Nickel titanium
Nickel titanium, commonly known as Nitinol, is a nearly equiatomic intermetallic alloy composed of approximately 55 weight percent nickel and 45 weight percent titanium, renowned for its unique shape memory effect and superelasticity arising from a reversible martensitic phase transformation.[1] This alloy demonstrates the ability to return to a predefined shape after deformation when subjected to specific temperatures or stresses, making it distinct from conventional metals.[2] Discovered in 1962 by metallurgist William J. Buehler at the U.S. Naval Ordnance Laboratory—where the name Nitinol derives from "Nickel," "Titanium," and "Naval Ordnance Laboratory"—the material was initially developed for potential use in missile components due to its high elasticity and fatigue resistance.[1][3] Buehler's serendipitous observation occurred during experiments with nickel-titanium compositions, revealing the shape memory behavior when a deformed sample spontaneously recovered upon heating.[4] Key physical properties include a density of about 6.5 g/cm³, a melting range of 1240–1310°C, and transformation temperatures tunable from −100°C to over 100°C through compositional adjustments or heat treatments.[1] Additionally, Nitinol offers excellent corrosion resistance, biocompatibility, and a Young's modulus ranging from 28–83 GPa depending on phase (martensite to austenite), generally lower than traditional titanium (~110 GPa) or stainless steel (~200 GPa) alloys, reducing stress shielding in load-bearing applications.[2][5] The alloy's defining characteristics—shape memory effect (SME), where it deforms in a low-temperature martensitic phase and recovers upon heating to the austenitic phase, and superelasticity (pseudoelasticity), enabling large recoverable strains up to 10% at body temperature—have driven its widespread adoption.[1][2] In biomedical fields, Nitinol is extensively used for self-expanding stents, orthodontic archwires, and orthopedic implants like scoliosis correction rods, leveraging its biocompatibility and ability to mimic soft tissue mechanics.[2] Beyond medicine, applications span aerospace actuators, naval couplings, vibration dampers, and consumer products such as eyeglass frames and flexible antennas, capitalizing on its durability, non-magnetic nature, and energy absorption capabilities.[1] Ongoing advancements in additive manufacturing further enhance its customization for complex structures in tissue engineering and minimally invasive devices.[2]Properties
Composition and Crystal Structure
Nickel-titanium (NiTi) alloys are primarily composed of nearly equiatomic mixtures of nickel and titanium, with the stoichiometric NiTi intermetallic compound forming at approximately 50 at% Ni, equivalent to about 55 wt% Ni due to the atomic mass difference between the elements. The binary Ni-Ti phase diagram reveals a complex system with multiple intermetallic phases, including the congruent-melting Ni₃Ti (on the Ni-rich side) and NiTi, as well as the NiTi₂ compound (on the Ti-rich side), which contribute to the alloy's microstructural stability by delineating regions of solid solution and eutectic reactions. These phases emerge from peritectic and eutectoid transformations during solidification, ensuring that near-equiatomic compositions yield predominantly the NiTi matrix essential for functional properties like the shape memory effect.[6][7] The crystal structure of NiTi undergoes a reversible martensitic transformation central to its behavior. At elevated temperatures (above the austenite finish temperature, typically around 100–200°C depending on composition), the alloy exists in the B2 austenite phase, an ordered body-centered cubic structure akin to the CsCl prototype, characterized by alternating Ni and Ti atoms at the corners and body center of the cubic unit cell. Upon cooling below the martensite start temperature, this transforms to the low-temperature B19' martensite phase, which adopts a monoclinic crystal structure (space group P2₁/m) with distorted orthorhombic-like features, enabling the twinned variants responsible for shape recovery. This structural shift from cubic symmetry to lower monoclinic symmetry accommodates the shear deformation without permanent distortion.[8][9][10] Deviations from the equiatomic composition significantly influence the phase transformation temperatures and overall stability. Ni-rich variants (e.g., 50.5–51 at% Ni) promote the formation of Ni₄Ti₃ precipitates during aging, depleting matrix Ni and thereby elevating transformation temperatures, which is leveraged to tune the austenite-martensite transition for specific applications. Conversely, Ti-rich compositions (e.g., below 50 at% Ni) stabilize higher transformation temperatures and incorporate Ti₂Ni precipitates, enhancing thermal stability but potentially reducing ductility. For instance, a mere 0.4 at% increase in Ni content from 49.8 at% to 50.2 at% can depress martensite start temperatures by approximately 40°C, underscoring the sensitivity of these alloys to stoichiometry. The intermetallic compounds Ni₃Ti and NiTi₂ play crucial roles in off-stoichiometric alloys by acting as secondary phases that pin grain boundaries and control precipitate distribution, thereby improving resistance to grain growth and maintaining phase purity in the NiTi matrix.[8][11][6]Mechanical and Thermal Characteristics
Nickel-titanium alloys, known as Nitinol, have a density of approximately 6.45 g/cm³ and a melting point of 1310 °C. These physical attributes contribute to their lightweight nature and high-temperature processability. Nitinol exhibits excellent corrosion resistance, primarily due to the spontaneous formation of a thin, stable titanium dioxide passive layer that protects against environmental degradation in physiological and aqueous environments. Furthermore, Nitinol demonstrates strong biocompatibility, with low cytotoxicity and minimal nickel ion release when surfaces are properly passivated, enabling safe implantation in the human body. The thermal properties of Nitinol are governed by its reversible martensitic phase transformation, which involves key temperatures: martensite start (Ms), martensite finish (Mf), austenite start (As), and austenite finish (Af). These transformation temperatures are highly tunable through precise control of nickel content (typically 49-51 at.%) and heat treatment, allowing ranges from -100 °C to 100 °C to suit specific functional requirements. For instance, superelastic grades often have Af temperatures between -65 °C and 45 °C, while shape memory variants may extend higher. Mechanically, Nitinol displays remarkable strength and ductility. Superelastic forms exhibit yield strengths (critical stress for phase transformation) ranging from 200 to 600 MPa, ultimate tensile strengths up to 1200 MPa, and elongations greater than 10%, far surpassing many conventional alloys in recoverable deformation. The stress-strain response features a characteristic hysteresis loop, where the area represents energy dissipation during austenite-to-martensite detwinning and reverse transformation.| Property | Typical Value/Range | Notes/Source Context |
|---|---|---|
| Density | 6.45 g/cm³ | Bulk alloy value; enables lightweight designs.[12] |
| Melting Point | 1310 °C | High thermal stability for processing.[13] |
| Yield Strength (Superelastic) | 200–600 MPa | Plateau stress at ~3% strain; varies with processing.[14] |
| Ultimate Tensile Strength | Up to 1200 MPa | Post-transformation fracture strength.[14] |
| Elongation | >10% | High ductility in tension.[14] |
| Transformation Temperatures (Ms to Af) | -100 °C to 100 °C | Tunable via composition and annealing.[15] |