TW202317682A - Multilayer expanded bead - Google Patents

Multilayer expanded bead Download PDF

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TW202317682A
TW202317682A TW111129682A TW111129682A TW202317682A TW 202317682 A TW202317682 A TW 202317682A TW 111129682 A TW111129682 A TW 111129682A TW 111129682 A TW111129682 A TW 111129682A TW 202317682 A TW202317682 A TW 202317682A
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ethylene
random copolymer
propylene random
expanded
molecular weight
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大井貴史
太田肇
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日商Jsp股份有限公司
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Abstract

The object of the invention is to provide a polypropylene-based resin multilayer expanded bead capable of in-mold forming an expanded bead molding with little variation in dimensional changes due to shrinkage after molding even if water cooling time after in-mold molding is shortened. The solution of the invention is that the foam core layer of the polyolefin-based resin multilayer expanded beads of the invention is composed of ethylene-propylene random copolymer (A) with a specific ethylene content the coating layer is composed of polyolefin-based resin (B), wherein the DSC curve of the polyolefin-based resin (B) has one or more melting peak, he melting peak temperature of at least one of the melting peaks is lower than the melting point (Tm) of the random copolymer (A),the weight average molecular weight (Mw) of the random copolymer (A) is within a specific range, and the ratio (Mw/Mn) of the weight average molecular weight (Mw) to the number average molecular weight (Mn) of the ethylene-propylene random copolymer (A) is within a specific range.

Description

多層發泡粒子multi-layer expanded particles

本發明有關多層發泡粒子,更詳言之有關模內成形用之多層發泡粒子。The present invention relates to multilayer expanded particles, and more specifically relates to multilayer expanded particles for in-mold molding.

聚丙烯系樹脂發泡粒子加工性優異,藉由模內成形所得之發泡粒子成形體可進行複雜形狀的賦形,機械強度、緩衝性、價格之均衡優異,故已作為緩衝包裝材、汽車構件、建築構件等使用。Polypropylene-based resin foamed particles have excellent processability, and the expanded particle molded body obtained by in-mold molding can be shaped into complex shapes. The balance of mechanical strength, cushioning performance, and price is excellent, so it has been used as cushioning packaging materials, automobiles, etc. Components, building components, etc.

作為該聚丙烯系數之發泡粒子有例如專利文獻1中揭示者。 [先前技術文獻] [專利文獻] Examples of expanded particles of the polypropylene modulus include those disclosed in Patent Document 1. [Prior Art Literature] [Patent Document]

[專利文獻1]日本特開2004-68016號公報[Patent Document 1] Japanese Unexamined Patent Publication No. 2004-68016

[發明欲解決之課題][Problem to be solved by the invention]

然而,使用專利文獻1所記載之多層發泡粒子以低的蒸氣壓進行模內成形時,若欲獲得複雜形狀的成形體或大型成形體,則蒸汽難以均勻行進至模具內的發泡粒子全體而有產生加熱不均之情況。其結果,成形後發生之收縮程度於各發泡粒子成形體之部分不同,或者容易產生尺寸偏差,而於嚴格管理成形體之尺寸上發生負擔過重等之問題。However, when in-mold molding is performed at a low steam pressure using the multilayered expanded beads described in Patent Document 1, if it is desired to obtain a molded article with a complex shape or a large molded article, it is difficult for the steam to travel uniformly to the entire expanded beads in the mold. However, uneven heating may occur. As a result, the degree of shrinkage after molding differs from part to part of each expanded bead molded body, or dimensional deviation tends to occur, resulting in problems such as excessive burden on strict control of the size of the molded body.

另一方面,為了解決此加熱不均之課題,若於更高的蒸氣壓進行模內成形、延長加熱時間、使模內之泡粒子充分加熱時,可減小尺寸偏差。然而,有模具成形後的冷卻時間變長,整體成形時間亦變長之虞。On the other hand, in order to solve the problem of uneven heating, if the in-mold molding is performed at a higher vapor pressure, the heating time is prolonged, and the bubble particles in the mold are fully heated, the size deviation can be reduced. However, there is a possibility that the cooling time after mold forming becomes longer, and the overall molding time may also become longer.

本發明之課題在於提供即使模內成形後之冷卻時間縮短,亦可於模內成形出成形後的收縮小、尺寸變化之偏差小的發泡粒子成形體之多層發泡粒子。 [用以解決課題之手段] The object of the present invention is to provide multi-layered expanded beads capable of in-mold forming an expanded bead molded body with less shrinkage after molding and less variation in dimensional change even if the cooling time after in-mold molding is shortened. [Means to solve the problem]

依據本發明,提供以下所示之多層發泡粒子。 [1] 一種多層發泡粒子,其係具有發泡芯層與被覆該發泡芯層之被覆層之多層發泡粒子,其特徵為 該發泡芯層係由乙烯成分含有率2.5質量%以上3.5質量%以下之乙烯-丙烯無規共聚物(A)構成, 該被覆層係由聚烯烴系樹脂(B)構成,藉由示差掃描熱量測定(DSC)所測定之該聚烯烴系樹脂(B)之DSC曲線具有一個以上之熔解波峰,該熔解波峰中之至少一個熔解波峰的熔解波峰溫度比該乙烯-丙烯無規共聚物(A)之熔點(Tm)低, 該乙烯-丙烯無規共聚物(A)之重量平均分子量(Mw)為20萬以上30萬以下,該乙烯-丙烯無規共聚物(A)之該重量平均分子量(Mw)相對於數平均分子量(Mn)的比(Mw/Mn)為3.5以上5以下。 [2] 如請求項1之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mz)相對於該乙烯-丙烯無規共聚物(A)之數平均分子量(Mn)的比(Mz/Mn)為9.5以上且未達13。 [3] 如前述1或2之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之熔點(Tm)為130℃以上150℃以下。 [4] 如前述1至3中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之結晶化溫度(Tc)與該乙烯-丙烯無規共聚物(A)之熔點(Tmc)滿足下述(1)式:

Figure 02_image001
(但,式中之Tmc、Tc之單位均為℃)。 [5] 如前述1至4中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mz)為50萬以上100萬以下。 [6] 如前述5之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mw)相對於該乙烯-丙烯無規共聚物(A)之數平均分子量(Mz)之比(Mz/Mw)為2以上5以下。 [7] 如前述1至6中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之撓曲彈性模數為750MPa以上。 [8] 如前述1至7中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之熔體流動速率為1g/10分鐘以上20g/10分鐘以下。 [9] 如前述1至8中任一項之多層發泡粒子,其中前述多層發泡粒子之體密度為10kg/m 3以上300kg/m 3以下。 [10] 如前述1至9中任一項之多層發泡粒子,其中構成前述多層發泡粒子之發泡芯層之平均氣泡徑為20μm以上400μm以下。 [11] 一種發泡粒子成形體,其係將如前述1至10中任一項之多層發泡粒子進行模內成形而成。 [12] 如前述11之發泡粒子成形體,其中前述發泡粒子成形體之50%變形時壓縮應力為100kPa以上500kPa以下。 [發明效果] According to the present invention, multilayer expanded particles shown below are provided. [1] A multi-layer expanded particle, which is a multi-layer expanded particle having a foam core layer and a coating layer covering the foam core layer, characterized in that the foam core layer is composed of an ethylene content of 2.5% by mass or more 3.5% by mass or less of ethylene-propylene random copolymer (A), the covering layer is composed of polyolefin resin (B), and the polyolefin resin (B) measured by differential scanning calorimetry (DSC) The DSC curve of ) has more than one melting peak, and the melting peak temperature of at least one of the melting peaks is lower than the melting point (Tm) of the ethylene-propylene random copolymer (A), the ethylene-propylene random copolymer The weight average molecular weight (Mw) of the substance (A) is not less than 200,000 and not more than 300,000, and the ratio of the weight average molecular weight (Mw) to the number average molecular weight (Mn) of the ethylene-propylene random copolymer (A) (Mw /Mn) is 3.5 or more and 5 or less. [2] The multilayer expanded particle as claimed in item 1, wherein the Z average molecular weight (Mz) of the aforementioned ethylene-propylene random copolymer (A) is relative to the number average molecular weight (Mz) of the ethylene-propylene random copolymer (A) ( The ratio (Mz/Mn) of Mn) is 9.5 or more and less than 13. [3] The multilayer expanded particle according to the above-mentioned 1 or 2, wherein the melting point (Tm) of the ethylene-propylene random copolymer (A) is 130°C or more and 150°C or less. [4] The multilayer expanded particle according to any one of the aforementioned 1 to 3, wherein the crystallization temperature (Tc) of the aforementioned ethylene-propylene random copolymer (A) is the same as that of the ethylene-propylene random copolymer (A). The melting point (Tmc) satisfies the following formula (1):
Figure 02_image001
(However, the units of Tmc and Tc in the formula are both °C). [5] The multilayer expanded particle according to any one of 1 to 4 above, wherein the Z-average molecular weight (Mz) of the ethylene-propylene random copolymer (A) is not less than 500,000 and not more than 1 million. [6] The multilayer expanded particle as described in the above-mentioned 5, wherein the Z-average molecular weight (Mw) of the aforementioned ethylene-propylene random copolymer (A) is relative to the number-average molecular weight (Mz) of the ethylene-propylene random copolymer (A). ) ratio (Mz/Mw) is 2 or more and 5 or less. [7] The multilayer expanded particle according to any one of 1 to 6 above, wherein the flexural modulus of elasticity of the ethylene-propylene random copolymer (A) is 750 MPa or more. [8] The multilayer expanded particle according to any one of 1 to 7 above, wherein the melt flow rate of the ethylene-propylene random copolymer (A) is not less than 1 g/10 minutes and not more than 20 g/10 minutes. [9] The multilayer expanded bead according to any one of 1 to 8 above, wherein the bulk density of the multilayer expanded bead is not less than 10 kg/m 3 and not more than 300 kg/m 3 . [10] The multilayered expanded bead according to any one of 1 to 9 above, wherein the average cell diameter of the foamed core layer constituting the multilayered expanded bead is not less than 20 μm and not more than 400 μm. [11] A molded expanded bead formed by in-mold forming the multilayered expanded bead described in any one of 1 to 10 above. [12] The expanded bead molded article according to the above 11, wherein the compressive stress at 50% deformation of the expanded bead molded article is not less than 100 kPa and not more than 500 kPa. [Invention effect]

依據本發明,可提供可縮短模內成形後之冷卻時間,即使冷卻時間縮短,亦可於模內成形出成形後的收縮小、尺寸變化之偏差小的發泡粒子成形體之多層發泡粒子。According to the present invention, the cooling time after in-mold molding can be shortened, and even if the cooling time is shortened, multi-layered expanded particles can be formed in the mold with small shrinkage after molding and small variations in dimensional changes. .

以下,針對本發明之多層發泡粒子詳細說明。 本發明之多層發泡粒子(以下亦簡稱發泡粒子)具有發泡芯層與被覆該發泡芯層之被覆層。此外,該發泡芯層係由乙烯-丙烯無規共聚物(A)(以下亦簡稱共聚物(A))構成,該被覆層係由聚烯烴系樹脂(B)構成。 Hereinafter, the multilayer expanded particle of the present invention will be described in detail. The multilayer expanded particle of the present invention (hereinafter also referred to as expanded particle) has a foamed core layer and a coating layer covering the foamed core layer. In addition, the foam core layer is composed of ethylene-propylene random copolymer (A) (hereinafter also referred to as copolymer (A)), and the covering layer is composed of polyolefin resin (B).

前述發泡芯層處於發泡狀態。所謂發泡狀態係指形成氣泡構造之狀態。 另一方面,前述被覆層可為發泡狀態,亦可為非發泡狀態,但較佳為非發泡狀態。又,非發泡狀態不僅為氣泡完全不存在(如後述,亦包含使樹脂粒子發泡時暫時形成之氣泡被破壞而使氣泡消滅者),亦包含在不影響所得成形體之機械強度的範圍內,稍存在微小氣泡者。 The aforementioned foam core layer is in a foamed state. The foamed state means a state in which a cell structure is formed. On the other hand, the aforementioned covering layer may be in a foamed state or in a non-foamed state, but is preferably in a non-foamed state. In addition, the non-foaming state is not only the absence of bubbles at all (as described later, it also includes the destruction of the bubbles temporarily formed when the resin particles are foamed to eliminate the bubbles), and also includes the range that does not affect the mechanical strength of the obtained molded body. Inside, those with slight air bubbles.

作為發泡芯層經被覆層被覆之態樣,可為發泡芯層完全經被覆層被覆,亦可為發泡芯層之一部分露出。所謂發泡芯層露出之構造,舉例為例如僅圓柱狀之發泡芯層的周面經被覆層被覆,而發泡芯層露出於圓柱的上面或底面之構造等。As an aspect in which the foam core layer is covered with the covering layer, the foam core layer may be completely covered with the covering layer, or a part of the foam core layer may be exposed. The structure in which the foam core layer is exposed is, for example, a structure in which only the peripheral surface of the cylindrical foam core layer is covered with the coating layer, and the foam core layer is exposed on the top or bottom of the cylinder.

其次,針對構成發泡芯層之乙烯-丙烯無規共聚物(A)加以說明。 該共聚物(A)之乙烯成分含有率為2.5質量%以上3.5質量%以下,較佳為2.6質量%以上3.3質量%以下。該含有率若在該範圍內,則具有適度機械強度,在低蒸氣壓下顯示充分之二次發泡性,故可適合作為模內成形用之發泡粒子使用。且,所得之發泡粒子之機械強度與可形性之均衡優異。 該含有率過小時,有無法在低蒸汽壓下進行模內成形之虞。另一方面,該含有率過大時,有剛性過於降低之虞。 Next, the ethylene-propylene random copolymer (A) constituting the foam core layer will be described. The copolymer (A) has an ethylene content of 2.5% by mass to 3.5% by mass, preferably 2.6% by mass to 3.3% by mass. If the content is within this range, it has moderate mechanical strength and exhibits sufficient secondary foamability under low vapor pressure, so it can be suitably used as expanded particles for in-mold molding. Furthermore, the resulting expanded particles have an excellent balance between mechanical strength and formability. If the content is too small, in-mold molding under low steam pressure may not be possible. On the other hand, when this content rate is too large, there exists a possibility that rigidity may fall too much.

又,共聚物(A)中,丙烯成分含有率較佳為95質量%以上,更佳超過96.5質量%且未達97.5質量%,又更佳超過96.7質量%且未達97.4質量%。共聚物(A)由於以丙烯成分為主成分,故被分類為丙烯系樹脂。Also, in the copolymer (A), the content of the propylene component is preferably at least 95% by mass, more preferably more than 96.5% by mass and less than 97.5% by mass, more preferably more than 96.7% by mass and less than 97.4% by mass. Since the copolymer (A) contains a propylene component as a main component, it is classified as a propylene-type resin.

本說明書中,乙烯-丙烯無規共聚物(A)之乙烯成分含有率可藉由利用IR光譜決定之習知方法求出。具體而言,藉由高分子分析手冊(日本分析化學會高分子分析研究座談會編,出版年月:1995年1月,出版社:紀伊國屋書店,頁碼:615~616,「II.2.3 2.3.4丙烯/乙烯共聚物」)中記載之方法,即由以特定係數修正乙烯之吸光度後之值與薄膜狀試驗片之厚度等的關係而定量之方法求出。In this specification, the ethylene content rate of the ethylene-propylene random copolymer (A) can be calculated|required by the conventional method determined using IR spectrum. Specifically, with the Handbook of Polymer Analysis (edited by the Symposium on Polymer Analysis of the Japanese Society of Analytical Chemistry, date of publication: January 1995, publisher: Kinokuniya Shoten, page number: 615~616, "II.2.3 2.3. The method described in 4 Propylene/Ethylene Copolymer") is a quantitative method obtained from the relationship between the value after correcting the absorbance of ethylene with a specific coefficient and the thickness of the film-shaped test piece.

乙烯-丙烯無規共聚物(A)之重量平均分子量(Mw)為20萬以上30萬以下,較佳為24萬以上28萬以下。重量平均分子量(Mw)在此範圍內之共聚物(A),可在低蒸汽壓下進行模內成形。所得發泡體之強度優異,於成形性與機械強度之均衡優異。The weight average molecular weight (Mw) of the ethylene-propylene random copolymer (A) is not less than 200,000 and not more than 300,000, preferably not less than 240,000 and not more than 280,000. The copolymer (A) having a weight average molecular weight (Mw) within this range can be molded in a mold under low vapor pressure. The resulting foam has excellent strength and a good balance between formability and mechanical strength.

此外,乙烯-丙烯無規共聚物(A)之重量平均分子量(Mw)相對於乙烯-丙烯無規共聚物(A)之數平均分子量(Mn)之比(Mw/Mn)為3.5以上5以下。 該比(Mw/Mn)若在此範圍內,則即使縮短水冷時間,所得成形體之尺寸變化偏差亦小。其理由認為是在利用水冷之冷卻早期階段容易引起樹脂之結晶化,即使縮短利用水冷的冷卻時間,亦難以引起尺寸變化。進而,可抑制二次發泡之偏差,抑制局部二次發泡過度進展、抑制蒸汽難以均等地行進至模具內,其結果,認為可將成形後之發泡粒子成形體之尺寸變化偏差抑制為較小。基於此點,比(Mw/Mn)較佳為3.7以上4.8以下,更佳為3.8以上4.5以下。 In addition, the ratio (Mw/Mn) of the weight average molecular weight (Mw) of the ethylene-propylene random copolymer (A) to the number average molecular weight (Mn) of the ethylene-propylene random copolymer (A) is 3.5 or more and 5 or less . If the ratio (Mw/Mn) is within this range, even if the water cooling time is shortened, the resulting molded body will have little variation in dimensional change. The reason for this is that the crystallization of the resin is likely to occur in the early stage of cooling by water cooling, and the dimensional change is difficult to occur even if the cooling time by water cooling is shortened. Furthermore, it is possible to suppress the deviation of the secondary foaming, suppress the excessive progress of the local secondary foaming, and suppress the difficulty in uniformly advancing the steam into the mold. smaller. From this point of view, the ratio (Mw/Mn) is preferably from 3.7 to 4.8, more preferably from 3.8 to 4.5.

且,乙烯-丙烯無規共聚物(A)之Z平均分子量(Mz)較佳為50萬以上100萬以下,更佳為60萬以上90萬以下,又更佳為65萬以上75萬以下。 又,Z平均分子量(Mz)相對於數平均分子量(Mn)之比(Mz/Mn)較佳為為9.5以上且未達13,更佳為10以上12以下。 比(Mz/Mn)若為此範圍內,則即使冷卻時間短,亦可使成形後之收縮所引起之成形體之每部分之尺寸變化偏差減小,可獲得發泡粒子成形體。 In addition, the Z average molecular weight (Mz) of the ethylene-propylene random copolymer (A) is preferably from 500,000 to 1 million, more preferably from 600,000 to 900,000, still more preferably from 650,000 to 750,000. Also, the ratio (Mz/Mn) of the Z average molecular weight (Mz) to the number average molecular weight (Mn) is preferably 9.5 or more and less than 13, more preferably 10 or more and 12 or less. If the ratio (Mz/Mn) is within this range, even if the cooling time is short, the variation in size of each part of the molded body due to shrinkage after molding can be reduced, and an expanded particle molded body can be obtained.

又,Z平均分子量(Mz)相對於重量平均分子量(Mw)之比(Mz/Mw)較佳為2以上5以下,更佳為2.5以上3.5以下,又更佳為2.6以上3.2以下。Also, the ratio (Mz/Mw) of the Z average molecular weight (Mz) to the weight average molecular weight (Mw) is preferably from 2 to 5, more preferably from 2.5 to 3.5, still more preferably from 2.6 to 3.2.

本發明所用之乙烯-丙烯無規共聚物(A)可藉由例如使比(Mw/Mn)為3.5以上5以下般之乙烯-丙烯無規共聚物以過氧化物等有機過氧化物氧化分解,藉由控制分子量而獲得。The ethylene-propylene random copolymer (A) used in the present invention can be oxidatively decomposed by using an organic peroxide such as a peroxide, for example, by making the ratio (Mw/Mn) of the ethylene-propylene random copolymer 3.5 to 5 , obtained by controlling the molecular weight.

本說明書中,數平均分子量(Mn)、重量平均分子量(Mw)、Z平均分子量(Mz)可藉由凝膠滲透層析法測定。 測定方法之細節於實施例中說明。 In this specification, number average molecular weight (Mn), weight average molecular weight (Mw), and Z average molecular weight (Mz) can be measured by gel permeation chromatography. The details of the assay method are described in the Examples.

乙烯-丙烯無規共聚物(A)之熔點(Tm)較佳為130℃以上150℃以下,更佳為135℃以上145℃以下。 該熔點(Tm)若在此範圍內,則多層發泡粒子可以低的蒸汽壓下成形。另一方面,所得成形體之耐熱性優異。 The melting point (Tm) of the ethylene-propylene random copolymer (A) is preferably from 130°C to 150°C, more preferably from 135°C to 145°C. If the melting point (Tm) is within this range, multilayer expanded particles can be molded under low steam pressure. On the other hand, the obtained molded body is excellent in heat resistance.

本發明所用之乙烯-丙烯無規共聚物(A)中,結晶化溫度(Tc)與熔點(Tm)較佳滿足下述(1)式。

Figure 02_image003
(但,式中之Tm、Tc之單位均為℃)。 In the ethylene-propylene random copolymer (A) used in the present invention, the crystallization temperature (Tc) and melting point (Tm) preferably satisfy the following formula (1).
Figure 02_image003
(However, the units of Tm and Tc in the formula are both °C).

若由結晶化溫度(Tc)與熔點(Tm)滿足(1)式之乙烯-丙烯無規共聚物(A)形成發泡芯層時,即使使用低壓蒸汽進行模內成形,亦可獲得良好發泡粒子成形體。此認為係因為在模內成形時之冷卻步驟中,滿足(1)式之乙烯-丙烯無規共聚物(A)有早期引起結晶化之傾向,即使縮短成形時之冷卻時間,亦難以引起尺寸變化。If the foam core layer is formed from the ethylene-propylene random copolymer (A) whose crystallization temperature (Tc) and melting point (Tm) satisfy the formula (1), good foaming can be obtained even if low-pressure steam is used for in-mold forming. Bubble particle shaped body. This is considered to be because the ethylene-propylene random copolymer (A) satisfying the formula (1) tends to cause crystallization early in the cooling step during in-mold molding, and it is difficult to cause dimensional changes even if the cooling time during molding is shortened. Variety.

由於上述理由,結晶化溫度(Tc)與熔點(Tm)較佳滿足下述(2)式,更佳滿足下述(3)式。

Figure 02_image005
For the above reasons, the crystallization temperature (Tc) and the melting point (Tm) preferably satisfy the following formula (2), more preferably satisfy the following formula (3).
Figure 02_image005

本說明書中,共聚物(A)之熔點意指基於JIS K7121-1987,藉由熱通量示差掃描熱量測定求出之DSC曲線之最大熔解波峰溫度。作為試驗片之狀態調節,採用「(2)進行一定熱處理後,測定熔解溫度之情況」,作為此時之冷卻速度採用每分鐘10℃。作為測定熔解溫度時之加熱速度採用每分鐘10℃。又,熔解波峰出現2個以上時,面積最大的熔解波峰的頂點溫度設為熔點。 關於發泡粒子及多層發泡粒子,可藉與上述相同之方法測定熔點(Tmf)。 又,於熔解波峰不清楚時,可參考熔點溫度附近之DSC的微分曲線(DDSC)之正負、零點,求出波峰位置。 In the present specification, the melting point of the copolymer (A) means the maximum melting peak temperature of the DSC curve obtained by heat flux differential scanning calorimetry based on JIS K7121-1987. As the state adjustment of the test piece, "(2) The case of measuring the melting temperature after a certain heat treatment" was adopted, and the cooling rate at this time was 10°C per minute. As the heating rate when measuring the melting temperature, 10°C per minute was adopted. Also, when two or more melting peaks appear, the apex temperature of the melting peak with the largest area is defined as the melting point. Regarding expanded particles and multilayered expanded particles, the melting point (Tmf) can be measured by the same method as above. Also, when the melting peak is not clear, the position of the peak can be obtained by referring to the positive, negative, and zero points of the DSC differential curve (DDSC) near the melting point.

本說明書中,結晶化溫度(Tc)意指基於JIS K7121-1987,藉由熱通量示差掃描熱量測定求出之結晶化波峰溫度。作為試驗片之狀態調節,採用「(2)進行一定熱處理後,測定熔解溫度之情況」,作為冷卻速度採用每分鐘10℃。又,共聚物(A)之結晶化發熱波峰出現2個以上時,面積最大之結晶化波峰之頂點溫度設為結晶化溫度。 關於發泡粒子及多層發泡粒子,可藉同樣方法測定結晶化溫度(Tcf)。 In this specification, the crystallization temperature (Tc) means the crystallization peak temperature obtained by heat flux differential scanning calorimetry based on JIS K7121-1987. As the state adjustment of the test piece, "(2) After performing a certain heat treatment, the case of measuring the melting temperature" was adopted, and 10°C per minute was adopted as the cooling rate. Also, when two or more crystallization exothermic peaks of the copolymer (A) appear, the peak temperature of the crystallization peak with the largest area is defined as the crystallization temperature. Regarding expanded particles and multilayer expanded particles, the crystallization temperature (Tcf) can be measured by the same method.

乙烯-丙烯無規共聚物(A)之撓曲彈性模數較佳為750MPa以上,較佳為800MPa以上1100MPa以下,更佳為820MPa以上1000MPa以下。該撓曲彈性模數若在此範圍內,則特別可獲得具有良好剛性之發泡粒子成形體。The flexural modulus of the ethylene-propylene random copolymer (A) is preferably at least 750 MPa, more preferably at least 800 MPa and at most 1100 MPa, more preferably at least 820 MPa and at most 1000 MPa. If the flexural elastic modulus is within this range, a molded expanded particle having particularly good rigidity can be obtained.

本說明書中,該撓曲彈性模數可依據JIS K7171:2008求出。In this specification, this flexural modulus can be calculated|required based on JISK7171:2008.

乙烯-丙烯無規共聚物(A)之熔體流動速率(MFR)較佳為1g/10分鐘以上20g/10分鐘以下,更佳為2g/10分鐘以上15g/10分鐘以下,又更佳為3g/10分鐘以上10g/10分鐘以下。該MFR若在此範圍內,則容易形成具有多層構造之發泡粒子,特別是成為獲得發泡粒子時之前驅物之多層構造的樹脂粒子。 又,乙烯-丙烯無規共聚物(A)之MFR係以JIS K7210:1999之試驗條件M(230℃/2.16kg荷重)測定之值。 The melt flow rate (MFR) of the ethylene-propylene random copolymer (A) is preferably not less than 1 g/10 minutes and not more than 20 g/10 minutes, more preferably not less than 2 g/10 minutes and not more than 15 g/10 minutes, and more preferably More than 3g/10 minutes and less than 10g/10 minutes. If the MFR is within this range, it is easy to form expanded particles having a multilayer structure, especially resin particles having a multilayer structure of a precursor when obtaining expanded particles. In addition, the MFR of the ethylene-propylene random copolymer (A) is a value measured by the test condition M (230 degreeC/2.16 kg load) of JISK7210:1999.

本發明中構成發泡芯層之乙烯-丙烯無規共聚物(A)中,亦可添加共聚物(A)以外之熱塑性樹脂、熱塑性彈性體等之聚合物成分。但,構成發泡芯層之樹脂,較佳含有80重量%以上之乙烯-丙烯無規共聚物(A),更佳含有90重量%以上。In the ethylene-propylene random copolymer (A) constituting the foam core layer in the present invention, polymer components such as thermoplastic resins and thermoplastic elastomers other than the copolymer (A) may be added. However, the resin constituting the foam core layer preferably contains 80% by weight or more of the ethylene-propylene random copolymer (A), more preferably 90% by weight or more.

且,發泡芯層中,可添加抗靜電劑、觸媒中和劑、滑劑、核劑、碳黑等之著色劑等之添加劑。添加劑之添加量取決於添加劑種類及用途,但相對於構成發泡芯層之共聚物(A)100重量份,較佳為15重量份以下,更佳為10重量份以下,又更佳為5重量份以下,特佳為3重量份以下。In addition, additives such as antistatic agents, catalyst neutralizing agents, slip agents, nucleating agents, and coloring agents such as carbon black may be added to the foam core layer. The amount of the additive depends on the type and use of the additive, but relative to 100 parts by weight of the copolymer (A) constituting the foam core layer, it is preferably 15 parts by weight or less, more preferably 10 parts by weight or less, and more preferably 5 parts by weight. It is not more than 3 parts by weight, particularly preferably not more than 3 parts by weight.

本發明之多層發泡粒子,如前述,具有發泡芯層與被覆層,發泡芯層經被覆層覆蓋。 該被覆層係由聚烯烴系樹脂(B)構成,藉由示差掃描熱量測定法(DSC)測定之該聚烯烴系樹脂(B)的DSC曲線具有一個以上之熔融波峰,其內之至少一個熔融波峰的熔融波峰溫度必須低於該乙烯-丙烯無規共聚物(A)之熔點(Tm)。藉由使被覆層滿足該構成,改善了發泡粒子之熔著性,可在比僅由發泡芯層所成之單層發泡粒子的成形溫度低的成形溫度下進行模內成形。 The multi-layer expanded particle of the present invention, as mentioned above, has a foam core layer and a coating layer, and the foam core layer is covered by the coating layer. The coating layer is made of polyolefin resin (B), and the DSC curve of the polyolefin resin (B) measured by differential scanning calorimetry (DSC) has more than one melting peak, and at least one of them melts The melting peak temperature of the crest must be lower than the melting point (Tm) of the ethylene-propylene random copolymer (A). By making the coating layer satisfy this constitution, the fusion property of the expanded bead is improved, and in-mold molding can be performed at a molding temperature lower than that of a single-layer expanded bead formed of only the foamed core layer.

此處,所謂「乙烯-丙烯無規共聚物(A)之熔點」係指藉由示差掃描熱量測定法(DSC)測定之乙烯-丙烯無規共聚物(A)的DSC曲線中出現2個以上熔解波峰時,面積最大的熔解波峰頂點的溫度(以下亦稱最大熔解波峰溫度)。 又,所謂「該聚烯烴系樹脂(B)之DSC曲線具有一個以上的熔解波峰,其內之至少一個熔解波峰之熔解波峰溫度低於該乙烯-丙烯無規共聚物(A)之熔點」係指於聚烯烴系樹脂(B)的DSC曲線中出現一個熔解波峰之情況,該熔解波峰的熔解波峰溫度低於乙烯-丙烯無規共聚物(A)之前述最大熔解波峰溫度。 又,於聚烯烴系樹脂(B)之DSC曲線中出現複數熔解波峰之情況,至少聚烯烴系樹脂(B)的DSC曲線之最低溫側的熔解波峰的熔解波峰溫度低於乙烯-丙烯無規共聚物(A)之最大熔解波峰溫度。 Here, the "melting point of the ethylene-propylene random copolymer (A)" means that two or more melting points appear in the DSC curve of the ethylene-propylene random copolymer (A) measured by differential scanning calorimetry (DSC). When melting the peak, the temperature at the top of the melting peak with the largest area (hereinafter also referred to as the maximum melting peak temperature). Also, the so-called "the DSC curve of the polyolefin resin (B) has more than one melting peak, and the melting peak temperature of at least one of the melting peaks is lower than the melting point of the ethylene-propylene random copolymer (A)" means Refers to the case where a melting peak appears in the DSC curve of the polyolefin resin (B), and the melting peak temperature of the melting peak is lower than the aforementioned maximum melting peak temperature of the ethylene-propylene random copolymer (A). Also, when multiple melting peaks appear on the DSC curve of the polyolefin resin (B), at least the melting peak temperature of the melting peak on the lowest temperature side of the DSC curve of the polyolefin resin (B) is lower than that of the ethylene-propylene random The maximum melting peak temperature of the copolymer (A).

本發明中,關於聚烯烴系樹脂(B)之熔解波峰溫度及乙烯-丙烯無規共聚物(A)之最大熔解波峰溫度滿足前述關係,進而,使構成發泡芯層之樹脂的分子量為特定範圍內,藉此可提高被覆層之熔著性,且於發泡芯層藉由控制二次發泡性與水冷時之結晶性,可獲得即使縮短水冷時間亦難以發生尺寸變化之偏差的發泡粒子。In the present invention, the melting peak temperature of the polyolefin resin (B) and the maximum melting peak temperature of the ethylene-propylene random copolymer (A) satisfy the aforementioned relationship, and furthermore, the molecular weight of the resin constituting the foam core layer is specified. In this range, the fusion of the coating layer can be improved, and by controlling the secondary foamability and crystallinity during water cooling of the foam core layer, even if the water cooling time is shortened, the deviation of the dimensional change can hardly occur. Bubble particles.

又,所謂「可在比僅由發泡芯層構成之單層發泡粒子的成形溫度低的成形溫度下進行模內成形」係指以由乙烯-丙烯無規共聚物(A)構成之單層構造之發泡粒子的模內成形溫度為基準,具有與由該單層構造之發泡粒子形成之成型體同樣特性(例如,表面外觀、熔著性、恢復性)之成形體,可在比該基準之模內成形溫度低的成形溫度下成形。Also, the term "can be in-mold molded at a molding temperature lower than the molding temperature of a single-layer expanded bead composed of only a foamed core layer" refers to a monolayer composed of an ethylene-propylene random copolymer (A). Based on the in-mold molding temperature of expanded particles with a layer structure, a molded product having the same characteristics (such as surface appearance, fusion property, and recovery) as a molded product formed of expanded particles with a single-layer structure can be produced in Molded at a molding temperature lower than the standard in-mold molding temperature.

其次,針對本發明中,構成被覆層之聚烯烴系樹脂(B)加以說明。 作為該聚烯烴系樹脂(B),較佳具有50質量%以上之烯烴成分,更佳為70質量%以上,更佳為90質量%以上。只要烯烴成分具有50質量%以上,則其組成、合成法未特別限制。具體而言,作為該聚烯烴系樹脂,舉例為例如聚丙烯系樹脂、聚乙烯系樹脂等,進而舉例該等之混合物等。 Next, in the present invention, the polyolefin-based resin (B) constituting the covering layer will be described. The polyolefin-based resin (B) preferably has an olefin component of 50 mass % or more, more preferably 70 mass % or more, more preferably 90 mass % or more. The composition and synthesis method are not particularly limited as long as the olefin component has 50% by mass or more. Specifically, examples of the polyolefin-based resin include polypropylene-based resins, polyethylene-based resins, and the like, and further, mixtures thereof, and the like.

作為該聚丙烯系樹脂,舉例為丙烯均聚物或丙烯與可共聚合之其他烯烴的共聚物等。作為可與丙烯共聚合之其他烯烴,可例示例如乙烯、及1-丁烯等之碳數4以上之α-烯烴。作為該共聚物,可例示例如丙烯-乙烯無規共聚物、丙烯-乙烯嵌段共聚物、丙烯-乙烯-丁烯無規共聚物等,進而例示該等之2種以上的混合樹脂等。Examples of the polypropylene-based resin include propylene homopolymers, copolymers of propylene and other copolymerizable olefins, and the like. Examples of other olefins that can be copolymerized with propylene include α-olefins having 4 or more carbon atoms, such as ethylene and 1-butene. As this copolymer, a propylene-ethylene random copolymer, a propylene-ethylene block copolymer, a propylene-ethylene-butene random copolymer, etc. are mentioned, for example, and the mixed resin etc. of 2 or more types of these are further exemplified.

作為該聚乙烯系樹脂,舉例為例如高密度聚乙烯、中密度聚乙烯、低密度聚乙烯、直鏈狀低密度聚乙烯、超低密度聚乙烯、乙烯-乙酸乙烯酯共聚物等,進而例示該等之2種以上之混合樹脂等。As the polyethylene-based resin, for example, high-density polyethylene, medium-density polyethylene, low-density polyethylene, linear low-density polyethylene, ultra-low-density polyethylene, ethylene-vinyl acetate copolymer, etc., further exemplified Mixed resins of two or more of these, etc.

又,本發明之被覆層,在不阻礙所需目的之範圍內,可添加聚烯烴系樹脂(B)以外之熱塑性樹脂、熱塑性彈性體等聚合物。但,其添加量相對於聚烯烴系樹脂(B)100質量份,較佳為5質量份以下。Furthermore, the coating layer of the present invention may contain polymers such as thermoplastic resins and thermoplastic elastomers other than the polyolefin-based resin (B) within the range that does not hinder the intended purpose. However, the amount added is preferably 5 parts by mass or less with respect to 100 parts by mass of the polyolefin resin (B).

被覆層中可添加抗靜電劑、觸媒中和劑、滑劑、碳黑等之著色劑等添加劑。該添加劑之添加量取決於添加既之種類及使用目的,但相對於形成被覆層之聚烯烴系樹脂(B)100重量份,較佳為15重量份以下,更佳為10重量份以下,又更佳為5重量份以下,特佳為3重量份以下。Additives such as antistatic agent, catalyst neutralizer, slip agent, colorant such as carbon black can be added to the coating layer. The amount of this additive added depends on the type of addition and the purpose of use, but relative to 100 parts by weight of the polyolefin resin (B) forming the coating layer, it is preferably 15 parts by weight or less, more preferably 10 parts by weight or less, and It is more preferably at most 5 parts by weight, particularly preferably at most 3 parts by weight.

其次,針對本發明之多層發泡粒子之物性加以說明。 該多層發泡粒子之體密度較佳為10kg/m 3以上300kg/m 3以下。 該體密度為此範圍內時,由本發明所特定出之冷卻時間的縮短效果將更顯著。亦即,先前技術中,該範圍內之體密度的多層發泡粒子由於發泡倍率比較高,故模內成形後之尺寸變化容易變大,有冷卻時間變長之傾向。相對於此,本發明之多層發泡粒子,冷卻時間的縮短效果更明顯。 又,若使用體密度在此範圍內之多層發泡粒子,則可獲得可使用於汽車內裝構件、汽車保險桿用芯材及汽車座椅用芯材為代表之各種用途的發泡粒子成形體。因該等理由,多層發泡粒子之體密度更佳為15kg/m 3以上200kg/m 3以下,又更佳為17kg/m 3以上100kg/m 3以下,再更佳為19kg/m 3以上50kg/m 3以下。 Next, the physical properties of the multilayer expanded particles of the present invention will be described. The bulk density of the multilayer expanded particles is preferably not less than 10 kg/m 3 and not more than 300 kg/m 3 . When the bulk density is within this range, the effect of shortening the cooling time specified by the present invention will be more remarkable. That is, in the prior art, multilayer expanded particles with a bulk density within this range tend to have large dimensional changes after in-mold molding due to a relatively high expansion ratio, and the cooling time tends to be prolonged. In contrast, the effect of shortening the cooling time is more obvious for the multi-layer expanded particles of the present invention. In addition, if the multi-layer expanded particles with a bulk density within this range are used, it is possible to obtain expanded particle moldings that can be used in various applications represented by automotive interior components, core materials for car bumpers, and core materials for car seats. body. For these reasons, the bulk density of the multilayer expanded particles is more preferably 15kg/ m3 to 200kg/ m3 , more preferably 17kg/ m3 to 100kg/ m3 , and more preferably 19kg/ m3 or more Below 50kg/ m3 .

多層發泡粒子之體密度之測定方法如下。首先,準備體積1L之量筒。邊去除多層發泡粒子之靜電,邊將多層發泡粒子以自然堆積狀態之方式填充至量筒的1L標線。藉由將該量筒內之多層發泡粒子的質量、即每1L體積之多層發泡粒子的質量換算為每1m 3體積的質量(kg/m 3),可測定多層發泡粒子之體密度(kg/m 3)。 The method for measuring the bulk density of multilayer expanded particles is as follows. First, prepare a graduated cylinder with a volume of 1 L. While removing the static electricity of the multi-layer expanded particles, fill the multi-layer expanded particles to the 1L marking line of the measuring cylinder in a natural accumulation state. By converting the mass of the multilayered expanded particles in the measuring cylinder, that is, the mass of the multilayered expanded particles per 1 L volume, to the mass per 1 m3 volume (kg/ m3 ), the bulk density of the multilayered expanded particles ( kg/m 3 ).

構成該多層發泡粒子之發泡芯層的平均氣泡徑較佳為20μm以上400μm以下,更佳為40μm以上250μm以下,又更佳為80μm以上200μm以下,特佳為100μm以上160μm以下。該平均氣泡徑在此範圍內時,成為模內成形性優異之多層發泡粒子,同時所得之發泡粒子成形體之成形後之尺寸恢復性優異。The average cell diameter of the foam core layer constituting the multilayer expanded particles is preferably from 20 μm to 400 μm, more preferably from 40 μm to 250 μm, still more preferably from 80 μm to 200 μm, particularly preferably from 100 μm to 160 μm. When the average cell diameter is within this range, multilayer expanded particles having excellent in-mold formability are obtained, and the obtained expanded particle molded product is excellent in dimensional recovery after molding.

前述發泡芯層之平均氣泡徑測定如下。 基於以顯微鏡拍攝將發泡芯層大致二等份之切斷面所得之放大照片,如下求出。首先,於發泡芯層之切斷面放大照片中,自發泡芯層之一表面遍及另一表面,畫出4條通過氣泡切斷面之大致中心的線段。但該線段係以形成自氣泡切斷面之大致中心朝切斷粒子表面沿等間隔的8個方向延伸之放射狀直線之方式畫出。其次,求出與該4條線段交叉之氣泡數總數N(個)。求出4條各線段長度的總和L(μm),將總和L除以總和N所得之值(L/N)設為發泡芯層1個的氣泡徑。針對10個發泡芯層進行此操作,將各氣泡徑相加並平均之值設為發泡芯層之平均氣泡徑。 The average cell diameter of the aforementioned foamed core layer was measured as follows. It is determined as follows based on an enlarged photograph obtained by taking a cut section of the foam core layer in approximately two equal parts with a microscope. First, in the enlarged photograph of the cut section of the foam core layer, from one surface of the foam core layer to the other surface, draw four line segments passing through the approximate center of the cut section of the foam. However, the line segment is drawn to form radial straight lines extending from the approximate center of the cut surface of the bubble toward the surface of the cut particle in eight directions at equal intervals. Next, the total number N (pieces) of the number of bubbles intersecting the four line segments is obtained. The sum L (μm) of the lengths of the four line segments was obtained, and the value (L/N) obtained by dividing the sum L by the sum N was defined as the cell diameter of one foam core layer. This operation was carried out for 10 foam core layers, and the value obtained by summing and averaging the respective cell diameters was set as the average cell diameter of the foam core layer.

本發明之多層發泡粒子中,獨立氣泡率較佳為75%以上,更佳為80%以上,又更佳為82%以上,特佳為85%以上。獨立氣泡率若在此範圍內,則成為二次發泡性優異之多層發泡粒子,並且所得發泡粒子成形體之機械物性良好。In the multilayer expanded particles of the present invention, the independent cell ratio is preferably at least 75%, more preferably at least 80%, even more preferably at least 82%, and most preferably at least 85%. If the closed cell ratio is within this range, multilayer expanded particles with excellent secondary expansion properties will be obtained, and the obtained expanded particle molded product will have good mechanical properties.

多層發泡粒子之獨立氣泡率測定如下。 將多層發泡粒子在大氣壓下、相對濕度50%、23℃之條件的恆溫室內放置10天進行養生。其次於恆溫室內,將鬆體積約20cm 3之養生後之多層發泡粒子作為測定樣品,藉由如下之通水淹沒法測定正確的表觀體積Va。測定表觀體積Va後之測定用樣品經充分乾燥後,依據ASTM-D2856-70中記載之順序C,藉由東芝貝克曼股份有限公司製空氣比較式比重計930測定經測定之測定用樣品之真體積Vx。然後,基於該等體積Va及Vx,藉由下述式(4)計算獨立氣泡率,將N=5之平均值設為多層發泡粒子之獨立氣泡率。 The independent cell ratio of the multilayer expanded particles was measured as follows. The multi-layer expanded particles are placed in a constant temperature room under the conditions of atmospheric pressure, relative humidity 50%, and 23°C for 10 days for health preservation. Next, in the constant temperature room, the multi-layer expanded particles with a loose volume of about 20 cm 3 after curing are used as a measurement sample, and the correct apparent volume Va is measured by the following water submersion method. After the apparent volume Va was measured, the sample for measurement was sufficiently dried, and according to the procedure C described in ASTM-D2856-70, the volume of the measured sample was measured with an air comparison type pycnometer 930 manufactured by Toshiba Beckman Co., Ltd. True volume Vx. Then, based on these equal volumes Va and Vx, the closed cell rate was calculated by the following formula (4), and the average value of N=5 was set as the closed cell rate of the multilayer expanded particles.

Figure 02_image007
但, Vx:以前述方法測定之多層發泡粒子之真體積,即,構成多層發泡粒子樹脂之容積與多層發泡粒子內之獨立氣泡部分之氣泡總容積之和(cm 3) Va:將多層發泡粒子沉入裝入水的量筒中,基於水位上升量測定之多層發泡粒子之表觀體積(cm 3) W:多層發泡粒子測定用樣品之重量(g) ρ:構成多層發泡粒子之樹脂密度(g/cm 3)
Figure 02_image007
However, Vx: the true volume of the multilayer expanded bead measured by the above-mentioned method, that is, the sum of the volume of the resin constituting the multilayer expanded bead and the total volume of the independent cells in the multilayer expanded bead (cm 3 ) Va: the volume of the multilayer expanded bead The apparent volume (cm 3 ) of the multilayered foamed particles measured based on the rise of the water level when the multilayered foamed particles sink into a graduated cylinder filled with water. Resin density of foam particles (g/cm 3 )

本發明中,多層發泡粒子之藉由熱通量示差掃描熱量測定法之升溫測定所得之第一次加熱的DSC曲線中,較佳出現聚丙烯系樹脂之固有吸熱波峰(以下,亦稱為「固有波峰」)與起因於發泡時之溫度處理而形成之二次結晶之高溫波峰。In the present invention, in the DSC curve of the first heating measured by the heat flux differential scanning calorimetry of the multilayer expanded particles, the inherent heat absorption peak of the polypropylene resin preferably appears (hereinafter also referred to as "Intrinsic peak") and the high-temperature peak of the secondary crystal formed by the temperature treatment during foaming.

具體而言,多層發泡粒子2mg以上10mg以下藉由熱通量示差掃描熱量測定法,以10℃/分鐘之升溫速度自23℃加熱到220℃時所得之DSC曲線(第1次加熱之DSC曲線),如圖1所示,較佳具有聚丙烯系樹脂之固有吸熱波峰a(以下,亦簡稱為「固有波峰」)與在該固有波峰之高溫側,源自因發泡時之溫度處理所形成之二次結晶的1個以上吸熱波峰b(以下亦簡稱為「高溫波峰」)。Specifically, the DSC curve obtained when the multilayer expanded particles are heated from 23°C to 220°C at a heating rate of 10°C/min by means of heat flux differential scanning calorimetry (DSC of the first heating) of 2 mg to 10 mg Curve), as shown in Figure 1, it is preferable to have the inherent endothermic peak a (hereinafter, also referred to as "intrinsic peak") of polypropylene resin and the high temperature side of the inherent peak, which is derived from the temperature treatment during foaming One or more endothermic peaks b of the formed secondary crystals (hereinafter also simply referred to as "high temperature peaks").

圖1係第1次加熱之DSC曲線的一例。圖1中,分別係a表示固有波峰,b表示高溫波峰,α表示相當於DSC曲線上80°C之點,T E表示熔解結束溫度,吸熱波峰b之高溫側拖尾表示回到基準線之位置時的溫度,β表示相當於高溫波峰之熔解結束溫度TE的DSC曲線上的點,γ係固有波峰a與高溫波峰b之間的谷底的點,δ係自點γ畫出與圖形之縱軸平行的直線,與直線(α-β)交叉之點。 Fig. 1 is an example of the DSC curve of the first heating. In Figure 1, a represents the inherent peak, b represents the high temperature peak, α represents the point corresponding to 80°C on the DSC curve, TE represents the end temperature of melting, and the high temperature tail of the endothermic peak b represents the return to the baseline β is the point on the DSC curve corresponding to the melting end temperature TE of the high-temperature peak, γ is the point at the bottom of the valley between the inherent peak a and the high-temperature peak b, and δ is the vertical line drawn from the point γ to the graph The point where a straight line parallel to the axis intersects with the straight line (α-β).

固有波峰之頂點溫度(固有波峰溫度)較佳為135℃以上145℃以下,更佳為138℃以上142℃以下。固有波峰溫度若在此範圍內,則藉由成形後之冷卻容易形成有助於剛性提高之結晶性高的結晶。 固有波峰之熔解結束溫度(γ)係對應於固有波峰a與高溫波峰b之間的谷底之溫度,較佳為150℃以上160℃以下,更佳為152℃以上155℃以下。 The peak temperature of the intrinsic peak (intrinsic peak temperature) is preferably from 135°C to 145°C, more preferably from 138°C to 142°C. If the intrinsic peak temperature is within this range, highly crystalline crystals which contribute to an increase in rigidity can be easily formed by cooling after molding. The melting end temperature (γ) of the intrinsic peak corresponds to the temperature at the bottom of the valley between the intrinsic peak a and the high temperature peak b, preferably between 150°C and 160°C, more preferably between 152°C and 155°C.

固有波峰之熔解熱量較佳為50J/g以上70J/g以下,更佳為55J/g以上65J/g。藉由使固有波峰之熔解熱量為此範圍內,提高了成形後之尺寸穩定性。The heat of fusion of the inherent peak is preferably from 50 J/g to 70 J/g, more preferably from 55 J/g to 65 J/g. By keeping the heat of fusion of the inherent peak within this range, the dimensional stability after molding is improved.

固有波峰之熔解熱量,係以前述圖1中,由連接點δ與點γ之直線(δ-γ)、直線(α-β)及固有波峰a之曲線所包圍之部分的面積而求出。The heat of fusion of the intrinsic peak is obtained from the area of the part surrounded by the straight line (δ-γ) connecting the point δ and the point γ, the straight line (α-β) and the curve of the intrinsic peak a in the aforementioned Figure 1.

高溫波峰之熔解熱量(以下亦簡稱高溫波峰熱量)較佳為10J/g以上20J/g以下,更佳為12J/g以上16J/g以下。 藉由使高溫波峰熱量為此範圍內,可獲得成形後難以發生尺寸變化、機械強度優異之發泡粒子成形體。 又,發泡芯層之高溫波峰可藉周知之方法調節,具體而言,該調整方法揭示於例如日本特開2001-151928號公報中。 The heat of fusion of the high-temperature peak (hereinafter also referred to as the high-temperature peak heat) is preferably 10 J/g to 20 J/g, more preferably 12 J/g to 16 J/g. By setting the high-temperature wave peak heat amount within this range, it is possible to obtain a molded expanded particle body that hardly undergoes dimensional changes after molding and has excellent mechanical strength. In addition, the high temperature wave peak of the foam core layer can be adjusted by a known method, specifically, the adjustment method is disclosed in, for example, Japanese Patent Application Laid-Open No. 2001-151928.

又,高溫波峰b雖於如前述測定之第1次加熱時之DSC曲線中被觀察到,但於第2次升溫所得之DSC曲線中則未觀察到。第2次加熱時之DSC曲線中,只觀察到構成發泡核心層之丙烯系樹脂固有之吸熱波峰。Also, although the high-temperature peak b was observed in the DSC curve at the first heating as measured above, it was not observed in the DSC curve obtained at the second heating. In the DSC curve at the time of the second heating, only an endothermic peak unique to the propylene-based resin constituting the foam core layer was observed.

高溫波峰之熔解熱量,係以圖1中,由直線(δ-γ)、直線(α-β)與高溫波峰b之曲線所包圍的部分的面積而求出。The heat of fusion of the high temperature peak is obtained from the area of the part surrounded by the curve of the straight line (δ-γ), straight line (α-β) and high temperature peak b in Figure 1.

總熔解波峰熱量較佳為50J/g以上90J/g以下,更佳為55J/g以上80J/g以下。總熔解波峰熱量係高溫波峰的熔解熱量與固有波峰之熔解熱量之合計。總熔解波峰熱量係藉由將多層發泡粒子2mg以上10mg以下以熱通量示差掃描熱量測定法,自以10℃/分鐘之升溫速度自23℃加熱至220°C時所得之DSC曲線求出。The total melting peak heat is preferably from 50 J/g to 90 J/g, more preferably from 55 J/g to 80 J/g. The total heat of melting peak is the sum of the heat of fusion of the high temperature peak and the heat of fusion of the inherent peak. The total melting peak heat is calculated from the DSC curve obtained when the multi-layer expanded particles are heated from 23°C to 220°C at a heating rate of 10°C/min by heat flux differential scanning calorimetry of 2 mg to 10 mg. .

其次,針對本發明之多層發泡粒子藉由模內成形所得之多層發泡粒子成形體(以下亦簡發泡粒子成形體或成型體)加以說明。 該發泡粒子成形體之成形體密度較佳為10kg/m 3以上300kg/m 3以下,更佳為11kg/m 3以上200kg/m 3以下,更佳為12kg/m 3以上100kg/m 3以下,特佳為15kg/m 3以上50kg/m 3以下。特別是發泡粒子成形體之成形體密度低時,由於有成形時間變長之傾向,故較佳使用本發明之發泡粒子。 Next, the multilayer expanded bead molded product obtained by in-mold molding of the multilayer expanded bead of the present invention (hereinafter referred to simply as the expanded bead molded product or molded product) will be described. The density of the expanded particle molded body is preferably from 10 kg/m 3 to 300 kg/m 3 , more preferably from 11 kg/m 3 to 200 kg/m 3 , more preferably from 12 kg/m 3 to 100 kg/m 3 Below, preferably 15kg/ m3 or more and 50kg/ m3 or less. In particular, when the density of the molded expanded bead molded product is low, the molding time tends to be longer, so it is preferable to use the expanded bead of the present invention.

發泡粒子成形體之50%變形時壓縮應力較佳為100kPa以上500kPa以下,更佳為120kPa以上300kPa以下,又更佳為140kPa以上200kPa以下。發泡粒子成形體之50%變形壓縮應力可依據JIS K6767:1999進行測定。The compressive stress at 50% deformation of the expanded particle molded body is preferably from 100 kPa to 500 kPa, more preferably from 120 kPa to 300 kPa, and more preferably from 140 kPa to 200 kPa. The 50% deformation compressive stress of the expanded particle molded body can be measured according to JIS K6767:1999.

發泡粒子成形體之熔著率較佳為70%以上。該情況下,成型體可充分發揮與構成多層發泡粒子之樹脂相應之剛性等之期望機械特性。基於提高該機械特性之觀點,成形體之熔著率更佳為80%以上,又更佳為90%以上。 該熔著率之測定方法於實施例中說明。 The fusion rate of the expanded particle molded body is preferably 70% or more. In this case, the molded article can fully exhibit desired mechanical properties such as rigidity corresponding to the resin constituting the multilayer expanded bead. From the viewpoint of improving the mechanical properties, the fusion ratio of the molded body is more preferably at least 80%, and more preferably at least 90%. The method for measuring the fusion rate is described in the examples.

接著,針對本發明之多層發泡粒子之製造方法加以說明。 該多層發泡粒子可藉由使由前述聚烯烴系樹脂(B)所成之樹脂粒子被覆層被覆由前述乙烯-丙烯無規共聚物(A)所成之樹脂粒子芯層的多層樹脂粒子發泡而獲得。 Next, the manufacturing method of the multilayer expanded particle of this invention is demonstrated. The multilayer expanded particles can be formed by making the resin particle coating layer made of the aforementioned polyolefin resin (B) cover the resin particle core layer made of the aforementioned ethylene-propylene random copolymer (A). Obtained by soaking.

本發明中,多層樹脂粒子例如可如下製造。 使用將樹脂粒子芯層用擠出機與樹脂粒子被覆層用擠出機之兩台擠出機與共擠出模嘴連結之裝置,對樹脂粒子芯層用擠出機供給所需之乙烯-丙烯無規共聚物(A)與根據需要之氣泡調節劑等之添加劑並熔融混練,形成樹脂粒子芯層形成用之樹脂熔融物。另外,藉由對樹脂粒子被覆層用擠出機供給所需之聚烯烴系樹脂(B)與根據需要之添加劑並熔融混練,形成樹脂粒子被覆層形成用之樹脂熔融物。其次,將樹脂粒子芯層形成用之樹脂熔融物導入共擠出模嘴內,形成線狀流動,同時將樹脂粒子被覆層形成用之樹脂熔融物導入共擠出模嘴內,形成樹脂粒子被覆層形成用之樹脂熔融物以圍繞樹脂粒子芯層形成用之樹脂熔融物的線狀流動之方式予以積層而形成多層構造之樹脂熔融物。將該多層構造之樹脂熔融物自附設於擠出機出口的模嘴的小孔擠出成一條以上的股狀,將該股線通入水中冷卻後切斷成適當長度,或自模嘴擠出到水中之同時予以切斷、冷卻等之手段,可製造多層樹脂粒子。本說明書中,有時將如此形成之多層構造稱為「鞘芯」構造。 In the present invention, the multilayer resin particle can be produced as follows, for example. The extruder for the core layer of resin particles and the extruder for the coating layer of resin particles are connected to a co-extrusion die to supply the required ethylene- The propylene random copolymer (A) is melt-kneaded with additives such as a cell regulator as needed to form a resin melt for forming a resin particle core layer. In addition, the resin melt for forming the resin particle coating layer is formed by supplying the required polyolefin resin (B) and additives as necessary to the extruder for the resin particle coating layer and melt-kneading them. Next, introduce the resin melt for forming the resin particle core layer into the co-extrusion die to form a linear flow, and at the same time introduce the resin melt for the resin particle coating layer into the co-extrusion die to form the resin particle coating The resin melt for layer formation is laminated so that the resin melt for core layer formation surrounds the linear flow of the resin particle core layer to form a resin melt with a multilayer structure. Extrude the multi-layered resin melt from the small hole of the die attached to the exit of the extruder into more than one strand, put the strand into water and cool it, cut it into an appropriate length, or extrude it from the die Multi-layered resin particles can be produced by means of cutting, cooling, etc. while going out into the water. In this specification, the multilayer structure thus formed may be referred to as a "sheath-core" structure.

關於使用共擠出模嘴製造多層樹脂粒子之方法,詳情記載於例如日本特公昭41-16125號公報、日本特公昭43-23858號公報、日本特公昭44-29522號公報、日本特開昭60-185816號公報等。Regarding the method of producing multi-layered resin particles using a co-extrusion die, details are described in, for example, Japanese Patent Publication No. 41-16125, Japanese Patent Publication No. 43-23858, Japanese Patent Publication No. 44-29522, and Japanese Patent Application Laid-Open No. 60. - Bulletin No. 185816, etc.

樹脂粒子芯層形成用之樹脂熔融物中,為了調整發泡芯層之氣泡徑,較佳添加氣泡調節劑。作為該氣泡調節劑,舉例為滑石、碳酸鈣、硼砂、硼酸鋅、氫氧化鋁、明礬等之無機物。其添加量相對於形成樹脂粒子芯層之共聚物(A)100重量份,較佳為0.001重量份以上10重量份以下,更佳為0.01重量份以上5重量份以下。 又,將氣泡調節劑添加於共聚物(A)時,氣泡調節劑可直接調配,但通常較佳考慮分散性等作成氣泡調節劑之母料添加。 To the resin melt for forming the resin particle core layer, it is preferable to add a cell regulator in order to adjust the cell diameter of the foamed core layer. Examples of the cell regulator include inorganic substances such as talc, calcium carbonate, borax, zinc borate, aluminum hydroxide, and alum. The amount added is preferably from 0.001 to 10 parts by weight, more preferably from 0.01 to 5 parts by weight, based on 100 parts by weight of the copolymer (A) forming the resin particle core layer. In addition, when adding the bubble regulator to the copolymer (A), the bubble regulator can be directly formulated, but it is generally preferable to add it as a masterbatch of the bubble regulator in consideration of dispersibility and the like.

多層樹脂粒子之重量,積於可確保多層發泡粒子於模內之均勻填充性,較佳為0.02mg以上20mg以下,更佳為0.1mg以上6mg以下。The weight of the multi-layered resin particles is sufficient to ensure the uniform filling of the multi-layered foamed particles in the mold, preferably 0.02 mg to 20 mg, more preferably 0.1 mg to 6 mg.

本發明之多層發泡粒子,可使用前述多層樹脂粒子,藉由例如所謂分散介質釋放發泡方法等製造。 該分散介質釋放發泡法中,將多層樹脂粒子與物理發泡劑等一起於高壓釜等之密封容器內分散於水等之分散介質中,將分散介質加熱至樹脂粒子的軟化溫度以上之溫度,使發泡劑含浸於多層樹脂粒子內。接著,邊將密閉容器內之壓力保持於發泡劑之蒸氣壓以上的壓力,邊開啟密閉容器內之水面下的一端,使含有發泡劑之發泡性多層樹脂粒子與水等之分散介質一起從密閉容器內向比密閉容器內的壓力低的壓力的環境下,通常於大氣壓下放出而發泡,藉此獲得多層發泡粒子。且,亦可自密封容器取出含有物理發泡劑之發泡多層樹脂粒子,以蒸汽等加熱介質加熱並發泡。 另一方面,以前述擠出裝置製作多層樹脂粒子時,將發泡劑壓入樹脂粒子之芯層形成用擠出機中製作發泡性熔融樹脂組成物。接著,將該發泡性熔融樹脂組成物以樹脂粒子之被覆層形成用的熔融樹脂予以積層,製作鞘芯構造的熔融樹脂組成物。然後,藉由將鞘芯構造之熔融樹脂組成物自模嘴擠出並發泡,進而切割成粒子狀之方法,可獲得發泡粒子。 The multilayered expanded particles of the present invention can be produced by, for example, the so-called dispersion medium release foaming method using the aforementioned multilayered resin particles. In the dispersion medium release foaming method, the multilayer resin particles are dispersed in a dispersion medium such as water in a sealed container such as an autoclave together with a physical foaming agent, and the dispersion medium is heated to a temperature above the softening temperature of the resin particles. , so that the foaming agent is impregnated in the multi-layered resin particles. Next, while keeping the pressure in the airtight container at a pressure above the vapor pressure of the foaming agent, one end of the water surface in the airtight container is opened, and the dispersion medium of the expandable multilayered resin particles containing the foaming agent and water etc. Together, they are released from the closed container to a pressure environment lower than the pressure in the closed container, usually at atmospheric pressure, and foamed to obtain multilayer expanded particles. Furthermore, the foamed multi-layered resin particles containing the physical foaming agent can also be taken out from the airtight container, heated with a heating medium such as steam, and foamed. On the other hand, when producing multi-layered resin particles with the aforementioned extruder, the foaming agent is pressed into the extruder for forming the core layer of the resin particles to produce a foamable molten resin composition. Next, the expandable molten resin composition is laminated with the molten resin for forming the coating layer of the resin particles to produce a molten resin composition having a sheath-core structure. Then, the expanded particles can be obtained by extruding the molten resin composition of the sheath-core structure from the die, foaming, and cutting into particles.

分散介質釋放發泡法中,自不產生發泡之高壓下朝產生氣泡之低壓下釋出時之高壓下與低壓下之差壓較佳為500kPa以上15000kPa以下。In the dispersion medium release foaming method, the pressure difference between the high pressure and the low pressure when releasing from a high pressure without foaming to a low pressure with bubbles is preferably 500 kPa or more and 15000 kPa or less.

作為分散介質釋放發泡法中使用的發泡劑,通常可舉例為丙烷、異丁烷、正丁烷、異戊烷、正戊烷、環戊烷、正己烷、環丁烷、環己烷、氯氟甲烷、三氟甲烷、1,1,1,2-四氟乙烷、1-氯-1,1-二氟乙烷、1,1-二氟乙烷、1-氯-1,2,2,2-四氟乙烷、氫氟烯烴等之有機物理發泡劑,或氮氣、二氧化碳、氬氣、空氣等之無機物理發泡劑。該等中,較佳為無臭氧層破壞且廉價的無機物理發泡劑,特別是氮氣、空氣、二氧化碳較佳。且,該等發泡劑亦可併用兩種以上。As a blowing agent used in the dispersion medium release foaming method, propane, isobutane, n-butane, isopentane, n-pentane, cyclopentane, n-hexane, cyclobutane, cyclohexane are generally exemplified. , Chlorofluoromethane, trifluoromethane, 1,1,1,2-tetrafluoroethane, 1-chloro-1,1-difluoroethane, 1,1-difluoroethane, 1-chloro-1, Organic physical blowing agents such as 2,2,2-tetrafluoroethane, hydrofluoroolefin, etc., or inorganic physical blowing agents such as nitrogen, carbon dioxide, argon, air, etc. Among these, non-ozone-depleting and cheap inorganic physical blowing agents are preferred, especially nitrogen, air, and carbon dioxide. In addition, these blowing agents may be used in combination of two or more.

發泡劑之使用量係根據欲獲得的多層發泡粒子之體密度與發泡溫度之關係適當決定。具體而言,於氮氣、空氣除外之前述發泡劑的情況下,發泡劑之使用量通常相對於樹脂粒子每100重量份為2重量份以上50重量份以下。且於氮氣、空氣之情況下,以使密閉容器內之壓力為15MPa(G)以上5MPa(G)以下的壓力範圍內,較佳為1.55MPa(G)以上3.5MPa(G)以下之壓力範圍內之量而使用。The amount of foaming agent used is appropriately determined according to the relationship between the bulk density of the multilayer foamed particles to be obtained and the foaming temperature. Specifically, in the case of the aforementioned foaming agent excluding nitrogen and air, the usage-amount of the foaming agent is usually not less than 2 parts by weight and not more than 50 parts by weight per 100 parts by weight of resin particles. And in the case of nitrogen and air, the pressure in the airtight container is within the pressure range of 15MPa(G) to 5MPa(G), preferably 1.55MPa(G) to 3.5MPa(G) Use within the amount.

密封容器中,作為用以使樹脂粒子分散之分散介質較佳為水,但只要為不溶解樹脂粒子者,均可使用,作為此種分散介質舉例為例如乙二醇、甘油、甲醇、乙醇等。In a sealed container, water is preferred as the dispersion medium for dispersing the resin particles, but any one that does not dissolve the resin particles can be used. Examples of such dispersion medium include ethylene glycol, glycerin, methanol, ethanol, etc. .

平均氣泡徑之大小係由發泡劑之種類與量、發泡溫度與氣泡調節劑之添加量而調節。體密度(發泡倍率)可根據發泡劑之添加量與發泡溫度,與發泡時之容器內壓力與大氣壓之差壓而調節。在適當範圍內,一般發泡劑之添加量越多,發泡溫度越高,該差壓越大,則所得發泡粒子之體密度越小。The size of the average cell diameter is adjusted by the type and amount of foaming agent, foaming temperature and the amount of foam regulator added. Bulk density (expansion ratio) can be adjusted according to the amount of foaming agent added, the foaming temperature, and the pressure difference between the pressure inside the container and the atmospheric pressure when foaming. Within an appropriate range, generally, the more the amount of foaming agent added, the higher the foaming temperature, and the larger the differential pressure, the smaller the bulk density of the foamed particles obtained.

密封容器內,於將樹脂粒子分散於分散介質中並加熱到發泡溫度時,可使用分散劑以防止多層樹脂粒子相互熔著。作為分散劑,只要不溶解於水等,即使加熱亦不熔融者,則無機系、有機系均可使用,但一般較佳為無機系。In a sealed container, when the resin particles are dispersed in the dispersion medium and heated to the foaming temperature, a dispersant can be used to prevent the multi-layered resin particles from being fused to each other. Both inorganic and organic dispersants can be used as long as they do not dissolve in water or the like and do not melt even when heated, but generally, inorganic ones are preferred.

作為無機系之分散劑,較佳為高嶺土、滑石、雲母、氧化鋁、氧化鈦、氫氧化鋁等之粉體。作為分散劑較佳為平均粒徑0.001μm以上100μm以下,特別是0.001μm以上30μm以下者。且分散劑之添加量相對於樹脂粒子100重量份,通常較佳為0.01重量份以上10重量份以下。As an inorganic dispersant, powders such as kaolin, talc, mica, alumina, titanium oxide, and aluminum hydroxide are preferred. The dispersing agent preferably has an average particle diameter of 0.001 μm to 100 μm, especially 0.001 μm to 30 μm. In addition, the amount of the dispersant to be added is usually preferably not less than 0.01 parts by weight and not more than 10 parts by weight relative to 100 parts by weight of the resin particles.

又作為分散助劑較佳使用十二烷基苯磺酸鈉、油酸鈉等之陰離子系界面活性劑或硫酸鋁。該分散助劑按於每100重量份樹脂粒子,通常較佳添加0.001重量份以上5重量份以下。It is also preferable to use anionic surfactants such as sodium dodecylbenzenesulfonate and sodium oleate or aluminum sulfate as a dispersing aid. The dispersing aid is usually preferably added in a range of not less than 0.001 parts by weight and not more than 5 parts by weight per 100 parts by weight of resin particles.

至造體密度小的多層發泡粒子時,較佳進行藉由分散介質釋放發泡方法等製造多層發泡粒子,進而使所得之多層發泡粒子發泡之所謂兩階段發泡。兩階段發泡中,將多層發泡粒子填充於可加壓之密閉容器中,藉由空氣等之氣體進行加壓處理,進行使多層發泡粒子之內壓提高至0.01MPa(G)以上0.6MPa(G)以下之操作後,自密閉容器內取出多層發泡粒子,使用蒸汽等之加熱介質進行加熱,藉此可容易獲得體密度小的多層發泡粒子。When producing multi-layered expanded particles with low density, it is preferable to perform so-called two-stage foaming in which multi-layered expanded particles are produced by a dispersion medium releasing foaming method, and then the obtained multi-layered expanded particles are expanded. In two-stage foaming, the multilayer foamed particles are filled in a pressurizable airtight container, and the pressure treatment is carried out by a gas such as air to increase the internal pressure of the multilayered foamed particles to 0.6 or more than 0.01MPa(G). After the operation below MPa (G), take out the multilayer expanded particles from the airtight container and heat them with a heating medium such as steam, thereby easily obtaining multilayer expanded particles with low bulk density.

發泡粒子成形體可利用以往習知之方法,藉由將前述多層發泡粒子填充至成形模具內,使用蒸汽等之加熱介質進行加熱成形而獲得。具體而言,將多層發泡粒子填充至成形模具內之後,藉由於模具內導入蒸汽,加多層發泡粒子加熱並發泡而相互熔著可獲得經賦形成形空間之形狀的成形體。 又,作為獲得低成形體密度之成形體的方法,有根據需要進行與前述之兩階段發泡中之操作相同的提高多層發泡粒子內之壓力的加壓處理,將多層發泡粒子內之內壓調整至0.01MPa(G)以上0.2MPa(G)以下後,進行模內成形之方法。 The expanded particle molded body can be obtained by filling the above-mentioned multi-layered expanded particles into a molding die, and then heat-molding it using a heating medium such as steam, using conventionally known methods. Specifically, after filling the multi-layered expanded particles into the forming mold, by introducing steam into the mold, the multi-layered expanded particles are heated and foamed to fuse with each other to obtain a molded body in the shape of the shaped space. Also, as a method of obtaining a molded article with a low molded article density, there is a pressure treatment to increase the pressure inside the multilayered expanded bead similar to the operation in the above-mentioned two-stage foaming, if necessary, and pressurize the inside of the multilayered expanded bead. The method of in-mold forming after adjusting the internal pressure to 0.01MPa(G) or more and 0.2MPa(G) or less.

使用本發明之多層發泡粒子進行模內成形時,成形蒸汽壓較佳為0.05MPa(G)以上0.46MPa(G)以下,更佳為0.07MPa(G)以上0.35MPa(G)以下,更佳為0.09MPa(G)以上0.32MPa(G)以下。When using the multi-layer expanded particles of the present invention for in-mold forming, the forming steam pressure is preferably not less than 0.05MPa(G) and not more than 0.46MPa(G), more preferably not less than 0.07MPa(G) and not more than 0.35MPa(G). Preferably, it is not less than 0.09 MPa (G) and not more than 0.32 MPa (G).

本發明中,藉由採用以使多層發泡粒子以於成形模內之壓縮率為4體積%以上25體積%以下,較佳為5體積%以上20體積%以下之方式填充後,利用蒸汽進行模內成形之方法,可獲得目的之發泡粒子成形體。In the present invention, after filling the multi-layer expanded particles with a compression ratio in the forming mold of 4% to 25% by volume, preferably 5% to 20% by volume, steam is used to carry out The method of in-mold molding can obtain the desired expanded particle molded body.

壓縮率之調整,係於將發泡粒子填充至成形模內(模腔)時,藉由開裂填充超過模腔體積之多層發泡粒子的量而進行。開裂填充係為了在將多層發泡粒子填充於成形模中時將成形模內之空氣從模具內排出,而效率良好地進行多層發泡粒子向成形模內之填充,而在多層發泡粒子填充時不使成形模完全封閉所進行之填充方法。又,所謂開裂係指成形模之開口部分,開裂於成形模內填充多層發泡粒子後,最終在導入蒸汽時關閉,結果將所填充之多層發泡粒子壓縮。 [實施例] The adjustment of the compressibility is carried out by cracking and filling the amount of the multi-layered expanded particles exceeding the volume of the cavity when the expanded particles are filled into the forming mold (cavity). Crack filling is to discharge the air in the forming mold from the mold when filling the multilayer expanded particles into the forming mold, and efficiently fill the multilayer expanded particles into the forming mold. A filling method that does not completely close the forming mold. Also, the so-called cracking refers to the opening part of the molding die, which is cracked after the multi-layer expanded particles are filled in the molding die, and finally closed when steam is introduced, resulting in compression of the filled multi-layer expanded particles. [Example]

以下,列舉實施例更詳細說明本發明。但本發明不受該等實施例之限制。Hereinafter, the present invention will be described in more detail with reference to examples. But the present invention is not limited by these examples.

實施例、比較例中作為原料使用之乙烯-丙烯無規共聚物(A)的種類、物性示於表1。Table 1 shows the types and physical properties of the ethylene-propylene random copolymer (A) used as a raw material in Examples and Comparative Examples.

Figure 02_image009
Figure 02_image009

實施例、比較例中作為原料使用之聚烯烴系樹脂(B)的乙烯-丙烯無規共聚物的種類、物性如下所示。 聚烯烴系樹脂(B):乙烯-丙烯無規共聚物,乙烯成分含量(3.0質量%),熔點134℃,撓曲彈性模數770MPa,MFR7g/10分(230℃/2.16kg荷重)。 The types and physical properties of the ethylene-propylene random copolymer of the polyolefin resin (B) used as a raw material in Examples and Comparative Examples are as follows. Polyolefin-based resin (B): ethylene-propylene random copolymer, ethylene content (3.0% by mass), melting point 134°C, flexural modulus 770MPa, MFR 7g/10min (230°C/2.16kg load).

氣泡調整劑使用硼酸鋅。Zinc borate is used as the air bubble regulator.

作為物理發泡劑使用二氧化碳。Carbon dioxide is used as physical blowing agent.

表1中,熔點(Tm)、結晶化溫度(Tc)、MFR、分子量(Mn)、分子量(Mw)、分子量(Mz)、撓曲彈性模數系藉由以下方法測定。In Table 1, melting point (Tm), crystallization temperature (Tc), MFR, molecular weight (Mn), molecular weight (Mw), molecular weight (Mz), and flexural modulus were measured by the following methods.

[熔點、熔解熱量、結晶化溫度之測定] 共聚物(A)、樹脂(B)之熔點、結晶化溫度係根據JIS K7121:1987求出。具體而言,將顆粒狀之樣品2mg作成試驗片,基於JIS K7121:1987中記載之熱通量示差掃描熱量測定法,以10℃/分鐘之升溫速度自30℃升溫至200℃後,以10℃/分鐘之冷卻速度降溫至30℃,再次以10℃/分鐘之升溫速度自30℃升溫至200℃時所得之DSC曲線所決定之吸熱波峰之頂點溫度設為熔點。且,自DSC曲線所得之吸熱波峰的熱量設為熔解熱量。 又,結晶化溫度係根據JIS K7121(1987)測定之值,將以加熱速度10℃/min自30℃加熱至200℃而熔融之樣品,以冷卻速度10℃/min將溫度降至30℃時所得之DSC曲線之結晶化熱量波峰的頂點溫度設為結晶化溫度(℃)。 又,測定裝置使用熱通量示差掃描熱測定裝置(T.A儀器公司製DSC.Q1000)。 [Measurement of melting point, heat of fusion, crystallization temperature] The melting point and crystallization temperature of the copolymer (A) and the resin (B) were determined in accordance with JIS K7121:1987. Specifically, 2 mg of a granular sample was made into a test piece, and based on the heat flux differential scanning calorimetry method described in JIS K7121:1987, the temperature was raised from 30°C to 200°C at a heating rate of 10°C/min, and then the test piece was heated at 10°C. Cool down to 30°C at a cooling rate of °C/min, and then heat up from 30°C to 200°C at a heating rate of 10°C/min. The peak temperature of the endothermic peak determined by the DSC curve is set as the melting point. And, the calorific value of the endothermic peak obtained from the DSC curve was set as the heat of fusion. In addition, the crystallization temperature is the value measured according to JIS K7121 (1987). When the sample is heated from 30°C to 200°C at a heating rate of 10°C/min and melted, the temperature is lowered to 30°C at a cooling rate of 10°C/min. The peak temperature of the heat of crystallization peak of the obtained DSC curve was defined as the crystallization temperature (° C.). In addition, a heat flux differential scanning calorimeter (DSC.Q1000 manufactured by T.A Instruments Co., Ltd.) was used as a measuring device.

(MFR(熔體流動速率)) 乙烯-丙烯無規共聚物(A)、聚烯烴系樹脂(B)的MFR係以JIS K7210:1999之試驗條件M(230℃/2.16kg荷重)測定。 (MFR(melt flow rate)) The MFR of the ethylene-propylene random copolymer (A) and the polyolefin resin (B) was measured in accordance with the test condition M (230° C./2.16 kg load) of JIS K7210:1999.

[分子量測定方法及測定條件] 試料之前處理:將試料30mg投入鄰-二氯苯20mL中,於145℃振盪使溶解後,將該溶液以孔徑為1.0μm的燒結過濾器熱過濾者作為分析試料,並於以下條件進行測定。 測定裝置      :HLC-8321GPC/HT型高溫凝膠滲透層析儀(TOSOH股份有限公司製) 解析裝置      :數據處理軟體Empower3(日本WATERS股份有限公司製) 管柱            :2根TSKgel GMH6-HT、2根TSKgel GMH6-HTL(分別為內徑7.5mm×長度300mm,TOSOH股份有限公司製) 移動相         :鄰-二氯苯(含0.025%BHT) 管柱溫度      :140℃ 檢測器         :示差折射率計(RI) 流速            :1.0mL/min 試料濃度      :0.15%(W/V)-鄰-二氯苯 注入量         :400μL 取樣時間間隔:1秒 管柱校正:單分散聚苯乙烯(TOSOH股份有限公司製) 分子量換算:聚丙烯(PP)換算/通用校正法 又表1中,係測定製造發泡粒子之前的原料之分子量。於製造發泡粒子之步驟中,由於並未推定分子量大幅變動,故認為取出發泡芯層部分,進行前述操作仍可測定分子量。 [Molecular weight determination method and measurement conditions] Pretreatment of the sample: put 30 mg of the sample into 20 mL of o-dichlorobenzene, shake it at 145°C to dissolve, then heat filter the solution with a sintered filter with a pore size of 1.0 μm as the analysis sample, and measure it under the following conditions. Measuring device: HLC-8321GPC/HT high temperature gel permeation chromatography (manufactured by TOSOH Co., Ltd.) Analysis device: data processing software Empower3 (manufactured by Japan WATERS Co., Ltd.) String: 2 pieces of TSKgel GMH6-HT, 2 pieces of TSKgel GMH6-HTL (inner diameter 7.5mm×length 300mm, manufactured by TOSOH Co., Ltd.) Mobile phase : o-dichlorobenzene (containing 0.025% BHT) Column temperature : 140°C Detector : Differential Refractometer (RI) Flow rate : 1.0mL/min Sample concentration : 0.15%(W/V)-o-dichlorobenzene Injection volume : 400μL Sampling interval: 1 second Column calibration: monodisperse polystyrene (manufactured by TOSOH Co., Ltd.) Molecular weight conversion: Polypropylene (PP) conversion/universal calibration method Also in Table 1, the molecular weights of raw materials before producing expanded particles were measured. In the step of producing expanded particles, since the molecular weight is not expected to fluctuate greatly, it is considered that the molecular weight can still be measured by taking out the expanded core layer and performing the above operation.

表1中,共聚物(A)、共聚物(B)之乙烯成分含量(wt%)係藉由上述方法測定。具體而言,如下般測定。In Table 1, the ethylene content (wt%) of the copolymer (A) and the copolymer (B) was measured by the above-mentioned method. Specifically, it measures as follows.

(乙烯成分含量) 聚丙烯系樹脂之乙烯成分含量係藉由利用IR光譜決定之習知方法求出。具體而言,以高分子分析手冊(日本分析化學會高分子分析研究座談會編,出版年月:1995年1月,出版社:紀伊國屋書店,頁碼及項目名:615~616「II.2.3 2.3.4丙烯/乙烯共聚物」,618~619「II.2.3 2.3.5丙烯/丁烯共聚物」)中記載之方法測定。首先,將聚丙烯樹脂在180℃環境下熱壓成形為薄膜狀,製作厚度不同之複數試驗片。其次,藉由測定各試驗片之IR光譜,讀取源自乙烯之722cm -1及733cm -1之吸光度(A722、A733)。其次,針對各試驗片,使用以下之式(5)~(7)計算聚丙烯系樹脂中之乙烯成分含量。針對各試驗片所得之乙烯成分含量進行算術平均之值設為聚丙烯系樹脂中之乙烯成分含量(單位:質量%)。

Figure 02_image011
但,式(5)~(7)中,K’a:各波數中所見之吸光係數(K’a=A/ρt),K’c:修正後之吸光係數,A:吸光度,ρ:樹脂之密度(單位:g/cm 3),t:薄膜狀之試驗片的厚度(單位:cm)。 (Ethylene Component Content) The ethylene component content of the polypropylene-based resin was determined by a known method determined using IR spectroscopy. Specifically, the Handbook of Polymer Analysis (edited by the Symposium on Polymer Analysis of the Japanese Society of Analytical Chemistry, date of publication: January 1995, publisher: Kinokuniya Shoten, page number and project name: 615~616 "II.2.3 2.3 .4 Propylene/ethylene copolymer", measured by the method described in 618~619 "II.2.3 2.3.5 Propylene/butylene copolymer"). First, the polypropylene resin was thermocompressed into a film at 180°C to produce a plurality of test pieces with different thicknesses. Next, by measuring the IR spectrum of each test piece, the absorbance (A722, A733) at 722 cm -1 and 733 cm -1 derived from ethylene was read. Next, for each test piece, the content of the ethylene component in the polypropylene-based resin was calculated using the following formulas (5) to (7). The arithmetic mean value of the ethylene content obtained for each test piece was set as the ethylene content (unit: mass %) in the polypropylene-based resin.
Figure 02_image011
However, in formulas (5)~(7), K'a: the absorption coefficient seen in each wave number (K'a=A/ρt), K'c: the corrected absorption coefficient, A: absorbance, ρ: Density of resin (unit: g/cm 3 ), t: thickness of film-like test piece (unit: cm).

樹脂之撓曲彈性模數係根據JIS K 7171 (2008)測定。又,測定裝置使用A&D公司製之Tensilon萬能測試積RTF-1350。The flexural elastic modulus of the resin was measured in accordance with JIS K 7171 (2008). In addition, as a measuring device, Tensilon universal tester RTF-1350 manufactured by A&D Co., Ltd. was used.

實施例1~4、比較例1~3 [多層樹脂粒子之製造] 使用於內徑50mm之樹脂粒子芯層擠出機及內徑30mm之樹脂粒子被覆層用擠出機之出口側附設多層股形成用模嘴之裝置。將表2所示之種類、量的乙烯-丙烯無規共聚物(A)與氣泡調整劑母料(相對於共聚物(A)100重量份為1重量份)供給至內徑50mm之樹脂粒子芯層用擠出機,同時將表2所示之種類、量的作為聚烯烴系樹脂之丙烯系樹脂(B)供給至內徑30mm之樹脂粒子被覆層用擠出機,分別在設定溫度200℃以上220℃以下的範圍內加熱、熔融並混練後,供給至該模嘴,於模嘴內合流為鞘芯狀(樹脂粒子芯層與樹脂粒子被覆層之質量比95∶5),自安裝於擠出機前端之金屬蓋之細孔,以於芯層之側面被覆有被覆層的多層股而共擠出,將共擠出之股通入水中進行水冷,以造粒機切斷為(1.2mg,L/D=2.9),獲得具有2層構造(鞘芯構造)之圓柱狀多層樹脂粒子(相對於圓柱之芯,於圓柱的周面形成被覆層)。 又,多層樹脂粒子的重量、L/D係自多層樹脂粒子群隨機擷取之100個多層樹脂粒子求出之算術平均值。 Embodiment 1~4, comparative example 1~3 [Manufacturing of multilayer resin particles] It is used in the exit side of the resin particle core layer extruder with an inner diameter of 50mm and the resin particle coating extruder with an inner diameter of 30mm. The type and amount of ethylene-propylene random copolymer (A) and cell regulator masterbatch (1 part by weight relative to 100 parts by weight of copolymer (A)) were supplied to resin particles with an inner diameter of 50 mm as shown in Table 2. The extruder for the core layer simultaneously supplies the type and amount of propylene-based resin (B) as the polyolefin-based resin shown in Table 2 to the extruder for the resin particle coating layer with an inner diameter of 30 mm, respectively at a set temperature of 200 After heating, melting and kneading in the range of ℃ to 220℃, it is supplied to the die nozzle and merged in the die nozzle to form a sheath core (the mass ratio of the resin particle core layer to the resin particle coating layer is 95:5), self-installation The thin hole of the metal cover at the front end of the extruder is co-extruded with the multi-layer strands covered with the coating layer on the side of the core layer, and the co-extruded strands are put into water for water cooling, and cut by a pelletizer ( 1.2 mg, L/D=2.9), and obtained cylindrical multilayered resin particles having a two-layer structure (sheath-core structure) (with respect to the core of the cylinder, a coating layer is formed on the peripheral surface of the cylinder). In addition, the weight and L/D of the multilayered resin particles are arithmetic mean values obtained from 100 multilayered resin particles randomly selected from the group of multilayered resin particles.

Figure 02_image013
Figure 02_image013

[多層發泡粒子之製造] 將所得之多層樹脂粒子20kg與分散介質的水60L一起饋入100L的高壓釜內,於分散介質中分別添加作為分散劑之高嶺土15g、作為分散助劑之烷基苯磺酸鈉12g及硫酸鋁3g,在密閉容器內壓入作為發泡劑的二氧化碳以成為2.2MPa(G)的容器壓力,在攪拌下加熱升溫至發泡溫度150℃,並在相同溫度保持15分鐘,調整高溫波峰熱量後,將高壓釜內容物與水一起釋放到大氣壓下,獲得多層發泡粒子。 [Manufacture of multi-layer expanded particles] Feed 20 kg of the obtained multilayer resin particles into a 100 L autoclave together with 60 L of water in the dispersion medium, and add 15 g of kaolin as a dispersant, 12 g of sodium alkylbenzenesulfonate and aluminum sulfate as a dispersant in the dispersion medium 3g, press carbon dioxide as a foaming agent into the airtight container to make the container pressure 2.2MPa(G), heat it up to the foaming temperature of 150°C under stirring, and keep it at the same temperature for 15 minutes, after adjusting the peak heat of high temperature , the contents of the autoclave were released to atmospheric pressure together with water to obtain multilayer expanded particles.

如此獲得之多層發泡粒子具有由聚丙烯系樹脂所成之發泡芯層與被覆該發泡芯層之聚烯烴系樹脂所成之被覆層。The multilayer expanded particles thus obtained have a core foam layer made of a polypropylene resin and a coating layer made of a polyolefin resin covering the core foam layer.

表2中,藉由前述方法測定多層發泡粒子之體密度、平均氣泡徑及獨立氣泡率。In Table 2, the bulk density, average cell diameter, and independent cell ratio of the multilayer expanded particles were measured by the aforementioned method.

表2中,藉由前述方法測定高溫波峰熱量、總熔解波峰熱量。In Table 2, the high temperature peak heat and the total melting peak heat were determined by the aforementioned method.

[發泡粒子成形體之製造] 作為成形模,使用具有縱向尺寸600mm×橫向尺寸1250mm×厚度方向尺寸50mm的內部尺寸之長方體狀之成形模腔的大型模具。 自模具完全關閉之狀態成為打開5mm的狀態(此時成形模腔之厚度方向尺寸55mm)下,將多層發泡粒子填充於成形模腔內。填充完成後,將模具完全關閉(開裂量5mm,10%)。隨後,將蒸汽供給至成形模腔內,加熱多層發泡粒子,藉由使發泡粒子二次發泡並熔融,獲得發泡粒子成形體。加熱方法係在打開兩面模具之排出閥的狀態下供給蒸汽5秒進行預加熱(排氣步驟)後,在比表2中記載之成形蒸氣壓低0.08MPa(G)的壓力下進行一方加熱,進而以比表2記載之成形蒸汽壓低0.04MPa(G)之壓力自相反方向進行一方加熱後,以表2所示之成形蒸汽壓進行兩面加熱(正式加熱)。加熱完成後,釋放壓力,將模具水冷至模具內之發泡粒子成形體的面壓為0.04MPa(G)後,打開模具,自模具取出發泡粒子成形體。所得之發泡粒子成形體於大氣壓、溫度80℃之環境下養生12小時。又,水冷時間係加熱完成後,進行水冷直至模具內之發泡粒子成形體的面壓成為0.04MPa(G)之時間。所得發泡粒子成形體的物性示於表2。又,表2所示之成形蒸汽壓表示於能獲得外觀良好之成形體之蒸汽壓之成形中之最低成形蒸汽壓。又,外觀良好之成形品之基準,係成型體的熔著率為80%以上,於成形體表面幾乎看不到間隙或凹陷者,為良好外觀之成形體。 [Manufacture of expanded particle molded body] As the forming die, a large die having a rectangular parallelepiped forming cavity with internal dimensions of 600 mm in length x 1250 mm in width x 50 mm in thickness direction was used. From the fully closed state of the mold to the state of opening 5mm (at this time, the dimension in the thickness direction of the molding cavity is 55mm), the multilayer expanded particles are filled in the molding cavity. After the filling is completed, the mold is completely closed (cracking amount 5mm, 10%). Subsequently, steam is supplied into the molding cavity to heat the multi-layered expanded particles, and the expanded particles are secondarily expanded and melted to obtain a molded body of expanded particles. The heating method is to supply steam for 5 seconds in the state of opening the discharge valve of the two-sided mold for preheating (exhaust step), then heat one side at a pressure 0.08MPa(G) lower than the forming steam pressure described in Table 2, and then After heating one side from the opposite direction at a pressure 0.04MPa(G) lower than the forming steam pressure shown in Table 2, heat both sides at the forming steam pressure shown in Table 2 (main heating). After the heating is completed, the pressure is released, and the mold is water-cooled until the surface pressure of the expanded particle molded body in the mold is 0.04 MPa (G), then the mold is opened, and the expanded particle molded body is taken out from the mold. The obtained expanded particle molded body was cured for 12 hours under an environment of atmospheric pressure and a temperature of 80°C. In addition, the water cooling time refers to the time for water cooling until the surface pressure of the expanded particle molded body in the mold becomes 0.04 MPa (G) after the heating is completed. Table 2 shows the physical properties of the obtained expanded particle molded body. In addition, the molding steam pressure shown in Table 2 represents the lowest molding steam pressure in the molding at which a molded product with a good appearance can be obtained. Also, the criteria for a molded article with good appearance is that the fusion rate of the molded article is 80% or more, and a molded article with a good appearance can hardly see gaps or depressions on the surface of the molded article.

表2中,成形體密度、收縮率、與基準尺寸的乖離率、50%變形時壓縮應力係如下測定。In Table 2, the molded body density, shrinkage rate, deviation rate from reference dimensions, and compressive stress at 50% deformation were measured as follows.

[發泡粒子成形體之成形體密度] 將發泡粒子成形體之重量除以從發泡粒子成形體之外形尺寸求出之體積後之值,並單位轉算為[kg/m 3]。 [Molded product density of expanded bead molded product] The value obtained by dividing the weight of the expanded bead molded product by the volume obtained from the external dimension of the expanded bead molded product, and the unit is converted into [kg/m 3 ].

[熔著率] 熔著率係藉由下述方法測定。 自發泡粒子成形體,隨機切出長度150mm,寬度75mm,厚度20mm之試驗片(留下至少單面的表皮)。對於該長方體形狀的成形體樣品,於長度方向中心部分於一表面(至少留下無切口之表皮)切出深度5mm的切口,以橫穿過整個寬度切入,將其作為試驗片。其次,於以中心間距離為70mm之方式平行立設且上端倒圓成半徑5mm的高度100mm、寬度80mm以上、厚度10mm的剛體所成之2片支撐板上,將該試驗片以設置切口之面朝向下側,且試驗片之長度方向與支撐板正交的方式均等跨設配製。其次,以前端經倒圓成半徑5mm之高度60mm、寬度80mm、厚度10mm的剛體所成之按壓板,以按壓板之厚度方向的中央部與試驗片的切口一致的方式設置,自試驗片的切口的相反側,將按壓板之按壓速度設為200mm/分鐘進行3點撓曲試驗,按壓直到試驗片斷裂,或直到試驗片從支撐板上脫離完全進入至支撐板之間為止。 其次,觀察試驗片之剖斷面,藉由目視分別測量於內部斷裂的發泡粒子與於界面剝離之發泡粒子數。其次,計算內部斷裂之發泡粒子相對於內部斷裂之發泡粒子與於界面剝離之發泡粒子之合計數的比率,將其以百分比表示作為熔著率(%)。 又,最初切口5mm上存在的發泡粒子均不列入計算。且,著眼於試驗片之斷裂面的1個發泡粒子時,於包含經破壞之部分與在發泡粒子間剝離之部分這兩者的情況下,考慮面積,於經破壞之部分的面積為50%以上的情況下計數為經破壞之數,於經破壞之部分的面積未達50%的情況下,計數為在發泡粒子間剝離之數。且,該試驗結果,於試驗片未完全斷裂之情況,非斷裂部分被視為全部經破壞,以刀子將非斷裂部分垂直(於試驗片之厚度方向)切斷,計數於切斷面存在之發泡粒子數作為於內部經破壞之發泡粒子數,如上述求出熔著率(%)。又所得發泡粒子成型體之熔著率均為90%以上。 [Fusion rate] The fusion rate was measured by the following method. Randomly cut out a test piece with a length of 150 mm, a width of 75 mm, and a thickness of 20 mm (leave at least one surface of the skin) from the expanded particle molded body. For this cuboid-shaped molded body sample, a notch with a depth of 5 mm was cut on one surface (leaving at least the skin without notch) at the central part in the longitudinal direction, so as to cut across the entire width, and this was used as a test piece. Next, place the test piece on the side where the cutout is set on two support plates made of rigid bodies with a height of 100 mm, a width of more than 80 mm, and a thickness of 10 mm, which are erected in parallel with a center-to-center distance of 70 mm and whose upper ends are rounded to a radius of 5 mm. Facing the lower side, and the length direction of the test piece is perpendicular to the support plate, and the preparation is equally straddled. Next, use a pressing plate made of a rigid body with a height of 60mm, a width of 80mm, and a thickness of 10mm after the front end is rounded to a radius of 5mm. On the opposite side, set the pressing speed of the pressing plate to 200mm/min to perform a 3-point flexure test, and press until the test piece breaks, or until the test piece breaks away from the support plate and completely enters between the support plates. Next, the cross-section of the test piece was observed, and the numbers of the expanded particles broken inside and the expanded particles peeled off at the interface were respectively measured by visual observation. Next, the ratio of internally broken expanded particles to the total number of internally broken expanded particles and expanded particles separated at the interface was calculated, and expressed as a percentage as a fusion rate (%). Also, the expanded particles existing on the initial 5 mm cut are not included in the calculation. And, when focusing on one expanded particle on the fractured surface of the test piece, considering the area including both the damaged part and the part peeled between the expanded particles, the area of the broken part is When it was 50% or more, it was counted as the number of broken parts, and when the area of the damaged part was less than 50%, it was counted as the number of peeling between expanded particles. Moreover, in the test results, when the test piece is not completely broken, the non-broken part is considered to be completely destroyed, and the non-broken part is cut vertically (in the thickness direction of the test piece) with a knife, and counted on the cut surface. The number of expanded particles was taken as the number of internally destroyed expanded particles, and the fusion rate (%) was determined as described above. The fusing rate of the obtained expanded particle molded body was all above 90%.

[收縮率] 發泡粒子成形體之收縮率[%]係將成形體之長邊長度的測定值代入(成形用模具之長邊尺寸[mm]-成形體之長邊長度[mm])/成形用模具之長邊尺寸[mm]×100而求出。又,所謂「成形體之長邊長度[mm]」,係將實施例及比較例所得之發泡粒子成形體在80℃的環境下養生12小時後,緩緩冷卻,進而於23℃之環境下養生6小時後之發泡粒子成形體進行長邊長度測量之值(n=10)。 [Shrinkage] The shrinkage rate [%] of the expanded particle molded body is to substitute the measured value of the length of the long side of the molded body into (the length of the long side of the mold for molding [mm] - the length of the long side of the molded body [mm]) / the length of the mold for the mold Long side dimension [mm] x 100 was calculated|required. In addition, the so-called "length of the long side [mm] of the molded body" means that the expanded particle molded bodies obtained in the examples and the comparative examples were kept in an environment of 80°C for 12 hours, then cooled slowly, and then placed in an environment of 23°C. The measured value of the length of the long side of the expanded particle molded body after 6 hours of curing (n=10).

[與基準尺寸之乖離率] 於實際之成形體時,成型體之收縮於成形體的每個部分並非均一引起。因此,並非完全再現該模具的形狀尺寸,而是成形體的各部分與模具之對應各部分之間產生尺寸差,於所得成形體產生變形。乖離率係亦考慮了相對於成為基準的模具模腔之尺寸的變形,顯現變形程度之測定值。 針對使用具有縱向尺寸600mm×橫向尺寸1250mm×厚度方向尺寸50mm之內部尺寸的長方體狀的成形模腔的模具藉由成形獲得之成形體,於長方體之各頂點如下般設置4個成為基準的點,測定乖離率。具體而言,假設具有前述模具模腔之尺寸的形狀,在假設的形狀中,在縱向與厚度方向所決定之一個平面(例如左側側面)選擇於斜向方向對向之兩個繳部分作為基準點(a1,b1)。 其次,推想以所得之發泡粒子成形體與假想之形狀兩者之偏差最小的方式重疊的狀態(或者,推想以重疊成為最大之方式重疊之狀態),測定前述基準點(a1,b1)與發泡粒子成形體之與前述基準點對應之部位(a2,b2)的長度方向之尺寸差。將此測定值設為a與b。進而,選擇由縱向與厚度方向決定之另一平面(例如右側側面)之斜向方向對向之兩個角部分作為基準點(c1,d1),同樣測定前述基準點(c1,d1)與發泡粒子成形體之前述基準點所對應之部位(c2,d2)的長度方向之尺寸差。將該測定值設為c、d。 其次將所得4個部位之長度方向之尺寸差(a,b,c,d)除以發泡粒子成形體之長度長度並平均之值作為與基準尺寸的乖離率。 [Deviation rate from standard size] In the actual molded body, the shrinkage of the molded body is not caused uniformly in each part of the molded body. Therefore, the shape and size of the mold are not completely reproduced, but a dimensional difference occurs between each part of the molded body and the corresponding parts of the mold, and deformation occurs in the resulting molded body. The deviation rate is also a measured value showing the degree of deformation relative to the deformation of the standard mold cavity size. For a molded body obtained by molding using a cuboid-shaped molding cavity having a longitudinal dimension of 600 mm x a lateral dimension of 1250 mm x a thickness direction dimension of 50 mm, four reference points are set at each vertex of the cuboid as follows, Measure the deviation rate. Specifically, assuming a shape with the size of the aforementioned mold cavity, in the hypothetical shape, a plane (such as the left side) determined by the longitudinal direction and the thickness direction is selected as the reference of two parts facing the oblique direction Point (a1, b1). Next, assuming a state where the obtained expanded particle molded body and the virtual shape are overlapped so that the deviation between them is the smallest (or a state where the overlap is estimated to be the largest), measure the aforementioned reference points (a1, b1) and The dimension difference in the longitudinal direction of the portion (a2, b2) corresponding to the aforementioned reference point of the expanded particle molded body. Let these measured values be a and b. Furthermore, select two corners opposite to the oblique direction of another plane (such as the right side) determined by the longitudinal direction and the thickness direction as the reference point (c1, d1), and measure the aforementioned reference point (c1, d1) and The size difference in the longitudinal direction of the part (c2, d2) corresponding to the above-mentioned reference point of the foam particle molded body. Let the measured values be c and d. Next, divide the dimensional differences (a, b, c, d) in the longitudinal direction of the obtained four parts by the length of the expanded particle molded body and take the average value as the deviation rate from the reference size.

[50%變形時之壓縮應力] 將長50mm×寬50mm×厚度25mm的試驗片除表皮以外予以切出,基於JIS K6767-1999,以壓縮速度10mm/分鐘進行壓縮試驗,求出將發泡粒子成形體壓縮至初始厚度的50%時的壓縮應力。試驗係對10個試驗片進行,所得之值的平均值設為50%變形時之壓縮應力。 [Compressive stress at 50% deformation] Cut out a test piece of length 50mm×width 50mm×thickness 25mm except for the skin, and conduct a compression test at a compression speed of 10mm/min based on JIS K6767-1999 to determine the compression of the expanded particle molded body to 50% of the initial thickness compressive stress at . The test was carried out on 10 test pieces, and the average value of the obtained values was set as the compressive stress at 50% deformation.

實施例1~4係使用滿足本發明之構成的乙烯-丙烯無規共聚物,製造多層發泡粒子之例。可於低蒸汽壓進行模內成形,冷卻步驟中的水冷卻時間比比較例短,見到水冷時間的縮短效果。且,收縮率、與基準尺寸的乖離率比比較例小。Examples 1 to 4 are examples of producing multilayer expanded particles using ethylene-propylene random copolymers satisfying the constitution of the present invention. In-mold molding can be performed at low steam pressure, and the water cooling time in the cooling step is shorter than that of the comparative example, and the effect of shortening the water cooling time can be seen. In addition, the shrinkage rate and the deviation rate from the reference size were smaller than those of the comparative example.

參考例1、參考例2係未設置被覆層之單層發泡粒子之例,藉由將參考例1、參考例2與實施例、比較例對比,可理解本發明之冷卻時間縮短之效果、即使縮短冷卻時間成形後之收縮等引起的尺寸變化的偏差小的效果,藉由設置被覆層而顯著呈現。Reference Example 1 and Reference Example 2 are examples of single-layer expanded particles without a coating layer. By comparing Reference Example 1 and Reference Example 2 with Examples and Comparative Examples, the effect of shortening the cooling time of the present invention can be understood, Even if the cooling time is shortened, the effect of small variation in dimensional changes due to shrinkage after molding, etc., is significantly exhibited by providing a coating layer.

參考例1係使用與實施例1相同的乙烯-丙烯無規共聚物,除了未設置被覆層以外,與實施例1同樣製造單層發泡粒子之例。 實施例1之成形蒸汽壓低於參考例1之成形蒸汽壓,確認具有滿足本發明構成之被覆層的發泡粒子,具有可縮短冷卻時間之效果。又,實施例1中,收縮率、整體乖離率均小於參考例1,可確認即使縮短冷卻時間,尺寸變化之偏差仍小。 參考例2係使用與比較例1相同的乙烯-丙烯無規共聚物,除了未設置被覆層以外,與比較例1同樣製造單層發泡粒子之例。 又,實施例1與比較例1係構成發泡芯層的乙烯-丙烯無規共聚物不同之例,參考例1與參考例2亦為構成發泡芯層的乙烯-丙烯無規共聚物不同之例。可知實施例1相對於比較例1之水冷時間減低之效果,比參考例1相對於參考例2之水冷時間減低效果格外大。此外,關於與基準尺寸之整體乖離率,亦可知設有被覆層的多層發泡粒子較優異。該等效果被認為是多層發泡粒子特有的效果。 Reference Example 1 is an example in which single-layer expanded particles were produced in the same manner as in Example 1, using the same ethylene-propylene random copolymer as in Example 1, except that no coating layer was provided. The forming steam pressure of Example 1 is lower than that of Reference Example 1, and it is confirmed that the expanded particles having a coating layer satisfying the structure of the present invention have the effect of shortening the cooling time. In addition, in Example 1, both the shrinkage rate and the overall deviation rate were lower than those in Reference Example 1, and it was confirmed that even if the cooling time was shortened, the variation in dimensional change was still small. Reference example 2 is an example in which single-layer expanded particles were produced in the same manner as in comparative example 1, using the same ethylene-propylene random copolymer as in comparative example 1, except that no coating layer was provided. Also, Example 1 and Comparative Example 1 are examples in which the ethylene-propylene random copolymers constituting the foam core layer are different, and reference example 1 and reference example 2 are also different in that the ethylene-propylene random copolymers constituting the foam core layer are different. example. It can be seen that the effect of reducing the water cooling time of Example 1 relative to Comparative Example 1 is much greater than that of Reference Example 1 relative to Reference Example 2. In addition, it can also be seen that the multilayered expanded particles provided with a coating layer are superior in the overall deviation rate from the reference size. These effects are considered to be effects specific to multilayer expanded particles.

a:固有波峰 b:高溫波峰 α:DSC線上相當於80℃之點 T E:熔解結束溫度 β:相當於熔解結束溫度T E之DSC曲線上的點 γ:固有波峰a與高溫波峰b間之谷底的點 δ:自點γ起之與圖表縱軸平行之直線與直線(α-β)相交的點 a: Intrinsic peak b: High temperature peak α: Point on the DSC line equivalent to 80°C T E : Melting end temperature β: Point on the DSC curve equivalent to melting end temperature T E γ: Between the inherent peak a and the high temperature peak b Point δ at the bottom of the valley: the point where a line parallel to the vertical axis of the chart from point γ intersects with the line (α-β)

[圖1]係顯示藉由熱通量示差掃描熱量測定之第1次加熱的DSC曲線之一例的圖式。[ Fig. 1 ] is a graph showing an example of the DSC curve of the first heating measured by heat flux differential scanning calorimetry.

Claims (12)

一種多層發泡粒子,其係具有發泡芯層與被覆該發泡芯層之被覆層之多層發泡粒子,其特徵為 該發泡芯層係由乙烯成分含有率2.5質量%以上3.5質量%以下之乙烯-丙烯無規共聚物(A)構成, 該被覆層係由聚烯烴系樹脂(B)構成, 藉由示差掃描熱量測定(DSC)所測定之該聚烯烴系樹脂(B)之DSC曲線具有一個以上之熔解波峰,該熔解波峰中之至少一個熔解波峰的熔解波峰溫度比該乙烯-丙烯無規共聚物(A)之熔點(Tm)低, 該乙烯-丙烯無規共聚物(A)之重量平均分子量(Mw)為20萬以上30萬以下,該乙烯-丙烯無規共聚物(A)之該重量平均分子量(Mw)相對於數平均分子量(Mn)的比(Mw/Mn)為3.5以上5以下。 A multi-layer expanded particle, which is a multi-layer expanded particle with a foam core layer and a coating layer covering the foam core layer, characterized in that The foam core layer is composed of ethylene-propylene random copolymer (A) with an ethylene content of 2.5% by mass to 3.5% by mass, The covering layer is made of polyolefin resin (B), The DSC curve of the polyolefin resin (B) measured by differential scanning calorimetry (DSC) has more than one melting peak, and the melting peak temperature of at least one of the melting peaks is higher than that of the ethylene-propylene random The melting point (Tm) of the copolymer (A) is low, The weight average molecular weight (Mw) of the ethylene-propylene random copolymer (A) is not less than 200,000 and not more than 300,000, and the weight average molecular weight (Mw) of the ethylene-propylene random copolymer (A) is relative to the number average molecular weight The ratio (Mw/Mn) of (Mn) is 3.5 or more and 5 or less. 如請求項1之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mz)相對於該乙烯-丙烯無規共聚物(A)之數平均分子量(Mn)的比(Mz/Mn)為9.5以上且未達13。The multilayer expanded particle as claimed in item 1, wherein the Z average molecular weight (Mz) of the aforementioned ethylene-propylene random copolymer (A) is relative to the number average molecular weight (Mn) of the ethylene-propylene random copolymer (A) The ratio (Mz/Mn) is 9.5 or more and less than 13. 如請求項1或2之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之熔點(Tm)為130℃以上150℃以下。The multilayer expanded particle according to claim 1 or 2, wherein the melting point (Tm) of the aforementioned ethylene-propylene random copolymer (A) is 130°C or higher and 150°C or lower. 如請求項1至3中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之結晶化溫度(Tc)與該乙烯-丙烯無規共聚物(A)之熔點(Tm)滿足下述(1)式:
Figure 03_image001
(但,式中之Tmc、Tc之單位均為℃)。
Multi-layer expanded particles as any one of claims 1 to 3, wherein the crystallization temperature (Tc) of the aforementioned ethylene-propylene random copolymer (A) is related to the melting point (Tc) of the ethylene-propylene random copolymer (A) ( Tm) satisfies the following formula (1):
Figure 03_image001
(However, the units of Tmc and Tc in the formula are both °C).
如請求項1至4中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mz)為50萬以上100萬以下。The multilayer expanded particle according to any one of claims 1 to 4, wherein the Z-average molecular weight (Mz) of the ethylene-propylene random copolymer (A) is not less than 500,000 and not more than 1 million. 如請求項5之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之Z平均分子量(Mw)相對於該乙烯-丙烯無規共聚物(A)之數平均分子量(Mz)之比(Mz/Mw)為2以上5以下。The multi-layer expanded particle as claimed in item 5, wherein the Z-average molecular weight (Mw) of the aforementioned ethylene-propylene random copolymer (A) is relative to the number-average molecular weight (Mz) of the ethylene-propylene random copolymer (A). The ratio (Mz/Mw) is 2 or more and 5 or less. 如請求項1至6中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之撓曲彈性模數為750MPa以上。The multilayer expanded particle according to any one of claims 1 to 6, wherein the flexural modulus of elasticity of the aforementioned ethylene-propylene random copolymer (A) is 750 MPa or more. 如請求項1至7中任一項之多層發泡粒子,其中前述乙烯-丙烯無規共聚物(A)之熔體流動速率為1g/10分鐘以上20g/10分鐘以下。The multilayer expanded particle according to any one of claims 1 to 7, wherein the melt flow rate of the aforementioned ethylene-propylene random copolymer (A) is not less than 1 g/10 minutes and not more than 20 g/10 minutes. 如請求項1至8中任一項之多層發泡粒子,其中前述多層發泡粒子之體密度為10kg/m 3以上300kg/m 3以下。 The multilayer expanded bead according to any one of claims 1 to 8, wherein the bulk density of the aforesaid multilayer expanded bead is not less than 10 kg/m 3 and not more than 300 kg/m 3 . 如請求項1至9中任一項之多層發泡粒子,其中構成前述多層發泡粒子之發泡芯層之平均氣泡徑為20μm以上400μm以下。The multilayer expanded particle according to any one of claims 1 to 9, wherein the average cell diameter of the foam core layer constituting the multilayer expanded particle is not less than 20 μm and not more than 400 μm. 一種發泡粒子成形體,其係將如請求項1至10中任一項之多層發泡粒子進行模內成形而成。A molded expanded particle, which is obtained by in-mold forming the multi-layered expanded particle according to any one of claims 1 to 10. 如請求項11之發泡粒子成形體,其中前述發泡粒子成形體之50%變形時壓縮應力為100kPa以上500kPa以下。The expanded bead molded body according to claim 11, wherein the compressive stress at 50% deformation of the expanded bead molded body is not less than 100 kPa and not more than 500 kPa.
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