The Yukawa–Tsuno equation, first developed in 1959,[1] is a linear free-energy relationship in physical organic chemistry. It is a modified version of the Hammett equation that accounts for enhanced resonance effects in electrophilic reactions of para- and meta-substituted organic compounds. This equation does so by introducing a new term to the original Hammett relation that provides a measure of the extent of resonance stabilization for a reactive structure that builds up charge (positive or negative) in its transition state. The Yukawa–Tsuno equation can take the following forms:
log
| kX | |
| k0 |
=\rho(\sigma+r(\sigma+-\sigma))
log
| kX | |
| k0 |
=\rho(\sigma+r(\sigma--\sigma))
where and represent the rate constants for an X-substituted and unsubstituted compound, respectively; represents the Hammett reaction constant; represents the Hammett substituent constant; and represent the Hammett substituent constants for reactions in which positive or negative charges are built up at the reactive center, respectively; and represents the Yukawa–Tsuno parameter.
The Hammett substituent constant,, is composed of two independent terms: an inductive effect and a resonance polar effect . These components represent the consequences of the presence of a particular substituent on reactivity through sigma and pi bonds, respectively. For a particular substituent, the value of is generally assumed to be a constant, irrespective of the nature of the reaction; however, it has been shown that for reactions of para-substituted compounds in which the transition state bears a nearly full charge, does not remain constant, and thus, the sum
\sigma=\sigmaR+\sigmaI
In their 1959 publication, Yukawa and Tsuno attributed observed deviations from Hammett Plot linearity in electrophilic reactions to additional resonance effects occurring through the pi bonds of substituent groups in their compounds. This implied that the inductive component of the Hammett substituent constant remains constant in such reactions, while the resonance component,, does not. From this assumption, the two scientists defined a new resonance substituent constant,, that is mathematically represented as follows:
\begin{align} G(R)&=\sigma+-\sigma\\ &=
| + | |
| (\sigma | |
| I |
+
| + | |
| \sigma | |
| R) |
-(\sigmaI+\sigmaR) \\ &=
| + | |
| \sigma | |
| R |
-\sigmaR \end{align}
for a reaction in which positive charge is built up at the reactive center in the transition state. In order to quantify the extent of the observed enhanced resonance effects, Yukawa and Tsuno introduced an enhanced resonance parameter,, that quantifies the "demand for resonance" at the reactive center.[2] Thus, the resultant Yukawa–Tsuno effective substituent constant is given by:
\sigma'=\sigma+rG(R)=\sigma+r(\sigma+-\sigma)
and the Yukawa–Tsuno equation (modified Hammett equation) takes the form:
\begin{align}log
| kX | |
| k0 |
&=\rho\sigma' \\ &=\rho(\sigma+r(\sigma+-\sigma)) \end{align}
Values of
\sigma+-\sigma
The enhanced resonance parameter,, is a measure of the influence of resonance on a new reaction. When
r=0
r>0
r<0
The enhanced resonance parameter is determined by first establishing the Hammett Reaction constant from data collected from meta-substituted compounds, and subsequently correlating the remaining data to fit the modified equation described above.
The Yukawa–Tsuno equation allows for treatment of both para- and meta- substituents, and it also better correlates data from reactions with high electron demand than the original Hammett equation.[4] However, this equation does not take into account the effects of various solvents on organic reactions. Also, Yukawa and Tsuno note that, even within a group of similar reactions, -values for more electron-withdrawing substituents tend to be higher than predicted—seen as a slight increase in slope on a Yukawa–Tsuno plot—and thus, are not as strongly correlated with the remainder of the data.