Thermocouple types and tolerance classes (IEC 60584)
Types K, J, T, N and E each have a defined EMF curve and tolerance classes 1, 2 and 3. The tolerance applies to new wire, not to a year-old thermocouple.
A thermocouple type is a promise about one thing: the voltage its junction produces at a given temperature, against a reference junction at 0 °C. IEC 60584-1 defines that curve for each letter type and then states how far a given piece of wire may deviate from it. Choosing a type is choosing a range, an output per degree, and a tolerance band — in that order of importance.
The five common base-metal types
Output below is the Seebeck coefficient at 20 °C, computed from the NIST ITS-90 reference functions, with what one microvolt of instrument error is worth in millikelvin at that point. That last column is the one that decides whether your readout is good enough.
| Type | Materials | Range (°C) | dE/dt at 20 °C | 1 µV is worth | E at 100 °C |
|---|---|---|---|---|---|
| K | NiCr–NiAl | −270 to 1372 | 40.3 µV/°C | 24.8 mK | 4.096 mV |
| T | Cu–CuNi | −270 to 400 | 40.3 µV/°C | 24.8 mK | 4.279 mV |
| J | Fe–CuNi | −210 to 1200 | 51.5 µV/°C | 19.4 mK | 5.269 mV |
| N | NiCrSi–NiSi | −270 to 1300 | 26.6 µV/°C | 37.6 mK | 2.774 mV |
| E | NiCr–CuNi | −270 to 1000 | 60.5 µV/°C | 16.5 mK | 6.319 mV |
Types K and T are almost indistinguishable in output at 20 °C — 40.33 against 40.27 µV/°C — and then diverge quickly: by 100 °C type T is producing 46.8 µV/°C against type K's 41.4. It is a reminder that a type's sensitivity is a curve, not a constant, and that a rule of thumb picked up at room temperature does not travel.
Tolerance classes
IEC 60584-1 states each class as the greater of a fixed value and a proportion of the temperature, over a stated range. For types K and N: class 1 is ±1.5 °C or ±0.004|t|; class 2 is ±2.5 °C or ±0.0075|t|; class 3 is ±2.5 °C or ±0.015|t| and covers sub-zero use only. The fixed term wins until the proportional term overtakes it — at 375 °C for class 1 and 333 °C for class 2.
| Type | −100 °C (cl 3) | −40 °C (cl 1) | 100 °C (cl 1) | 100 °C (cl 2) | 400 °C (cl 1) | 1000 °C (cl 1) |
|---|---|---|---|---|---|---|
| K | ±2.50 | ±1.50 | ±1.50 | ±2.50 | ±1.60 | ±4.00 |
| T | ±1.50 | ±0.50 | ±0.50 | ±1.00 | — (to 350 °C) | — |
| J | — (not defined) | ±1.50 | ±1.50 | ±2.50 | ±1.60 | — |
| N | ±2.50 | ±1.50 | ±1.50 | ±2.50 | ±1.60 | ±4.00 |
| E | ±2.50 | ±1.50 | ±1.50 | ±2.50 | ±1.60 | — |
Two things fall out of that table. Type T's class 1 band is three times tighter than everyone else's across the cold-chain range, which is why it is the default for freezers, cold rooms and transport qualification. And type K's class 1 tolerance at 1000 °C is ±4 °C — a number worth quoting to anyone who believes a thermocouple is an accurate device.
The noble-metal types
- Types R and S (Pt–PtRh) reach 1600 °C and are the laboratory reference types above the range of base-metal wire. Output is low — around 6 µV/°C at 100 °C — so they demand a good readout.
- Type B (PtRh–PtRh) reaches 1700 °C and produces almost nothing below 50 °C, which conveniently makes it insensitive to the temperature of its own reference junction.
- All three are expensive, and all three are poisoned by contact with metal vapour or reducing atmospheres. They are not a general-purpose upgrade; they are a high-temperature necessity.
What the tolerance class does not tell you
The classes apply to new wire, as delivered. A thermocouple used in a steep temperature gradient develops inhomogeneity — the composition of the wire changes along its length, and the emf it produces starts to depend on where the gradient sits rather than only on the junction temperature. Move the same thermocouple to a different immersion depth and it reads differently. No calibration corrects this, because the calibration was performed with the gradient in one place and your process puts it somewhere else.
That is the fundamental reason a platinum resistance thermometer beats a thermocouple for precise work in the range where both are available. If you need better than about a degree below 400 °C, the question is not which thermocouple type — it is whether a thermocouple is the right instrument at all.
Tolerance class is not measurement uncertainty. A class 1 type K is not a ±1.5 °C measurement until you have accounted for the reference junction, the extension leads, the readout, and the state of the wire. Calibrate the thermocouple with its own instrument and use the certificate instead.
Frequently asked questions
- Why is Type T preferred for freezers and cold rooms?
- Its class 1 tolerance is ±0.5 °C across the sub-zero range against ±1.5 °C for types K, N and E — three times tighter. It is also stable in moist conditions, and the copper leg keeps lead resistance low. For −80 to +50 °C work it is the obvious base-metal choice.
- Which thermocouple type has the highest output?
- Type E, at 60.5 µV/°C near room temperature, against 51.5 for J, 40.3 for K and T, and 26.6 for N. Higher output means a given microvolt of instrument noise or offset costs fewer millikelvin — 16.5 mK on a type E against 37.6 mK on a type N.
- What is the difference between class 1 and class 2?
- Both are stated as the greater of a fixed limit and a proportion of |t|. For type K, class 1 is ±1.5 °C or ±0.004|t| and class 2 is ±2.5 °C or ±0.0075|t|. They are identical in effect at 100 °C only in the sense that both are on their fixed terms there — ±1.5 against ±2.5 °C. At 1000 °C the gap is ±4 °C against ±7.5 °C.
- Is type N really better than type K?
- For stability at high temperature, yes — it was designed to address type K's drift and its ordering effects between 250 and 600 °C. The tolerance classes are identical, so the benefit does not show up in the specification; it shows up in how far the thermocouple has moved when you recalibrate it.
- Can I use a type K above 1372 °C?
- No. That is where the NIST reference function for type K stops, so there is no defined relationship between emf and temperature beyond it. Above that range you are into the noble-metal types R, S and B.
- Does the tolerance class apply after the thermocouple has been in service?
- No, and this is the most misunderstood point about thermocouples. Classes apply to new wire. Thermal cycling in a gradient makes the wire inhomogeneous, after which its reading depends on immersion depth and the gradient's position — something no calibration certificate can correct.
References
- [1]IEC 60584-1:2013 — Thermocouples, Part 1: EMF specifications and tolerances
- [2]IEC 60751:2022 — Industrial platinum resistance thermometers and platinum temperature sensors
General technical guidance written against the cited sources. It is not regulatory or legal advice and does not replace the applicable standard, guideline or a qualified reviewer's judgement.
Have a question on this topic?
Ask ValiTrac AI and see the evidence and calculation behind the answer.
Ask ValiTrac AIFree calculator: Pt100 converter
Convert between resistance and temperature for Pt100 / Pt1000 sensors, with class AA, A, B and C tolerances at that temperature.
Open the calculatorCalibration on ValiTrac
Support calibration workflows, uncertainty budgets and certificate generation.
Open the calibration worksheetRelated articles
How thermocouples are calibrated
Comparison against a reference in a bath or furnace, with the reference junction realised. Ignore it on a type K at 420 °C and you read 398 °C.
Uncertainty budget for a thermocouple calibration
Inhomogeneity, reference junction and extension leads join the comparison budget. At 400 °C on a type K, inhomogeneity alone carries 85 % of the variance.
Maintaining calibration equipment between calibrations
References drift, baths contaminate, inserts wear, batteries die. Maintenance and intermediate checks find those before the next calibration does.