Cellulose sorbents obtained by the action of Lewis acids

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Pure & Appl. Chern., Vol. 61, No. 11, pp. 1993-1996, 1989. Printed in Great Britain. @ 1989 IUPAC Cellulose sorbents obtained by the action of Lewis acids V. A. Afanasevi P. I. Sarybaeva. A. S. Sultankulova, T. V. Vasilkova Institute of Organic Chemistry, Kirghiz Academy of Sciences, Frunze, USSR Abstract - An investigation has been carried out of the mechanism of the destruction of cellulose in anhydrous media in the presence of aprotic acids, such as TiCI4, SbCI5. SnCI4. AICl3, of the type (MX,) [ll. This enables us to determine the conditions for the formation of cellulose with a maxi- mum degree of polymerization. On the basis of these results methods have been developed for producing a new type of cellulose powder modified by Le- wis acids. This cellulose is different from that obtained by hydrolysis to a maximum degree of polymerization in the presence of protic acids as the catalyst. The difference lies in the complex structural nature of the cellulose powder. Cellulose powder (CP), modified by Lewis acids in the thermocatalytic destruction process with aprotic acids of the type MXn (TiCI4, SbCI5, SnCI4, AIC13, etc) in organic solvents' 11, 21, differs from microcrystalline (MC) cellulose obtained by hydrolysis to a maximum degree of polymerization in the presence of protic acids. The difference consists in the complex structural characteristics of CP. Scanning electron microscopic studies of CP have shown the presence of numerous deep fissures in and transverse fractures of the fibers (Fig. 1). only a weakly defined structure; the separation of fibers into more elementary formations are not typical. of a brittle destruction. The surface of the fibers has The fracture site is as a rule in an irregular tapered form characteristic This makes it possible to describe the destruction process on the basis of the mechanism of polymer destruction due to the external load. Such destruction involves the simulta- neous fracturing of numerous glucoside bonds through all the sections of the fiber. Ac- cording to a widely held concept, the fracturing of macromolecules under the action of a mechanical load results from the accumulation of a critical concentration of thermal energy acting on the chemical bond (the thermofluctuation hypothesis 131 1. tions of thermocatalytic destruction the external mechanical load is absent we can assume that the internal stretching serves as a source of stress. This stress lowers the energy barrier of the degradation process in the macromolecule. plained as follows. As is known, the crystalline and amorphous zones in cellulose differ in their thermophysical properties. ter mobility of the elementary linkages as compared with the crystalline zones. the supermolecular structure of cellulose is characterized lengthwise by a regularly alternat- ing ordered and disordered zones, the same macromolecule can cross several zones with dif- ferent thermophysical characteristics. It also known that cellulose has a negative coefficient of longitudinal thermal expansion [41. Id view of the entropy nature of the resilience of elastic polymers, the negative coefficient of thermal expansion can be regarded as a result of the transverse and at the same time longitudinal compression of zones due to an increase in the conformational mobility of inter- atomic linkages with an increase in temperature. It can be assumed that the longitudinal compression of the amorphous zones is the internal source of the resultant stresses. These stresses act on the glucoside linkages of the macromolecules passing through in the adjacent regions of the crystallites. This facilitates their fracture as a result of the simultaneous action of thermal fluctuations and coordination of the active centers in the macromolecules with the acidic reagents. Local fractures of fibrils within a bundle of macromolecules can be considered to be submicro- scopic cracks. ternal mechanical stresses. brittle destruction of the primary cellulose fibers which we have observed during our electron microscopic investigation of the samples (Fig. 1). On the analogy of the kinetic theory of mechanical destruction of solid bodies we can assume that the thermocatalytic destruction of the cellulose fibers is caused by the progressive accumulation of submicroscopic cracks un- til they reach a critical concentration. which led to the fracturing of fibers along the traverse cracks [3]. Since under the condi- The internal stretching can be ex- The amorphous zones have greater heat capacity and entropy owing to the grea- But since IS The stresses weaken the glucoside bonds. These cracks are analogous to fractures in the macromolecules caused by ex- These defects do not yet give rise to macroscopic effects of the Following this the cracks merge into larger cracks 1993

Transcript of Cellulose sorbents obtained by the action of Lewis acids

Page 1: Cellulose sorbents obtained by the action of Lewis acids

Pure & Appl. Chern., Vol. 61, No. 11, pp. 1993-1996, 1989. Printed in Great Britain. @ 1989 IUPAC

Cellulose sorbents obtained by the action of Lewis acids V. A. Afanasevi P. I . Sarybaeva. A. S. Sultankulova, T. V. Vasilkova

Ins t i tu te of Organic Chemistry, K i rgh iz Academy of Sciences, Frunze, USSR

Abstract - A n investigation has been car r ied o u t o f t h e mechanism of the dest ruct ion of cellulose in anhydrous media in the presence of aprot ic acids, such as TiCI4, SbCI5. SnCI4. AICl3, of the t y p e (MX,) [ll. This enables u s t o determine the condit ions f o r the formation of cellulose w i th a maxi- mum degree of polymerization. On t h e basis of these resul ts methods have been developed f o r producing a new t y p e o f cellulose powder modified by Le- wis acids. Th is cellulose i s d i f fe ren t f rom tha t obtained by hydro lys is t o a maximum degree of polymerization in the presence of p ro t i c acids as the cata lyst . The dif ference lies in the complex s t ruc tu ra l nature of t h e cellulose powder.

Cellulose powder (CP), modified by Lewis acids in the thermocatalytic dest ruct ion process w i th aprot ic acids of the t y p e MXn (TiCI4, SbCI5, SnCI4, AIC13, e tc ) in organic solvents'

11, 21, d i f fe rs f rom microcrystal l ine (MC) cellulose obtained by hydro lys is t o a maximum degree of polymerization in the presence of p ro t i c acids. The dif ference consists in the complex s t ruc tu ra l characterist ics of CP.

Scanning electron microscopic studies of CP have shown the presence of numerous deep f issures in and t ransverse f ractures of t h e f ibers (F ig . 1 ) . on ly a weakly defined structure; the separation of f ibers in to more elementary formations are no t typical. o f a b r i t t l e destruction.

The surface of t h e f ibers has

The f r a c t u r e s i te i s as a r u l e in an i r regu la r tapered form characterist ic

Th is makes it possible t o describe the dest ruct ion process on the basis of t h e mechanism of polymer dest ruct ion due t o the external load. Such dest ruct ion involves t h e simulta- neous f r a c t u r i n g of numerous glucoside bonds t h r o u g h all the sections of t h e f i b e r . Ac- cord ing t o a widely held concept, the f r a c t u r i n g of macromolecules under t h e action of a mechanical load resul ts f rom the accumulation of a cr i t ica l concentration of thermal energy act ing on the chemical bond ( t h e thermofluctuation hypothesis 131 1 . t ions of thermocatalytic dest ruct ion the external mechanical load i s absent we can assume tha t the in ternal s t re tch ing serves as a source of stress. Th is stress lowers the energy bar r ie r o f the degradation process in the macromolecule. plained as follows.

As is known, the crysta l l ine and amorphous zones in cellulose d i f f e r in t h e i r thermophysical propert ies. t e r mobil i ty o f the elementary l inkages as compared w i th the crysta l l ine zones. the supermolecular s t ruc tu re of cellulose is characterized lengthwise by a regu la r ly alternat- ing ordered and disordered zones, the same macromolecule can cross several zones w i th dif- ferent thermophysical characterist ics.

I t also known tha t cellulose has a negative coefficient o f longitudinal thermal expansion [41. I d view of the ent ropy na ture of the resil ience of elastic polymers, the negative coeff icient o f thermal expansion can be regarded as a resul t o f the t ransverse and a t t h e same time longitudinal compression of zones due t o an increase in the conformational mobil i ty o f in te r - atomic l inkages w i th an increase in temperature. I t can be assumed tha t t h e longitudinal compression of the amorphous zones i s the in ternal source of the resul tant stresses. These stresses act on the glucoside l inkages of the macromolecules passing t h r o u g h in the adjacent regions of the crystal l i tes. T h i s faci l i tates the i r f rac tu re as a resu l t o f the simultaneous action of thermal f luctuations and coordination of the active centers in the macromolecules w i th t h e acidic reagents.

Local f ractures of f i b r i l s wi th in a bundle of macromolecules can b e considered t o be submicro- scopic cracks. ternal mechanical stresses. b r i t t l e dest ruct ion of the pr imary cellulose f ibers which we have observed during our electron microscopic investigation of the samples (F ig . 1 ) . On the analogy of t h e k inet ic theory of mechanical dest ruct ion of sol id bodies we can assume tha t the thermocatalytic dest ruct ion o f the cellulose f ibers i s caused by the progressive accumulation of submicroscopic cracks un- til they reach a cr i t ica l concentration. which led t o the f r a c t u r i n g of f ibers along the t raverse cracks [3 ] .

Since under the condi-

The in ternal s t re tch ing can be ex-

The amorphous zones have greater heat capacity and ent ropy owing t o the grea- B u t since

IS

The stresses weaken the glucoside bonds.

These cracks are analogous t o f ractures in the macromolecules caused by ex- These defects do not ye t g ive r i se t o macroscopic effects of the

Following t h i s the cracks merge in to larger cracks

1993

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( C )

Fig. 1 Fractured fragments of f ibers. Scanning electron microscope: a - CP-SbCI5 ( ~ 5 2 3 0 ) ; c - CP-TiCI4 ( ~ 2 0 7 0 )

b - CP - AIC13 ( ~ 4 1 9 0 ) d - CP-SnCI4 ($5230).

By examining the thermodestruction of cotton cellulose in the presence of TiCI4 by the low- angle x - ray scattering method we have analyzed the accumulation dynamics OF microcracks having dimensions of the order 90-100 A . increases l inearly wi th time. Our observations accord wi th the situation of the general de- struct ion of polymers under external stresses.

The mechanism of the destructive reaction of cellulose macromolecules in the presence of Lewis acids can be described as the coordination of the central oxygen atom in the acid wi th the semi-acetal (cycl ic o r glucoside) oxygen atom. to r bonds owing to the vacant orbital in the central oxygen atom and unpaired electrons of the oxygen atoms. As a resul t the carbon-oxygen bond becomes weaker and the f rac tu r ing of the bond takes place:

We have found tha t the concentration of the pores

This results in the formation of donor-accep-

HOH2C MXn I 0 7

HOH2C MXn L 6 -

I

II

HOH2C L O -

R - 0

HOH C HOH2C , L o -

L O - R 21 0 0 / - \rO;R

R-O-\YH / --I

AXn

K-"- '4 OH OH

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Cellulose sorbents obtained by the action of Lewis acids 1995

T(OC)

In this, according t o va r ian t I o f t h e reaction t h e f i rst carbon atom changes i n t o a carbonium ion, and according t o va r ian t II a f r a c t u r i n g o f t h e glucoside bond takes place a t t h e same time, leading t o t h e dest ruct ion o f t h e macromolecular chain.

T h e formation o f t h e MX -cellulose complex i s i nd i rec t l y confirmed by a small increase in t h e or ig ina l mass o f t h e cellu'lose. T h i s increase has been observed in all cases fol lowing t h e re - moval of an excess o f t h e cata lyst by washing t h e sample. If such cellulose i s subjected t o heat treatment a t 80-100 OC, t h e magnitude o f t h e average degree o f polymerization (DP o f these samples decreases considerably as compared w i t h t h e sample t h a t has been driegVat 20 OC; in other words, t h e sample undergoes destruction(cf., Table 1).

Changes in DPav caused by t h e drying temperature ( t h e samples were k e p t f o r 5 min in 0.1% MXn solut ion followed by washing o f f an excess o f t h e cata lyst )

1

TABLE 1.

T h e average degree of polymerization ( D P SnC14-C6H,4 AIC13-CC14

powder according to x-ray diffraction

20 1800 1390 1 DUO

?ore size (10 Large small

. .

105 200 320 240

Th is dest ruct ion can b e a t t r i bu ted t o t h e pre l iminary formation o f a Lewis acid-cellulose com- plex. A n i n f r a r e d spectral analysis shows the appearance of absorption bands which can b e a t t r i bu ted t o t h e formation o f oxygen-metal bonds. Thus, t h e i n f ra red spect ra o f cellulose samples-qestroyed in t h e presence o f TiCI,, a re found t o contain absorption bands a t 1100- 1000 cm due t o t h e C - 0 - T i bond.

As a resu l t of such a treatment we obtain cellulose in t h e form o f a powder whose character- is t ics are summarized in Table 2.

TABLE 2.

Lewis ac id DPav Fract ion w i t h Mois ture Ash content COOH-group CO-group

Some proper t ies of cellulose obtained by thermocatalyt ic dest ruct ion in the presence o f d i f f e ren t Lewis acids

DP4200 ( % I conten t (%) ( % I I%) (8 )

T i c & 110 100 4.1 0.34 0.69 0.48 SbCI5 120 100 5.2 0.32 0.65 0.45 SnCI4 130 97 4.1 0.34 0.54 0.42

BF3.O(Et I2 130 100 4.4 0.04 0.18 0.38

AIC13 150 95 5.1 0.31 0.12 0.24

Concn.of pores (~-10'3 cm-3 large small

1.09

1.02

0.97

1.02

0.91

Sample

Or ig ina l C

CP-AIC13

CP-SbCI5

CP-TiCI4

CP-SnCIu

92 CP-SnCI4

CP-TiCI4

CP-AIC13

CP-SbCI5

MC

a4

a2

81

79

Degree r-rap diff- :action ( X )

191 77

196 101

221 97

202 95

197 100

186 90

0.76

0.70

0.68

0.65

0.62

57 3676

312 2541

163 1816

ao a70

60 558

21 265 -1 Or ig ina l c

ialysis lrystalli te limensions

(A) 71

77

67

a3

56

90

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Sample

The total concentrat ion of t h e o rde red por t ion o f t h e f i be rs remains a t t h e or ig ina l level o r somewhat below it ( t h e Nelson-O'Connor index; cf., Table 3 ) .

The obtained t r u e dimensions of t h e crysta l l i tes (cf. , Table 4) make it possible t o conclude t h a t in t h e presence of Lewis acids t h e reaction o f cellulose along t h e glucoside bonds de- s t roys t h e cellulose crysta l l i tes t o a lesser degree as compared w i t h hyd ro l ys i s in t h e p re - sence o f hydrochlor ic acid: t h e dimensions of t h e crysta l l i tes a re on ly 3-14% smaller t han t h e or ig ina l ones; while f o r MC samples they a re smaller by 22%. by the re la t ive ly small amount o f water-soluble f rac t i on formed (2-5%) ve rsus t h e 10% weight loss in t h e case o f h y d r o l y t i c d k t r u c t i o n .

A comparison o f t h e modified cellulose samples and MC samples by t h e low-angle x - r a y dif- ract ion method (Tab le 4) shows t h a t t he dimensions o f t h e micro- and submicrofissures, cap- i l lar ies and pores a re pract ica l ly identical. in CP samples i s 2-6 times greater t han t h e poros i ty o f t h e MC samples. We bel ieve t h a t t h e d i f ference in t h e degree o f poros i ty o f cellulose powders i s due t o t h e d i f ference in t h e abi l- i ty o f Lewis acids t o penetrate deep i n t o t h e cellulose f ibers . A n d consequently, t h e dif- ference i s due t o the number o f t ransverse cross l i nks formed by t h e coordinational reaction between t h e centra l atoms o f t h e Lewis acid and t h e oxygen atom in t h e polymer chain, as well as t o t h e establishment of bonds w i t h t h e carbonium ions formed in t h e course o f de- s t ruct ion.

T h e d is turbance o f t h e c rys ta l lattice, t h e formation o f a developed system o f micro- and submicro-capil laries, pores and f issures p rov ide a high internal specif ic sur face area o f t h e cellulose powders produced. In Table 5 are suamarized data on t h e specif ic sur face area o f samples which have been obtained by t h e gas-chromatographic method f rom t h e retent ion time o f n-hexane vapors and by t h e adsorption of benzoic acid f rom heptane solutions. p le served as t h e standard. ment [61 t he surface of modif ied cellulose powders in some cases reaches >500 m Ig.

These resu l t s a re also confirmed

A t t h e same time t h e concentrat ion o f t h e pores

A MC sam- It was found t h a t under t h e condit ions o f an addit ional t rea t -

Specif ic surface area (m' lq) x - r a y d i f f rac t ion gas-chromatographic sorpt ion of benzoic acid

TABLE 5. Specif ic sur face area and t h e absorption ab i l i t y o f cellulose powder

CP-SnCI4 3.5 86 10.1

CP-SbCI5 3.4

CP-AICl3 0.7

57

1.9

2.7

1.8

MC 1.5 1.8 1 .o Original C 0.6 1.7

The high poros i ty o f modified cellulose powders resu l t s in t h e i r greater adsorption o f t h e bromophenol b lue as compared w i t h t h e adsorption o f t h e d y e by t h e hyd ro l yzed cellulose.

A comparative s t u d y has been ca r r i ed ou t o f t h e separation capacity o f thin layers o f cel lu- lose powders obtained by t h e dest ruct ion o f cellulose in ethanol solut ions o f d i f f e ren t Lewis acids and t h a t o f MC powders. area of t he cellulose powders pract ica l ly have no ef fect on t h e i r separation capacity. sorbents w i t h part icles 20.1 - (0.5 mm in diameter p rov ide a good separation o f such amino acids mixtures as glycine-alanine-valine-leucine and alanine-phenylalanine-tyrosine-tryptophan. A good separation has been obtained also f o r t h e fol lowing mixtures: threonine-serine, g lu ta- mic acid-aminosuccinic acid, and arginine-lysine-histidine ( t h e d i f ference in Rf o f these compounds i s constant, be ing equal t o approximately 0.09) . a s ing le- run chromatographic separation appear as well-defined spots. t i on proceeds wi thout t h e formation o f t h e band-effect.

The resu l t s show t h a t t h e dif ferences in t h e specif ic sur face A l l t h e

Amino acids already on T h e separa-

1.

2.

3.

4.

5.

6.

REFERENCES R . I. Saybaeva, T . V. Vasilkova, V . A. Afanasev, l z v . Akad. Nauk K i rqh iz SSR No.2, 42-48 (1979). R. I. Sarybaeva, T. V. Vasilkova. Inventor 's Cert i f icate (USSR) No. 730692. Cf., u. - I zob. No. 16 ( 1980). G. M. Bartenev. T h e Stabi l i ty and Destruct ion Mechanism of Polymers, Khimiya, Moscow (19841, p.279. Yu. K . Godovsky. Thermal Physical Methods o f lnves t iqa t inq Polymers, Khimiya, Moscow [ 1976). I. N. Zhurkov, V. S. Kuksenko, A. I. Slutsker. Fiz. Tverdoqo Tela, 11, No.2, 296-307 (1969). R . I . Sarybaeva, T . V . Vasilkova, V . A. Afanasev ,, L. I. Dernovaya, Yu. A. Eltekov. Izv. Akad. Nauk K i rqh iz SSR, N0.2, 50-54 (1981).