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The '''Vogel-Fulcher-Tammann law''' (VFT law) is an empirical relationship describing the dramatic slowing of dynamics in [[supercooled liquid]]s as they approach the [[glass transition]]. It states that a transport property—typically viscosity η or structural relaxation time τ—increases exponentially with decreasing temperature according to a modified Arrhenius form: η = η_0 exp(B/(T − T_0)), where T_0 is a temperature slightly below the [[Kauzmann temperature]] and B is a material-specific constant. The divergence at T_0 suggests a thermodynamic singularity, though whether this divergence is real or an artifact of the empirical fit remains one of the field's persistent questions.

== Historical Origins ==

The law was discovered independently by three researchers in the 1920s: Hans Vogel, Gordon Fulcher, and Hessel Tamman. Each observed that the viscosity of glass-forming liquids could not be fit by a simple Arrhenius law, which assumes a temperature-independent activation barrier. Instead, the apparent activation barrier itself increases as temperature decreases, as if the liquid must surmount ever-larger obstacles to rearrange its structure. This 'super-Arrhenius' behavior is the hallmark of fragile liquids, and the VFT law remains the most common functional form used to fit their temperature dependence.

== Connection to the Adam-Gibbs Theory ==

The [[Adam-Gibbs theory]] provides a thermodynamic rationale for the VFT law. It posits that the relaxation time depends on the size of the cooperative regions that must rearrange simultaneously, and that this size scales inversely with the [[configurational entropy]]. As the configurational entropy decreases toward zero at the [[Kauzmann temperature]], the cooperative regions diverge in size, and the relaxation time diverges with them. The Adam-Gibbs derivation yields a temperature dependence that closely resembles the VFT form, with the divergence temperature T_0 identified as the Kauzmann temperature T_K.

This connection is elegant but not airtight. The VFT law is empirical; the Adam-Gibbs theory is a thermodynamic argument. The agreement between them may be profound, or it may be a case of two different approximations converging to the same functional form. The divergence at T_0 has never been observed experimentally, because real liquids fall out of equilibrium at the glass transition temperature T_g, which lies above T_0. The VFT law therefore describes an extrapolated regime, not a measured one.

== Criticism and Alternatives ==

Critics of the VFT law argue that its apparent divergence is an artifact of the fitting function. Other empirical forms—such as the parabolic law, the power law, or the Mauro-Yue-Ellison-Gupta-Allan (MYEGA) equation—fit experimental data equally well without predicting a singularity. The parabolic law, in particular, is motivated by the [[mode-coupling theory]] and predicts a finite viscosity at all temperatures, consistent with the idea that the glass transition is a kinetic arrest rather than a thermodynamic singularity.

The debate over the VFT law is therefore a proxy for the larger debate over whether the glass transition has an underlying thermodynamic critical point. If the VFT divergence is real, then the glass transition is a masked phase transition. If the VFT divergence is merely a fitting artifact, then the glass transition is purely kinetic. The VFT law sits at the center of this disagreement because it is the oldest, most widely used, and most conceptually suggestive of the empirical fitting forms.

The VFT law is treated as the standard workhorse of glass physics, but its conceptual load is disproportionate to its empirical status. Three fitting parameters for a curve that never reaches its predicted divergence is not a theory—it is a very good interpolation dressed in theoretical ambition. The glass transition community's continued reliance on the VFT form as evidence for an underlying singularity is a case study in how a convenient empirical formula can become a conceptual prison.