Phase Transformations & Kinetics

martensite

/ MAR-ten-site /

Martensite is what you get when you cool austenite so fast the carbon atoms have no time to move: the crystal is forced to change shape without any diffusion. Instead of atoms strolling to new positions, the whole lattice shears cooperatively in an instant, trapping the carbon where it sits. This is the hard, brittle phase behind a quenched steel's cutting edge.

Rapid quenching skips past all the C-curves of the TTT and CCT diagrams and reaches the martensite-start temperature (Ms) with the carbon still dissolved. The FCC austenite then snaps into a body-centered-tetragonal (BCT) structure, like BCC iron but stretched along one axis by the trapped carbon squeezed into it. That stretched, carbon-jammed lattice makes dislocation motion extremely hard, so martensite is very hard and strong but brittle. It is diffusionless (athermal): the amount formed depends on how far below Ms you cool, not on how long you hold.

Martensite is the reason steel can be hardened at all, but as-quenched it is often too brittle to use and the quench builds dangerous internal stresses (a cracking risk). So it is almost always tempered afterward to trade a little hardness for much-needed toughness. Note that hardness rises with carbon content, and getting fully martensite through a thick part depends on hardenability, not just quench speed.

Water-quenching 0.8 percent C austenite forms BCT martensite around 60 to 65 Rockwell C: extremely hard, but so brittle it would shatter under impact until it is tempered.

Diffusionless shear traps carbon and makes steel hard.

Martensite is not on the iron-carbon phase diagram; it is a non-equilibrium product of fast cooling. Its hardness comes from trapped carbon, so low-carbon steels form only soft martensite.

Also called
馬氏體