JPH0132186B2 - - Google Patents
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- Publication number
- JPH0132186B2 JPH0132186B2 JP59227690A JP22769084A JPH0132186B2 JP H0132186 B2 JPH0132186 B2 JP H0132186B2 JP 59227690 A JP59227690 A JP 59227690A JP 22769084 A JP22769084 A JP 22769084A JP H0132186 B2 JPH0132186 B2 JP H0132186B2
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- particles
- ceramic material
- ceramics according
- ceramics
- manufacturing
- Prior art date
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- 239000002245 particle Substances 0.000 claims description 49
- 239000013078 crystal Substances 0.000 claims description 23
- 239000000919 ceramic Substances 0.000 claims description 20
- 239000000463 material Substances 0.000 claims description 20
- 238000004519 manufacturing process Methods 0.000 claims description 13
- 238000000034 method Methods 0.000 claims description 13
- 238000007731 hot pressing Methods 0.000 claims description 12
- 229910010293 ceramic material Inorganic materials 0.000 claims description 9
- 229910000906 Bronze Inorganic materials 0.000 claims description 6
- 239000010974 bronze Substances 0.000 claims description 6
- KUNSUQLRTQLHQQ-UHFFFAOYSA-N copper tin Chemical compound [Cu].[Sn] KUNSUQLRTQLHQQ-UHFFFAOYSA-N 0.000 claims description 6
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 claims description 6
- 229910052721 tungsten Inorganic materials 0.000 claims description 6
- 239000010937 tungsten Substances 0.000 claims description 6
- 238000007716 flux method Methods 0.000 claims description 4
- 239000011230 binding agent Substances 0.000 claims description 2
- 229910052745 lead Inorganic materials 0.000 claims description 2
- 238000000465 moulding Methods 0.000 claims description 2
- 238000010438 heat treatment Methods 0.000 description 7
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 6
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 4
- 238000000635 electron micrograph Methods 0.000 description 4
- 239000000203 mixture Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000010287 polarization Effects 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 238000003825 pressing Methods 0.000 description 3
- 238000005406 washing Methods 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 239000003153 chemical reaction reagent Substances 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- ZKATWMILCYLAPD-UHFFFAOYSA-N niobium pentoxide Chemical compound O=[Nb](=O)O[Nb](=O)=O ZKATWMILCYLAPD-UHFFFAOYSA-N 0.000 description 2
- 238000003786 synthesis reaction Methods 0.000 description 2
- 101710134784 Agnoprotein Proteins 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 229910052797 bismuth Inorganic materials 0.000 description 1
- JCXGWMGPZLAOME-UHFFFAOYSA-N bismuth atom Chemical compound [Bi] JCXGWMGPZLAOME-UHFFFAOYSA-N 0.000 description 1
- 238000009835 boiling Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 239000002270 dispersing agent Substances 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000005098 hot rolling Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 239000004570 mortar (masonry) Substances 0.000 description 1
- 230000005693 optoelectronics Effects 0.000 description 1
- 239000011819 refractory material Substances 0.000 description 1
- 238000004062 sedimentation Methods 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 238000003756 stirring Methods 0.000 description 1
- 239000011882 ultra-fine particle Substances 0.000 description 1
Landscapes
- Compositions Of Oxide Ceramics (AREA)
- Ceramic Products (AREA)
Description
〔発明の属する技術分野〕
本発明はセラミツクスの製造方法に関するもの
で、特に異なる方向から複数回熱間加圧すること
によつて、セラミツクスを構成する形状異方性を
有する粒子を一軸方向に揃え、配向性の良いセラ
ミツクスを製造する方法に関する。
〔発明の背景〕
圧電材料の中には、本来比較的良好な誘電特
性、圧電特性および電気光学効果を有する材料が
ある。一例として、タングステンブロンズ型の結
晶構造を有する強誘電体材料が挙げられるが、こ
の材料の結晶系では、結晶粒子が針状等の大きい
寸法異方性を有しており、分極容易な方向が限定
される。したがつて、この材料を圧電セラミツク
スに用いようとしても、セラミツクスではその粒
子の結晶軸が任意の方向を向いているため、外部
から電界を印加しても効率の良い分極処理を行な
うことができず、この材料が本来有している良好
な圧電特性および電気光学効果を利用することが
不可能であつた。このため、この結晶系に対する
研究は、主として単結晶材料としての応用研究に
向けられている。
一方、ビスマス層状化合物よりなる強誘電体材
料では、その粒子が板状をなしており、したがつ
て一軸加圧のホツトプレス法等によつて結晶粒子
が配向されたセラミツクス、したがつて効率の良
い分極処理が可能なセラミツクスを製造すること
ができ、良好な圧電特性を示すものが得られてい
る。しかしながら、上述の針状結晶粒子よりなる
タングステンブロンズ型構造の材料においては、
一軸加圧のホツドプレス法を行なつたのみでは、
加圧面内に針状粒子がランダムに配向するのみ
で、特定の方向に粒子を揃えることは不可能であ
るため、良好な圧電特性を示すものが得られなか
つた。
〔発明の目的〕
そこで本発明では、寸法異方性を有する粒子よ
りなるセラミツクス材料から、前記粒子を一軸方
向に配向させたセラミツクスを得るための製造方
法を提供することを目的とする。
〔発明の概要〕
本発明は、予め成長させた寸法異方性を有する
粒子よりなるセラミツクス材料に成形用バインダ
を加えて所定の形状に予備成形し、この成形体に
対し、異なる方向から熱間での加圧(ホツトプレ
ース)を行なうことによつて上記目的を達成して
いる。
上記の寸法異方性を有する粒子としては、例え
ばフラツクス法によつて形成されたタングステン
ブロンズ型の結晶構造を有する例えばPbNb2O6
等の針状または棒状結晶粒子が用いられる。
〔発明の実施例〕
以下本発明の実施例について詳細に説明する。
結晶粒子が針状または棒状等の寸法異方性を有す
る材料として種々のものが考えられるが、ここで
は、粒子を一軸方向に配向させた場合、その粒子
の一軸配向性が確認し易く、また粒子を一軸方向
に配向させることにより、その優れた誘電特性、
圧電特性および電気光学特性を活用することが期
待されるタングステンブロンズ型の結晶構造を有
する強誘電体材料を選び、本発明の有効性を実証
することにする。
上記のタングステンブロンズ型の結晶構造を有
する強誘電体材料としては、PbNb2O6、
Sr2NaNb5O15、Sr2KNb5O15、PbXBa1-XNb2O6、
SrXBa1-XNb2O6、(Pb、K)Nb2O6、
K3Li2Nb5O15、Ba2NaNb5O15、Ba2LiNb5O15、
K3Li2Nb5-XTaXO15、(Pb、Ba、La)Nb2O6等が
その主成分として挙げられるが、ここでは
PbNb2O6を用いた実施例について述べる。
まず、PbNb2O6の針状結晶粒子をフラツクス
法で合成した。ここで用いる試薬はすべて純度
99.5%以上の高純度の試薬である。PbOとNb2O5
をPbNb2O6の組成となるように調合し、900℃の
温度で2時間仮焼成したものに、等重量のKClを
加え、電動乳鉢で15分間混合した混合物約100グ
ラムをアルミナ製るつぼに入れ、900゜〜1200℃の
温度で1〜8時間加熱して反応させた。
上記の熱処理後、混合物を熱湯を入れた2リツ
トルのガラスビーカー内に入れて洗浄を行ない、
KCl部分を除去した。その際、イオン交換した水
の熱湯を用い、撹拌しながら洗浄し、熱湯を取り
替えて反復洗浄した。この熱湯を10回以上取り替
えて洗浄を行なつたところ、得られたPbNb2O6
の針状粒子末に残存するCl-イオンは、AgNO3溶
液を用いた検出によつては検出不能であつた。
かくて得られた針状および柱状の粒子を電子顕
微鏡で観察した結果を第1図a,bに示す。第1
図aの粒子は、KClフラツクス中で温度1050℃で
5時間熱処理して得られたものであり、第1図b
の粒子は、温度1200℃で5時間熱処理して得られ
たものである。合成温度が900℃未満では針状粒
子の発達が不良で短いものしか得られなかつた。
また1200℃を超える温度では、粒子が太く成長
し、粒子の寸法異方性が少なくなるため、この材
料では熱処理温度は900゜〜1200℃の範囲が適当で
あつた。特に1000゜〜1100℃の温度で合成したも
のの針状比(長さ/太さまたは直径)が大きく、
20〜40であつた。また合成時間が短か過ぎると粒
子の成長が進行せず、長過ぎると粒子の成長が進
み過ぎて太くなり、針状比が1に近くなるため、
本実施例では1〜8時間の熱処理によつて、粒子
の長さ2μm以上、針状比が1.2以上で100以下の寸
法異方性を有する粒子を得た。特に1050゜〜1100
℃の範囲内で3〜6時間反応させたものの針状比
は大きく、5時間反応させたものでは直径1.5〜
2μmで針状比が20〜40と大きい良好な針状粒子を
得た。
次にこの針状粒子よりなる粉末をイオン交換水
の中に投入し、更に分散剤を加えて十分に分散さ
せた後、沈降分級によつて、大きな粒子と超微粉
とを除き、針状粒子のみを取り出した。この分散
液を過し、かつ過しながらよく洗浄して乾燥
した。
この針状粒子よりなるセラミツクス材料に7重
量%のPVA溶液を8重量%加えながら造粒し、
さらに整粒したものを、第2図aに示すように、
直径15mm、高さ約20mmの円柱状成形体に予備成形
した。この円柱状成形体の底面上で互いに直交す
る2方向をそれぞれX軸およびY軸とし、円柱の
高さ方向をZ軸とする。
次にこの成形体を、内径40mmの高純度アルミナ
製のダイスに入れ、上下方向すなわちZ軸方向の
第1回目のホツトプレス(熱間加圧)を行なつ
た。この場合の圧力P1と加圧の方向、ホツトプ
レス後の試料の形状を第2図bに示す。この場
合、アルミナ製ダイスと試料を150℃/時で昇温
し、1200℃の温度において100Kg/cm2の圧力を印
加し、3時間のホツトプレスを行なつた。
上記第1回目のホツトプレス後、一旦降温して
試料を取出し、この試料に対し、第1回目の加圧
方向と直角の方向から加圧しうるように試料の方
向を変えて再びアルミナ製のダイス中にセツト
し、昇温して、第2図cに示すように、第2回目
のホツトプレスを、Z軸と直角なY軸の方向から
圧力P2をもつて行なつた。この第2回目のホツ
トプレスは、温度1250℃において100Kg/cm2の圧
力を3時間加えて行ない、試料を第2図cに示す
形状にした。
なお、ここでは一軸方向のみから加圧できるホ
ツトプレス装置を用いたため、上記のように第1
回目のホツトプレスを行なつた試料を一旦降温し
てダイス内から取り出したが、互いに直交する2
軸方向から加圧できるホツトプレス装置を用いれ
ば、Z軸方向からの第1回目の加圧に引続き、Y
軸方向からの第2回目の加圧を連続して行なうこ
とができ、これにより、同様の効果が得られるこ
とはいうまでもない。また、本実施例では、第2
図aに示すように試料を円柱状に予備成形した
が、この成形体の形状は直方体あるいは立方体で
あつてもよく、また第1回目の加圧をY軸方向か
ら行ない、第2回目の加圧をZ軸方向から行なつ
ても得られる効果に変りはない。
第2回目のホツトプレス後、取り出された試料
は、第3図aに示すように、円柱が径方向に押し
つぶされた形状をしている。また第3図bに示す
ように、この試料のX軸、Y軸、Z軸に垂直な面
をそれぞれSX、SY、SZとして、各面における粒
子の配向状態を電子顕微鏡で観察した。
まずZ軸からの第1回目のホツトプレスを行な
つた試料のSX面およびSZ面をそれぞれ鏡面研磨
した後、温度1150℃で熱エツチングしてから観察
した結果を第4図a,bに示す。この第4図から
明らかなように、加圧方向に垂直なSZ面では針状
の粒子がランダムに配向している。一方加圧方向
と平行なSX面では、加圧方向に配向した粒子は
見られない。このことから、粒子は加圧方向に垂
直な方向に配向することが理解される。
次に第3図bのように、互いに直交る2方向か
ら2回のホツトプレスを行なつた試料における
SX面、SY面、SZ面の電子顕微鏡写真を第5図a,
b,cに示す。この図から明らかなように、寸法
異方性を有する粒子は、2回のホツトプレスのそ
れぞれの圧力の方向に対して直交するX軸方向に
配向している。
第6図はX線回折パターンを示し、第6図aは
合成した針状粒子粉末、第6図bはSY面、第6図
cはSX面である。第6図aはPbNb2O6がランダ
ムな方向を向いているときの回折パターンであ
り、第6図bでは、第6図aに比較して(h、
k、o)の面指数を持つ回折線の相対強度が強
く、第6図cにおいては、(o、o、l)の面指
数を持つ回折線の相対強度が強く、(h、k、o)
の指数を持つ面からの回折ピークはほとんど観察
されなかつた。
この事実は、針状結晶粒子の長軸方向が一方向
に配向している場合は、結晶学的な結晶軸もまた
特定の一軸方向に配向していることを示してい
る。
次に第7図に示すような板サンプルを切出して
誘電特性および圧電特性を測定した。ここで、試
料()は、SY面に対向する一対の電極を備え、電
極と平行な方向に粒子の長軸が配向している。試
料()は、SX面に対向する一対の電極を備え、電
極と垂直な方向に粒子の長軸が配向している。
測定用サンプルの形状は、厚さ1mm、短辺5
mm、長辺7mmの長方形の角板であり、誘電率は
1kHzにおける静電容量から求めた。圧電諸定数
は、共振、反共振を生じる周波数、およびインピ
ーダンスより求めた。分極処理は、温度110℃に
おいて、厚さ1mm当り2kVの電圧を10分間印加し
て行なつた。測定結果を下記の第1表に示す。な
お、第1表には、比較のために、第1回目のZ軸
の方向からのみのホツトプレスを行なつた試料に
おいて、加圧方向に対し垂直なSZ面に対向する一
対の電極を備えた試料(′)の特性と、加圧方向に
平行なSX面に対向するる一対の電極を備えた試
料(′)の特性とを併せて示してある。
[Technical field to which the invention pertains] The present invention relates to a method for manufacturing ceramics, and in particular, by hot pressing multiple times from different directions, particles having shape anisotropy constituting ceramics are aligned in a uniaxial direction, This invention relates to a method for producing ceramics with good orientation. [Background of the Invention] Some piezoelectric materials inherently have relatively good dielectric properties, piezoelectric properties, and electro-optic effects. One example is a ferroelectric material with a tungsten bronze crystal structure. In this material's crystal system, the crystal grains have large dimensional anisotropy, such as needle shapes, and the direction of easy polarization is Limited. Therefore, even if this material is used in piezoelectric ceramics, the crystal axes of the particles in ceramics are oriented in arbitrary directions, so efficient polarization cannot be performed even when an external electric field is applied. First, it has been impossible to take advantage of the good piezoelectric properties and electro-optical effects inherent to this material. For this reason, research on this crystal system is mainly directed to applied research as a single crystal material. On the other hand, in a ferroelectric material made of a bismuth layered compound, the particles are in the form of a plate. Ceramics that can be polarized can be manufactured, and ceramics that exhibit good piezoelectric properties have been obtained. However, in the above-mentioned material with a tungsten bronze type structure consisting of acicular crystal grains,
If you only use the hot press method with uniaxial pressure,
Since the acicular particles are only randomly oriented within the pressurized surface and it is impossible to align the particles in a specific direction, it has not been possible to obtain one that exhibits good piezoelectric properties. [Object of the Invention] Therefore, an object of the present invention is to provide a manufacturing method for obtaining ceramics in which the particles are uniaxially oriented from a ceramic material made of particles having dimensional anisotropy. [Summary of the Invention] The present invention involves adding a molding binder to a ceramic material made of pre-grown particles with dimensional anisotropy, pre-forming it into a predetermined shape, and hot-rolling the molded body from different directions. The above objective is achieved by applying pressure (hot place). Examples of particles having the above-mentioned dimensional anisotropy include, for example, PbNb 2 O 6 having a tungsten bronze crystal structure formed by a flux method.
Needle-shaped or rod-shaped crystal particles are used. [Embodiments of the Invention] Examples of the present invention will be described in detail below.
Various materials can be considered as materials with crystal grains having dimensional anisotropy, such as needle-like or rod-like shapes. By uniaxially orienting the particles, its excellent dielectric properties,
A ferroelectric material having a tungsten bronze type crystal structure, which is expected to utilize piezoelectric properties and electro-optical properties, will be selected to demonstrate the effectiveness of the present invention. Ferroelectric materials having the above-mentioned tungsten bronze type crystal structure include PbNb 2 O 6 ,
Sr2NaNb5O15 , Sr2KNb5O15 , PbXBa1 - XNb2O6 , _ _
Sr X Ba 1-X Nb 2 O 6 , (Pb, K)Nb 2 O 6 ,
K 3 Li 2 Nb 5 O 15 , Ba 2 NaNb 5 O 15 , Ba 2 LiNb 5 O 15 ,
The main components include K 3 Li 2 Nb 5 -X Ta
An example using PbNb 2 O 6 will be described. First, acicular crystal particles of PbNb 2 O 6 were synthesized using a flux method. All reagents used here are pure
It is a reagent with a high purity of over 99.5%. PbO and Nb2O5
was prepared to have a composition of PbNb 2 O 6 , pre-calcined at a temperature of 900℃ for 2 hours, an equal weight of KCl was added, and the mixture was mixed for 15 minutes in an electric mortar. Approximately 100 grams of the mixture was placed in an alumina crucible. and heated at a temperature of 900° to 1200°C for 1 to 8 hours to react. After the above heat treatment, the mixture was washed by placing it in a 2 liter glass beaker filled with boiling water.
The KCl moiety was removed. At that time, washing was performed using hot water of ion-exchanged water while stirring, and repeated washing was performed by replacing the hot water. After washing by changing the hot water more than 10 times, the obtained PbNb 2 O 6
The Cl - ions remaining at the end of the needle-like particles could not be detected by detection using an AgNO 3 solution. The results of observation of the thus obtained acicular and columnar particles using an electron microscope are shown in FIGS. 1a and 1b. 1st
The particles in Figure a were obtained by heat treatment in a KCl flux at a temperature of 1050°C for 5 hours, and the particles in Figure 1 b
The particles were obtained by heat treatment at a temperature of 1200°C for 5 hours. When the synthesis temperature was lower than 900°C, the development of needle-like particles was poor and only short particles were obtained.
Furthermore, at temperatures exceeding 1200°C, the particles grow thicker and the dimensional anisotropy of the particles decreases, so a heat treatment temperature range of 900° to 1200°C was appropriate for this material. In particular, those synthesized at temperatures between 1000° and 1100°C have a large needle-like ratio (length/thickness or diameter).
It was between 20 and 40. Also, if the synthesis time is too short, the particles will not grow, and if it is too long, the particles will grow too much and become thicker, resulting in an acicular ratio close to 1.
In this example, particles having a length of 2 μm or more, an acicular ratio of 1.2 or more, and a dimensional anisotropy of 100 or less were obtained by heat treatment for 1 to 8 hours. Especially 1050°~1100
The acicular ratio was large for those reacted for 3 to 6 hours within the temperature range, and the diameter was 1.5 to 1.5 for those reacted for 5 hours.
Good acicular particles with a diameter of 2 μm and a large acicular ratio of 20 to 40 were obtained. Next, this powder consisting of acicular particles is poured into ion-exchanged water, and a dispersant is added to fully disperse the powder. After that, large particles and ultrafine particles are removed by sedimentation classification, and the acicular particles are I took out the chisel. The dispersion was filtered and thoroughly washed and dried. This ceramic material made of acicular particles is granulated while adding 8% by weight of 7% by weight PVA solution,
Further, the sized particles are as shown in Figure 2a.
It was preformed into a cylindrical molded body with a diameter of 15 mm and a height of about 20 mm. The two mutually orthogonal directions on the bottom surface of this cylindrical molded body are defined as the X axis and the Y axis, respectively, and the height direction of the cylinder is defined as the Z axis. Next, this molded body was placed in a high-purity alumina die having an inner diameter of 40 mm, and a first hot press (hot pressing) was performed in the vertical direction, that is, in the Z-axis direction. The pressure P1 in this case, the direction of pressure application, and the shape of the sample after hot pressing are shown in FIG. 2b. In this case, the alumina die and the sample were heated at a rate of 150° C./hour, a pressure of 100 Kg/cm 2 was applied at a temperature of 1200° C., and hot pressing was performed for 3 hours. After the first hot press, the temperature is lowered, the sample is taken out, the direction of the sample is changed so that pressure can be applied from the direction perpendicular to the first press, and the sample is placed in the alumina die again. Then, as shown in FIG. 2c, a second hot press was carried out at a pressure P 2 from the direction of the Y axis perpendicular to the Z axis. This second hot pressing was carried out at a temperature of 1250° C. and a pressure of 100 Kg/cm 2 was applied for 3 hours to form the sample into the shape shown in FIG. 2c. Note that since we used a hot press device that can apply pressure only from one axis, the first
The sample that had been hot-pressed for the first time was once cooled down and taken out from the die, but two pieces perpendicular to each other were
If you use a hot press device that can apply pressure from the axial direction, following the first press from the Z-axis direction,
It goes without saying that the second pressurization from the axial direction can be performed successively, and thereby similar effects can be obtained. In addition, in this embodiment, the second
As shown in Figure a, the sample was preformed into a cylindrical shape, but the shape of this molded body may be rectangular or cubic.The first pressurization was performed from the Y-axis direction, and the second pressurization There is no difference in the effect obtained even if the pressure is applied from the Z-axis direction. After the second hot pressing, the sample taken out has a shape in which a cylinder is crushed in the radial direction, as shown in FIG. 3a. In addition, as shown in Figure 3b, the planes perpendicular to the X -axis, Y - axis, and Z - axis of this sample were designated S . First, the S show. As is clear from FIG. 4, the acicular particles are randomly oriented in the SZ plane perpendicular to the pressing direction. On the other hand, in the S X plane parallel to the pressure direction, no particles oriented in the pressure direction are observed. From this, it is understood that the particles are oriented in a direction perpendicular to the direction of pressurization. Next, as shown in Figure 3b, the sample was hot-pressed twice from two directions perpendicular to each other.
Electron micrographs of the S X plane, S Y plane, and S Z plane are shown in Figure 5 a.
Shown in b and c. As is clear from this figure, the particles having dimensional anisotropy are oriented in the X-axis direction perpendicular to the direction of pressure in each of the two hot presses. FIG. 6 shows the X-ray diffraction pattern, FIG. 6a shows the synthesized acicular particle powder, FIG. 6b shows the S Y plane, and FIG. 6c shows the S X plane. Figure 6a shows the diffraction pattern when PbNb 2 O 6 is oriented in a random direction, and Figure 6b shows (h,
In Fig. 6c, the relative intensity of the diffraction line with the plane index of (o, o, l) is strong, and the relative intensity of the diffraction line with the plane index of (h, k, o) is strong. )
Almost no diffraction peaks from planes with indexes were observed. This fact indicates that when the long axis of the acicular crystal grain is oriented in one direction, the crystallographic crystal axis is also oriented in a specific uniaxial direction. Next, a plate sample as shown in FIG. 7 was cut out and its dielectric properties and piezoelectric properties were measured. Here, the sample () includes a pair of electrodes facing the S Y plane, and the long axis of the particles is oriented in a direction parallel to the electrodes. The sample () is equipped with a pair of electrodes facing the S The shape of the sample for measurement is 1 mm thick, short side 5
It is a rectangular square plate with a long side of 7 mm and a dielectric constant of
It was determined from the capacitance at 1kHz. Piezoelectric constants were determined from the frequencies at which resonance and antiresonance occur, and impedance. The polarization treatment was performed at a temperature of 110° C. by applying a voltage of 2 kV per 1 mm of thickness for 10 minutes. The measurement results are shown in Table 1 below. For comparison, Table 1 shows samples that were hot-pressed only from the Z-axis direction for the first time, with a pair of electrodes facing the S Z plane perpendicular to the pressing direction. The characteristics of the sample ('), which was prepared in the same way, and the characteristics of the sample ('), which had a pair of electrodes facing each other in the S
以上の説明で明らかなように、本発明によれ
ば、結晶学的に異方性を有する材料の単結晶を製
作しなくても、単結晶と同様の所望の特性を有す
るセラミツクス材料を製造することができる。
単結晶の育成には材料の融点よりも高い温度を
必要とするが、本発明の方法によれば、焼結温度
で目的とするセラミツクスを得ることができるた
め、加熱源、加熱方法の選択の幅が広く、また、
耐火物、るつぼ等も、より低温で使用できるた
め、より安価で経済的な材料を得ることも可能で
ある。
また本発明によれば、単結晶の育成の困難な材
料でも、比較的容易に焼成でき、異方性を利用す
る材料を提供することが可能となつた。
As is clear from the above description, according to the present invention, a ceramic material having the same desired properties as a single crystal can be produced without producing a single crystal of a material having crystallographic anisotropy. be able to. Growing a single crystal requires a temperature higher than the melting point of the material, but according to the method of the present invention, the desired ceramic can be obtained at the sintering temperature, so the selection of the heating source and heating method can be made easier. It is wide and also
Since refractories, crucibles, etc. can also be used at lower temperatures, it is also possible to obtain cheaper and more economical materials. Further, according to the present invention, even a material whose single crystal is difficult to grow can be fired relatively easily, and it has become possible to provide a material that utilizes anisotropy.
第1図a,bはフラツクス法で合成した
PbNb2O6系粒子の電子顕微鏡写真、第2図a〜
cは本発明の方法における成形体とホツトプレス
の方向との関係を示す説明図、第3図a,bは第
2回目のホツトプレスの方向と電子顕微鏡で観察
した試料の面の方向とを示す説明図、第4図a,
bは第1回目のホツトプレスによる粒子配向状態
を示す電子顕微鏡写真、第5図a〜cは第2回目
のホツトプレスによる粒子配向状態を示す電子顕
微鏡写真、第6図a〜cはX線回折図、第7図は
第2回目のホツトプレスを行なつた試料から切り
出した板状サンプルの方向を示す説明図である。
Figure 1 a and b were synthesized using the flux method.
Electron micrographs of PbNb 2 O 6 -based particles, Figure 2 a~
Fig. 3c is an explanatory diagram showing the relationship between the molded body and the direction of hot pressing in the method of the present invention, and Fig. 3a and b are explanatory diagrams showing the direction of the second hot pressing and the direction of the surface of the sample observed with an electron microscope. Figure 4a,
b is an electron micrograph showing the state of particle orientation obtained by the first hot pressing, FIGS. 5 a to c are electron micrographs showing the state of particle orientation obtained by the second hot pressing, and FIGS. , FIG. 7 is an explanatory diagram showing the direction of a plate-shaped sample cut out from a sample subjected to the second hot pressing.
Claims (1)
なるセラミツクス材料に成形用バインダを加えて
所定の形状に予備成形し、この成形体に対し第1
の方向から第1回目の熱間加圧を行ない、次に前
記第1の方向とは異なるそれに垂直な第2の方向
から第2回目の熱間加圧を行ない、これにより前
記粒子を一軸方向に配向させたセラミツクスを得
ることを特徴とするセラミツクスの製造方法。 2 特許請求の範囲第1項記載のセラミツクスの
製造方法において、前記粒子が結晶粒子および非
結晶粒子の少なくとも一方よりなる前記方法。 3 特許請求の範囲第1項または第2項記載のセ
ラミツクスの製造方法において、前記寸法異方性
を有する粒子が針状および棒状の粒子の少なくと
も一方よりなる前記方法。 4 特許請求の範囲第3項に記載されたセラミツ
クスの製造方法において、前記粒子がフラツクス
法により合成され、かつその針状比が1を越え
100以下の範囲にある前記方法。 5 特許請求の範囲第1項〜第4項のうちの何か
れ1つに記載されたセラミツクスの製造方法にお
いて、前記粒子が異方性結晶構造を有する結晶粒
子よりなる前記方法。 6 特許請求の範囲第5項記載のセラミツクスの
製造方法において、前記セラミツクス材料が圧電
材料よりなる前記方法。 7 特許請求の範囲第5項記載のセラミツクスの
製造方法において、前記セラミツクス材料が強誘
電体材料よりなる前記方法。 8 特許請求の範囲第1項記載のセラミツクスの
製造方法において、前記セラミツクス材料が、タ
ングステンブロンズ型の結晶構造を有する結晶粒
子よりなる前記方法。 9 特許請求の範囲第8項記載のセラミツクスの
製造方法において、前記セラミツクス材料が、 PbNb2O6、(Pb、K)Nb2O6、Sr2NaNb5O15、
Sr2KNb5O15、PbXBa1-XNb2O6、SrXBa1-X
Nb2O6、K3Li2Nb5O15、Ba2NaNb5O15、
Ba2LiNb5O15、K3Li2Nb5-XTaXO15、(Pb、Ba、
La)Nb2O6 のうちの少なくとも1つを含むものである前記方
法。 10 特許請求の範囲第1項〜第9項のうちの何
れか1つに記載されたセラミツクスの製造方法に
おいて、前記第1回目および第2回目の熱間加圧
が連続して行なわれる前記方法。[Scope of Claims] 1. A molding binder is added to a ceramic material made of particles having dimensional anisotropy grown in advance, and the molded body is preformed into a predetermined shape.
A first hot press is carried out in the direction of , and then a second hot press is carried out in a second direction different from the first direction and perpendicular thereto, whereby the particles are uniaxially A method for producing ceramics, characterized by obtaining ceramics oriented in the following manner. 2. The method for manufacturing ceramics according to claim 1, wherein the particles are at least one of crystalline particles and amorphous particles. 3. The method for manufacturing ceramics according to claim 1 or 2, wherein the particles having dimensional anisotropy are at least one of needle-shaped and rod-shaped particles. 4. In the method for manufacturing ceramics as set forth in claim 3, the particles are synthesized by a flux method, and the acicular ratio thereof exceeds 1.
Said method in a range of 100 or less. 5. The method for producing ceramics as set forth in any one of claims 1 to 4, wherein the particles are crystal particles having an anisotropic crystal structure. 6. The method for manufacturing ceramics according to claim 5, wherein the ceramic material is a piezoelectric material. 7. The method for manufacturing ceramics according to claim 5, wherein the ceramic material is made of a ferroelectric material. 8. The method for manufacturing ceramics according to claim 1, wherein the ceramic material comprises crystal grains having a tungsten bronze type crystal structure. 9. In the method for manufacturing ceramics according to claim 8, the ceramic material comprises PbNb 2 O 6 , (Pb,K)Nb 2 O 6 , Sr 2 NaNb 5 O 15 ,
Sr 2 KNb 5 O 15 , Pb X Ba 1-X Nb 2 O 6 , Sr X Ba 1-X
Nb 2 O 6 , K 3 Li 2 Nb 5 O 15 , Ba 2 NaNb 5 O 15 ,
Ba 2 LiNb 5 O 15 , K 3 Li 2 Nb 5-X Ta X O 15 , (Pb, Ba,
La) Nb 2 O 6 . 10. The method for producing ceramics according to any one of claims 1 to 9, wherein the first and second hot pressings are performed consecutively. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59227690A JPS61106463A (en) | 1984-10-31 | 1984-10-31 | Manufacture of ceramics |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59227690A JPS61106463A (en) | 1984-10-31 | 1984-10-31 | Manufacture of ceramics |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61106463A JPS61106463A (en) | 1986-05-24 |
| JPH0132186B2 true JPH0132186B2 (en) | 1989-06-29 |
Family
ID=16864812
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59227690A Granted JPS61106463A (en) | 1984-10-31 | 1984-10-31 | Manufacture of ceramics |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61106463A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2644779A1 (en) * | 1989-03-22 | 1990-09-28 | Centre Nat Rech Scient | CERAMIC COMPOSITION HAVING A HIGH DIELECTRIC CONSTANT |
| US6620237B2 (en) * | 2001-11-15 | 2003-09-16 | Spectra, Inc. | Oriented piezoelectric film |
| CN102863024B (en) * | 2012-10-10 | 2014-02-05 | 西北工业大学 | Preparation method of cylindrical strontium sodium niobate crystallite powder |
-
1984
- 1984-10-31 JP JP59227690A patent/JPS61106463A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61106463A (en) | 1986-05-24 |
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