Materials
Jominy End-Quench Test for Steel Hardenability
A single 25.4 mm steel bar, heated to 850 °C and then blasted on one end by a 24 °C water jet while the other end cools slowly in still air, produces a hardness gradient that can drop from 60 HRC at the quenched face to 25 HRC just 30 mm away. That gradient, read off with a Rockwell hardness tester every 1.6 mm, is the whole point of the Jominy end-quench test — the standard way engineers measure a steel's hardenability.
Hardenability is not the same as hardness. It is the depth to which a steel forms hard martensite when quenched, governed almost entirely by alloy chemistry rather than by carbon content alone. The Jominy test, standardized as ASTM A255 and ISO 642, imposes a reproducible continuum of cooling rates along one specimen so that a single experiment maps hardness against cooling rate for a given heat of steel.
- TypeStandardized materials test (hardenability)
- Governing standardASTM A255 / ISO 642 / SAE J406
- Specimen25.4 mm dia × 100 mm cylinder
- Quench24 °C ± 2 °C water jet, 12.7 mm nozzle
- Key metricHRC vs. Jominy distance (J1.6, J8, ...)
- InventedWalter Jominy & A.L. Boegehold, 1938
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What the test is and where it's used
The Jominy end-quench test measures hardenability — how deeply a steel hardens on quenching — using a single machined bar and one controlled quench. It was developed in 1938 by Walter E. Jominy and A. L. Boegehold at General Motors Research, and remains codified in ASTM A255, ISO 642, and SAE J406.
It is the workhorse test wherever quench-and-temper steels must be specified by cross-section: automotive gears, crankshafts, axle shafts, drive-line components, bearings, springs, fasteners, and forgings. Steelmakers publish Jominy curves (often as a scatter H-band) for guaranteed-hardenability "H" grades such as 4140H and 8620H.
- Design use: confirm a part section will reach a target core hardness after quench.
- Purchasing use: accept or reject heats against an H-band.
- Process use: pick a grade and quench medium together so the core makes >50 % martensite.
Because every steel has nearly the same thermal conductivity, distance along the bar maps one-to-one onto cooling rate — so one bar characterizes an entire alloy.
How the test works, step by step
The mechanism is a deliberately engineered cooling-rate gradient along one specimen:
- Machine: a 25.4 mm diameter × 100 mm long cylinder with a small support flange at the top.
- Austenitize: heat to the grade's austenitizing temperature (e.g. 845–870 °C for 4140), hold ~30 min to fully dissolve carbon into FCC austenite.
- End-quench: drop the bar into a fixture so its lower face sits 12.7 mm above a 12.7 mm orifice; a free-standing column of 24 °C ± 2 °C water strikes only the bottom face. Transfer must take under 5 s to avoid pre-cooling.
- Cool: the quenched end cools at ~270 °C/s and forms martensite; heat conducts axially away, so each position up the bar cools progressively slower.
Grind two flat, parallel lands 0.4 mm deep along the bar (removing any decarburized skin), then read Rockwell C hardness starting 1.6 mm from the quenched end and continuing in 1/16-inch (1.6 mm) steps. Plotting HRC versus distance yields the Jominy curve: high, flat hardness near the end where martensite dominates, falling where slower cooling lets pearlite, ferrite, and bainite form.
Key quantities and a worked example
Hardness at the quenched end is set by carbon content (≈ 60 HRC at 0.6 %C fully martensitic); the rate of falloff is set by alloying. The core relationship links Jominy distance to cooling rate at 700 °C — e.g. J1.6 ≈ 270 °C/s, J8 ≈ 28 °C/s, J16 ≈ 10 °C/s, J40 ≈ 3 °C/s.
Grossmann's ideal critical diameter DI converts this into a single number: the largest bar diameter that would harden to 50 % martensite at its center in an ideal quench (severity H = ∞). It is built multiplicatively from composition:
DI = DI,C × fMn × fSi × fNi × fCr × fMo
- DI,C = base ideal diameter from carbon + ASTM grain size (e.g. ~0.22 in at 0.4 %C, grain size 7).
- fx = multiplying factor for each element, roughly f = 1 + k·(wt%). Chromium (k ≈ 2.16) and molybdenum (k ≈ 3.0) are the strongest per-percent; nickel is weak.
Worked example (4140, 0.40 C / 0.9 Mn / 0.95 Cr / 0.2 Mo): DI,C ≈ 0.21 in; fMn ≈ 3.0, fCr ≈ 3.05, fMo ≈ 1.6, fSi ≈ 1.2 → DI ≈ 0.21 × 3.0 × 3.05 × 1.6 × 1.2 ≈ 3.7 in (≈ 94 mm), the hallmark of a deep-hardening alloy steel.
Using Jominy data in real design and selection
The engineering payoff is the Lamont / equivalent-cooling-rate method, which ties a Jominy position to a real bar. Each location in a round bar quenched at severity H (Grossmann's quench severity: still oil ≈ 0.25–0.30, agitated oil ≈ 0.5, still water ≈ 1.0, agitated brine ≈ 2–5) cools at a rate equal to some Jominy distance. Charts give, for example: the center of a 50 mm round in still oil cools like J12–J14.
Design procedure:
- Fix the required core hardness (say 40 HRC for a fatigue-critical shaft).
- Choose the quench medium and part diameter, then read the equivalent Jominy distance for the critical location (surface, 3/4-radius, or center).
- Pick a grade whose published Jominy curve still exceeds the target hardness at that distance.
This lets you trade alloy cost against quench severity: a leaner steel plus a faster quench, or a richer alloy plus a gentle oil quench that limits distortion and quench cracking. Guaranteed-hardenability H-grades ship with a min/max Jominy band so heat treaters can set furnace and quench parameters with confidence.
How it compares to related tests and concepts
Versus a hardness test: a Rockwell or Brinell reading gives hardness at one point; Jominy gives hardness as a function of cooling rate, i.e. hardenability. High hardness ≠ high hardenability — a 1080 plain-carbon steel gets very hard at the surface but shallow-hardens.
- Grossmann bar test: the older method quenches many bars of different diameters and sections each to find the one that is 50 % martensitic at center. It directly yields Dcrit and DI but is slow and wastes material; Jominy replaced it with one bar.
- Calculated DI (multiplying factors / SAE J406): predicts hardenability from chemistry alone — cheap for melt control, but empirical and less accurate for high-alloy or boron steels.
- CCT / TTT diagrams: give the full microstructure-vs-cooling-rate map; Jominy is essentially a fast physical sampling of the CCT behavior at fixed austenitizing conditions.
- End-quench for aluminum/Ni: the same fixture is adapted to study quench sensitivity in age-hardening alloys, though "hardenability" there means retained solute, not martensite.
Failure modes, trade-offs, and significance
The test's precision depends on rigid control of its variables — most scatter comes from procedural drift, not the steel:
- Water temperature and jet height: the 24 °C ± 2 °C water and 65 mm free column height directly set the end cooling rate; a hot lab or wandering nozzle shifts the whole curve.
- Delay in transfer: >5 s to the fixture lets the end pre-cool, softening J1.6.
- Decarburized or non-parallel ground flats: grinding too shallow leaves a soft skin; grinding-induced heat can temper the surface — both bias HRC low. Always grind wet.
- Grain size and austenitizing: coarser prior-austenite grains and higher soak temperatures both increase measured hardenability, so austenitizing must match the grade spec.
Trade-offs: high hardenability eases through-hardening of thick sections but raises quench-crack and distortion risk and worsens weldability (higher carbon equivalent). Significance: nearly 90 years on, the Jominy curve is still how the steel supply chain communicates hardenability — the bridge between a mill certificate's chemistry and whether a finished shaft will survive its fatigue loads.
| Distance from quenched end | Approx. cooling rate | AISI 1045 (plain C) | AISI 4140 (Cr-Mo) | AISI 4340 (Ni-Cr-Mo) |
|---|---|---|---|---|
| J1.6 mm (1/16 in) | ~270 °C/s | 55–58 HRC | 57–60 HRC | 57–60 HRC |
| J8 mm (5/16 in) | ~28 °C/s | 30–35 HRC | 52–56 HRC | 55–58 HRC |
| J16 mm (10/16 in) | ~10 °C/s | 24–28 HRC | 42–48 HRC | 52–56 HRC |
| J25 mm (16/16 in) | ~6 °C/s | 22–26 HRC | 35–40 HRC | 48–53 HRC |
| J40 mm (25/16 in) | ~3 °C/s | 20–24 HRC | 30–35 HRC | 42–48 HRC |
Frequently asked questions
What is the difference between hardness and hardenability?
Hardness is the resistance to indentation at a point, set mainly by carbon content and microstructure. Hardenability is the depth to which martensite forms on quenching, set mainly by alloying elements. A plain-carbon steel can be very hard at the surface yet have low hardenability (soft core), which is exactly what the Jominy curve reveals.
Why is only carbon content, not alloying, what sets the maximum hardness?
The peak hardness at the quenched end depends on the carbon dissolved in the martensite — about 60 HRC at 0.6 %C. Alloying elements (Cr, Mo, Mn, Ni) barely change that peak; instead they slow the diffusion-controlled transformations (pearlite, bainite) so martensite forms at slower cooling rates, flattening and extending the Jominy curve to greater distances.
What does the Grossmann ideal critical diameter DI represent?
DI is the diameter of a round bar that would just harden to 50 % martensite at its center under an ideal, infinitely severe quench (H = ∞). It condenses a full Jominy curve into one number and is computed from composition as DI = DI,C × fMn × fSi × fNi × fCr × fMo, letting you rank steels by hardenability from chemistry alone.
How does Jominy distance relate to a real quenched part?
Each position in a real bar cools at a rate equal to some point along the Jominy specimen. Using quench-severity (H) charts — still oil H ≈ 0.25, still water H ≈ 1.0, agitated brine H ≈ 2–5 — you convert a part's diameter and quench medium into an equivalent Jominy distance, then read the expected hardness off that steel's published curve.
What water temperature and setup does ASTM A255 require?
The specimen (25.4 mm × 100 mm) is austenitized, then held so its lower face is 12.7 mm above a 12.7 mm orifice. A free column of water at 24 °C ± 2 °C strikes only the end face, rising about 65 mm above the nozzle unimpeded. Transfer from furnace to fixture must take under 5 seconds to keep the end cooling rate reproducible.
What are the most common sources of error in the Jominy test?
Delayed transfer (pre-cooling the end), wrong water temperature or jet height, and improper preparation of the flat lands — grinding too shallow leaves a decarburized soft skin, while dry grinding tempers the surface. Austenitizing at the wrong temperature or with a coarse grain size also shifts the curve, since both raise apparent hardenability.