Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6046556B2 - Manufacturing method of piezoelectric ceramics - Google Patents
[go: Go Back, main page]

JPS6046556B2 - Manufacturing method of piezoelectric ceramics - Google Patents

Manufacturing method of piezoelectric ceramics

Info

Publication number
JPS6046556B2
JPS6046556B2 JP53103023A JP10302378A JPS6046556B2 JP S6046556 B2 JPS6046556 B2 JP S6046556B2 JP 53103023 A JP53103023 A JP 53103023A JP 10302378 A JP10302378 A JP 10302378A JP S6046556 B2 JPS6046556 B2 JP S6046556B2
Authority
JP
Japan
Prior art keywords
thickness
pressure
composition
sintering
piezoelectric ceramics
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP53103023A
Other languages
Japanese (ja)
Other versions
JPS5529166A (en
Inventor
正光 西田
俊一郎 河島
一朗 上田
宏 大内
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP53103023A priority Critical patent/JPS6046556B2/en
Priority to GB7928900A priority patent/GB2028791B/en
Priority to US06/067,681 priority patent/US4226827A/en
Priority to DE19792933978 priority patent/DE2933978A1/en
Publication of JPS5529166A publication Critical patent/JPS5529166A/en
Publication of JPS6046556B2 publication Critical patent/JPS6046556B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Inorganic Insulating Materials (AREA)
  • Compositions Of Oxide Ceramics (AREA)

Description

【発明の詳細な説明】 本発明は圧電磁器材料の製造方法に関するものであり、
厚みたて振動に関するエネルギーとじ込め共振子を構成
することがてき、機械的質係数QMおよび電気機械結合
係数に、、に。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a piezoelectric ceramic material,
An energy confinement resonator for thick vertical vibrations can be constructed, and the mechanical quality factor QM and electromechanical coupling coefficient are...

3が大きく、薄板に加工することのできる高周波共振子
用等に適する圧電磁器材料を提供するものである。
The present invention provides a piezoelectric ceramic material having a large size and suitable for use in high frequency resonators, etc., which can be processed into a thin plate.

テレビジョン受像機などの高周波回路のIC化が進むに
つれて、IC回路の周辺部品、特にリアクタンス回路の
固体化、無調整化、高性能化が強く要望されている。
As the use of ICs in high-frequency circuits such as television receivers progresses, there is a strong demand for peripheral components of IC circuits, especially reactance circuits, to be solid-state, non-adjustable, and high-performance.

圧電磁器共振子はこの要望を満すことのできるものとし
て期待されている。圧電磁器を高周波共振子として用い
る場合、共振周波数が厚さで決まる厚み振動、特に厚み
たて振動を用いるのが有利である。厚みたて振動の周波
数定数は2000H2−m程度であるから、もし50M
H2の共振周波数を得ようとすると、磁器共振子の厚さ
は40μm程度という非常に薄い板に加工しなければな
らない。さらに、厚みたて振動を共振子やフィルタに使
用するときに重要なことは不要共振の除去である。不要
振動の除去には、エネルギーとじ込め法が有効である。
厚みたて振動の基本波共振に、このエネルギーとじ込め
法が適用できる条件としては、(2−Cg。・S牙。)
/(2−2C83・ S〒、)で与えられるポアソン比
σが113より大きいことが必要である。ただし、C崎
よ厚みたて振動に関連した弾性ステイフネス、S牙、は
厚みすベリ振動に関連した弾性コンプライアンスである
。また、高周波領域で低損失の共振子を得よううとする
と、機械的質係数QMが20曜度以上であることが必要
である。従来の焼成法ては機械的に弱い材料しか得られ
ず、200μm程度の厚さまでにしか研摩できないため
に、厚みたて振動によつても約10MH2以上の共振子
を得ることは困難であつた。
Piezoelectric ceramic resonators are expected to be able to meet this demand. When using a piezoelectric ceramic as a high-frequency resonator, it is advantageous to use thickness vibration, particularly thickness vertical vibration, in which the resonant frequency is determined by the thickness. The frequency constant of thickness vibration is about 2000H2-m, so if 50M
In order to obtain the resonant frequency of H2, the magnetic resonator must be processed into a very thin plate with a thickness of about 40 μm. Furthermore, when using thick vertical vibration in a resonator or filter, it is important to remove unnecessary resonance. The energy confinement method is effective for removing unnecessary vibrations.
The conditions under which this energy confinement method can be applied to the fundamental wave resonance of thick vertical vibration are (2-Cg.・S fan.)
It is necessary that Poisson's ratio σ given by /(2-2C83·S〒,) is larger than 113. However, the elastic stiffness related to the vertical vibration, S, is the elastic compliance related to the vertical vibration. Further, in order to obtain a resonator with low loss in a high frequency region, it is necessary that the mechanical quality factor QM is 20 degrees or more. Conventional firing methods yield only mechanically weak materials and can only be polished to a thickness of approximately 200 μm, making it difficult to obtain resonators of approximately 10 MH2 or higher even by thickness vibration. .

さらに、これまではσについての測定例がほとJんどな
く、113以上のσを持つ組成範囲は明らかにされてい
なかつた。
Furthermore, until now there have been very few examples of measurement of σ, and the composition range with σ of 113 or more has not been clarified.

そして、QMが26程度以上でしかもσが113以上で
、200μm以下の薄板に加工できる材料はこれまでに
得られていなかつた。本発明は、113以上のσと20
0景上のQMをも丁ち、30μm程度の薄板にまで加工
することができる結合係数に、の大きな高周波用の圧電
磁器材料を得る方法に関するもので、(1−w)(Pb
Til−z−ZrZO3)+WMnO2(ただし、0.
48≦z≦0.64,0.004≦w≦0.06,Pb
の0〜10原子%(イ)はのぞく)をSr,Ca,Ba
のうちのいずれか一種または一種以上で置換する)の組
成のものを限られた条件で加熱加圧焼結することによつ
て得られをことを見出したことにもとづくものである。
以下、実施例をあげて説明する。PbO,SrCO3,
CaCO3,BaCO3,TiO2,zrO2,MnO
2の原料を下表の組成になるように秤量し、ボールミル
で17時間湿式混合した。
Until now, no material has been obtained that has a QM of about 26 or more, a σ of 113 or more, and can be processed into a thin plate of 200 μm or less. The present invention has a σ of 113 or more and a σ of 20
It concerns a method of obtaining a piezoelectric ceramic material for high frequencies with a large coupling coefficient that can be processed into a thin plate of about 30 μm, including the QM on the zero view, and (1-w) (Pb
Til-z-ZrZO3)+WMnO2 (however, 0.
48≦z≦0.64, 0.004≦w≦0.06, Pb
Sr, Ca, Ba
The present invention is based on the discovery that it can be obtained by heating and pressurizing sintering under limited conditions.
Examples will be described below. PbO, SrCO3,
CaCO3, BaCO3, TiO2, zrO2, MnO
The raw materials No. 2 were weighed to have the composition shown in the table below, and wet mixed in a ball mill for 17 hours.

スラリーを淵過、乾燥させてから、約850℃で2時間
仮焼したのち、再びボールミルで湿式粉砕した。粉砕し
たものを乾燥させたのち、直径30TIrm1厚さ17
圏の円板を圧力500kg/dで成形し、それを下表に
示した条件で加熱加圧焼結した。その後900℃で4時
間焼鈍処理を行なつた。比較のため、同じ条件で作つた
粉体を成形し、普通焼成した。これらの焼成した試料か
ら直径6w0nの円板を切り出し、それを最低30μm
の厚みになるまで研摩した。機械的に弱い試料は30μ
mの厚さになるまでに割れてしまい、所望の薄板素子を
得ることができなかつた。なお、圧電的性質は厚さ0.
3朗の円板試料に金電極を設けて、それを160゜Cの
シリコンオイル中で5KV/?の直流電界を印加した試
料について測定した。K33は5×1×1、TrOlL
3の寸法の棒状試料で測定した。焼成条件と研摩限界と
の関係を第1表に示す。
After the slurry was filtered and dried, it was calcined at about 850° C. for 2 hours, and then wet-pulverized again using a ball mill. After drying the crushed material, diameter 30TIrm1 thickness 17
A circular disk was molded at a pressure of 500 kg/d, and it was sintered under heat and pressure under the conditions shown in the table below. Thereafter, annealing treatment was performed at 900° C. for 4 hours. For comparison, a powder made under the same conditions was molded and fired normally. Cut out a disk with a diameter of 6w0n from these fired samples, and cut it into a size of at least 30μm.
It was polished to a thickness of . 30μ for mechanically weak samples
The thin plate element cracked by the time the thickness reached m, making it impossible to obtain the desired thin plate element. Note that the piezoelectric properties are good at a thickness of 0.
A gold electrode was provided on a 3-ring disk sample, and it was heated to 5KV/? in silicone oil at 160°C. Measurements were made on a sample to which a DC electric field of . K33 is 5×1×1, TrOOL
Measurements were made using a rod-shaped sample with dimensions of 3. Table 1 shows the relationship between firing conditions and polishing limits.

普通焼成では、表の焼成条件で最大の密度の磁器が得ら
れるが、200μm以下の厚さにまで研摩す,ることが
できなかつた。しかし、本発明の加熱加圧焼結によれば
、きわめて薄い磁器素体を得ることがてきる。加熱加圧
焼結の温度が1050〜1300℃の場合に、30μm
まで研摩することができた。焼結時の加圧力が100k
g/dより小さいと焼結不足!で不均一な試料となり、
磁器を200μm以下の厚さにまで研摩することが困難
であつた。圧力が100〜500k9/CTlの範囲で
加熱加圧焼結することにより、30μmの厚さまで研摩
可能な磁器が得られた。加熱時間については、0.時間
以下では焼結くが不均一であり、100μm以下の薄板
に研摩加工するのに耐える材料が得られない。また、2
酌間以上の焼結は、磁器の強度の低下と生産性の低下が
大きくなるため、好ましくない。したがつて、本発明の
方法における加熱加圧焼結の条件の範囲は温度1050
〜1300℃、圧力100〜500k9/C!11時間
0.5〜2@間の範囲である。第1表はPbの一部をS
rで置換した組成物の研摩限界を示すものてあるが、P
bの一部をBaまた゛はCaで置換した組成物でも同様
の結果が得られた。
In normal firing, porcelain with maximum density can be obtained under the firing conditions shown in the table, but it was not possible to polish the porcelain to a thickness of 200 μm or less. However, according to the heat and pressure sintering of the present invention, an extremely thin ceramic body can be obtained. 30μm when the temperature of heating and pressure sintering is 1050 to 1300℃
I was able to polish it up to. Pressure force during sintering is 100k
If it is smaller than g/d, sintering is insufficient! This results in a non-uniform sample.
It was difficult to polish porcelain to a thickness of 200 μm or less. Porcelain that can be polished to a thickness of 30 μm was obtained by heat-pressing sintering at a pressure in the range of 100 to 500 k9/CTl. Regarding heating time, 0. If the sintering time is shorter than that, the sintering will be non-uniform, and a material that can withstand polishing into a thin plate of 100 μm or less cannot be obtained. Also, 2
Sintering at a depth greater than 100 degrees is undesirable because it significantly reduces the strength of the porcelain and the productivity. Therefore, the range of conditions for heating and pressure sintering in the method of the present invention is a temperature of 1050°C.
~1300℃, pressure 100~500k9/C! The range is between 0.5 and 2 for 11 hours. Table 1 shows a part of Pb
There is a table showing the polishing limit of compositions substituted with r, but P
Similar results were obtained with a composition in which part of b was replaced with Ba or Ca.

第1図に1250℃、200kg/Cltl4時間の条
件で加熱加焼した磁器試料(w=0.00&Pbの原子
%をSrで置換した組成)のzに対するσの変化の様子
を示す。
FIG. 1 shows the change in σ with respect to z for a ceramic sample (w=0.00 & composition in which atomic percent of Pb was replaced with Sr) heated and baked under the conditions of 1250° C. and 200 kg/Cltl for 4 hours.

第1図から明らかなように、σはzの値が0.55のと
き最大を示した。この場合のKtとK33はそれぞれ0
.55および、0.70で大きな値を示した。zの変化
によるσの変化の傾向は、wの値、置換する元素の種類
(Sr,BaまたはCa)および加熱加圧条件によつて
はほとんど変わらない。厚みたて振動の基本波のエネル
ギーとじ込め条件、すなわちσ〉113の条件を満たく
範囲はw=0.008でPbの5原子%をSrで置換し
た組成では0.48≦z≦0.64の組成範囲である。
なお、wが0.004〜0.06の楊合およびPbの置
換元素がBaまたはCaの場合にも、上記のzの範囲内
ではσ〉113の条件は満たされた。第2図に温度12
50℃、圧力200kg/Cltで4時間加熱加圧焼結
した試料(z=0.60,Pbの10原子%を?で置換
した組成)のwによるQMの変化を示した。
As is clear from FIG. 1, σ was maximum when the value of z was 0.55. In this case, Kt and K33 are each 0
.. 55 and 0.70 showed large values. The tendency of the change in σ due to the change in z does not change much depending on the value of w, the type of element to be substituted (Sr, Ba or Ca), and the heating and pressurizing conditions. The range that satisfies the energy confinement condition of the fundamental wave of the thickness vertical vibration, that is, the condition of σ>113, is w=0.008, and for a composition in which 5 at.% of Pb is replaced with Sr, 0.48≦z≦0. 64 composition range.
Note that the condition of σ>113 was satisfied within the above range of z also in the case where w was 0.004 to 0.06 and the substituent element for Pb was Ba or Ca. Figure 2 shows temperature 12
The change in QM due to w of a sample (z=0.60, composition in which 10 atomic % of Pb was replaced with ?) which was heated and pressure sintered at 50° C. and a pressure of 200 kg/Clt for 4 hours is shown.

QMはwが0.02のとき最大になる。この傾向は、z
の値、Pbの置換元素の種類(Sr,Ba,またはCa
)および加熱加圧焼結の条件によつては変わらなあ。第
2図によりQMが200以上になるwの範囲は0.00
4〜0.06である。なお、PbのSr,?またはCa
による置換が10原子%を越える組成はKtの低下がい
ちぢるしいため10原子%以下の置換に限定した。
QM is maximum when w is 0.02. This tendency is
value, type of substituting element for Pb (Sr, Ba, or Ca
) and may vary depending on the heating and pressure sintering conditions. According to Figure 2, the range of w where QM is 200 or more is 0.00.
4 to 0.06. In addition, Sr of Pb,? or Ca
In compositions in which substitution exceeds 10 at.%, the decrease in Kt is significant, so the substitution is limited to 10 at.% or less.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明にかかる方法で作られた試料の組成とポ
アソン比σとの関係の一例を示す図、第2図は同じく組
成と機械的質係数QMとの関係の一例を示す図である。
FIG. 1 is a diagram showing an example of the relationship between the composition and Poisson's ratio σ of a sample made by the method according to the present invention, and FIG. 2 is a diagram showing an example of the relationship between the composition and the mechanical quality factor QM. be.

Claims (1)

【特許請求の範囲】 1(1−w)〔PbTi_1_−_zZr_zO_3+
wMnO_2で表わされる組成において、0.48≦z
≦0.64,0.004≦w≦0.006なる範囲内の
組成物(ただし、Pbの0〜10原子%(0はのぞく)
をSr,Ca,Baのうちのいずれか一種または一種以
上で置換する)を温度1050〜1300℃および圧力
100〜500kg/cm^2で0.5〜24時間加熱
加圧焼結することを特徴とする圧電磁器の製造方法。
[Claims] 1 (1-w) [PbTi_1_-_zZr_zO_3+
In the composition represented by wMnO_2, 0.48≦z
Composition within the range of ≦0.64, 0.004≦w≦0.006 (however, 0 to 10 at% of Pb (0 is excluded)
is replaced with one or more of Sr, Ca, and Ba) is heated and pressure sintered at a temperature of 1050 to 1300°C and a pressure of 100 to 500 kg/cm^2 for 0.5 to 24 hours. A method for manufacturing piezoelectric ceramics.
JP53103023A 1978-08-23 1978-08-23 Manufacturing method of piezoelectric ceramics Expired JPS6046556B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP53103023A JPS6046556B2 (en) 1978-08-23 1978-08-23 Manufacturing method of piezoelectric ceramics
GB7928900A GB2028791B (en) 1978-08-23 1979-08-20 Preparing piezoelectric ceramics
US06/067,681 US4226827A (en) 1978-08-23 1979-08-20 Method for preparing piezoelectric ceramics
DE19792933978 DE2933978A1 (en) 1978-08-23 1979-08-22 METHOD FOR PRODUCING PIEZOELECTRIC CERAMICS

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP53103023A JPS6046556B2 (en) 1978-08-23 1978-08-23 Manufacturing method of piezoelectric ceramics

Publications (2)

Publication Number Publication Date
JPS5529166A JPS5529166A (en) 1980-03-01
JPS6046556B2 true JPS6046556B2 (en) 1985-10-16

Family

ID=14343036

Family Applications (1)

Application Number Title Priority Date Filing Date
JP53103023A Expired JPS6046556B2 (en) 1978-08-23 1978-08-23 Manufacturing method of piezoelectric ceramics

Country Status (1)

Country Link
JP (1) JPS6046556B2 (en)

Also Published As

Publication number Publication date
JPS5529166A (en) 1980-03-01

Similar Documents

Publication Publication Date Title
US3068177A (en) Ferroelectric ceramic materials
JP3282576B2 (en) Piezoelectric ceramic composition
US6083415A (en) Piezoelectric ceramic composition
US3006857A (en) Ferroelectric ceramic composition
EP0012583B1 (en) Piezoelectric ceramic production
JPS6046556B2 (en) Manufacturing method of piezoelectric ceramics
JP2884635B2 (en) Piezoelectric ceramics and method of manufacturing the same
JPS6022513B2 (en) piezoelectric porcelain
JPS60136103A (en) Dielectric porcelain composition
JPS6046557B2 (en) Manufacturing method of piezoelectric ceramics
JPS5923048B2 (en) dielectric resonator
US4226827A (en) Method for preparing piezoelectric ceramics
JPH0226794B2 (en)
JP2881424B2 (en) Piezoelectric ceramic
JP2515437B2 (en) Method for manufacturing dielectric porcelain
JP3508244B2 (en) Piezoelectric ceramic composition and method for producing the same
JPS63182255A (en) Piezoelectric ceramic composition
JP4467168B2 (en) Piezoelectric ceramic and piezoelectric element
JPS6132838B2 (en)
JPS5949650B2 (en) Materials for dielectric resonators
JPS628960B2 (en)
JP3125590B2 (en) High frequency dielectric ceramic composition
JPS5943104B2 (en) piezoelectric ceramic material
JPH08133827A (en) Piezoelectric ceramic composition and method for producing the same
JPH0517216A (en) Piezoelectric ceramics