The Stern-Volmer plot is used to study the interaction dynamics between a fluorescent emitter and a quencher (a substance that reduces the fluorescence intensity). The plot shows the ratio of the fluorescence intensity as a function of the quencher’s concentration [Q], described by Eq. 1:
 
Where I0 and I are the fluorescence intensity in the absence and presence of a quencher respectively and KSV is the Stern-Volmer constant. For systems showing only dynamic quenching, KSV can be determined from the slope of the Stern-Volmer plot, as shown in Figure 1.
Figure 1. Example of an intensity Stern-Volmer plot of the system fac-Ir(ppy)3 and the quencher 2,4dinitrotoluene. The slope provides the Stern-Volmer constant.
The Stern-Volmer constant provides information about the sensitivity of the quenching system and, for dynamic quenching, is given by Eq. 2: 
Since the relative change in intensity I0/I is proportional to a corresponding change in fluorescence lifetime, Eq. 1 can also be written as a function of lifetime (Eq. 3). This allows a dynamic quenching interaction to also be characterised from changes in the fluorescence lifetime. The Stern-Volmer constant KSV and bimolecular quenching constant, kq, can be determined as a function of changes in lifetime with quencher concentration (Figure 2).  
Figure 2. Example of a lifetime Stern-Volmer plot of the system fac-Ir(ppy)3 and the quencher 2,4dinitrotoluene. The slope provides the Stern-Volmer constant.
A linear relationship in the Stern-Volmer (SV) plot is the most common behaviour of fluorescence quenching. However, upward, or downward deviation behaviour is also possible (Figure 3).
Figure 3. Stern-Volmer plot for quenching systems showing linear relationship (red curve); upward deviation relationship (blue curve); and downward deviation (green curve).
A linear relationship is most associated with dynamic quenching, where the quenching is mainly due to collisions between the emitter and quencher molecules. However, the linear relationship on the Stern-Volmer plot can also be associated with a purely static quenching system. Since static quenching does not show changes in the emission lifetime as a function of the quencher concentration lifetime measurements can be used to distinguish between the two.1
The upward/positive deviation is found in systems in which both static and dynamic quenching are contributing to the decrease in fluorescence intensity. A downward/negative deviation is generally associated with the presence of two emitters with different Stern-Volmer constants, e.g., for the same concentration of quencher, the emitters will be quenched at different rates. In most cases, at lower concentrations of quencher, a linear relationship is evident; however, as the quencher concentration increases, the relationship becomes non-linear.

 
															 
															 
															 
															