Glass transition temperature

Glass transition temperature

The glass transition temperature, "T"g, is the temperature at which an amorphous solid, such as glass or a polymer, becomes brittle on cooling, or soft on heating. More specifically, it defines a pseudo second order phase transition in which a supercooled melt yields, on cooling, a glassy structure and properties similar to those of crystalline materials e.g. of an isotropic solid material. [The IUPAC Compendium of Chemical Terminology, 66, 583 (1997).] "T"g is usually applicable to wholly or partially amorphous solids such as common glasses and plastics (organic polymers).

Below the glass transition temperature, "T"g, amorphous solids are in a glassy state [A. Varshneya. "Fundamentals of inorganic glasses." Boston, Academic Press (1994).] and most of their joining bonds are intact. In inorganic glasses, with increased temperature more and more joining bonds are broken by thermal fluctuations so that broken bonds (termed configurons) begin to form clusters. Above "T"g these clusters become macroscopic large facilitating the flow of material. In organic polymers, secondary, non-covalent bonds between the polymer chains become weak above "T"g. Above "T"g glasses and organic polymers become soft and capable of plastic deformation without fracture. This behavior is one of the things which make most plastics useful. [But such behavior is not exhibited by crosslinked thermosetting plastics which, once cured, are set for life and will shatter rather than deform, never becoming plastic again when heated, nor melting.]

It is important to note that the glass transition temperature is a kinetic parameter, and thus parametrically depends on the melt cooling rate. Thus the slower the melt cooling rate, the lower "T"g. In addition, "T"g depends on the measurement conditions, which are not universally defined.O. V. Mazurin, Yu. V. Gankin: "Glass transition temperature: problems of measurements and analysis of the existing data"; Proceedings, International Congress on Glass, July 1-6, 2007, Strasbourg, France.]

The bond system of an amorphous material changes its Hausdorff dimension from Euclidian 3 below "T"g (where the amorphous material is solid), to fractal 2.55±0.05 above "T"g, where the amorphous material is liquid. [M.I. Ojovan, W.E. Lee. "J. Phys.: Condensed Matter", 18, 11507-11520 (2006).]

Time dependency

Consider a molecular liquid which is slowly cooling down. At a certain temperature, the average kinetic energy of molecules no longer exceeds the binding energy between neighboring molecules and growth of organized solid crystal begins. Formation of an ordered system takes a certain amount of time since the molecules must move from their current location to energetically preferred points at crystal nodes. As temperature falls, molecular motion slows down further and, if the cooling rate is fast enough, molecules never reach their destination — the substance enters into dynamic arrest and a disordered, glassy solid (or supercooled liquid) forms. In fact, Walter Kauzmann has argued that if such an arrest did not happen, at still lower temperatures a thermodynamically paradoxical situation would arise, where the undercooled liquid would have to be denser and of a lower enthalpy than the crystalline phase. Such arrest apparently takes place at certain temperature, which is called the "calorimetric ideal glass transition temperature" "T"0c. This means that glass transition is not merely a kinetic effect, i.e. merely the result of fast cooling of a melt, but there is an underlying thermodynamic basis for glass formation. [cite journal | author= Baeurle SA, Hotta A, Gusev AA | title= On the glassy state of multiphase and pure polymer materials | journal=Polymer | year=2006 | volume=47 | pages=6243–6253 | doi=10.1016/j.polymer.2006.05.076] The glass transition temperature "T"g → "T"0c as "dT""⁄""dt" → 0.

A full discussion of "T"g requires an understanding of mechanical loss mechanisms (vibrational and resonance modes) of specific (usually common in a given material) functional groups and molecular arrangements. Factors such as heat treatment and molecular re-arrangement, vacancies, induced strain and other factors affecting the condition of a material may have an effect on "T"g ranging from the subtle to the dramatic. "T"g is dependent on the viscoelastic materials properties, and so varies with rate of applied load. The silicone toy 'Silly Putty' is a good example of this: pull slowly and it flows; hit it with a hammer and it shatters.


The IUPAC Compendium of Chemical Terminology, 1997, 66, 583 defines the glass transition as a second order phase transition in which a supercooled melt yields, on cooling, a glassy structure and properties similar to those of crystalline materials e.g. of an isotropic solid material. Phase transitions are associated with the symmetry breaking [A.Z. Patashinskioe and V.L. Pokrovskioe, Fluctuation Theory of Phase Transitions (Pergamon, Oxford, 1979).] . The translation-rotation symmetry in the distribution of atoms and molecules is unchanged at the liquid-glass transition, which retains the topological disorder of fluids. Symmetry changes at glass transition can be viewed when considered not for atoms but for bonds. The disordered material changes its symmetry, namely the Hausdorff dimension of bonds, from Euclidian 3D below to fractal 2.55±0.05- dimensional above the glass transition temperature. [cite journal | author = M. Ojovan and W. Lee | title = Topologically disordered systems at the glass transition | year = 2006 | journal = | volume = 18 | issue = 50 | pages = 11507 | doi = 10.1088/0953-8984/18/50/007]


"T"g can be significantly decreased by addition of plasticisers into the polymer matrix. Smaller molecules of plasticizer embed themselves between the polymer chains, increasing the spacing and free volume, and allowing them to move past one another even at lower temperatures. The "new-car smell" is due to the initial outgassing of volatile small-molecule plasticizers used to modify interior plastics (e.g., dashboards) to keep them from cracking in the cold, winter weather. The addition of nonreactive side groups to a polymer can also make the chains stand off from one another, reducing "T"g. If a plastic with some desirable properties has a "T"g which is too high, it can sometimes be combined with another in a copolymer or composite material with a "T"g below the temperature of intended use. Note that some plastics are used at high temperatures, e.g., in automobile engines, and others at low temperatures.

In glasses (including amorphous metals and gels), "T"g is related to the energy required to break and re-form covalent bonds in a somewhat less than perfect (may be regarded as an understatement) 3D lattice of covalent bonds. The "T"g is therefore influenced by the chemistry of the glass. E.g., add B, Na, K or Ca to a silica glass, which have a valency less than 4 and they help break up the 3D lattice and reduce the "T"g. Add P which has a valency of 5 and it helps re-establish the 3D lattice, increasing "T"g.


Measurement of "T"g for glasses

250px|thumb|Measurement_of_Tg by DSC. Tg is the temperature corresponding to point A. [ "T"g measurement of glasses] ] ]


250px|thumb|Determination_of_Tg for glasses by dilatometry. The linear sections below and above "T"g are marked green; "T"g is the temperature at the point of intersection of the corresponding red regression lines.]

In contrast to the viscosity the thermal expansion, heat capacity, and many other properties of inorganic glasses show a "relatively" sudden change at the glass transition temperature. This effect is used for measurement by Differential scanning calorimetry (DSC) and dilatometry.



Proteins also possess a glass transition temperature below which both anharmonic motions and long-range correlated motion within a single molecule are quenched. The origin of this transition is primarily due to "caging" by glassy water [cite journal | author= Vitkup D, Ringe D, Petsko GA, Karplus M | title= Solvent mobility and the protein 'glass' transition | journal=Nature Structural Biology | year=2001 | volume=7 | pages=34&ndash;38 | doi= 10.1038/71231 Entrez Pubmed|10625424] , but can also be modeled in the absence of explicit water molecules, suggesting that part of the transition is due to internal protein dynamics. [cite journal | author= Salsbury FR, Han WG, Noodleman L, Brooks CL | title= Temperature-dependent behavior of protein-chromophore interactions: A theoretical study of a blue fluorescent antibody| journal=Chemphyschem | year=2003 | volume=4 | pages=848&ndash;855 | doi= 10.1002/cphc.200300694 Entrez Pubmed|12961983]


Glass transition temperature of some materials

Polymer"T"g (°C)
Polyethylene (LDPE)−105 or −30 also cited
Polypropylene (atactic)−20
Poly(vinyl acetate) (PVAc)28
Polyethylene terephthalate (PET)69
Poly(vinyl alcohol) (PVA)85
Poly(vinyl chloride) (PVC)81
Polypropylene (isotactic)0
Poly-3-hydroxybutyrate (PHB)15
Poly(methylmethacrylate) (atactic)105
Chalcogenide AsGeSeTe245
Avatrel; Polynorbornene215
Tyre Rubber100-160 [Citation
inventor-last =GALIMBERTI
inventor-first =Maurizio
inventor2-last =CAPRIO
inventor2-first =
publication-date =03.07.2003
issue-date = 21.12.2001
country-code =EU
patent-number =WO03053721
Soda-lime glass520-600
Fused quartz1175


References and footnotes

* For glass transition temperatures of various resins, see "Engineered Materials Handbook—Desk edition." (1995). ASM International. ISBN 0871702835. p. 369.
* For glass transition temperatures of various glasses, see Mazurin, O.V. "Handbook of Glass Data." (1993). Elsevier. ISBN 0444816356.

External links

* [ Vogel-Tammann-Fulcher Equation Parameters]
* [ Fragility thy name is glass]
* [ On the glassy state of multiphase and pure polymer materials ]
* [ Liquid fragility and the glass transition in water and aqueous solutions]
* [ Colloidal Glasses]

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