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CLADDING TECHNOLOGY SHANXI CO., LTD
CLADDING · BIMETAL PRODUCT · BIMETAL PRESSURE VESSEL TECHNICAL STUDY

Measurement of Thickness of Stainless Steel and Nickel-Based Overlay Layers

Literature Overview

Accurate measurement of overlay layer thickness is a critical quality control activity in bimetal product manufacturing and pressure vessel fabrication. Unlike base material thickness measurement, which is straightforward with standard ultrasonic or magnetic methods, overlay thickness measurement presents unique challenges due to the layered structure, potential intermetallic zones, and the need to distinguish between the overlay layer, the transition zone, and the base material.

Fundamental Measurement Challenges

The measurement challenge arises from several factors inherent to weld overlay structures:

Measurement Methods Comparison

Method Principle Typical Accuracy Applicable Materials Limitations
Contact ultrasonic Time-of-flight of ultrasonic pulse ±0.1–0.3 mm All metallic overlays Requires coupling agent, affected by roughness
Eddy current Electromagnetic induction ±0.05–0.15 mm Non-magnetic overlays on magnetic base Limited penetration, affected by conductivity
Magnetic thickness gauge Magnetic force measurement ±0.1–0.2 mm Non-magnetic overlays on ferromagnetic base Only for non-magnetic overlay on magnetic substrate
X-ray radiography Density contrast imaging ±0.2–0.5 mm All combinations Requires access from both sides, expensive
Metallographic sectioning Direct optical measurement ±0.05 mm All materials Destructive, time-consuming
Beta backscatter Beta particle attenuation ±0.05–0.1 mm Thin overlays (0.05–5 mm) Limited thickness range, requires calibration
Beta transmission Beta particle transmission ±0.05 mm Thin overlays Requires access from both sides

Process-Specific Considerations

For Strip Cladding (Electroslag Welding)

Strip cladding produces a well-defined overlay layer with relatively flat surfaces, making thickness measurement more straightforward. The typical overlay thickness range is 2–10 mm, and the interface between overlay and base is generally sharp due to the low dilution rates (5–15%) characteristic of ESW. Contact ultrasonic measurement is the preferred method, with accuracy typically within ±0.1 mm for overlay thicknesses above 2 mm.

For Multi-Pass Arc Welding Overlay

Multi-pass GTAW or GMAW overlay creates a more complex layered structure with varying dilution rates between passes. The first pass typically has 20–35% dilution, while subsequent passes range from 5–15%. This creates a gradient in composition and microstructure that makes the overlay-base boundary ambiguous. Metallographic sectioning is often required for accurate assessment, particularly for thin overlays (1–3 mm) where ultrasonic methods lose resolution.

For Powder Cladding (PTA and Laser Cladding)

Powder cladding produces very thin, well-defined overlay layers (0.1–2.0 mm) with low dilution (5–15%). The sharp interface and uniform composition make these layers amenable to eddy current and beta backscatter measurement. However, the thin layer thickness requires high-resolution measurement systems with appropriate calibration.

Standards and Acceptance Criteria

Standard Measurement Method Acceptance Criteria
ASTM A263/A264 Ultrasonic or metallographic Minimum specified thickness
EN 10028-7 Ultrasonic measurement Minimum thickness per specification
NB/T 47002 Ultrasonic or metallographic Minimum 1.5 mm or as specified
ASME VIII Div.1 Ultrasonic thickness measurement Minimum 0.019T or as specified
API 934 Method per procedure Minimum specified overlay thickness

Engineering Practice Insights

In engineering practice, the choice of measurement method should be guided by the following considerations:

  1. For production quality control: Contact ultrasonic measurement is the most practical method for in-line inspection of clad plates and pressure vessel shells. It is non-destructive, rapid, and provides adequate accuracy for verifying minimum overlay thickness specifications. Calibration should be performed on test coupons with known overlay thicknesses representative of the production material combination.
  2. For dispute resolution and acceptance testing: Metallographic sectioning provides the most definitive measurement but is destructive and time-consuming. It should be reserved for critical applications, qualification testing, or when non-destructive measurement results are questionable.
  3. For research and development: Beta backscatter and eddy current methods provide excellent accuracy for thin overlay layers and are suitable for parameter optimization studies and process development work.

Common Measurement Errors and Countermeasures

Error Source Impact Countermeasure
Surface roughness Underestimation of thickness Surface grinding or use of roughness-compensated probes
Incorrect calibration material Systematic error Calibrate on representative test coupons
Temperature effects Velocity change in ultrasonic measurement Temperature compensation or measurement at controlled temperature
Interface geometry Signal interpretation error Use of phased array or TOFD for angled interfaces
Multiple layers Signal interference Frequency selection and signal processing optimization

Study Reflections

The measurement of overlay layer thickness is often underestimated in terms of its importance to overall quality assurance. In practice, I have encountered numerous cases where dimensional nonconformance was discovered only during final inspection, leading to costly rework or rejection of otherwise sound components. The key lesson is that measurement capability must be established before production begins, with appropriate calibration, procedure qualification, and operator training. Furthermore, the measurement strategy should be integrated into the overall quality plan from the design stage, ensuring that the selected method provides adequate accuracy for the specified tolerance. Future developments in phased array ultrasonics and automated eddy current systems promise to improve measurement accuracy and throughput, but the fundamental challenge of distinguishing overlay from base material in gradient transition zones remains a subject of ongoing research.