Bundles are inspected under time pressure with the unit down and everyone waiting, which is exactly when the wrong technique gets chosen because it is the one the contractor brought. The decision is more constrained than it looks: magnetism rules out half the options before anyone has said what they are looking for.
A tube bundle is thousands of thin-walled, small-bore, hard-to-reach components, and it usually has to be inspected in the window between pulling it and putting it back. Nobody has time to do everything properly, so the plan has to be right first time.
Two questions decide it, in this order.
This is not a preference, it is a constraint, and it eliminates methods outright.
| Tube material | Behaves as | Available |
|---|---|---|
| Brass, admiralty, cupronickel, titanium, austenitic stainless | Non-magnetic | Conventional ECT, IRIS |
| Carbon steel, ferritic and martensitic stainless | Ferromagnetic | RFT, tube MFL, IRIS |
| Duplex, cold-worked or contaminated austenitics | Partly magnetic | Partial-saturation ECT, IRIS |
Conventional eddy current does not work on a ferromagnetic tube. The permeability of the material swamps the response and the small changes you are trying to measure disappear into it. This is not a sensitivity limitation to be worked around; it is why remote field testing exists.
Conventional eddy current (ECT) is the fastest thing on the list. A probe goes down the tube and comes back in seconds, and phase analysis of the signal gives both an estimate of depth and an indication of whether the flaw is on the inside or the outside. It is very good at discrete damage — pitting, ID and OD attack, cracking — and it is the standard screen for a non-magnetic bundle. Its weakness is gradual, uniform thinning over a long length, which produces a slow drift the technique is not well suited to quantifying.
Remote field testing (RFT) is what you use on carbon steel tubes. The signal travels out through the tube wall, along outside it, and back in through the wall again, so it passes through the thickness twice. That gives it a useful property: it responds to ID and OD wall loss roughly equally, which no other electromagnetic method here does. The price is resolution. RFT sees volume more than it sees sharpness, so it reports general wall loss well and small isolated pits poorly. It is also slower than ECT.
Tube MFL is the other option for ferromagnetic tubes: saturate the wall magnetically and detect the flux that leaks out at a defect. It is fast and it is sensitive to sharp localised pitting, which is exactly what RFT is weakest at. It is correspondingly poor at gradual general thinning, because gentle wall loss does not leak much flux. RFT and MFL are close to complementary, which is why some programmes run both.
IRIS — the internal rotary inspection system — is ultrasonic. A rotating mirror spins an ultrasonic beam around the inside of the tube while the probe is drawn along it, and what comes back is an actual thickness profile in millimetres, at every point, on any material, magnetic or not. It is the reference method, the one whose numbers you can put into a calculation.
It needs water coupling and it needs the tube clean — genuinely clean, bare metal, no scale and no deposit. Cleaning a bundle to IRIS standard takes longer than the inspection does, and a tube that is not clean enough returns a signal that is not just inaccurate but often absent. It is also several times slower per tube than any of the electromagnetic methods. Nobody IRIS-inspects a whole bundle if they can avoid it.
Screen everything with the fast electromagnetic method the material allows, rank the tubes by indication severity, then IRIS the worst of them to turn indications into thicknesses.
All of these methods degrade near the tubesheet. The roll transition, the tube end and the tubesheet itself distort the signal for the electromagnetic techniques and interrupt the geometry for IRIS, and the result is a zone at each end of every tube where sensitivity is reduced or the data is thrown away.
That zone is not a random place to be blind. The tube-to-tubesheet crevice is where deposits settle and stay, where under-deposit and crevice attack concentrate, and where residual stress from the rolling operation is highest. The most likely place for damage is the place the inspection is weakest.
There is no clever technique that removes this. What removes it is knowing about it: when a bundle leaks and the screen said the tubes were sound, the tube ends are the first place to look, and a programme that supplements the standard scan with a technique aimed specifically at the tube-end zone is making a deliberate choice rather than hoping.
The detection methods list covers IRIS, remote field, eddy current and the tank and heater techniques alongside them, each with what it misses.
Open the detection methodsWho writes this. A mechanical engineer with twelve years in oil and gas — in-line inspection, fired heater and furnace inspection, and pipeline integrity. What is here comes from the published standards and from what those years in the field actually looked like. It is not written by an API-certified inspector.
This is not an assessment. Nothing on this site may be used to justify a decision about real equipment. Assessing plant requires the current editions of the applicable codes, data from a licensed source, and a competent engineer who signs for the answer. · Integrity Field Guide