Polymer International Polym Int 53:1169–1175 (2004) DOI: 10.1002/pi.1527 Chain structure of polyethylene/polypropylene in-reactor alloy synthesized in gas phase with spherical Ziegler–Natta catalyst Zhisheng Fu, Zhiqiang Fan,∗ Yanzhong Zhang and Junting Xu The Institute of Polymer Science, Department of Polymer Science and Engineering, Zhejiang University, Hangzhou 310027, China Abstract: Two polyethylene/polypropylene (PE/PP) in-reactor alloy samples were synthesized by multistage gas-phase polymerization using a spherical Ziegler–Natta catalyst. The alloys show excellent toughness and stiffness. FTIR, 13 C-NMR and thermal analysis proved that the alloys are mainly composed of polyethylene, PE-block-PP copolymer and polypropylene. There are also a few percent of ethylenepropylene segmented copolymer with very low crystallinity. The block copolymer fraction accounts for more than 25 % of the alloy. The role of the block copolymer as compatibilizer between PE and PP is believed to be the key factor that results in the excellent toughness–stiffness balance of the material. 2004 Society of Chemical Industry Keywords: chain structure; PE/PP in-reactor alloy; gas phase; spherical catalyst; mechanical properties INTRODUCTION Modification of polypropylene (PP) aimed at improving impact strength is a topic of great significance in science and industry.1 – 6 Among the ways to toughen PP, in-reactor blending of PP with other polyolefins (eg, ethylene-propylene statistical copolymer) by sequential multi-stage polymerization has been proved superior both in respect of polymer properties and production cost.4 – 10 Polypropylene/poly(ethylene-copropylene) (PP/EPR) in-reactor alloy has been industrialized on large scale. However, because there is more than 10 % of statistical copolymer with very low modulus in the PP/EPR in-reactor alloy, this kind of toughened PP suffers from a significant drop in flexural modulus as compared to PP homopolymer. A possible way to overcome this drawback is to replace the EPR with polyethylene (PE) in the alloy, as PE is a crystalline polymer with moderate rigidity. Though the preparation of PP/PE blends by multi-stage polymerization was reported many years ago,11 the toughness–stiffness balance of the material seems not to be attractive, and commercialization of this kind of polyolefin is quite limited compared to PP/EPR in-reactor alloy (so-called block PP or PP-b). Chain structure and physical properties of propyleneethylene sequential polymerization products, which were prepared by using TiCl3 -based catalysts, have been studied by several groups.12 – 16 As the PP and PE homopolymer chains were not separated from the block copolymer chains in these studies, the structure of the components of the studied polyolefins were not identified on solid experimental bases. Since the 1990s, the main progress in the production of PP in-reactor alloy has been the use of a spherical Ziegler–Natta catalyst.5,6,10,17 PP/EPR alloy synthesized by spherical catalyst is in the form of regular spherical granules and shows better mechanical properties compared to the conventional catalyst system. The main reason for the better properties of the spherical in-reactor alloy is the more uniform dispersion of the second polymer in the alloy, as the polymer formed in the second stage (ie EPR) is limited to the tiny pores of the spherical polymer particles produced in the first stage of polymerization. The polymerization process also benefits from the spherical shape of the polymer granules, as risks of scaling and fouling in the reactor can be reduced. However, the preparation of PP/PE in-reactor alloy using spherical Ziegler–Natta catalyst has not been reported in the literature. Recently we have studied the chain-structure of PP/PE in-reactor alloy using a super-active spherical Ziegler–Natta catalyst.18 It was found that the in-reactor alloys show both high impact strength and high flexural modulus. Such good balance between toughness and stiffness is very important for applications as high-performance structural materials. However, when the in-reactor alloy is synthesized by first polymerizing propylene to form spherical PP granules in the first stage and then polymerizing ∗ Correspondence to: Zhiqiang Fan, The Institute of Polymer Science, Department of Polymer Science and Engineering, Zhejiang University, Hangzhou 310027, China E-mail: fanzq@zju.edu.en Contract/grant sponsor: Special Funds for Major State Basic Research Projects; contract/grant number: G1999064803 (Received 30 June 2003; revised version received 17 August 2003; accepted 3 February 2004) Published online 1 June 2004 2004 Society of Chemical Industry. Polym Int 0959–8103/2004/$30.00 1169 Z Fu et al ethylene in the second stage, the particles of the final product are mostly broken. This phenomenon actually eliminates the advantages of using a spherical catalyst. In this paper, we will report on the chain structure and mechanical properties of a new type of in-reactor alloy composed of PP and PE, which is synthesized by polymerizing ethylene in the first stage and propylene in the second stage in a sequential reaction mode. To distinguish this type of polyolefin alloy from the conventional PP/PE alloy reported in the literature, we name it as PE/PP in-reactor alloy. Our experiment results show that the granules of the PE/PP alloy are mostly in the spherical form, and the toughness–stiffness balance of the alloy is even better than that of the conventional PP/PE alloy. EXPERIMENTAL Synthesis of the PE/PP alloy The PE/PP in-reactor alloy was synthesized in a threestage polymerization process. In the first stage, or the pre-polymerization stage, the slurry polymerization of propylene was conducted in a well-stirred glass reactor for 30 min. A high-yield spherical Ziegler–Natta catalyst, TiCl4 /MgCl2 ·ID (ID is internal donor diisobutyl phthalate), kindly donated by the Beijing Research Institute of Chemical Industry, was used in the polymerization. The catalyst has a Ti content of 3 wt%. Al(C2 H5 )3 (Fluka) was used as the cocatalyst (with Al/Ti = 60) and Ph2 Si(OCH3 )2 as the external donor (Al/Si = 25). 30 ml petroleum ether (bp 60–90 ◦ C) was used as the solvent. Propylene pressure in the pre-polymerization stage was 1 atm, and the temperature was 50 ◦ C. A catalyst efficiency of 15–20 g PP/g catalyst was obtained in this stage. After the pre-polymerization, the slurry containing the pre-polymerized catalyst was transferred to a 0.5 l jacketed Buchiglasuster autoclave. Propylene in the slurry was removed by evacuating the autoclave to 5 mmHg for 3 s, and ethylene was filled into the autoclave to 0.6 MPa. Ethylene homopolymerization was carried out for 1 h. Polymerization temperature for the high ethylene content sample (HEP) was 70 ◦ C, and that for the low ethylene content sample (LEP) was 60 ◦ C. It was found that after about 20 min of ethylene polymerization, all the petroleum ether in the reactor was thoroughly absorbed into the polymer granules, so the polymerization can be regarded as a gas-phase process. At the end of this stage, ethylene was removed by evacuating to 5 mmHg for 3 min, and propylene was filled to the autoclave and then continuously supplied to the reactor at 0.7 MPa for 2 h. After the gas-phase propylene polymerization stage, the reaction was terminated, and the product was washed with ethanol and dried in vacuum. The total catalyst efficiency for the three-stage polymerization is in the range of 3–4 × 103 g polymer/g catalyst. Fractionation of PE/PP alloy A modified Kumagawa extractor was used to carry out temperature-gradient extraction fractionation 1170 (TGEF) of the polymer.19 n-Octane was used as the solvent to successively extract the sample at a number of controlled temperatures (room temperature, 90, 110 and 120 ◦ C). Five fractions were collected at 25, 90, 110, 120 and >120 ◦ C from each alloy, in which the >120 ◦ C fraction is the residual sample after the extraction. The fractions were named 25 ◦ C fraction, 90 ◦ C fraction, 110 ◦ C fraction, 120 ◦ C fraction and >120 ◦ C fraction. Purified fractions were obtained after concentrating the extract solutions, precipitating the polymer, washing and drying the fractions in vacuum. Measurements FTIR spectra of the alloys and the fractions were recorded on a Bruker Vector-22 spectrometer. Thin films of polymer prepared by hot pressing were used as samples. 13 C-NMR spectra of the fractions were measured on a Bruker AMX400 NMR spectrometer at 100 MHz o-Dichlorobenzene-d4 was used as solvent to prepare the polymer solution of 20 wt%. The spectra were recorded at 120 ◦ C, with hexamethyldisiloxane as internal reference. Broadband decoupling and a pulse delay of 5 s were employed. Typically 1000 transients were collected. Ethylene content of the samples was determined based on the peak intensity data. Differential scanning calorimetry (DSC) analysis of the fractions was performed with a Perkin-Elmer Pyris 1 thermal analyzer under nitrogen atmosphere. About 5 mg sample was sealed in an aluminium sample pan, heated to 180 ◦ C for 30 min, and annealed at 130, 120, 110, 100, 90, 80, 70 and 60 ◦ C, respectively, each for 12 h. The DSC scan was then recorded at a heating rate of 5 ◦ C min−1 from 30 ◦ C to 180 ◦ C. The intrinsic viscosity of polymer fractions was measured using an Ubbelohde viscometer at 135 ◦ C with decahydronaphthalene as solvent. Notched Charpy impact strength of the alloy samples was measured on a Ceast impact strength tester according to ASTMD 256. The flexural modulus and flexural strength were measured following ASTMD 709 on a REGER-2000 electronic tester. Sample plates with sizes of 150 × 150 × 4 mm for mechanical properties measurements were prepared by compression molding at 180 ◦ C for 5 min under a pressure of 20 MPa. The samples were then cooled to room temperature in about 2 h. The sample strips for the tests were cut from the plates following ASTM. RESULTS AND DISCUSSION Structure and properties of the alloys To investigate the influence of ethylene content in the PE/PP alloy on its structure and properties, two samples containing different amounts of ethylene were synthesized and studied in this work. Figure 1 shows the morphology of the PE/PP in-reactor alloy granules. It can be seen that most of the granules have a spherical shape, and the size distribution of the granules is rather Polym Int 53:1169–1175 (2004) Polyethylene/polypropylene chain structure Figure 1. Morphology of the PE/PP in-reactor alloy granules. Figure 2. FTIR spectra of HEP and LEP. Table 1. The chemical composition and mechanical properties of HEP and LEP Sample HEP LEP the two samples were fractionated into five fractions by TGEF. C2 (wt%) Impact strength (kJ m−2 ) Flexural strength (MPa) Flexural modulus (MPa) 82.3 43.4 94 90 19.6 25.7 2007 2634 narrow. This is a feature beneficial to the large-scale production of PE/PP alloy in an industrial process. In Table 1 the chemical composition and main mechanical properties of the two samples are listed. Though these two samples have very different ethylene contents, they show quite similar impact strength. The value of impact strength is much higher than that of a conventional iPP homopolymer (about 4 kJ m−2 ). The flexural modulus of the alloys is also higher than that of conventional iPP (about 1600 MPa). This means that the PE/PP in-reactor alloy has an excellent balance of toughness and stiffness. Figure 2 shows the FTIR spectra of the two PE/PP samples. It can be seen that the doublet at 720–730 cm−1 is present in both samples, meaning that both contain crystalline PE chains or segments. The bands at 998 cm−1 and 841 cm−1 , which represent isotactic PP chains, are also present in both samples. Therefore, the PE/PP alloys are mainly composed of PE and iPP chains or segments. According to our previous work, there are quite a lot of PEblock-PP copolymer chains present in the PP/PE in-reactor alloy.18 These block copolymer chains act as compatibilizer between the PE and PP phases. To see if such a block copolymer also exists in the PE/PP alloy, Fractionation results Table 2 lists the results of TGEF fractionation. The two samples show very different fraction distributions. The main difference is reflected in the amount of the >120 ◦ C fraction. The sample containing lower ethylene content (LEP) has a markedly higher amount of >120 ◦ C fraction. FTIR spectra of the fractions from the two samples are shown in Fig 3. In all the fractions collected between 25 and 120 ◦ C the doublet bands at 720–730 cm−1 are clearly seen. The bands at 998 cm−1 and 841 cm−1 are also detectable in these fractions. This means that the four fractions extracted between 25 and 120 ◦ C are all block copolymers of PE and PP. Differences in the lengths of the PE and PP segments may have caused the differences in solubility. On the other hand, the compositions of the >120 ◦ C fractions from the two samples are quite different. The >120 ◦ C fraction of sample LEP is nearly pure iPP, while that of HEP is mainly composed of PE. In our previous work,18 we found that PE homopolymer fractions can be eluted at lower than 120 ◦ C in temperature rising elution fractionation (TREF), and PP chains of high isotacticity are extracted by TGEF only at temperatures higher than 120 ◦ C. Therefore, the fractionation result of HEP is surprising at first sight. However, when we considered the very small weight fraction of the >120 ◦ C fraction of HEP, we began to suspect that the molecular weight may have influenced the fractionation results. By comparing the intrinsic viscosity data of the fraction extracted at Table 2. Fraction distribution and ethylene content of LEP and HEP LEP Sample Fraction (◦ C) Fraction content (wt%) C2 (mol%) C2 (wt%) HEP 25 90 110 120 >120 25 90 110 120 >120 0.3 32.9 24.6 3.4 58.5 48.4 37.7 95.7 93.7 25.4 33.2 24.9 33.2 0.9 0.6 0.2 87.0 81.7 4.1 59.7 49.7 47.1 98.8 98.2 47.5 77.1 69.2 1.1 92.3 88.9 Polym Int 53:1169–1175 (2004) 1171 Z Fu et al Figure 3. FTIR spectra (1400–600 cm−1 ) of the fractions extracted from LEP and HEP at (a) 25 ◦ C; (b) 90 ◦ C; (c) 110 ◦ C; (d) 120 ◦ C; (e) >120 ◦ C. 120 ◦ C with that at >120 ◦ C (Table 3) and supposing that the two fractions have similar Mark–Houwink constants (this is reasonable as both fractions are mainly composed of polyethylene), it is clearly seen that the >120 ◦ C fraction of sample HEP has a much higher molecular weight than the 120 ◦ C fraction. On the other hand, the 120 ◦ C and >120 ◦ C fractions of LEP have quite similar intrinsic viscosity values. 1172 Therefore, we may say that a small portion of PE chains can be fractionated according to molecular weight by TGEF. Based on the FTIR analysis, we can deduce that the 25 ◦ C fraction is PP-block-PE in which the PP segments have low or medium isotacticity. The 110 and 120 ◦ C fractions are PP-block-PE of low and high PP content, respectively. The >120 ◦ C fraction is PP Polym Int 53:1169–1175 (2004) Polyethylene/polypropylene chain structure Table 3. Intrinsic viscosity of fractions extracted at 120 and >120 ◦ C from LEP and HEP LEP Sample [η](g/ml)−1 HEP 120 ◦ C fraction >120 ◦ C fraction 120 ◦ C fraction >120 ◦ C fraction 210.2 238.7 270.3 347.3 homopolymer when the PE/PP alloy has a high PP content, but a small amount of high molecular weight PE fraction may be found insoluble after extraction at 120 ◦ C when the alloy has a low PP content. According to the fraction distribution data in Table 2, we can say that sample HEP is mainly composed of the 110 and 120 ◦ C fractions, which are PE and PE-block-PP or its mixture with PE, respectively, and LEP contains large amounts of PP homopolymer, besides the block copolymer fractions. NMR analysis In order to confirm the chain structure of the different fractions, 13 C-NMR spectra of the 90, 110, 120 and Figure 4. 13 >120 ◦ C fractions from HEP and LEP were recorded, and these are shown in Fig 4. The spectra of the two 90 ◦ C fractions are quite similar to each other. There is a strong peak at 28.1 ppm, which is the methylene signal of long polyethylene sequences. There are several peaks corresponding to the PPP sequence, such as Pββ at 20.0 ppm, Tββ at 26.8 ppm and Sαα at 44.6 ppm, meaning that there are long PP segments in the polymer chain. The peaks at 35.7–36.0 ppm (Sαδ , Sαγ ), 31.3 ppm (Tδδ ), 25.4 ppm (Sβδ ), 22.9 ppm (Sββ ) and 18.1 ppm (Pδδ ) indicate that there are also sequences such as PPEP, PPEE, EPE and PEP in the chain.20 The peaks at 12.2, 21.0 and 30.3 ppm could be ascribed to high-boiling-point hydrocarbons that may come from the TGEF solvent. The spectra of the 110 ◦ C fractions are characteristic of PE-block-PP copolymer with very low PP content. Considering that PP homopolymers are soluble in n-octane only at a temperature higher than 120 ◦ C, the possibility that these fractions are PE/PP mixture can be ruled out. The 110 ◦ C fraction of HEP has lower content of long PP sequences than that of LEP. The junction structure between the blocks C-NMR spectra of the fractions extracted from LEP and HEP at (a) 90 ◦ C; (b) 110 ◦ C; (c) 120 ◦ C; (d) >120 ◦ C. Polym Int 53:1169–1175 (2004) 1173 Z Fu et al represented by the Sαδ , Sβδ and Tβδ peaks were not detected, which may mean that both blocks are very long. The two 120 ◦ C fractions also show 13 C-NMR signals typical of PE and PP. In the spectrum of the 120 ◦ C fraction from HEP, trace amount of Sβδ carbon was detected, which is an indication that the PE and PP segments are actually connected to form a block copolymer. Considering that there is a propylene pre-polymerization stage before the ethylene polymerization, it is very probable that there is also some PP-block-PE-block-PP triblock copolymer in the final product, besides the expected diblock copolymer. However, the amount of such a triblock copolymer is very limited, because the weight of PP produced in the pre-polymerization stage is only about 20 g/g catalyst, a value much lower than the estimated total amount of block copolymers [when the total yield is 3000 g polymer/g catalyst and 20 wt% of it is the block copolymer (see Table 2), about 600 g block copolymer/g catalyst will be formed]. In other words, the triblock copolymer will account for less than 10 % of the whole block copolymer component. But it is still unclear whether, and to what extent, the triblock copolymer chains contribute to the excellent mechanical properties of the materials. It is also noteworthy that the 120 ◦ C fraction from HEP has a lower propylene content than that from LEP. Considering that the former has a higher intrinsic viscosity value than the latter, we believe that molecular weight may also influence the TGEF fractionation of PE/PP inreactor alloy. The 13 C-NMR spectra of the two >120 ◦ C fractions are very different from one another. The >120 ◦ C fraction from LEP is actually pure iPP, whereas the fraction from HEP is basically pure PE. Thermal analysis To verify the existence of crystallizable PE and PP segments in the fractions, thermal analyses of annealed samples of the fractions were made using DSC. Multistep annealing of the samples makes sure that the PE and PP segments of different lengths form lamellae of different thickness, thus the DSC melting curve can reflect the presence of these different lamellae. As shown in Fig 5, DSC melting curves of the five fractions from LEP are very different from each other. The room-temperature fraction is completely amorphous. Though the FTIR spectrum of this fraction shows the presence of PE segments with carbon number larger than 10, these PE segments are still not long enough to form crystalline lamellae. On the other hand, the PP segments in this fraction have too low isotacticity to form crystals. Therefore, the room-temperature fraction is actually segmented ethylene-propylene copolymer. Such a low amount of segmented copolymer could be produced during switching of monomers, because there will be a little 1174 ethylene left in the reactor (ie ethylene dissolved in the polymer granules) after switching monomer from ethylene to propylene. The 90 ◦ C fraction shows several weak endothermic peaks in the range 80–120 ◦ C. By considering the results of 13 C-NMR and FTIR analysis, we believe that these endotherms are mainly caused by the melting of PE lamellae of relatively short thickness. This means that the PE segments in this fraction are long enough to form crystals, but there are also many short PE segments, as the peaks are much weaker than a PE homopolymer. The DSC curve of the 110 ◦ C fraction shows a strong peak at 132.9 ◦ C, which is close to the melting temperature of PE homopolymer. There is also a very weak endothermic peak at about 140 ◦ C, which may be caused by the PP crystalline phase. Considering the 13 C-NMR results, we may conclude that this fraction is composed of PE-block-PP copolymer with very long PE segments and relatively short PP segments. However, the existence of pure PE in this fraction cannot be ruled out. Considering that there is an ethylene homopolymerization stage in synthesizing the Figure 5. DSC curves of the five fractions from LEP. Polym Int 53:1169–1175 (2004) Polyethylene/polypropylene chain structure alloy, we believe that pure PE may account for the main part of this fraction. The melting curve of the 120 ◦ C fraction shows two major melting peaks at temperatures similar to twice of PE and PP, respectively. Moreover, there is a weak shoulder at 142.6 ◦ C. From the result of 13 C NMR analysis, it can be said that this fraction is mainly composed of PE-block-PP copolymer with very long PE and PP segments. The weak endotherm at 142.6 ◦ C indicates that the crystallization of a part of the PP segment close to the conjunction point has been interfered with by the PE phase, resulting in the formation of an imperfect PP crystalline phase. Finally, the >120 ◦ C fraction shows only one strong endotherm at 165 ◦ C, meaning that it is nearly pure PP. By combining the results of FTIR, NMR and DSC analysis, we can get a clear map of the chain structure and structure distribution of the PE/PP alloy. In both samples, PE homopolymer is mainly found in the 110 ◦ C fraction, and PP homopolymer exists in the >120 ◦ C fraction. The 120 ◦ C fraction is mainly composed of block copolymer with very long PE and PP segments. These three fractions constitute more than 95 % of the alloy. Results presented in this paper also show that TGEF is very similar to TREF18,21 in terms of the fractionation mechanism. The extraction temperature, similar to the elution temperature in TREF, is mainly determined by the chemical composition and crystallinity of the fraction. It is the higher extraction temperature of crystalline PP segments than the PE segments that makes the extraction temperature of PE-blockPP lower than that of PP but higher than that of PE. Molecular weight of the fractions can influence their solubility to a certain extent, and this will add unexpected complexity to the explanation of the fractionation results. As shown in Table 2, both samples have plenty of ethylene in the 110 ◦ C and 120 ◦ C fractions, but the HEP sample has a much lower propylene content than LEP. This difference in composition may explain the difference in the mechanical properties of the two samples. The higher flexural strength and flexural modulus of LEP compared with HEP can mainly be attributed to the higher propylene content of the former. However, some kind of synergistic effect between the PP and PE phases may also play an important role, as the flexural modulus of the alloy is even higher than that of a PP homopolymer, and the impact strength of the alloy is also very high. The role of the block copolymer fractions as the compatibilizer between PE and PP should be the key factor to form this kind of synergistic effect. CONCLUSIONS Two PE/PP in-reactor alloy samples were synthesized by multi-stage gas-phase polymerization using a Polym Int 53:1169–1175 (2004) spherical Ziegler–Natta catalyst. The alloys show excellent toughness–stiffness balance. Both samples can be fractionated by temperature-gradient extraction fractionation according to the chain structure of the fractions. The 110, 120 and >120 ◦ C fractions constitute more than 95 % of the alloy with high propylene content, while the alloy with low propylene content has almost no fraction extracted at higher than 120 ◦ C. By FTIR, 13 C-NMR and thermal analysis, it is proved that the alloy is mainly composed of polyethylene, PE-block-PP copolymer and polypropylene. There are also a few percent of ethylene-propylene segmented copolymer with very low crystallinity. The block copolymer fraction accounts for more than 25 % of the alloy. The role of the block copolymer as compatibilizer between PE and PP is believed to be the key factor that results in the excellent toughness–stiffness balance of the material. ACKNOWLEDGEMENTS Support by the Special Funds for Major State Basic Research Projects (grant no. G1999064803) is gratefully acknowledged. REFERENCES 1 Wu S, Polym Eng Sci 30:753 (1990). 2 Van der Wal A, Mulder JJ, Oderkerk J and Gaymans RJ, Polymer 39:6781 (1998). 3 Liang JZ and Li RKY, J Appl Polym Sci 77:409 (2000). 4 Galli P, Prog Polym Sci 19:959 (1994). 5 Galli P and Vecellio G, Prog Polym Sci 26:1287 (2001). 6 Cecchin G, Morini G and Pelliconi A, Macromol Symp 173:195 (2001). 7 Liu NC and Baker WE, Polymer 35:988 (1994). 8 Zhang YQ, Fan ZQ and Feng LX, J Appl Polym Sci 84:445 (2002). 9 Fan ZQ, Zhang YQ, Xu JT, Wang HT and Feng LX, Polymer 42:5559 (2001). 10 Galli P and Haylock JC, Makromol Chem Macromol Chem Symp 63:19 (1992). 11 Allport DC and Janes WH (Eds), Block Copolymers, John Wiley, New York (1973). 12 Ke B, J Polym Sci 42:115 (1960); 61:47 (1962). 13 Barrall EM, Roger H, Porter S and Johnson JF, J Appl Polym Sci 9:3061 (1965). 14 Carman CJ and Wilkes CE, Rubber Chem Tech 44:781 (1971). 15 Prabbu P, Schindler A and Gilbert RD, Polym Prepr 19:642 (1978). 16 Wang LX, Qi YC, Chen DL and Huang BT, Acta Polymerica Sinica (in Chinese) 1987(2):81 (1987). 17 Miller RC, Modern Plastics Mid-October Encyclopedia Issue 84 (1990). 18 Xu JT, Fu ZS, Fan ZQ and Feng LX, Eur Polym J 38:1739 (2002). 19 Sacchi MC, Fan ZQ, Forlini F, Tritto I and Locatelli P, Macromol Chem Phys 195:2806 (1994). 20 Tritto I, Fan ZQ, Locatelli P, Sacchi MC, Camurati I, and Galimberti M, Macromolecules 28:3342 (1995). 21 Feng Y and Hay JN, Polymer 39:6723 (1998). 1175