11
Effect of Plasticizer Type on Gelation and Fusion of PVC Plastisol, Dialkyl Phthalate Series* N. NAKAJIMA and S-Y. KWAK Institute of Polymer Engineering The University of Akron Akron, Ohio 44325-0301 Different grades of PVC resins and a variety of plasticizers are used to adjust processability and properties of plastisol. The plastisol, which is a dispersion of fine particles of PVC in plasticizer, is coated on a substrate and heated in an oven to gel and fuse. In the gelation stage the resin particles become swollen with plasticizer and then, in the fusion stage the entire system fuses to become one homogeneous phase. The finished products are flexible PVC such as coated fabrics and surgical globes. Different plasticizers, because of the difference in solvent power, affect the process of gelation and fusion, and hence, processabil- ity. This paper examines such an effect systematically by employing a homolo- gous series of plasticizers, dialkyl phthalates. The progress of gelation and fusion are followed by the measurements of dynamic moduli and by the observation with a scanning electron microscope. As it may be expected, the shorter the alkyl chain, the higher the solvent power of the plasticizer. INTRODUCTION lexible PVC (polyvinyl chloride) products may be F made through two distinctly different routes. One is to use resins made through suspension polymer- ization (1). The resin is a porous powder of approxi- mately 100pm size (2). The powder may absorb a large quantity of liquid plasticizer and yet remain free-flowing; or the resin-plasticizer mixture may be compounded and pelletized. The other route uses resins made through emulsion polymerization. The resulting emulsion of PVC is spray-dried; the dried powder contains the primary particles of about 1 pm and smaller as well as the agglomerated particles, which are ground to the size smaller than 20pm. The proportion of the primary particles and the ag- glomerated particles may be for example 85 to 15. The powder is mixed with a plasticizer in approxi- mately equal volume to prepare a paste called “plastisol” (3, 4). The compound made with the suspension resins may be melt-processed with plastics-processing equipment such as an extruder, injection molding machine, compression molding, and calendering. Although plastisol may also be processed through these equipments, its real advantage is the much lower viscosity of the paste compared to the melt, rendering unique fabrication techniques. The plasti- ~. -~ *Prepared for presentation at the 139th meeting of the Rubber Division, American Chemical Society. May 21-24. 1991, Toronto, Ontario. Canada. sol may be coated on a substrate with high speeds, such as fabric coating: it may be made into films and sheets: dip coating may be used to make com- plex shapes like boots and surgical gloves; the rota- tional molding and slush-molding may be used to make hollow objects. Uses of relatively inexpensive equipment, particularly inexpensive mold are an- other advantage of plastisol. After plastisol is coated on the substrate, it is heated in an oven to gel and fuse. In the gelation stage the resin particles become swollen with plasti- cizer and in fusion stage they fuse to become a uniform mass. In this process the system changes from a pasty liquid to viscoelastic melt. The devel- opment of modulus is important in some processes, e.g. foaming, where the generation of the desired cell structure is intimately related to the viscoelastic properties of the system (5). Rheological property is one of the most important criterion for selecting the resin grade and plasticizer type for a given formulation. The rheological re- quirements may be divided into two areas; one is the rheology at room temperature, where the coat- ing operation is performed (6). The other area is the development of modulus during gelation and fusion (7) as mentioned already. This study and many pre- ceding studies concern the latter area. In one paper the viscoelastic finger-printing typical commercial grade of resins (dispersion resins) were presented (8). In another, the viscoelastic profile was related to the morphological changes accompanying gelation 21 2 JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4

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Effect of Plasticizer Type on Gelation and Fusion of PVC Plastisol, Dialkyl Phthalate Series*

N. NAKAJIMA a n d S-Y. KWAK

Institute of Polymer Engineering The University of Akron Akron, Ohio 44325-0301

Different grades of PVC resins and a variety of plasticizers are used to adjust processability and properties of plastisol. The plastisol, which is a dispersion of fine particles of PVC in plasticizer, is coated on a substrate and heated in an oven to gel and fuse. In the gelation stage the resin particles become swollen with plasticizer and then, in the fusion stage the entire system fuses to become one homogeneous phase. The finished products are flexible PVC such as coated fabrics and surgical globes. Different plasticizers, because of the difference in solvent power, affect the process of gelation and fusion, and hence, processabil- ity. This paper examines such an effect systematically by employing a homolo- gous series of plasticizers, dialkyl phthalates. The progress of gelation and fusion are followed by the measurements of dynamic moduli and by the observation with a scanning electron microscope. As it may be expected, the shorter the alkyl chain, the higher the solvent power of the plasticizer.

INTRODUCTION

lexible PVC (polyvinyl chloride) products may be F made through two distinctly different routes. One is to use resins made through suspension polymer- ization (1). The resin is a porous powder of approxi- mately 100pm size (2). The powder may absorb a large quantity of liquid plasticizer and yet remain free-flowing; or the resin-plasticizer mixture may be compounded and pelletized. The other route uses resins made through emulsion polymerization. The resulting emulsion of PVC is spray-dried; the dried powder contains the primary particles of about 1 pm and smaller as well as the agglomerated particles, which are ground to the size smaller than 20pm. The proportion of the primary particles and the ag- glomerated particles may be for example 85 to 15. The powder is mixed with a plasticizer in approxi- mately equal volume to prepare a paste called “plastisol” (3, 4).

The compound made with the suspension resins may be melt-processed with plastics-processing equipment such as an extruder, injection molding machine, compression molding, and calendering. Although plastisol may also be processed through these equipments, its real advantage is the much lower viscosity of the paste compared to the melt, rendering unique fabrication techniques. The plasti-

~. -~ *Prepared for presentation at the 139th meeting of the Rubber Division, American Chemical Society. May 21-24. 1991, Toronto, Ontario. Canada.

sol may be coated on a substrate with high speeds, such as fabric coating: it may be made into films and sheets: dip coating may be used to make com- plex shapes like boots and surgical gloves; the rota- tional molding and slush-molding may be used to make hollow objects. Uses of relatively inexpensive equipment, particularly inexpensive mold are an- other advantage of plastisol.

After plastisol is coated on the substrate, it is heated in an oven to gel and fuse. In the gelation stage the resin particles become swollen with plasti- cizer and in fusion stage they fuse to become a uniform mass. In this process the system changes from a pasty liquid to viscoelastic melt. The devel- opment of modulus is important in some processes, e.g. foaming, where the generation of the desired cell structure is intimately related to the viscoelastic properties of the system (5).

Rheological property is one of the most important criterion for selecting the resin grade and plasticizer type for a given formulation. The rheological re- quirements may be divided into two areas; one is the rheology at room temperature, where the coat- ing operation is performed (6). The other area is the development of modulus during gelation and fusion (7) as mentioned already. This study and many pre- ceding studies concern the latter area. In one paper the viscoelastic finger-printing typical commercial grade of resins (dispersion resins) were presented (8). In another, the viscoelastic profile was related to the morphological changes accompanying gelation

21 2 JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4

Effect of Plasticizer Type on Gelation and Fusion

and fusion (9). Among the available material vari- ables the plasticizer type makes a most significant effect on the development of modulus (10). Appar- ently the difference of solvent power of the plasti- cizer plays the key-role.

From the morphological observation with a scan- ning electron microscope, SEM, the following four steps were identified as the gelation and fusion pro- ceed: (i) a portion of polymer dissolves into plasti- cizer: the dissolution of polymer may come from the surface of some particles. However, there appears to be the particle-particle differences in solubility that some particles dissolve earlier and others remain long after most have dissolved. (ii) The plasticizer containing the dissolves polymer looks like it is glueing particles together. As more polymer dis- solves, this phase becomes the matrix with rela- tively minor amount of particles dispersed in it. (iii) Simultaneously with the step (i), the polymer parti- cles become swollen with plasticizer. (iv) A s the swelling continues the particles form clusters and eventually coalesce to form a uniform mass. For a given PVC-plasticizer system all four steps may be occurring at some stage of gelation and fusion. How- ever, in the examples seen by SEM, steps (i) and (ii) dominate in some system and (iii) and (iv) dominate in others. The former example is the tricresylphos- phate (TCP) system at above 100°C. The latter ex- ample is the dioctylsebacate (DOS) system. With the di-2-ethylhexyl phthalate (DOP) system it is not clear as to which step dominates. With the dibenzylseba- cate (DBS) system the coalescence of the swollen particles appears to be the dominant reaction.

The difference in the solvent power of the above plasticizer comes from very different chemical struc- ture. In order to examine more detail of the effect of solvent power, we have chosen a homologous series of dialkylphthalates, dimethyl-(DMP), (iso) hexyl-(DHP) di-2-ethylhexyl-(DOP) and di-isooctyl- (DIOP). As before both viscoelastic measurements and morphological observation have been performed.

EXPERIMENTAL

Materials

The PVC resin in this study in one of the represen- tative dispersion resins, Geon 121, a product of the B. F. Goodrich Company.

The homologous series of plasticizers are di- methyl phthalate (DMP), di-(iso)hexyl phthalate (DHP), di-2-ethylhexyl phthalate (DOP) and di-isooc- tyl phthalate (DIOP). The chemical structures and physical properties of these four plasticizers are given in Table 1 and Table 2, respectively.

The plastisol formulation is given in Table 3.

Plastisol Preparation

Plastisols were prepared by mixing the dry PVC powder with liquid plasticizer containing epoxidized soybean oil and stabilizer. A small amount of

Table 1. Chemcial Structures of Plasticizers.

Name Chemical Structure

di-methyl phthalate (DMP)

di-(iso)hexyl phthalate (DHP)

di-2-ethylhexyl phthalate P O P )

di-isooctyl phthalate (DIOP)

(c loH 10'4) 0

(C24H 38'4)

-0-c- i" -c-c-c-c 0

-0-c-c-c-c-c-c 'd 1-C

-o-c-c--C---c t i l i (C24H3804)

0 c c

-0-c-c-c-c-c-c l

Table 2. Physical Properties of Plasticizers.

Molecular Specifica Weight Gravity

Name (g /mole) ("C/"C)

DMP 194 1.190 DHP 334 1.008 DOP 390 0.982 DIOP 390 0.982

'Ref. 11

Table 3. Plastisol Formulation.

Component Parts by Weight

PVC resin 100 (I.V. 1.20 dl/g)a Plasticizer 57 Epoxidized soybean oil 3 Barium, cadmium, zinc stabilizer 2

'1.V. = inherent viscosity in cyclohexanone at 30'C (12).

the plasticizer was slowly added to the dry PVC powder while stirring manually with a stainless steel spatula.

The manual stirring was continued until all plas- ticizer was added and the mixture changed to a viscous fluid. Then. a mechanical stirrer

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4 21 3

N. Nakajima and S-Y. Kwak

with a two-blade propeller was used for a further homogenization.

After mixing was completed, air bubbles in plasti- sols were removed by applying vacuum, but slowly in order to prevent foaming. Then, the plastisols were aged for two weeks before their use. The aging is necessary because viscosity increases initially pri- marily because of deagglomeration but it stabilizes after two weeks (13).

Viscoelastic Measurements

A Rheometrics Mechanical Spectrometer (RMS), model RMS-605, was used in the dynamic oscilla- tory mode with a controlled heating rate. The 25 mm-diameter parallel discs were used with a gap setting of 2 mm. In this study, the cone and plate assembly can not be used because, during the heat- ing cycle, the gap change, which, although very slight, can have a significant effect on the accuracy of the results. The frequency of oscillation was maintained to be 1 Hz.

Heating was started from room temperature to 190°C with a programmed increase rate of 5"C/min. After allowing a few minutes for equilibrating to the desired temperature, the measurements were made. The shear strain amplitude was 25% in the range from room temperature to about 60°C where gela- tion started. After this temperature, the strain am- plitude was reduced to 2.5%. The 25% was large enough to obtain accurate torque signals when the moduli were low in the beginning of measurement, i.e., in the fluid state. The 2.5% was small enough not to disturb the system at the later stage of the measurement. At this strain amplitude, the system did not indicate non-linearity .

Morphological Observations

A Scanning Electron Microscope (SEMI, IS1 model SX-40 was used to observe the morphological changes of PVC plastisol during gelation and fusion.

The samples for SEM were made by using Rheo- metrics Mechanical Spectrometer. The plastisols were loaded between upper and lower plate of RMS and then heated up to a desired temperature with- out imposing shear strain to the system. The sam- pling temperatures were selected with reference to the viscoelastic data and the stepwise increase of temperature of about 5°C for every minute was used. The samples were immersed in liquid nitrogen and then freeze-fractured.

RESULTS

Viscoelastic Measurements

Figures 1 to 4 are changes of elastic modulus, G', and loss modulus, G", during gelation and fusion as a function of temperature. For the first three sys- tems, PVC-DOP, -DIOP, and -DHP, with the increase of temperature, the moduli decrease initially. At slightly above 60°C. the gelation process begins and the elastic and the loss moduli increase very steeply

PVC/DOP

7 10

6 10

5 10

4 10

3 10

2 10

45 95 145 195

TEMPERATURE ( "C )

Fig. 1 . Viscoelastic profile of gelation and fusion of a plastisol made with PVC-DOP.

with temperature by three orders of magnitude. A first peak or a shoulder appears in the curves and then the moduli increase more gradually (DOP and DIOP) or level off (DHP). The maximum values of the moduli are between 125°C and 135°C for DOP and DIOP systems. The second maxima appear for DHP system between 110 and 125°C. With further in- crease in temperature the moduli decease indicating the end of gelation and dominance of fusion, melting of microcrystallites (14). Figure 4 shows the vis- coelastic profile of PVC-DMP system, which is quite different from that of other three systems. When the PVC-DMP plastisol was aged for two weeks, the sys- tem turned into a solid cake, which is no longer paste-like. The solid-like state of the PVC-DMP sys- tem at the lower temperature ranges is indicated by the magnitude of the elastic modulus. At 55"C, the magnitude of the elastic modulus is approaching lo5 Pa, which is comparable in magnitude to those of the shoulder or the first peak of other three sys- tems. The fact indicates that the gelation already started at room temperature. With further increase in temperature, the moduli increase slightly and remain constant up to 120°C and then decrease gradually, indicating the dominance of the fusion step. In all four systems the maximum of the elastic modulus occurs at a higher temperature than that of the loss modulus. The reason for this is not known yet.

21 4 JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4

Effect of Plasticizer T y p e o n Gelation a n d Fusion

PV C/ DI 0 P PVClDMP

7 10

h

N

5 > 6 3 10

2 3 5

w

0 m

n 10 0 2 v, v,

9. 4 10

v,

3 0 3 0 3

0 10

$I

4 w 2

10 45 95 145 195

TEMPERATURE ( "C )

Fig. 2. Viscoelastic profile of gelation and fus ion of a plastisol m a d e wi th PVC-DZOP.

PVC/DHP

7 10

6 10

-

5 10

-

W I 10

45 95 145 195

TEMPERATURE ( " C )

Fig. 3. Viscoelastic profile of gelation and fus ion of a plastisol m a d e wi th PVC-DHP.

7 10

h

N

E,

2 10 -2 6

w

b v,

2 5

s 4

n 10 0 I v, m

b 10

3 v,

3 n 0 3 0

10 I- m

2 2

10

0-0 G'

A-A G"

45 95 145 195

TEMPERATURE ( ' C )

Fig. 4. Viscoelastic profile of gelation and fus ion of a plastisol m a d e wi th PVC-DMP.

Morphological Observation

Table 4 lists sampling temperatures which were chosen on the basis of characteristic features of the viscoelastic curves. The sampling temperatures of the PVC-DMP system are somewhat arbitrary be- cause no clear feature is observed in the moduli.

The SEM micrographs of the fracture surfaces of the PVC-DIOP system are shown in Figs. 5 through 8 at two magnifications of 2000x and 5000x. At 90°C individual particles are still identifiable and the presence of agglomerates is also apparent. But some particles may be swollen somewhat with the plasticizer. At 130°C which is the second maxi- mum in loss modulus, changes in morphology are obvious such that only a limited number of particles are identifiable and that the interparticle boundaries are obscured. The texture of the fracture surface looks like a ghost of particles. At 159°C the fusion has taken over and the particulate morphology has disappeared. At 193°C. the fusion seems to be com- pleted, because the fracture surfaces are very simi- lar at 159 and 193°C.

The S E M observations of the PVC-DOP system are very similar to those reported before (14). They are also similar to PVC-DIOP system. Therefore, they are not shown here.

Figures 9 through 13 are the SEM photographs of the PVC-DHP system. At 83°C the particles of PVC are clearly identifiable. At 104°C the original parti-

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4 21 5

N. N a k a j i m a and S-Y. K w a k

Table 4. Sampling Temperature for Morphological Observation.

Characteristic Temperature ("C)

Behavior PVC-DIOP PVC-DHP PVC-DMP

- ~ 2 5 Room temperature - First peak (or shoulder) 90 83 90 Valley after first peak - 104 -

Completion of fusion 193 193 190

Second peak in G 130 126 130 Dominance of fusion 159 159 160

PVC/DIOP (130°C)

PVC/DIOP (90OC)

Fig. 6. Scanning electron micrographs of PVC-DIOP plas- tisol at 130°C.

Fig. 5. Scanning electron micrographs of PVC-DIOP plas- tisol at 90°C.

cles are still visible but much swelling of particles is already taking place. At 126°C no particle is visible and particles must have fused to form a plasticized matrix. At 159°C and 193°C the interparticle boundaries have disappeared.

Figures 14 through 1 7 are the S E M photographs of the PVC-DMP system. At 25°C the original parti- cles are clearly visible but some degree of swelling has already started. In general, the plasticizers such

as DOP and DIOP are rather a poor solvent which has little effect on the PVC resin at room tempera- ture. From the fact that swollen particles exist at 25°C DMP is considered to be the best solvent of the four plasticizers in this study. At 90°C PVC particles are on the verge of losing their boundaries. The disappearance of interparticle boundaries is much more progressed compared to that of PVC-DIOP sys- tem at the same temperature. At 130 and 160°C the interparticle boundaries disappeared almost com- pletely. At 19O"C, there is no indication of particle boundaries.

DISCUSSION

Viscoelastic Measurements

In Figs. 18 and 19 the elastic moduli and loss moduli are plotted separately for four PVC-plasti- cizer systems. With the increase of temperature, the elastic and the loss moduli of three systems except for the PVC-DMP decrease initially below 60°C. This

21 6 JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4

Effect of Plasticizer Type on Gelation and Fusion

PVC/DIOP (159°C) PVC/DIOP (193°C)

Fig. 7. Scanning electron micrographs of PVD-DIOP plas- tisol at 159°C.

indicates that they remain a suspension of PVC solids in a plasticizer. At slightly above 60°C. the gelation process begins. The temperature, where the first peak or the shoulder appears at 83-90°C corre- sponds approximately to the glass transition tem- perature of the PVC (15). In the PVC-DHP system, the temperature where the first peak appears is somewhat lower and the magnitude of modulus in the first peak is higher compared to the PVC-DOP and the PVC-DIOP system. This indicates the better solvent power of DHP.

Concerning the PVC-DMP system, the plasticizer appears to have penetrated into some of the PVC particles and swelled or even dissolved them at room temperature, Fig. 14. This system has gelled at room temperature similar to other three systems at the higher temperature where the first peak (or shoulders) appear. The moduli of the PVC-DMP sys- tem at 50°C (and probably even at room tempera- ture) are as high as those of other three systems at the higher temperatures.

Fig. 8. Scanning electron micrographs of PVC-DIOP plas- tisol at 193'C.

After passing the second maxima, the elastic and the loss moduli decrease for two reasons. One is the normal temperature dependence, primarily at- tributable to the thermal expansion. The other is caused by the loss of the network junctions by melt- ing of the PVC microcrystallites.

The gelation and fusion profiles presented in Figs. 18 and 19 show an apparent effect of solvent power of plasticizers. There are apparent differences in gelation and fusion behavior, particularly at the temperature range from 60°C to 120°C. One of the most obvious and systematic differences is the first peak (or shoulder) in the elastic and the loss moduli, indicating that the solvent power plays a significant role while the gelation is progressing. A quantitative comparison for three systems except for PVC-DMP is made by taking the temperature of the first peak (or shoulder) and the magnitude of moduli at the same temperature, Table 5. From the viscoelastic data, the lower the peak temperature and the higher the magnitude of moduli indicate the better solvent.

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4 21 7

N. N a k a j i m a a n d S-Y. K w a k

PVC/DHP (83°C) PVC/DHP (104°C)

Fig. 9. Scann ing electron micrographs of PVC-DHP plas- tisol at 83'C.

Because the PVC-DMP system has high moduli at room temperature, obviously DMP is the best sol- vent. The order of solvent power is DMP, DHP, DOP/DIOP. It is well known that polar (ester) groups in the homologous series of dialkyl phthalates are the main functional groups responsible for plasticization (1 1).

During gelation and fusion process, PVC plastisol changes from a suspension of PVG particles in a liquid plasticizer to a uniform mass. The morpho- logical study with SEM provides direct and unique information which is not obtainable from other measurements.

As before (10) a large variation in solubility of particles is observed: some particles have swollen, while others appear to be least affected. The cause of the variation was explained on the basis of differ- ence in the heat history during drying. Those parti- cles that become agglomerated may be slower to be touched by the plasticizer, while the decrease in

Fig. 10. Scann ing electron micrographs of PVC-DHP plustisol at 104°C.

crystallinity by partial melting may facilitate swelling. Although speculative, differences in syn- diotacticity or in the surface coverage with emulsi- fier may also occur among the particles.

In the beginning of gelation [i) a portion of PVC dissolves into plasticizer, (ii) some particles become swollen with plasticizer and (iii) other particles ap- pear unaffected. Because the solvent power, i.e. polymer-solvent interaction, is concentration depen- dent, the following mechanism was postulated; if a given plasticizer is a relatively better solvent at di- lute regions but poorer at high concentrations, the above process (i) should dominate over the process (ii). If the converse is the case, the swelling should be the dominant reaction but not the dissolution. In the previous study TCP seem to give the former, and DOS the latter. However, with DOP it was not clear whether one process dominates over the other or not. In the present study of the alkylphthalate se- ries, again we cannot tell which process dominates.

21 8 JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Yo/. 13, No. 4

Effect of Plasticizer Type on Gelation and Fusion

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4 21 9

220

N . N a k a j i m a and S-Y. K w a k

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Vol. 13, No. 4

Effect of Plasticizer T y p e on Gelation a n d Fusion

PVClDMP (190°C)

Fig. 17. Scann ing electron micrographs of PVC-DMP plastisol at 190°C.

Although the SEM photographs provide direct viewing of the morphological changes, the differ- ences in the solvent power are shown to be relative and qualitative. In this regard viscoelastic method is superior in that the difference is clearly demon- strated quantitatively in Figs. 18 and 19. The ex- tent of differences in the temperature dependence of moduli are important in processing (8).

CONCLUSIONS

Solvent power of a dialkyl phthalate series, DOP, DIOP, DHP, and DMP, in PVC plastisol was exam- ined as they affect progress of gelation and fusion. The viscoelastic measurements and morphological observations were performed. As demonstrated bv

G' of All Plastisols

6 10

5 10

4 10

3 10

V-V PVC-DMP

+-+ PVC-DHP

A-A PVC-DOP

0-0 PVC-DIOP

10 45 95 145 195

TEMPERATURE ( "C )

Fig. 18. Changes of elastic moduli of f o u r plastisols dur - i ng gelation a n d fu s ion .

7 10

6 10

N-

5 -2 2 10

5 v

b v)

3 -f 3

0 I cn cn

4 10

9 3

10

2 the development of elastic and loss modulus thk i n

G" of All Plastisols

V-V PVC-DMP

+-+ PVC-DHP

A-A PVC-DOP

a-0 PVC-DIOP

I I 1 I "

45 95 145 195

TEMPERATURE ( "C )

solvent power is in the order of better to poorer, DMP, DHP, and DOP/DIOP. The DOP and DIOP sys- terns gave an identical behavior.

In the morphological observation significant dif- ferences in solubility were observed among the par-

Fig. 19. Changes of loss moduli of four plastisols during gelation a n d f u s i o n ,

JOURNAL OF VINYL TECHNOLOGY, DECEMBER 1991, Yo/. 13, No. 4 221

N. N a k a j i m a a n d S-Y. K w a k

Table 5. Viscoelastic Data at the First Peak, Peak Temperature, and interaction Parameter.

Data DOP DiOP DHP DMP

G’(dyne /cm *) 3.43 x 105 2.48 x l o 5 2.90 x l o 6 (8.65 x 1 05)’ G”(dyne/cm *) 3.40 X 1 O5 2.40 x 105 1.36 x lo6 (5.82 x 1 0 5 ) a

- T (“C) 90 90 83 ‘Moduli at 50°C.

5 . N. Nakajima, D. W. Ward, and E. A. Collins, Polym.

6. E. A. Collins, D. J. Hoffmann, and P. L. Soni, Rubber

7. N. Nakajima and D. W. Ward, Rubber Chem. Technol.,

Eng. Sci., 19, 210 (1979).

Chem. Technol. 52. 676 (1979).

ticles; some became swollen while others appear unaffected. In the SEM photographs the solvent power of DMP, DHP, DOP, and DIOP were shown to be in agreement with the results of the viscoelastic measurements. 54, 1096 (1981).

REFERENCES 1. J . A. Davidson and K. L. Gardner, “Vinyl Polymers

(PVC), Poly(viny1 chloride),.’ Kirk-Othmer; Encyclope- dia of Chemical Technology, 3rd ed.. Vol. 23, p. 886, John Wiley (1983).

2. J. A. Davidson and D. E. Witenhafer, J . Polym. Sci.. Polyrn. Phys. 18 51 (1980).

3. J . A. Davidson and K. L. Gardner. “Plastisols,” Kirk- Othmer; Encyclopedia of Chemical Technology, 3rd ed., Vol. 23. p. 922, John Wiley (1983).

4. C. A. Brighton, G. C. Marks, and J. C. Benton, “Plasti- sols,” Encyclopedia of Polymer Science and Technol- ogy, Vol. 14, p. 370, John Wiley, New York (1971).

8. N. Nakajima and D. W. Ward, J. Appl. Polyrn. Sci.,

9. N. Nakajima, J. D. Isner, and E. R. Harrell, J. Macro-

10. N. Nakajima and M. R. Sadeghi, Intern. Potym. Proc.,

11. J. K. Sears and J . R. Darby, The Technology of Plasti-

12. C. A. Daniels and E. A. Collins, J. Macromol. Sci.

13. N. Nakajima and C. A. Daniels, J . Appl. Polyrn. Sci.,

14. N. Nakajima and E. R. Harrell, Adu. Polm. Technol. 6.

28. 807 (1983).

mol. Sci. Phys.. B20(3), 349 (1987).

IV, 16 (1989).

cizers, John Wiley & Sons, New York (1982).

Phys., B10, 287 (1974).

25, 2019 (1980).

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