• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    A method for producing piezoelectric ceramics of a Pb(Sn alpha Sb1- alpha )O3-PbTiO3-PbZrO3 system is disclosed which comprises providing a piezoelectric ceramic composition expressed by the general formula: xPb(Sn alpha Sb1- alpha )O3-yPbTiO3- zPbZrO3 wherein subscripts alpha , x and y are mole fractions of the respective components and have the following values, x+y+z= 1.00, 1/4</= alpha </=3/4, said composition falling within a polygonal area defined by points A, B, C, D and E in FIG. 3, forming powder of the composition into forming bodies, and firing the forming bodies in an oxygen atmosphere containing not less than 80 vol % of oxygen. The firing in the oxygen atmosphere is effected at a temperature not less than 1000 DEG C. A part of lead in the composition may be replaced with not more than 20 atomic percent of at least one metal selected from the group consisting of Ba, Ca, Sr and Cd. The composition may contain a small amount of Mn, Mg and/or Cr. Fine dense ceramics with low porosity, small average size and fine grain size are produced which can be applied to various electronic parts.
    公开号:SU1068029A3
    申请号:SU792806600
    申请日:1979-08-16
    公开日:1984-01-15
    发明作者:Огава Тосио
    申请人:Мурата Мануфакчуринг Ко.Лтд (Фирма)；
    IPC主号:
    专利说明:

    at least one compound kAl1; CEC, barium, strontium, cadmium at the rate of substitution up to 20 at,% of lead in the final product,
    3. The method according to p. 1, about tl and h ay u and u with there; that the values of k, i, Z lie in the AF5ri ria polygon of the triple diagram (with the exception of the direct DN); the boundaries of which correspond to the values
    4 The method according to claim 1, about tl and h Fyu C and and so. that green, (,: /, Z in the polygon J / KLG: In the ternary diagram, the patterns of which correspond to the values
    The invention is related to the field of piezotechnics and can be applied in various devices with piezoelectric ceramics, in particular, plt fabrication of light elements, work: on surface acoustical waves
    Of the natural: - manufacturing method and;:. A: and of electrical ceramic materials of the United Nations titanate Baon or lead zirconate titanate according to about 5 hours of environmental technology with isoto; Likewise about / xng in air;: LU; o; 1 atmog bé re 1.
    However, it is not possible in a manner to obtain a sufficiently hilly and impassable ceramics, which impedes it; for use in devices with the use of surface wolf clumps and specimens of small thickness, and Caic;: cG to obtain a base amplitude l g-ud vibration
    The closest to the well-known method of making piezoelectric ceramic material:; and on the basis of the system
    ; pj (, „,) o, ..) 5 -;: Px.-n,,
    where 1/4 i with. 3/4, and the quantities;, h 2 lats in the polygon A BCD BF on the ternary diagram, the boundaries of the horizon correspond to values
    6, Method according to claim: 1; w u and u about tem; what is obhsig a: iisphere of seawater on schnot gzh temiyTc-jv ;;; y; e1 ;; iEani ioodn.lh with ;; a ;; nee Pii:; .vindG; tin .; : ur .. tchtana and zirconia, molding jaroTDEOK and their roasting G2.
    However, such a cut off will allow the piezoelectric material to be of high quality, and the fur is notable for: -;: pores,:
    distance of invention
    The indicated pejib,; io that, according to method:; 1 e .S oel ek; gkkchessk ikT; ; ial: E on axis
      o-t-ix 3 le 1/4 o-i 3/4. rs values x, / lie in a polygon; nickel ABCDE is a rotary diagram — excluding direct 1E), whose boundaries correspond to the values by mixing the starting compounds of lead, tin, antimony, titanium and zirconium, forming blanks and their firing, the initial mixture was additionally introduced with 0.05–5 wt.%, at least one oxide from the group MnO2, MgO, Cr 202, and the roasting was carried out in an oxygen atmosphere with an O2 content of 80% by volume. In this case, it is possible to additionally introduce into the charge at least one compound of calcium, barium, strontium, cadmium, at the rate of replacing neither up to 20% at% of the content of the final product. The values X, v, 2 can also lie in the polygon on the triple diagram E (except for the direct AN), whose boundaries correspond to the values of X, Y, 2 lie in a lot on the triple diagonal boundaries whose boundaries correspond to the values of X, Y, 2 lie in the NBCOLP polygon on a triple diameter, the boundaries of which correspond to the values. Calcination in an oxygen atmosphere begins at a temperature not lower than 1000 s. The composition enclosed in the AFGH polygon is preferably designed for use in high temperature electromechanical converters. Compositions enclosed in a polygon: 7 / KLGM, can preferably be used in resonators of piezoelectric filters, and in a polygon NBCOLP - for elements operating on surface waves. The starting materials are weighed in accordance with the formula ХРЬ {.) Oz-4GT103 - PbZrO, where d. It is in the range of 1 / 4-3 / 4. Additive components (compounds Mn, Mg, Cr) are added to the mixture in the form of oxides, carbonates, hydroxides, oxalates, and other compounds that decompose during heat treatment to form oxides. The mixture is moistened and stirred in a ball mill for at least 10 hours, then calcined at bbO-EOS C, rubbed on wetting with suitable binders, dried, granulated and molded blanks (disks, plates) at a pressure of 700-1000 kg / cm. The billets are calcined at 1100-1350 ° C in an atmosphere containing at least 80% by volume of oxygen. Ceramics of these compositions form an intermediate phase with a pyrochlore type structure of composition Pb2 ni2 Sb2 2; 07-ot, which is located at the grain boundaries in the early stages of burning. This phase exists up to about 1200 ° C, when the formation of the final product occurs, and affects the microstructure and properties of ceramics. Oxygen defects of the pyrochloric phase promote the transfer of oxygen ions to the grain boundaries, which makes it possible to manufacture fine-grained and dense ceramics. At the final stage, the pyrochlore phase goes into the perovskite phase Pb (YAG.Pj) OZ. When roasting in an atmosphere with more than 80% oxygen, the mobility of oxygen ions through oxygen defects of the pyrochloro phase increases dramatically without evaporation of the lead oxide and the agglomeration of the liquid phase. The oxygen content of 95% provides a low-porous material with high mechanical strength. The firing can be carried out in two ways: first, when sintering in an atmosphere with a high oxygen content begins immediately before the appearance of tightly spaced pores, otherwise saying about 1000 ° C, or sintering in an atmosphere with a high concentration of oxygen is carried out at all stages
    2 hours. The calcined material is ground with the corresponding organic binders, dried and granulated to obtain a fine powder. The resulting powder is formed into plates in the form of a square with a side of 50 mm and a thickness of 1.2 mm or in disks with a diameter
    1 / 20,010,980.01
    3 / 40,010,600,39
    3 / 40.01-0,600.39
    2 / 30,010,550,44
    1 / 20.01 0.440.55
    1 / 30,010,400,59
    3 / 40,010,400,59
    1 / 20,010,400,59
    1 / 40,010,400,59
    1 / 20,010,300,69
    3 / 40,010,300,69
    3 / 40,010,040,95
    1 / 30,030,770,20 1 / 40,040,010,95
    3 / 40,050,550,40
    1 / 20,050,550,40
    1 / 40,050,550,40
    1 / 40,050,550,40
    1 / 20,050,350,60
    1 / 20,050,300,65
    1 / 20,050,300,65
    3 / 40,050,100,85
    3 / 40,050,100,85
    22 mm and a thickness of 1.2 mm under a pressure of 1000 kg / cm. Plates and discs are fired using corundum tube furnace, shown in FIG. 1, at 1250s for 2 hours in an oxygen atmosphere. The oxygen concentration in the atmosphere is given in Table. one.
     Table 1
    Continued table. one
    5.0
    2.0
    100 90
    - - 1,0
    85
    0.1 0.1 100
    L, 5 1.5
    90
    O, 7 100 1 O O 100
    90
    95
    Continued table. one
    il3 nOJiyxfeilHCJ
    y g: luzozlekt} obyat rozoyagch H; v; e radia, pg, H (i have a kolpba; /; way of J telling on asryc
    BOJTHax o III oiOB Jitttiyie to s mode p; evil (m1el | her;
    , cs
    marshalling;
    about and
    , i;, KCK SI (-, b:; {en i; yyrpinm:;: i3jftreh; name T ;;; LPO}.; (and;: l-icc: Jl spy;: ;;;; G: (: adj} ke11: eat. i4; f; i i о;; .1 з j 11 к т р} i, О to V / mm,;
     TzpOV: - ;; l; j (GGOTYPOG Oh, fire
    ; T; og: og; . l / n-i-ovi, and. bridge i; coefficient: electromechanical bond (Kr); ff; -; tsig: nta mechanical dobrokl-. : ip:
    fluctuations in tol3 flow. It is kept in pebn ibUC for the first: tsmkmichesky aging, then - (electrofusion coefficient: ko;;;; eZi K,; k fvexaHH4ecKyic jTHoci-b (Od,)) After this re: op-c again / They are placed in a furnace under conditions to conduct thermal aging, i determine 1frame: nt nt electric; anic linkage (K) a new starek is carried out; Tiie ;; iio after copying for 11Cn and g; bezozozlektricheskie Yuetsmu results of the JO;: oole second cycle of the terrestrial ronk, display the characteristics of the:; ork, aging signal of the acoustical wave , M podereni: sozffitsienta kicheskoy communication on poverhsticheskkh waves (K) th coefficient ientral - .. / - - 1 /
    , e J5 with 1-,; and the surface spacing (L) Impea:. I: -i) comb eE, Lo: with: richeokuyu: 1 permeability:; ; - resonators, working at -1 me radial expansion, U1ats; rop, the work of those with a mode of thickness - measured with: 10 ohmcGly 1 -10ot. OddsvjiGi / rom €: hanicheoko sz zi,. and: spe1; r; -tion 1t of mechanical :: .- 1: ... p - -.) is measured with .and: -; тг-; |;,::; р (mercury scheme ;,
    112
    2 Loss I | 1pri races. simple scientific research institute,
    1DB / CM 351518 31.9 30.3 5.0 506 361885 30.7 30.3 1.3 777 18.7 +40 495 33 20.18 25.4 25.0 1.6 916 17.2 +21
    19.25,4132016.6 -25 477 113 0.6
     --- 8.9 -75 250 239 0.4
    - -.
    - - 11., з -70 217 275 0.5
    26.85,0101 26,45,4705
    28,11,4724 28,81,0741
    28,41,41359 17.6 +15 426 46 0.3
    19.65.31664 16.5 +41 410 153 0.5 19.44.91703 15,, 3 +10 402 161 0.4 - - 15.4 -65 301 218 0.6 - - 15.3 - 58,297,225 0.3
    - -
    - -.-.
    18.95., 5653 35.64.8 80
    32,36,1536
    34,51,4102 32,44,7174
    4.56.3976 16.0 +32 378 175 0.4
    Continued table. 2 579 105 0.5 566 108 0.6
    | (hdpri pacI I simple I ipaHei I cues, i dB. / CM 905 26 1318 21.1 20.9 0.9 894 25 1523 21.0 20.8 1.0 1753 3 133 - - 512 27 2558 20.6 19.6 4.9 437192019-45962573 -28410108-- 66310 40112125-67292 534252108-4.84.5 6.3 68 40324 19565.05.0 0, 37513328-- 71 303 2448593-- 3079118-- 2947294-- 2156618-- 2736128-- 2445466-- 2355248 The composition of ceramics goes beyond the limits of volume
    The electromechanical coupling coefficient for acoustic surface waves (Kdduu) is obtained from the following equation:
    (V2- V,) / - /, 1-1 + (1/2 ()
    where the velocity of the acoustic surface wave, if there is no metal layer in the propagation path; V2 is the velocity of the acoustic surface of the wave if a metal layer is provided along the propagation path.
    tf
    Continued table. 2
    The temperature coefficient of the center frequency is obtained from the following equation:
    51 10V ° C,
      max, 5AW
    f
    20 ° C
    f 20 s - central frequency
    with 2 oc;
    - maximum value
    center frequency mav when temperature changes from to
    + 8 ° C; 00 34 18 -15.0 -42 543 121 0.5 -9.9 -75 566 110 0.6 64 28 of the present invention
    mimimal value of the center frequency at HSMGbietiMH tempera, Cr
    tours from -20 C to
    80;
    The losses due to propagation in filtrac on acoustic surface wolves are determined as follows. Acoustic surface waves with a central frequency of 10 i-ir (as shown in Fig. 3) are prepared using these plates of piezoelectric ceramics by providing comb electrodes.
    T
    T,
    on a surface
    -1 2 plates, g i. .ji j -i
    T electrodes
    comb electrode us from
    and e. (p, p.,
    distance (size
    electrodes decree; in fig 5) „
    Losses when calculated from

    V DG) / C
    during the propagation of acoustic surface waves from a converter electrode T
    to converting elg dam T2 and Tj appropriately.
    From Tables 1 and 2, it can be seen that piezoelectric ceramics are obtained on the basis of the system} -b (Yap ..,: L ,, / (i, -p; less than 25%, and with hermetic aging the rate of change K is small,
    Piezoelectric ceramics are composed of small spherical ones with the same size; At that time, cannon ceramics of the ororp being compared; -; ca was made up of large, differently sized grains. This is proved by the h - :: o formation of the intermediate phase, i.e. pyrochlore phase with oxygen defon: the volume that occurs in the system Pb: g; ,,,:: i /, ,, - The pyrochloride phase with an oxygen defect, is irritated
    by the formula b2ivjo /: 1) 2..1 (, / 7-0 / - formed at the early vvr; -firing at the grain boundaries, and there is a flesh of about 12 eO:;: in solid solids, At: ITOM o; ia limits grain growth, pore agglomeration does not occur, such as: -; oxygen contributes to the mobility of gaseous oxygen at grain boundaries. 1a ap. 1;
    Thus, it is possible to create fine-grained and dense piezoelectric ceramics with a small pore size and low porosity, which has high mechanical strength, due to its
    :
    three :
    1Q
    : t in
    for use in elements on acoustic surface waves. The reason for the lack of experimental data in a number of columns is that the composition is not intended for use in these areas.
    Example 2. This example is provided as an explanation of the properties of piezoelectric ceramics intended for use in acoustic surface wave filters. In the example, the composition is 7, 90 (6 0.02) 528 7.86 (J 0.01) 477 7.75 (i 0.03) 282 7.87 (6 0.02) 519 7.84 (6 0, 01) 394 7.73 (6 0.04) 212 7.85 (d 0.03) 427 7.85 ((e 0.01) 456 7.73 Y 0.02) 271 (air 1 7.86 (6 0.02; 27-3 Hot pressing 7.85 (6 0.01) 366 34-1 90 7.75 (6 0.03.) 243 34-2 20 (BLOG: 7.85 (6 0.02 ) 375 34-3 Hot pressor 7.90 (C; 0.01) 400 18-1 100 7.79 (6 0.02) 236 18-2 20 (second
    you, corresponding to the compositions of samples 19 and 31 in example 1. The control samples are prepared as in example 1, except that they change the oxygen concentration (shown in Table 3).
    For comparison, compression is made on samples of the same compositions as these samples. Hot pressing was carried out at 350 kg / cm for 2 hours at 1200 ° C.
    Physical and mechanical properties of the samples are presented in table. 3
    Table 3 1518 1355 672 1437 1058 563 1197 1125 -3 683 GZ
    2
    2 1
    8-15 8-15
    12
    Surround; density ceramics are determined by the metsdom gi; g1rcm: tatlchesx; weighed using polished specimens with: a thin layer of wax, their norpyiKasoa in papna c); chiCIM hexachlor-1-3 -:; bu. aiineiiObi inn 1,6829 // c-i- 1-РИ 20:;:; , ilp ved s tobp, 3 results and yugs of the average z.gkchjiuoi-, measurement pl, every o6pari.a, B tabl ,, -5р; к: до;: г) also. ;; other view on: en; 1о ; - y,
     and
    Ra, Yag.: Er TKKJ (H pi ;;; 6jHnyr iron oi, the irrelevant common e; u; t; (.) By the name of the group with IC1: ol :; ;; a :: i:; -ECN: 1; ol: rovp;: Samples, ;; i.; -:: m vopoa to Ramica outrkdol l ;;. RR: r- (Mo:; Ui pa roseo electrO |; o: T; micrcsslola: noJlb30Ba - uiOM; a :;; p: glian pfioa;; under 13;: p1nut; x ;; golne.; uni mri J2C (V l 1 a-M () sfs; p ((l-l-i-l-g lead JliH l ;: J L L SLR-iH: l: Gllg ug, tee to lasGlll l loi d (l (; og L -; -. 1l-tl ::. I7. Lyut taordosl, il Znkhlsk: l . (iU /,); KoTOj-) yL :, f; al gl-lgy7; a; from c 1ll: l ura7P1eni
    JiiJO-ii ocT ;; ka 5-; ziib oprs; prr; yHKi) Upcaj; bKoic; i i-ioro device and three KOiKT, raztso; 5-30 thickness O; 5zerek opredo.
    1LL Laura - Vl Uto spherical,
    P G; and g-1 with p 3. 3TfjT example with: Lu1L): DL with-bieni properties of piezoelectric Dllgeel-yyyy ceramics for ceramics; -1-al vibration fopof. 1c; 1 favor: from the following: v; , solo constructions for compositions: li n; 5, 2 / - and 34, Test images; slug as described in example 2. Kon:) oxygen oxygen is 3, (.; oagl ss 25 and 34) for use in question l 1 sllerally - x ceramics vibration jC: MHaH chlotnes-hardness L) l ka bend, lgll: cl 3cpL- :: rystalla and average pa ::; lar or glr. 2 ,. lll.l-; al 1; g) uds abl. 3
    ;,;,;; L МИ О О Л Л Л Л РО РО РО РО
     ,;, - llllllg.: K: samples 21-1 and 27-2 g: one lm l l l lg-) to the existing pressure: .L1 KOje6aH: ift 0.01 s, PX (:: All lladikitsu poglcadi zlkril; lsl s; ldll varies from 3 to; LL ir. For each of the values of s: l (lgl moz kol mo; dnosli use: 1 zl;: l- o lll; o; l Colilestio: ;;; l ll ; .amil ((zibrato; eov gufed; sllgro L; Hijf about 34-l and 34-2: 1:: lllllg aiov orllygikyu on thermal ullit. -oiiiKM way. In vnenie 20 min
    2c. In the test using 36 samples.
    From FIG. 5 and 6 it can be seen that the firing process at a high oxygen concentration provides for obtaining vibrators designed to operate at elevated temperatures with high-rise resistance to thermal shocks,
    Example 4 "This Example 1 is provided as an explanation of the properties of piezoelectric ceramics for use in ceramic filters.
    The samples are prepared, their composition corresponds to the composition of samples 18 and 28, the method of manufacturing according to example 2. The oxygen concentration for each sample is given in Table 3. The composition of sample 18 is suitable for use in filters with a longitudinal type of vibration, the composition of sample 28 is for filters with variations in thickness. Control samples were prepared by the hot pressing method of Example 2.
    Bulk density, Vickers hardness, bending strength, grain size and average ceramic size are determined in Example 2. The results are presented in Table. 3
    In tab. 3 for comparison, the results of testing a dna N2
    but
    ig.2
    g
    The cores made from the composition of 0.48 РЬТ10з-0.52 РъггОз + 0.5 wt.% АХ OC + 0, 5 wt.% SiO of the known technology. The control samples for comparison of R-1 and R-2 are prepared by roasting in an acidic atmosphere, the oxygen concentration is given in Table. 3, and samples P, -1) were prepared by hot pressing under the specified conditions.
    Given in Table. 3, Vickers hardness data, flexural strength, grain size and average pore size are average values for ten measurements.
    From tab. 3 that it is possible to obtain piezoelectric ceramics with low porosity, small average pore size and fine grains in comparison with ceramics obtained by hot pressing. In addition, the obtained ceramics have Vickers hardness and high bending strength in comparison with the samples obtained by hot pressing.
    Although there is a likelihood of contamination by impurities such as AlgO, Si02, etc., contained in the raw materials or materials used to create the lead atmosphere, such impurities are permissible.
    gPbTiO,
    5i) ljWOO
    f (-f 0 / KSHHfffl :: // iP / ff / 7p (- // TSCffyfl 2-7, /,;
    FIG. 6
    权利要求:
    Claims (4)
    [1]
    1. METHOD FOR PRODUCING A PIEZOELECTRIC CERAMIC MATERIAL on the basis of the system x Pc (G)) 0 3 - | -J ri 0 3 - ζ o7.go e , where 1/4 4 r G 3/4, and the quantities x, y, ζ lie in the ABCDE polygon on the ternary diagram (except for the straight line AB), whose boundaries correspond to the values
    X At ζ A 0.01 0.9 9 0.00 AT 0.01 0.04 0.95 from 0.04 0.01 0.95 D 0.40 0.01 0.59 E 0.40 0.60 0.00
    by mixing the starting compounds of lead, tin, antimony, titanium and zirconium, forming blanks and firing them, characterized in that, in order to improve the quality of products, an additional 0.05-5 wt.% is added to the initial charge, at least one oxide from the group Mn0 2 , m k 0, Cr, and firing is carried out in an oxygen atmosphere with an O 2 content of 80 vol%.
    s shshyishi y ./
    5 Fig. 1
    SU ,,, 1068029
    [2]
    2. The method according to π. 1, with the fact that the charge is additionally introduced at least one compound'calcium, barium, strontium, cadmium from the calculation note .....
    niya up to 20 at,% lead in the final product,
    [3]
    3, The method of π. 1, it follows from the fact that the quantities k, h, ζ lie in the polygon AFQH On the ternary diagram (except for the straight line AN), the boundaries of which correspond to the values
    X 3 2 BUT 0.01 0/9 9 0.00 F 0, 01 0.40 0.59 (; 0, 2 -5 0.50 0.25 N 0. 3 5 0.65 0, 00
    [4]
    4, The method of claim of
    one ,
    0, 010, 01 0, 0 ' 6 0thirty 0Q 39690; fifteenABOUT 2 About 0 , 60. from Gg . . . L1 - -H. ... j ! j '; · /.· about (,, 2 50, - fifty 0 25 well 0.150 6 0 0 , 2 5 5 " Way Yu n tone about t l and h a- U ill about 2th with l by - what are the quantities l at Z lie in a lot Golyiken & COlP I sk triple chart , the borders of which horn FROM; sort of veto TV at yut '/ beginnings
    I made it clear that the quantities y, .ζ lie in the polygon h / CGSM in the ternary diagram, whose boundaries correspond to the value2
    ϋ :. 01 0 44 0.55 0 01 0 , C t 0, 9 5 at s; C 4 ϋ , ϋ Λ 0.95 0 ;2 5 0 01 0-, 7 4 0 25 from0.50 0 . fifteen about , f - - 0.50 6. Cn os ;about by and: 1. about l and h and th 0 I am by - what obheig in at-
    oxygen sphere begin at a temperature not lower than 1С00 с С.
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    同族专利:
    公开号 | 公开日
    US4255272A|1981-03-10|
    DE2932870C2|1989-01-19|
    NL7906251A|1980-02-19|
    NL186935B|1990-11-01|
    JPS5939913B2|1984-09-27|
    DE2932870A1|1980-02-28|
    NL186935C|1991-04-02|
    JPS5527672A|1980-02-27|
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    申请号 | 申请日 | 专利标题
    JP53101212A|JPS5939913B2|1978-08-17|1978-08-17|
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