The Mayo–Lewis equation or copolymer equation in polymer chemistry describes the distribution of monomers in a copolymer. It was proposed by Frank R. Mayo and Frederick M. Lewis.[1]
The equation considers a monomer mix of two components
M1
M2
* | |
M | |
1 |
* | |
M | |
2 |
k
* | |
M | |
1 |
+M1\xrightarrow{k11
* | |
M | |
1 |
+M2\xrightarrow{k12
* | |
M | |
2 |
+M2\xrightarrow{k22
* | |
M | |
2 |
+M1\xrightarrow{k21
r1=
k11 | |
k12 |
r2=
k22 | |
k21 |
The copolymer equation is then:[3] [4] [2]
d\left[M1\right] | = | |
d\left[M2\right] |
\left[M1\right]\left(r1\left[M1\right]+\left[M2\right]\right) | |
\left[M2\right]\left(\left[M1\right]+r2\left[M2\right]\right) |
with the concentrations of the components in square brackets. The equation gives the relative instantaneous rates of incorporation of the two monomers.[4]
Monomer 1 is consumed with reaction rate:[5]
-d[M1] | |
dt |
=k11[M1]\sum[M
*] | |
1 |
+k21[M1]\sum[M
*] | |
2 |
*] | |
\sum[M | |
1 |
*] | |
\sum[M | |
2 |
Likewise the rate of disappearance for monomer 2 is:
-d[M2] | |
dt |
=k12[M2]\sum[M
*] | |
1 |
+k22[M2]\sum[M
*] | |
2 |
Division of both equations by
*] | |
\sum[M | |
2 |
d[M1] | |
d[M2] |
=
[M1] | |
[M2] |
\left(
| ||||||||||||||||||||||
|
\right)
The ratio of active center concentrations can be found using the steady state approximation, meaning that the concentration of each type of active center remains constant.
| |||||||
dt |
=
| |||||||
dt |
≈ 0
The rate of formation of active centers of monomer 1 (
* | |
M | |
2 |
+M1\xrightarrow{k21
* | |
M | |
1 |
+M2\xrightarrow{k12
k21[M1]\sum[M
*] | |
2 |
=k12[M2]\sum[M
*] | |
1 |
or
| |||||||
|
=
k21[M1] | |
k12[M2] |
Substituting into the ratio of monomer consumption rates yields the Mayo–Lewis equation after rearrangement:[4]
d[M1] | |
d[M2] |
=
[M1] | |
[M2] |
\left(
| ||||||||||
|
\right)=
[M1] | |
[M2] |
\left(
| |||||||
|
\right)=
[M1] | |
[M2] |
\left(r1\left[M1\right]+\left[M2\right]\right) | |
\left(\left[M1\right]+r2\left[M2\right]\right) |
It is often useful to alter the copolymer equation by expressing concentrations in terms of mole fractions. Mole fractions of monomers
M1
M2
f1
f2
f1=1-f2=
M1 | |
(M1+M2) |
Similarly,
F
F1=1-F2=
dM1 | |
d(M1+M2) |
These equations can be combined with the Mayo–Lewis equation to give[6] [4]
F1=1-F
|
This equation gives the composition of copolymer formed at each instant. However the feed and copolymer compositions can change as polymerization proceeds.
Reactivity ratios indicate preference for propagation. Large
r1
* | |
M | |
1 |
M1
r1
* | |
M | |
1 |
M2
r2
* | |
M | |
2 |
M2
M1
r1 ≈ r2>>1
r1 ≈ r2>1
r1 ≈ r2 ≈ 1
r1 ≈ r2 ≈ 0
r1
r2
r1>>1>>r2
r<1
Calculation of reactivity ratios generally involves carrying out several polymerizations at varying monomer ratios. The copolymer composition can be analysed with methods such as Proton nuclear magnetic resonance, Carbon-13 nuclear magnetic resonance, or Fourier transform infrared spectroscopy. The polymerizations are also carried out at low conversions, so monomer concentrations can be assumed to be constant. With all the other parameters in the copolymer equation known,
r1
r2
One of the simplest methods for finding reactivity ratios is plotting the copolymer equation and using nonlinear least squares analysis to find the
r1
r2
The Mayo-Lewis method uses a form of the copolymer equation relating
r1
r2
r2=
f1 | \left[ | |
f2 |
F2 | (1+ | |
F1 |
f1r1 | |
f2 |
)-1\right]
For each different monomer composition, a line is generated using arbitrary
r1
r1
r2
r1
r2
Fineman and Ross rearranged the copolymer equation into a linear form:[11]
G=Hr1-r2
where
G=
f1(2F1-1) | |
(1-f1)F1 |
H=
| |||||||
|
Thus, a plot of
H
G
r1
-r2
The Fineman-Ross method can be biased towards points at low or high monomer concentration, so Kelen and Tüdős introduced an arbitrary constant,
\alpha=(HminHmax)0.5
where
Hmin
Hmax
H
η=
\left[r | ||||
|
\right]\mu-
r2 | |
\alpha |
where
η=G/(\alpha+H)
\mu=H/(\alpha+H)
η
\mu
-r2/\alpha
\mu=0
r1
\mu=1
A semi-empirical method for the prediction of reactivity ratios is called the Q-e scheme which was proposed by Alfrey and Price in 1947.[13] This involves using two parameters for each monomer,
Q
e
M1
M2
k12=P1Q2exp(-e1e2)
while the reaction of
M1
M1
k11=P1Q1exp(-e1e1)
Where P is a proportionality constant, Q is the measure of reactivity of monomer via resonance stabilization, and e is the measure of polarity of monomer (molecule or radical) via the effect of functional groups on vinyl groups. Using these definitions,
r1
r2