Formationmechanism of high‐pressure water penetration induced fiber orientation in overflow water‐assisted injection molded short glass fiber‐reinforced polypropylene
Abstract:Recently, there has been growing interest in water‐assisted injection molding (WAIM) not only for its advantages over gas‐assisted molding (GAIM) and conventional injection molding (CIM), but also for its great potential advantages in industrial applications. To understand the formation mechanism of water penetration induced fiber orientation in overflow water‐assisted injection molding (OWAIM) parts of short glass fiber‐reinforced polypropylene (SGF/PP), in this work, the external fields and water penetration… Show more
“…Secondly, as the water pressure increased, the radial squeezing force of water directly acting on the melt/fiber interface also increased, resulting in an increase in the viscous friction between the fibers and melt, which also increased the shear stress acting on fibers. Nevertheless, the unstable water penetration at the front of part led to a random fiber orientation near the water channel, 26 and increasing the water pressure had little influence on improving this (as shown in Figure 13), which was quite consistent with the previous investigations 24,26 . Therefore, increasing the water pressure could significantly facilitate the ordered fiber orientation at the rear position, but it had a limited influence on the fiber orientation at the front position.…”
Section: Resultssupporting
confidence: 84%
“…According to the previous investigations, the water penetration process is similar to the gas penetration process in GAIM 26,39 . In the water penetration stage, once water/gas was injected, it would cool the melt near the water channel layer, where the viscosity of melt would be high.…”
Section: Resultsmentioning
confidence: 94%
“…As we know, with the increase of water injection delay time, the time for the mold wall to cool the melt also increased before water was injected, which caused the high‐viscosity melt near the mold wall to thicken toward the center of the mold cavity 11,26 . This, in turn, decreased the melt volume flowing with water (shown in Figure 19), resulting in a reduction in the region where the melt was subjected to strong shear action 49 ; secondly, the penetration resistance of pressurized water increased rapidly with the increase of water injection delay time, which in turn reduced the velocity difference of melt between the mold wall and the water channel.…”
Section: Resultsmentioning
confidence: 99%
“…As shown in Figure 6, with the increase of water injection time, the shear stress gradient significantly increased along the thickness direction. According to previous investigations, the fluctuating penetration behavior of high‐pressure water occurred near the water inlet, resulting in random fiber orientation near the water channel and nonuniformity of residual wall thickness distribution 24,26 . In this work, the proportion of residual wall thickness was used to reflect the water penetration behavior, the proportion of residual wall thickness refers to the ratio of residual wall thickness at the selected position to the radius of mold cavity.…”
Section: Resultsmentioning
confidence: 99%
“…To solve the aforementioned equations, boundary conditions in the SSWAIM process must be specified 26,32 . A schematic diagram of the boundary conditions is shown in Figure 1a, and others are listed below.…”
It is a critical requirement to have an insight into the mechanism of flow-induced fiber orientation in short-shot water-assisted injection molding (SSWAIM) of fiberreinforced polymer for improving the structural rigidity and service life of molded parts. However, this mechanism is still unclear, which stunts the development of SSWAIM. In this work, the mechanism of flow-induced fiber orientation in SSWAIM parts of short-glass-fiber-reinforced polypropylene (SGF/PP) was clarified through numerical research and experimental verification. The results showed that the difference of fiber orientation distribution at different positions both in the radial direction and along the flow direction between SSWAIM parts and conventional injection molding (CIM) parts was mainly due to the strong flow field caused by the high-pressure water penetration in SSWAIM. Moreover, fiber orientation in the SSWAIM part depended not only on its position both in the radial direction and along the flow direction, but also on the processing parameters. At the front of SSWAIM part, fiber orientation changed greatly in the radial direction and presented an obvious "shell layer-core layer-water channel layer" hierarchical structure across the part thickness, whereas this phenomenon became more inconspicuous with increasing the distance of the selected position from the water injection inlet.Short-shot size is the principal parameter affecting the fiber orientation, and within the range of investigated processing parameters, smaller short-shot size, shorter water injection delay time, higher water pressure, and lower melt temperature could significantly facilitate fiber orientation across the part thickness.
“…Secondly, as the water pressure increased, the radial squeezing force of water directly acting on the melt/fiber interface also increased, resulting in an increase in the viscous friction between the fibers and melt, which also increased the shear stress acting on fibers. Nevertheless, the unstable water penetration at the front of part led to a random fiber orientation near the water channel, 26 and increasing the water pressure had little influence on improving this (as shown in Figure 13), which was quite consistent with the previous investigations 24,26 . Therefore, increasing the water pressure could significantly facilitate the ordered fiber orientation at the rear position, but it had a limited influence on the fiber orientation at the front position.…”
Section: Resultssupporting
confidence: 84%
“…According to the previous investigations, the water penetration process is similar to the gas penetration process in GAIM 26,39 . In the water penetration stage, once water/gas was injected, it would cool the melt near the water channel layer, where the viscosity of melt would be high.…”
Section: Resultsmentioning
confidence: 94%
“…As we know, with the increase of water injection delay time, the time for the mold wall to cool the melt also increased before water was injected, which caused the high‐viscosity melt near the mold wall to thicken toward the center of the mold cavity 11,26 . This, in turn, decreased the melt volume flowing with water (shown in Figure 19), resulting in a reduction in the region where the melt was subjected to strong shear action 49 ; secondly, the penetration resistance of pressurized water increased rapidly with the increase of water injection delay time, which in turn reduced the velocity difference of melt between the mold wall and the water channel.…”
Section: Resultsmentioning
confidence: 99%
“…As shown in Figure 6, with the increase of water injection time, the shear stress gradient significantly increased along the thickness direction. According to previous investigations, the fluctuating penetration behavior of high‐pressure water occurred near the water inlet, resulting in random fiber orientation near the water channel and nonuniformity of residual wall thickness distribution 24,26 . In this work, the proportion of residual wall thickness was used to reflect the water penetration behavior, the proportion of residual wall thickness refers to the ratio of residual wall thickness at the selected position to the radius of mold cavity.…”
Section: Resultsmentioning
confidence: 99%
“…To solve the aforementioned equations, boundary conditions in the SSWAIM process must be specified 26,32 . A schematic diagram of the boundary conditions is shown in Figure 1a, and others are listed below.…”
It is a critical requirement to have an insight into the mechanism of flow-induced fiber orientation in short-shot water-assisted injection molding (SSWAIM) of fiberreinforced polymer for improving the structural rigidity and service life of molded parts. However, this mechanism is still unclear, which stunts the development of SSWAIM. In this work, the mechanism of flow-induced fiber orientation in SSWAIM parts of short-glass-fiber-reinforced polypropylene (SGF/PP) was clarified through numerical research and experimental verification. The results showed that the difference of fiber orientation distribution at different positions both in the radial direction and along the flow direction between SSWAIM parts and conventional injection molding (CIM) parts was mainly due to the strong flow field caused by the high-pressure water penetration in SSWAIM. Moreover, fiber orientation in the SSWAIM part depended not only on its position both in the radial direction and along the flow direction, but also on the processing parameters. At the front of SSWAIM part, fiber orientation changed greatly in the radial direction and presented an obvious "shell layer-core layer-water channel layer" hierarchical structure across the part thickness, whereas this phenomenon became more inconspicuous with increasing the distance of the selected position from the water injection inlet.Short-shot size is the principal parameter affecting the fiber orientation, and within the range of investigated processing parameters, smaller short-shot size, shorter water injection delay time, higher water pressure, and lower melt temperature could significantly facilitate fiber orientation across the part thickness.
In water‐assisted injection molding processes, it is crucial to understand the mechanisms governing the formation of hollow structures and identify the key factors influencing their morphology and dimensional accuracy. This work combined experimental analysis and numerical simulation to investigate the influence of different mold cavities and main processing parameters on hollow structures in overflow water‐assisted injection molded parts of short‐glass‐fiber‐reinforced polypropylene, that is, hollow shape and hollow ratio. The results show that the hollow shape and hollow ratio depended not only on the cross‐sectional location but also on the cross‐sectional shape of the mold cavity. For the circular parts, the hollow shape resembled the cross‐sectional shape of the mold cavity, with a relatively small and uniform hollow ratio across cross‐sectional locations. For the noncircular parts, the hollow shape varied considerably with increasing distance from the water inlet. Moreover, the results also show that except for the influence of water‐injection delay time on the uniformity of the hollow ratio, higher melt temperature (250°C), shorter water‐injection delay time (0 s), and higher water pressure (10 MPa) contributed to the hollow shape being closer to the cross‐sectional shape of mold cavities and made hollow ratios relatively larger and more uniform.
Based on the self‐assisted injection experimental platform, experimental studies on gas‐assisted injection molding (GAIM), and water‐assisted injection molding (WAIM) of 2 curved pipe fittings by adopting short‐shot method were carried out. UDF model was constructed for numerical simulation analysis. The influence rules of auxiliary medium and bending angle on the terminal morphology, inner wall surface quality at bending angle, medial and lateral residual wall thickness, variation range, and residual wall thickness deviation rate of short‐shot fluid assisted injection molding (SSFAIM) bending samples were compared. Meanwhile, the influence mechanism was investigated. The following experimental findings were obtained. SSFAIM had secondary penetration, while water produced multiple penetrations. There are multiple vacuum shrinkage pores in the unpenetrated area at the end of the SSWAIM sample, as well as serious shrinkage depressions on the surface. The shape of the penetration front of water is arc‐shaped with many penetration holes. The shape of the penetration front of the gas at the end of the SSGAIM sample is “pointy.” Compared with the SSWAIM sample, the residual wall thickness of SSGAIM has a narrow distribution range when the bending angle is 0°. With the increase of the bending angle, the “foaming” phenomenon of the inner wall surface quality at the bending angle of the SSGAIM sample becomes less and less obvious. Moreover, the deviation of the inner and outer residual wall thickness of SSGAIM is more obvious than that of SSWAIM due to the increase of bending angle.
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