# Correlation of Processing, Inner Structure, and Part Properties of Injection Moulded Thin-Wall Parts on Example of Polyamide 66

Authors: Dietmar Drummer; Steve Meister
Journal: International Journal of Polymer Science
 (2014)

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## Abstract

In micro- and thin-wall injection moulding the process conditions affect the developed internal structures and thus the resulting part properties. This paper investigates exemplarily on polyamide 66 the interactions of different cooling conditions on the morphological and crystalline structures. The investigations reveal that a slow cooling rate of the melt results in a homogeneous morphology and a higher degree of crystallinity and also a favoured crystalline structure. Consequently, the dielectric behaviour and light transmitting part properties are affected.


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## Body

## 1. Introduction

Microsystems technology is reputed as a prospective key technology. The primary areas of application for polymer microparts are found in medical technology or biotechnology, as components of optical systems, microgears in microfluidics, as electronics, and microelectromechanical systems [1, 2]. Due to increasing requirements for these microcomponents, a rise in the demand for higher part quality and the reproducibility simultaneously occurs [3].A reduction in part dimensions causes an increase in cooling that affects its morphological and mechanical properties [4–7]. Furthermore, long-term properties can also be affected [8–10]. To counteract this, new technologies and processing strategies have been developed. For example, a slow cooling of the melt using low conductive mould materials or a dynamic temperature control of the cavity can be executed [11–15]. A transfer of the mechanical material properties in microparts, determined and validated on standardized test specimens, is only partially possible [16, 17]. Consequently, it is necessary to investigate the effects of part dimensions on the usable material properties [18–20].In addition to the influence on the degree of crystallinity, the formation of crystalline structures is also affected by the process conditions. For example, polyamide 66 shows a polymorphic structure with two known stable crystal structures. These are denoted asα and γ [21, 22]. The α crystals are favoured by annealing or crystallization at higher temperatures whereas the γ crystals can be obtained at lower temperatures [21, 23]. According to Radusch et al. [24] the α crystals are more stable due to a better crystal perfection, whereas the γ structure can be transformed into the α by thermal treatment. Furthermore, Kolesov et al. [25] have shown that for polyamide 6 mechanical properties, for example, stiffness, increase with higher fraction of α crystals. The different crystalline forms can be detected amongst other technologies with DSC measurements [26, 27] and small-angle (SAXS) and wide-angle X-ray scatterings (WAXS) [24, 26, 28] or infrared spectroscopy [21, 25, 29].Furthermore, the internal structure of a polymer part affects the dielectric behaviour and was described for varied polymers [30–34]. In the case of polyamide 66 there are three relaxation peaks known [21]. These are labelled generally as α, β, and γ relaxations which are occurring at temperatures of 50°C, −80°C, and −140°C. Nuriel et al. [35] have shown that for higher crystalline polyamide 66 the relaxation shifts to a higher temperature. This correlates with an increasing activation energy for the relaxation process, which affects significantly the α relaxation.The cooling conditions affect, besides the mechanical properties, the optical part properties [36]. As shown by Kolesov et al. [25] a faster cooling leads to a higher light transmission, especially at a lower wavelength. This effect is due to the crucial effect of spherulite size in comparison to the size of lamella on the light scattering and transparency. Similar effects are described for the semicrystalline materials PE and PP [37, 38].However, a general representation of the interactions between the process conditions, the formation of internal structures, and the resulting part properties has not been done yet. Problems can be found in the modeling and understanding of the process, the investigation of internal structures into detail, or the influences on the part properties [4]. The aim of this paper is to correlate different process conditions (i.e., modified cooling conditions) with the resulting internal structures and the effect on part properties.


## 2. Materials and Methods

### 2.1. Material

The used material was a semicrystalline polyamide 66 (PA66) Ultramid A3K manufactured by BASF SE. The material was chosen because of its good flow properties and its relevance for the production of common micro- and thin-wall parts. Characteristic values of the material are shown in Table1.Table 1
Material properties (manufacturer’s data).
Parameter
PA66 Ultramid A3K
Density (ρ) (kg·m−3)
1130
Melting temperature (°C)
260
Crystallization temperature (°C)
236


### 2.2. Specimen and Processing

To investigate the effects of process conditions on the internal part properties a plate with a square-based shape with a length of 35 mm and a thickness of 0.5 mm was used (Figure1). For injection moulding an Arburg Allrounder 370 U 700–30/30 injection moulding machine is utilized, equipped with a position-controlled screw with a diameter of 15 mm. To achieve a dynamic mould temperature a variotherm temperature control system (type: SWTS 200, Single Temperiertechnik GmbH) is used. The system employs water as the circulating fluid and has a heating and cooling circuit-switching device. The heating circuit allows for a fluid temperature of up to 200°C. The master mould is maintained at a constant temperature for the purpose of processing stability, and only the temperature of the cavity inserts is actively controlled. This mould technology and the implemented dynamic mould tempering process allow for a significant variation of the part’s morphology and crystalline structure. These cavity inserts were built-up layer by layer from a steel powder using a rapid tooling process (LaserCusing, Concept Laser GmbH). This manufacturing process allows for a complex design of cooling channels (less than 2 mm behind the cavity surface) while also ensuring an optimized tempering of the cavity.Figure 1
Geometry of the used plate specimen.The combinations of insulation from the master mould and conformal cooling channels are conducive to particularly rapid temperature changes in the cavity. This allows a mould temperature during injection moulding to affect significantly the morphology development in the microspecimens. For this three different mould temperatures were selected: the minimal and maximal temperature to realize a reproducible process and a middle temperature according to standard process conditions. The mould temperature is measured by temperature sensors near the cavity. The curves of the temperature for the different mould temperatures during injection are shown in Figure2. The mould temperature is highlighted when the melt is injected in the defined tempered mould. After injection the mould is cooled down for safe ejection of part and runner. Relevant processing conditions for the materials are shown in Table 2.Table 2
Processing parameters.
Material
Melt temperature
[°C]
Mould temperature during injection
[°C]
Melt flow velocity
[cm3 s−1
]
PA 66
290
60/100/1801
18
1See also Figure 2.Figure 2
Mould temperatures during the injection moulding process to achieve varied morphology in the specimens (close-to-cavity measurement).


### 2.3. Characterization

#### 2.3.1. Morphology and Crystallinity

The crystalline morphology was investigated on 10µm thick cuts using polarised light microscopy. These cuts were taken out from the middle of the specimen along the injection direction.For crystallinity characterisation, infrared microscopy (Advantage, Spectra Tech Inc., Shelton, CT, USA) was applied. Three transmission measurements of thin cuts were carried out on each part. The ratior of extinction of the absorbance bands at 1199 cm−1 for the crystalline part and of 1180 cm−1 for the amorphous part describes the degree of crystallinity, as shown by Kohan [21]. The ratio r allows for an approximate calculation of the degree of crystallization with the following equation [39]:
(1)
f
r
=
-
1.30591
+
20.0028
r
-
1.86991
r
2
.
Furthermore, the two important crystalline modifications for the PA66, the α and the γ modifications, can be characterized by the extinction of typical absorbance bands. The band at a wavelength of 1417 cm−1 is typical for the α modification, whereas the γ modification affects the 1438 cm−1 band [21, 29]. To compare the relative amount of the different crystalline structures the ratios of these bands 1417 cm−1/1438 cm−1 are used, the so-called polymorphy-ratio. An increasing value describes a higher fraction of α and correlates with a slower cooling rate of the material.


#### 2.3.2. Dielectric Behaviour

For dielectric thermal analysis (DETA) a circular blank with a diameter of 25 mm was taken out of the specimens. These blanks were characterized using a dynamic mechanical analyzer (DMA; RSA-G2, TA Instruments) with a DETA measuring system Agilent 4294. Before testing the specimens were dry conditioned. The DETA was carried out at four frequencies of 2 × 103 to 2 × 106 Hz between a temperature sweep of 20 and 120°C (heating rate 2 K min−1). The DETA measurement allows the characterization of the reversible stored energy ε
′ in the material and the proportional dissipated energy ε
′′. These values are used to calculate the dissipation factor tan
δ according to
(2)
tan
δ
=
ε
′′
ε
′
.The dissipation factortan
δ is often used and evaluated in technical applications of dielectric relaxation spectroscopy, especially for electrotechnical characterization of a material. Besides, in contrast to the local-resolved FTIR analysis by means of the DETA measurements only integral properties can be characterized that means layer dependent properties cannot be detected.


#### 2.3.3. Translucence

The translucence of the specimens was analyzed with an UV/VIS spectrometer Lambda 18 (Perkin Elmer Inc.). Therefore, the transmission of the light through the specimens was measured at a wavelength of 250–850 nm (visible range ca. 380–780 nm).


## 2.1. Material

The used material was a semicrystalline polyamide 66 (PA66) Ultramid A3K manufactured by BASF SE. The material was chosen because of its good flow properties and its relevance for the production of common micro- and thin-wall parts. Characteristic values of the material are shown in Table1.Table 1
Material properties (manufacturer’s data).
Parameter
PA66 Ultramid A3K
Density (ρ) (kg·m−3)
1130
Melting temperature (°C)
260
Crystallization temperature (°C)
236


## 2.2. Specimen and Processing

To investigate the effects of process conditions on the internal part properties a plate with a square-based shape with a length of 35 mm and a thickness of 0.5 mm was used (Figure1). For injection moulding an Arburg Allrounder 370 U 700–30/30 injection moulding machine is utilized, equipped with a position-controlled screw with a diameter of 15 mm. To achieve a dynamic mould temperature a variotherm temperature control system (type: SWTS 200, Single Temperiertechnik GmbH) is used. The system employs water as the circulating fluid and has a heating and cooling circuit-switching device. The heating circuit allows for a fluid temperature of up to 200°C. The master mould is maintained at a constant temperature for the purpose of processing stability, and only the temperature of the cavity inserts is actively controlled. This mould technology and the implemented dynamic mould tempering process allow for a significant variation of the part’s morphology and crystalline structure. These cavity inserts were built-up layer by layer from a steel powder using a rapid tooling process (LaserCusing, Concept Laser GmbH). This manufacturing process allows for a complex design of cooling channels (less than 2 mm behind the cavity surface) while also ensuring an optimized tempering of the cavity.Figure 1
Geometry of the used plate specimen.The combinations of insulation from the master mould and conformal cooling channels are conducive to particularly rapid temperature changes in the cavity. This allows a mould temperature during injection moulding to affect significantly the morphology development in the microspecimens. For this three different mould temperatures were selected: the minimal and maximal temperature to realize a reproducible process and a middle temperature according to standard process conditions. The mould temperature is measured by temperature sensors near the cavity. The curves of the temperature for the different mould temperatures during injection are shown in Figure2. The mould temperature is highlighted when the melt is injected in the defined tempered mould. After injection the mould is cooled down for safe ejection of part and runner. Relevant processing conditions for the materials are shown in Table 2.Table 2
Processing parameters.
Material
Melt temperature
[°C]
Mould temperature during injection
[°C]
Melt flow velocity
[cm3 s−1
]
PA 66
290
60/100/1801
18
1See also Figure 2.Figure 2
Mould temperatures during the injection moulding process to achieve varied morphology in the specimens (close-to-cavity measurement).


## 2.3. Characterization

### 2.3.1. Morphology and Crystallinity

The crystalline morphology was investigated on 10µm thick cuts using polarised light microscopy. These cuts were taken out from the middle of the specimen along the injection direction.For crystallinity characterisation, infrared microscopy (Advantage, Spectra Tech Inc., Shelton, CT, USA) was applied. Three transmission measurements of thin cuts were carried out on each part. The ratior of extinction of the absorbance bands at 1199 cm−1 for the crystalline part and of 1180 cm−1 for the amorphous part describes the degree of crystallinity, as shown by Kohan [21]. The ratio r allows for an approximate calculation of the degree of crystallization with the following equation [39]:
(1)
f
r
=
-
1.30591
+
20.0028
r
-
1.86991
r
2
.
Furthermore, the two important crystalline modifications for the PA66, the α and the γ modifications, can be characterized by the extinction of typical absorbance bands. The band at a wavelength of 1417 cm−1 is typical for the α modification, whereas the γ modification affects the 1438 cm−1 band [21, 29]. To compare the relative amount of the different crystalline structures the ratios of these bands 1417 cm−1/1438 cm−1 are used, the so-called polymorphy-ratio. An increasing value describes a higher fraction of α and correlates with a slower cooling rate of the material.


### 2.3.2. Dielectric Behaviour

For dielectric thermal analysis (DETA) a circular blank with a diameter of 25 mm was taken out of the specimens. These blanks were characterized using a dynamic mechanical analyzer (DMA; RSA-G2, TA Instruments) with a DETA measuring system Agilent 4294. Before testing the specimens were dry conditioned. The DETA was carried out at four frequencies of 2 × 103 to 2 × 106 Hz between a temperature sweep of 20 and 120°C (heating rate 2 K min−1). The DETA measurement allows the characterization of the reversible stored energy ε
′ in the material and the proportional dissipated energy ε
′′. These values are used to calculate the dissipation factor tan
δ according to
(2)
tan
δ
=
ε
′′
ε
′
.The dissipation factortan
δ is often used and evaluated in technical applications of dielectric relaxation spectroscopy, especially for electrotechnical characterization of a material. Besides, in contrast to the local-resolved FTIR analysis by means of the DETA measurements only integral properties can be characterized that means layer dependent properties cannot be detected.


### 2.3.3. Translucence

The translucence of the specimens was analyzed with an UV/VIS spectrometer Lambda 18 (Perkin Elmer Inc.). Therefore, the transmission of the light through the specimens was measured at a wavelength of 250–850 nm (visible range ca. 380–780 nm).


## 2.3.1. Morphology and Crystallinity

The crystalline morphology was investigated on 10µm thick cuts using polarised light microscopy. These cuts were taken out from the middle of the specimen along the injection direction.For crystallinity characterisation, infrared microscopy (Advantage, Spectra Tech Inc., Shelton, CT, USA) was applied. Three transmission measurements of thin cuts were carried out on each part. The ratior of extinction of the absorbance bands at 1199 cm−1 for the crystalline part and of 1180 cm−1 for the amorphous part describes the degree of crystallinity, as shown by Kohan [21]. The ratio r allows for an approximate calculation of the degree of crystallization with the following equation [39]:
(1)
f
r
=
-
1.30591
+
20.0028
r
-
1.86991
r
2
.
Furthermore, the two important crystalline modifications for the PA66, the α and the γ modifications, can be characterized by the extinction of typical absorbance bands. The band at a wavelength of 1417 cm−1 is typical for the α modification, whereas the γ modification affects the 1438 cm−1 band [21, 29]. To compare the relative amount of the different crystalline structures the ratios of these bands 1417 cm−1/1438 cm−1 are used, the so-called polymorphy-ratio. An increasing value describes a higher fraction of α and correlates with a slower cooling rate of the material.


## 2.3.2. Dielectric Behaviour

For dielectric thermal analysis (DETA) a circular blank with a diameter of 25 mm was taken out of the specimens. These blanks were characterized using a dynamic mechanical analyzer (DMA; RSA-G2, TA Instruments) with a DETA measuring system Agilent 4294. Before testing the specimens were dry conditioned. The DETA was carried out at four frequencies of 2 × 103 to 2 × 106 Hz between a temperature sweep of 20 and 120°C (heating rate 2 K min−1). The DETA measurement allows the characterization of the reversible stored energy ε
′ in the material and the proportional dissipated energy ε
′′. These values are used to calculate the dissipation factor tan
δ according to
(2)
tan
δ
=
ε
′′
ε
′
.The dissipation factortan
δ is often used and evaluated in technical applications of dielectric relaxation spectroscopy, especially for electrotechnical characterization of a material. Besides, in contrast to the local-resolved FTIR analysis by means of the DETA measurements only integral properties can be characterized that means layer dependent properties cannot be detected.


## 2.3.3. Translucence

The translucence of the specimens was analyzed with an UV/VIS spectrometer Lambda 18 (Perkin Elmer Inc.). Therefore, the transmission of the light through the specimens was measured at a wavelength of 250–850 nm (visible range ca. 380–780 nm).


## 3. Results and Discussion

### 3.1. Morphology

The process conditions, especially the cooling of the polymer melt, affect the morphology of thin-wall parts as discussed above. The morphological structure of the different manufactured specimens is shown in Figure3. A mould temperature of 60°C leads to a fast cooling of the material (especially in the surface area which has direct contact with the mould) already during the injection phase. This entails a significant amorphous-like surface layer and only small single spherulites in the core area. An increasing mould temperature of 100°C reduces the cooling velocity resulting in a smaller surface layer and an increasingly spherulitic morphology. The mould temperature of 180°C during injection results in an almost homogeneous morphology over the entire cross section. This is due to the reduced cooling velocity of the melt and the sufficient time for crystallization of the polymer. Only the surface area reveals a smaller spherulitic structure.Figure 3
Morphology in dependence of process conditions.


### 3.2. Crystallinity

Correlating with the influence on the morphology the different cooling conditions also affect the degree of crystallinity. The degree of crystallinity of the different manufactured specimens is shown in Figure4. All the parts show a different gradient over the cross section, with a low degree in the surface area and an increasing value to the core area. Furthermore, the parts that had been injection moulded at a mould temperature of 60°C show a low degree of crystallinity over the complete cross section. Those parts injection moulded at higher mould temperatures show an increased degree of crystallinity. The degree of crystallinity is approximately 5% higher as in the parts injection moulded at 60°C. In addition, a further increase of the mould temperature up to 180°C during the melt injection shows less effect on the degree of crystallinity. At a mould temperature of 100°C the degree of crystallinity reaches a depth of ca. 100 µm from the surface, a maximum value, and decreases to the core. This is attributed to a shear induced nucleation (which favors the crystallization process) in the surface and a more thermal crystallization in the core and correlates with the results of other works [40, 41]. A mould temperature of 180°C does not show such a difference in crystallinity across the thickness. These specimens reveal a nearly homogeneous degree of crystallinity over the cross section.Figure 4
Degree of crystallinity over the cross section in dependence of process conditions.In Figure5 the ratio of the absorbance bands of 1417 cm−1 to 1438 cm−1 (polymorphy-ratio) is illustrated over the cross section of the specimens. An increasing ratio suggests a higher fraction of α crystal modification due to a slower cooling rate. The values of the ratio of the specimens show a low value in the surface area and a higher ratio in the core area. Accordingly, due to the high cooling rate in the surface area the γ modification is preferably formed at ca. 100 µm from the surface. This correlates with the degree of crystallinity, which is also reduced in the surface area. Furthermore, the specimens injection moulded at 60°C and 100°C reveal a decreasing ratio in the core which also correlates with the degree of crystallinity.Figure 5
Polymorphy-ratio of the absorbance at a wavelength of 1417 cm−1 (α modification) and 1438 cm−1 (β modification) over the cross section in dependence of process conditions.The specimens injection moulded at 180°C have a higher polymorphy-ratio, thus a higher fraction ofα crystals due to the slower cooling. Furthermore, these specimens show an almost constant ratio in the core and the difference of the ratio between core and surface is also reduced which correlates with the above discussed homogeneously morphological structure and the degree of crystallinity across the thickness. Consequently, based on defined process conditions, that is, defined cooling conditions during processing, the molecular chains can reach a more compact packaging during crystallization. This allows a higher crystal perfection resulting in an increasing fraction of α crystals.


### 3.3. Dielectric Behaviour

Figure6 shows the dissipation factor of the dielectric measurements of the PA66. The investigations are focused on the α relaxation; thus the temperature range of 20–120°C is of interest for the investigations. As expected, the α relaxation is affected by the frequency, in which a higher frequency shifts the relaxation to a higher temperature [35].Dissipation factortan
δ at varied frequencies for the specimens injection moulded at 60°C and 180°C.
(a)
(b)However, the measurements reveal that the process induced modified internal properties affect the dielectric behaviour of the material. The specimens with the favoured crystalline morphology reveal a shift of the dissipation factor to a higher value. This is due to a higher loss factor that means more energy is dissipated by the material for the relaxation process. This effect was already described [35]. Because of the higher degree of crystallinity and also the favoured crystalline structure (i.e., an increased α crystal modification) more energy is used to activate the relaxation process.Figure7 focuses on the peak temperature and the relaxation factor for the α relaxation. It reveals as mentioned above the shift of the relaxation temperature with increasing frequency. Furthermore, the process induced modified inner structure leads also to a shift of the temperature. The observed temperature shift amounts to more than 3 K, but with increasing frequency the temperature shift diminishes which reflects the viscoelastic nature of polymers by obeying the time-temperature superposition principle [35].Peak temperature (left) and dissipation factor (right) of theα relaxation in dependence of frequency and process conditions.
(a)
(b)The dissipation factor is also affected by the frequency and the internal structure. A higher frequency increases the dissipation factor, similar to the temperature shift. The influence of the inner structure, due to a reduced cooling rate, affects also the dissipation factor as mentioned above. The change in the process induced inner structure leads ton approximately 50% higher dissipation factor independent of the applied frequency. Consequently, the dissipation factor correlates constantly with the degree and the modification of the crystalline properties. However, it is not possible with these results to separate stringently the influence of the amount of crystallinity and the crystalline modifications. Further investigations should reveal the influence of degree of crystallinity and crystalline modifications on the dielectric properties.


### 3.4. Translucence

Figure8 shows the transmission of the material shown in dependence of the cooling conditions. The specimens obtain a transmission of 90% in the visible light area at the upper end. The degree of transmission decreases slightly with reduced wavelength. At the lower end of the visible light the light absorption increases and only 67 to 75% of the light is transmitted.Figure 8
Normalized light transmission of the specimens in dependence of cooling conditions as function of the wavelength.As expected, the specimen injection moulded at a low mould temperature shows a higher value of light transmittance as the specimens injection moulded at higher mould temperatures. This is due to the fact that the process induced higher degree of crystallinity and more spherulitic morphology (see Figure3) as a result of the slower cooling rate. This correlates with the results of Kolesov et al. [25] for PA6 or other semicrystalline polymers [37, 38]. However, the difference of light transmittance in the lower end of the visible light band seems to have little effect on the amount of perceived brightness, because this is mostly attributed to the light transmittance in the wavelength between 500 and 600 nm [42].


## 3.1. Morphology

The process conditions, especially the cooling of the polymer melt, affect the morphology of thin-wall parts as discussed above. The morphological structure of the different manufactured specimens is shown in Figure3. A mould temperature of 60°C leads to a fast cooling of the material (especially in the surface area which has direct contact with the mould) already during the injection phase. This entails a significant amorphous-like surface layer and only small single spherulites in the core area. An increasing mould temperature of 100°C reduces the cooling velocity resulting in a smaller surface layer and an increasingly spherulitic morphology. The mould temperature of 180°C during injection results in an almost homogeneous morphology over the entire cross section. This is due to the reduced cooling velocity of the melt and the sufficient time for crystallization of the polymer. Only the surface area reveals a smaller spherulitic structure.Figure 3
Morphology in dependence of process conditions.


## 3.2. Crystallinity

Correlating with the influence on the morphology the different cooling conditions also affect the degree of crystallinity. The degree of crystallinity of the different manufactured specimens is shown in Figure4. All the parts show a different gradient over the cross section, with a low degree in the surface area and an increasing value to the core area. Furthermore, the parts that had been injection moulded at a mould temperature of 60°C show a low degree of crystallinity over the complete cross section. Those parts injection moulded at higher mould temperatures show an increased degree of crystallinity. The degree of crystallinity is approximately 5% higher as in the parts injection moulded at 60°C. In addition, a further increase of the mould temperature up to 180°C during the melt injection shows less effect on the degree of crystallinity. At a mould temperature of 100°C the degree of crystallinity reaches a depth of ca. 100 µm from the surface, a maximum value, and decreases to the core. This is attributed to a shear induced nucleation (which favors the crystallization process) in the surface and a more thermal crystallization in the core and correlates with the results of other works [40, 41]. A mould temperature of 180°C does not show such a difference in crystallinity across the thickness. These specimens reveal a nearly homogeneous degree of crystallinity over the cross section.Figure 4
Degree of crystallinity over the cross section in dependence of process conditions.In Figure5 the ratio of the absorbance bands of 1417 cm−1 to 1438 cm−1 (polymorphy-ratio) is illustrated over the cross section of the specimens. An increasing ratio suggests a higher fraction of α crystal modification due to a slower cooling rate. The values of the ratio of the specimens show a low value in the surface area and a higher ratio in the core area. Accordingly, due to the high cooling rate in the surface area the γ modification is preferably formed at ca. 100 µm from the surface. This correlates with the degree of crystallinity, which is also reduced in the surface area. Furthermore, the specimens injection moulded at 60°C and 100°C reveal a decreasing ratio in the core which also correlates with the degree of crystallinity.Figure 5
Polymorphy-ratio of the absorbance at a wavelength of 1417 cm−1 (α modification) and 1438 cm−1 (β modification) over the cross section in dependence of process conditions.The specimens injection moulded at 180°C have a higher polymorphy-ratio, thus a higher fraction ofα crystals due to the slower cooling. Furthermore, these specimens show an almost constant ratio in the core and the difference of the ratio between core and surface is also reduced which correlates with the above discussed homogeneously morphological structure and the degree of crystallinity across the thickness. Consequently, based on defined process conditions, that is, defined cooling conditions during processing, the molecular chains can reach a more compact packaging during crystallization. This allows a higher crystal perfection resulting in an increasing fraction of α crystals.


## 3.3. Dielectric Behaviour

Figure6 shows the dissipation factor of the dielectric measurements of the PA66. The investigations are focused on the α relaxation; thus the temperature range of 20–120°C is of interest for the investigations. As expected, the α relaxation is affected by the frequency, in which a higher frequency shifts the relaxation to a higher temperature [35].Dissipation factortan
δ at varied frequencies for the specimens injection moulded at 60°C and 180°C.
(a)
(b)However, the measurements reveal that the process induced modified internal properties affect the dielectric behaviour of the material. The specimens with the favoured crystalline morphology reveal a shift of the dissipation factor to a higher value. This is due to a higher loss factor that means more energy is dissipated by the material for the relaxation process. This effect was already described [35]. Because of the higher degree of crystallinity and also the favoured crystalline structure (i.e., an increased α crystal modification) more energy is used to activate the relaxation process.Figure7 focuses on the peak temperature and the relaxation factor for the α relaxation. It reveals as mentioned above the shift of the relaxation temperature with increasing frequency. Furthermore, the process induced modified inner structure leads also to a shift of the temperature. The observed temperature shift amounts to more than 3 K, but with increasing frequency the temperature shift diminishes which reflects the viscoelastic nature of polymers by obeying the time-temperature superposition principle [35].Peak temperature (left) and dissipation factor (right) of theα relaxation in dependence of frequency and process conditions.
(a)
(b)The dissipation factor is also affected by the frequency and the internal structure. A higher frequency increases the dissipation factor, similar to the temperature shift. The influence of the inner structure, due to a reduced cooling rate, affects also the dissipation factor as mentioned above. The change in the process induced inner structure leads ton approximately 50% higher dissipation factor independent of the applied frequency. Consequently, the dissipation factor correlates constantly with the degree and the modification of the crystalline properties. However, it is not possible with these results to separate stringently the influence of the amount of crystallinity and the crystalline modifications. Further investigations should reveal the influence of degree of crystallinity and crystalline modifications on the dielectric properties.


## 3.4. Translucence

Figure8 shows the transmission of the material shown in dependence of the cooling conditions. The specimens obtain a transmission of 90% in the visible light area at the upper end. The degree of transmission decreases slightly with reduced wavelength. At the lower end of the visible light the light absorption increases and only 67 to 75% of the light is transmitted.Figure 8
Normalized light transmission of the specimens in dependence of cooling conditions as function of the wavelength.As expected, the specimen injection moulded at a low mould temperature shows a higher value of light transmittance as the specimens injection moulded at higher mould temperatures. This is due to the fact that the process induced higher degree of crystallinity and more spherulitic morphology (see Figure3) as a result of the slower cooling rate. This correlates with the results of Kolesov et al. [25] for PA6 or other semicrystalline polymers [37, 38]. However, the difference of light transmittance in the lower end of the visible light band seems to have little effect on the amount of perceived brightness, because this is mostly attributed to the light transmittance in the wavelength between 500 and 600 nm [42].


## 4. Conclusions

In micro- and thin-wall injection moulding the process conditions, especially the cooling conditions, have particularly great importance in the development of the internal structure during processing of thermoplastic polymers. Consequently, the properties in use are also influenced. The investigations in this paper discuss the influence of different process conditions exemplarily on PA66 on the formation of the inner structure of an injection moulded micropart and the resulting properties in use.(1)
A faster cooling of the polymer melt leads as expected to a modified morphology. A slow cooling, due to increased mould temperatures during injection, reduces or inhibits the development of a surface layer and allows a more homogeneous morphology. This also affects the degree of crystallinity which increases with a reduced cooling rate.
(2)
Reduced cooling conditions favour also the development of crystalline modifications. In the case of the used PA66 moreα crystals are formed by slow cooling. This was revealed by FTIR spectroscopy and correlates also with DETA measurements.
(3)
The influence of the dielectric behaviour can be used for material analysis as for modifying part properties with regard to their applications.
(4)
However, the influence of the inner structure can also affect the properties in use which was exemplarily shown on the light transmittance. The translucence can be reduced (or increased) with slow (or fast) cooling of the part due to a modified crystalline structure. But since the light transmittance is influenced below a wavelength of approximately 400 nm, the effect on visible translucence will be rather small for the applied polymer. However, this effect has to be investigated in further studies.Future investigation should also reveal more in detail the relationship between process conditions, the developed inner structures, and the resulting part properties. Particularly, correlations with static and dynamic mechanical properties and the effect of physical or chemical ageing are of interest, as well as the transfer to other polymers.



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*Source: 718926-2014-12-21.xml*