- Stern-Volmer relationship
The Stern-Volmer relationship, named after
Otto Stern andMax Volmer , [ O. Stern and M. Volmer "Über die Abklingzeit der Fluoreszenz", "Physik. Zeitschr." 20 183-188 (1919) as cited in Mehra and Rechenberg, Volume 1, Part 2, 2001, 849.] allows us to explore the kinetics of a photophysical "intermolecular" deactivation process.Processes such as
fluorescence andphosphorescence are examples of "intramolecular" deactivation (quenching) processes. An "intermolecular" deactivation is where the presence of another chemical species can accelerate the decay rate of a chemical in its excited state. In general, this process can be represented by a simple equation::
or
:
where A is one chemical species, Q is another (known as a quencher) and * designates an excited state.
The kinetics of this process follows the Stern-Volmer relationship::Where is the intensity, or rate of fluorescence, without a quencher, is the intensity, or rate of fluorescence, with a quencher, is the quencher rate co-efficient, is the fluorescence lifetime of A, without a quencher present and is the concentration of the quencher.Permyakov, Eugene A.. [Luminescent Spectroscopy of Proteins] , CRC Press, 1993.]
For "diffusion-limited" quenching ("i.e.", quenching in which the time for quencher particles to diffuse toward and collide with excited particles is the limiting factor, and almost all such collisions are effective), the quenching rate coefficient is given by , where is the ideal gas constant, is temperature in Kelvin and is the viscosity of the solution. This formula is derived from the
Stokes-Einstein relation . In reality, only a fraction of the collisions with the quencher are effective at quenching, so the true quenching rate coefficient must be determined experimentally. [ [http://www.stetson.edu/~wgrubbs/datadriven/quenching/quenchingwtg.html Fluorescence lifetimes and dynamic quenching] ]See also
Optode , a chemical sensor that makes use of this relationshipSources and notes
Wikimedia Foundation. 2010.