIS.

• The demonstration that precision EIS can be used to quantify key physical properties of corrosion product layers — such as surface coverage and diffusion characteristics.

These outcomes not only advance the science of corrosion but also provide practical tools and benchmarks for researchers and industry alike. Achieving reproducibility in HPHT electrochemical testing has long been a challenge; this work proves it is possible with the right approach. The success of this collaboration also emphasises a pressing need in corrosion testing to the wider community: standardised methodologies for electrochemical testing in autoclaves.

Without clear standards, comparing data across institutions becomes difficult, and model calibration remains speculative.  By publishing detailed methods and validating their approach, this project offers a foundation on which others can build.

The methods and findings shared here are intended to empower others facing similar challenges in autoclave corrosion testing. As CCS, hydrogen, and geothermal technologies continue to expand, the need for reliable, high-precision corrosion data will only grow. This study provides a blueprint for how that data can be generated and used.

Next Steps: The team welcomes further collaboration to extend this methodology to multi-impurity systems and operational-scale environments. For more information or to explore partnership opportunities, contact Dr Danny Burkle (LBBC) and Professor Richard Barker (University of Leeds).

6. References

[1] R De Motte et al., E Basilico, R Mingant, J Kittel, F Ropital, P Combrade, S Necib, V Deydier, D Crusset, S Marcelin, “A Study by Electrochemical Impedance Spectroscopy and Surface Analysis of Corrosion Product Layers Formed During CO2 Corrosion of Low Alloy Steel”. Corrosion Science 172, (2020): p. 108666.

[2] R Jacklin, Characterising Protective Corrosion Product Development in Demanding CO2 Environments. Doctor of Philosophy thesis, University of Leeds, 2023.

[3] A Sykes et al., R Jacklin, D Burkle, R C Woollam, J Owen, R Barker, “The Effect of CO2 Partial Pressure on the Formation and Protective Characteristics of Iron Carbonate Corrosion Products”. AMPP Annual Conference + Expo, paper no. AMPP-2024-20666 (New Orleans, Louisiana, USA: Association for Materials Protection and Performance, 2024).

[4] W Li et al., B Brown, D Young, S Nešić, “Investigation of Pseudo-Passivation of Mild Steel in CO2 Corrosion”. Corrosion 70, (2014): p.
294-302.

[5] M Nordsveen et al., S Nešić, R Nyborg, A Stangeland, “A Mechanistic Model for Carbon Dioxide Corrosion of Mild Steel in the Presence of Protective Iron Carbonate Films-Part 1: Theory and Verification”. Corrosion 59, 5 (2003): p. 443-456.

[6] A Lazanas, M  Prodromidis, Electrochemical Impedance Spectroscopy – A Tutorial. ACS Measurement Science Au. 2023, 3.

[7] R Barker et al., D Burkle, T Charpentier, H Thompson, A Neville, A review of iron carbonate (FeCO3) formation in the oil and gas industry, Corrosion Science, Volume 142, 2018.