Tammann and Hüttig temperatures

Tammann temperature was pioneered by German astronomer, solid-state chemistry, and physics professor Gustav Tammann in the first half of the 20th century.[1]^: 152 He had considered a lattice motion very important for the reactivity of matter and quantified his theory by calculating a ratio of the given material temperatures at solid-liquid phases at absolute temperatures. The division of a solid's temperature by a melting point would yield a Tammann temperature. The value is usually measured in Kelvins (K): [1]^: 152

${\displaystyle T_{\text{Tammann}}={\beta }{\times }T_{\text{melting point}}({\text{in K}})}$ [5]

where ${\displaystyle {\beta }}$ is a constant dimensionless number.

The threshold temperature for activation and diffusion of atoms at surfaces was studied by de:Gustav Franz Hüttig, physical chemist on the faculty of Graz University of Technology, who wrote in 1948 (translated from German):[6][7]

In the solid state the atoms oscillate about their position in the lattice. ... There are always some atoms which happen to be highly energized. Such an atom may become dislodged and switch places with another one (exchange reaction) or it may, for a time, travel about aimlessly. ... the number of diffusing atoms increases with rising temperature, first slowly, and in the higher temperature ranges more rapidly. For every metal there is a definite temperature at which the exchange process is suddenly accelerated. The relationship between this temperature and the melting point in degrees K is constant for all metals. ... On the basis of these elementary processes, sintering is analyzed in relation to the coefficient α which is the fraction of the melting point in degrees K ... When α is between 0.23 and 0.36, activation as a result of the surface diffusion takes place. Loosening or release of adsorbed gasses occurs simultaneously.

The Hüttig temperature for a given material is

${\displaystyle T_{\mathrm {\text{Hüttig}} }=\alpha \times T_{\mathrm {mp} }}$

where ${\displaystyle T_{\text{mp}}}$ is the absolute temperature of the material's bulk melting point (usually specified in Kelvin units) and ${\displaystyle \alpha }$ is a unitless constant that is independent of the material, having the value ${\displaystyle \alpha =0.3}$ according to some sources,[4][8] or ${\displaystyle \alpha =1/3}$ according to other sources.[9][10][11] It is an approximation to the temperature necessary for a metal or metal oxide surfaces to show significant atomic diffusion along the surface, sintering, and surface recrystallization. Desorption of adsorbed gasses and chemical reactivity of the surface often increase markedly as the temperature is increases above the Hüttig temperature.

The Tammann temperature for a given material is

${\displaystyle T_{\mathrm {Tammann} }=\beta \times T_{\mathrm {mp} }}$

where ${\displaystyle \beta }$ is a unitless constant usually taken to be ${\displaystyle 0.5}$, regardless of the material.[4][8][9][10] It is an approximation to the temperature necessary for mobility and diffusion of atoms, ions, and defects within a bulk crystal. Bulk chemical reactivity often increase markedly as the temperature is increased above the Tammann temperature.

The following table gives example Tammann and Hüttig temperatures calculated from each compound's melting point T_mp according to:

T_Tammann = 0.5 × T_mp

T_Hüttig = 0.3 × T_mp

• Chemical kinetics – Study of the rates of chemical reactions
• Chemical thermodynamics – Study of chemical reactions within the laws of thermodynamics
• Glass transition – Reversible transition in amorphous materials
• Surface melting – thin film of liquid at interface between solid and gasPages displaying wikidata descriptions as a fallback