The Absolute Rate Constants of Anionic Co-polymerization in the

The lack of termination in anionic polymerization permits one to determine directly the absolute rate constants of anionic co-polymerization. A capill...
1 downloads 0 Views 899KB Size
RATECONSTANTS OF COPOLYMERIZATION IN STYREXE SYSTEMS

March 5, 1963

[CONTRIBUTION FROM

THE DEPARTMENT OF CHEMISTRY, STATEUNIVERSITY COLLEGE OF AT SYRACUSE UNIVERSITY, SYRACUSE 10, hTEW YORK]

533

FORESTRY

The Absolute Rate Constants of Anionic Co-polymerization in the System Styrene-crMethylstyrene. The Effect of Polymer Structure on the Rate of Polymerization BY D. N. BHATTACHARYYA, C. L. LEE, J. SMIDAND M. SZWARC RECEIVED MAY10, 1962 The lack of termination in anionic polymerization permits one to determine directly the absolute rate constants of anionic co-polymerization, 4 capillary flow technique suitable for this purpose has been described. The systems investigated styrene and living polystyrene or- or p-methylstyrene. It was shown that here involved: living poly-or-methylstyrene the rate of addition of styrene to or-methylstyrene- ion depends on the counter-ion and on the structure of the polymer. I n particular, the nature of the penultimate unit, the type of linkage between the last unit and the penultimate unit and the size of polymeric molecule were shown to be factors influencing the rate constant of copolymerization.

+

The copolymerization of two monomers X and B involves four propagation steps, i.e. -A* -A* -B* *wB*

+ A + -A.A* + B +-AB* + A + -BA* + B +-BB*

kl.1

+

The addition of a monomer B to a solution of living polymers possessing terminal .A units leads to7 the reaction -A-

ki.2

k2.i ki.2

The star used in these equations represents a groiving chain and kl,', k',,, etc., denote the respective rate constants which are assumed to be independent of the nature of the preceding units and the type of their linkage. The success of this scheme in accounting for the numerous results of radical copolymerization provides perhaps the best argument for its validity (see the recent review of this field in Walling's monograph "Free Radicals in Solution"). The assumption that kl,', k l , ~etc., , are independent of the character of the preceding units is only a first approximation, and it was realized' that for some systems a more elaborated treatment2 might be required. In fact, systems have been reported3B4in which the effect of penultimate units upon the rate of growth is significant. The common technique used in studies of copolymerization kinetics is based on the relation that exists between the composition of the copolymer and of the feed.' This method, although satisfactory for radical Copolymerization, might fail in other systems, e.g., in anionic copo1ymerization.j It is desirable, therefore, to develop alternative techniques for determining the copolymerization rate constants in anionic polymerization. A novel technique useful for such a study is described in the present paper. This method is suitable for determining the absolute values of the rate constants of anionic copolymerization, while only their ratios could be determined by the conventional method. I t has the added advantage that it permits the direct investigation of the influence of the preceding units and of their mode of linkage upon the rate constants of propagation. The Method of Attack.-Under suitable conditions anionic polymerization may proceed without termination. The resulting polymer, referred to as a "living" polymer,6retains its ability to grow a t least for the time required to complete the experiment. The addition of a monomer to a solution of such polymers initiates further polymerization which may be followed by any suitable method. Since the concentration of growing ends can be determined, the results lead to the absolute values of the respective rate constants. (1) T. Alfrey, J. J. Bohrer a n d H. M a r k , "Copolymerization," Interscience Publishers, Inc., New York, N. Y . , 1952. (2) E. Mertz, T. Alfrey a n d G. Goldfinger, J . Polymer Sci.,1, 75 (1946). (3) pi. G . B a r b , ibid., 11, 117 (1953). (4) G. E. H a m , ibid.,45, 169 (19fiO). i.i)R. K . G r a h a m , D. L. I)unkelherg?r and W. E. (:node, J. A m C h m . SOC., 82, ,100(iwn). (6) (EL) .\I. Szwarc, 11. T.cvyantl K .3 l i l k o ~ i ~ c lY1h, i L , 7 8 , L"i>li ( l ! l X i ) , (tr) 31. S z r v w c , \'alum, 178, l l ( j 8 (1!)5G).

+ B + M-X.B-

k12

(1)

This reaction is then followed by reactions I1 and 111 m hich represent the homo-polymerization of the monomer R

+ +

h ~ ~ 1 . B - H + mvd.B B -A.Bn .BB --f wAB-1.B-

k'J,A

(11)

(111)

k2 2

The experiments are carried out under conditions which minimize the extent of the latter reactions. This is achieved by having higher concentrations of --A- than that of the monomer B, and by extrapolating the results to zero conversion, ;.e., by shortening the time of the reaction. Thus, the rate constant of copolymerization, kl,z, is determined by the initial rate of reaction. Mathematical Treatment of the Problem.-In the absence of termination the kinetics of the polymerization described by the equations I, I1 and 111is given by the differential equations -d [ -.i-]/dt = k i , ,[ ~ ~ 1 [B] -1 -d[Bl/dt = { k 1 , 2 [ . w A - I k2,z[-ABn-lj

+

(1) [Bl

(2)

in which we assume, for mathematical simplicity, that k'zz = k22. This simplification is permissible, since we shall be only concerned with the cases where the extent of homopropagation of the monomer B is negligible. A general solution of these equations is complicated. However, the results may be simplified if kl,z[-A-] >> k2,2[wABn-] or if kl,2 = k2,*, In the former case, the equations are reduced to -d[B]/dt

=

ki.?[*A-]

[B]

(3)

where Lw-4-I

=

[ ~ A - l o- ([Blo - [BI)

If the decrease in the monomer concentration [R]" - [B] is denoted by x , then equation 3 may be rewritten in the conventional form for a bholecular process, i.e. -d%/dt = ki,?(Ai, - %)(Bo-

(4)

X )

Hence, aplot of (Ao - Bo)-1 In { Bo(A40-x)/X~(B~ - x)} versus time should result in a straight line with a slope equal to k1.2, for a sufficiently short time interval. I n the second case when kl,? = k n 2 one may rewrite equation 2 in the form -d[Bl/dt

=

k1,2[-A-]o[Bl

+

- ki.r)[-XBn-I

[Bl

(5)

and for the initial stages of the polymerization, ( 5 ) is reduced to the conventional equation describing a first order reaction -d[B]/dt

ki.z[*S-]o[B]

(6)

The validity of this approximation is further strengthened if [ - t - ] " > [B]". Hence, for ( k l , z - k ? z ) [ R J " the plot of -(In [R]) [-.4 1"

-

( 7 ) I'm the sake r , l b r e v i t y t h e gr Na+ > K + > Cs+. On the other hand, the comparison of N a + and K + seems to be confusing. Actually, the data presented in Table I seem to indicate that for the same concentration of the growing ends the di-potassium salt of a-methylstyrene tetramer reacts slightly faster than the sodium salt. This observation may be misleading since i t is impossible to prepare the potassium salt of a-methylstyrene tetramer without contaminating i t with some amount of the dimer.g The dimer is more reactive than the tetramer and its presence in the potassium salt may account for the observed discrepancy. The following explanation may account for the observed counter-ion effect. Let us assume that in the transition state the counter-ion is located between the last unit of the polymer and the new one which is being added. as

CH3

CHzk- K +

I

Ph, T y p e of polymer

x B;

11

-2

Concn. living ends, X 103 M

Init. concn. of styrene, X lo* M

4.25 4.0

3.1 3.1

kw. I. mole-1

Yo Conversion 40-67 36-67

sec.-l

141 137

Kate constant of styrene addition to di-sodium salt of polystyrene possessing one unit of a-niethylstyrene a t each living end linked iii a head-to-tail fashioii Concn. of living ends X 10s M

Init. concn. of styrene X 10' M

2.:g 2.(i 3.3 3.8

2 . fj 2.6 2.7

1.5

Yo Conversion .It-fil X( )Hi1 34 -54 28-46

kw,

I. mole-] see.-'

Zion 1x10 1iOO

1470

Its increasing size interferes then with the nionomer's approach, making the incipient C-C bond longer, the activation energy of the process higher, and the rate constant lower. The structural factors affecting the rate of addition of styrene t o a-methylstyrene- ions seem to be steric in nature. The addition to cumene-, K + (see Table 111) is undoubtedly the fastest, the addition to a-niethylstyrene- unit preceded by styrene units (see Table I V ) is somewhat slower, and the addition to poly-a-methylstyrene possessing the terminal head-to-tail units (see Table IV) is by far the slowest. The rates of addition to the a-iiiethylstyrciic dimer or tctranicr, i n which all (12) (a) hi. Szwarc, "Advaiices in Clicmislry Series," No. 21, l!lG2, 11. !)ti, (I)) J. Sinid a n d M. Szwarc, . I I'ulymer . Sci., 61, 37 ( l W 2 ) .

537

RATECONSTANTS OF COPOLYMERIZATION IN STYRENE SYSTEMS

March 5, 1963

the units are presumably linked in a head-to-head or tail-to-tail fashion, are faster then the addition to the head-to-tail linked poly-a-methylstyrenes, although they are still slower than the other additions. The reactions involving the head-to-tail linked polya-methylstyrenes need further consideration. These polymers were prepared from the di-potassium salt of a-methylstyrene dimer by adding to it desirable amounts of a-methylstyrene. The polymer A (see Table IV) was formed by adding an amount of monomer sufficient to polymerize two molecules of a-methylstyrene with each dimer. (Of course, more than two equivalents had to be added to achieve such a result, since a fraction of the monomer remains in solution in equilibrium with the living polymer, see e.g., the paper by Vrancken, Smid and Szwarc.13) The polymer B (see Table IV) was prepared by adding twenty equivalents of the monomer to the dimer, thus producing a longer chain of head-to-tail linked units. The structure of the dimer was established9#14 as CH3

CHB

I 1

I

K+, -CCHzCHzC-, K +

I

Ph

Ph

The tetramer A = Tz should therefore have the structure CH3 CH3

CH3 CH)

Ph

Ph

I t 1 1 K+, -CCHzCCHzCHzCCHzC-, K + = T2 I I I 1 Ph

in the solution of Tz tetramer or the polymer were not responsible for the low rate constant of addition. It is interesting to notice that further addition of a-methylstyrene to the head-to-tail linked tetramer does not affect its reactivity (see Table IV). This observation parallels that made during the studies of equilibria between oligomers and polymers of a-methylstyrene and their monomer.13 The equilibrium constant was found to be larger for the addition to the headto-head linked terminal units than for the head-to-tail linked ones, and in the latter case, further increase in the length of the chain had no effect upon the equilibrium constant. Finally, attention should be drawn to the fact that the rate of addition to the dimer is greater than to the head-to-head-tail-to-tail linked tetramer, in spite of the fact that these two polymers possess identical terminal and penultimate units. This observation parallels again that ma.de in the course of the equilibrium studies.I3 Two interpretations may be suggested for these results : either the electrostatic repulsion between the neighboring ends of the dimer contributes to the free energy and activation energy of the process, or the binding of two dimers into tetramer affects the steric requirements of their terminal units, as is indeed shown by the models. We prefer the latter interpretation, since the rate of addition to cumene potassium was found to be extremely large, and of course no electrostatic repulsion may be invoked in this case.

Ph

First order reaction

although i t may also contain a small amount of CH3

-

laminar flow

CH3 CHB CH3

I I

I

l l

l l

K +,-CCH~CHZCCH~CCHZC-, K+ I

Ph

Ph

Ph

Ph

On the other hand, the tetramer TI produced directly from the monomer was shown to have the s t r ~ c t u r e ~ . ~ ~ CH3

Na+,

CH3 CH3

Ph

Ph

Ph

-

CH3

I I I -C!YLHZCHZC-CCHZCH~C-, I I I /

Na+ = TI

J. Smid amrl &I. Szwarc, 3'rons. 1:a~oiiay Sot., 68,

L'O:j(i (1902).

( I 1) C . 1;. lcraiik, c l