JPH0582340B2 - - Google Patents
Info
- Publication number
- JPH0582340B2 JPH0582340B2 JP1120328A JP12032889A JPH0582340B2 JP H0582340 B2 JPH0582340 B2 JP H0582340B2 JP 1120328 A JP1120328 A JP 1120328A JP 12032889 A JP12032889 A JP 12032889A JP H0582340 B2 JPH0582340 B2 JP H0582340B2
- Authority
- JP
- Japan
- Prior art keywords
- displacement
- voltage
- present
- hysteresis
- electrostrictive
- 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 - Lifetime
Links
- 239000000463 material Substances 0.000 claims description 22
- 239000000203 mixture Substances 0.000 claims description 13
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims 2
- 229910052681 coesite Inorganic materials 0.000 claims 1
- 229910052906 cristobalite Inorganic materials 0.000 claims 1
- 239000000377 silicon dioxide Substances 0.000 claims 1
- 235000012239 silicon dioxide Nutrition 0.000 claims 1
- 229910052682 stishovite Inorganic materials 0.000 claims 1
- 229910052905 tridymite Inorganic materials 0.000 claims 1
- 238000006073 displacement reaction Methods 0.000 description 55
- 230000000694 effects Effects 0.000 description 8
- 229910004298 SiO 2 Inorganic materials 0.000 description 5
- 239000000919 ceramic Substances 0.000 description 4
- 239000002184 metal Substances 0.000 description 3
- 229910010293 ceramic material Inorganic materials 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000005498 polishing Methods 0.000 description 2
- 229910010413 TiO 2 Inorganic materials 0.000 description 1
- 230000005856 abnormality Effects 0.000 description 1
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 238000007731 hot pressing Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000010298 pulverizing process Methods 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
- 239000013585 weight reducing agent Substances 0.000 description 1
Landscapes
- Compositions Of Oxide Ceramics (AREA)
Description
[産業上の利用分野]
本発明は緩和型強誘電体を主成分とする電歪素
子材料に関し、更に詳しくは電圧印加により、大
きい機械的変位が発生すると共に電圧−変位ヒス
テリシスが小さく、高精度制御を必要とし、且つ
高信頼性の電圧駆動型変位素子に好適な電歪素子
材料に関する。
[従来の技術]
従来より、電磁方式に代わる新方式の駆動源と
して、例えば、圧電磁器等の電気歪効果を利用
し、電気的エネルギーを機械的エネルギーに変換
する機能素子、いわゆる電圧駆動型変位素子(以
下変位素子と称する)の実用化が微小位置制御機
器等多岐に渡つて進められてきている。更に最近
に至つては機械的変位が大きい事は勿論の事、高
精度制御、小型・軽量化、更に高信頼性の要求が
増々高まつてきている。
この種の変位素子は、例えば、第3図に示す如
く、金属製弾性板1に両面から挟む様に、電極を
付与した圧電磁器板3,3′を接着剤等を用いて
貼り合わせたバイモルフ構造を成すものが知られ
ている。
この変位素子に直流或は交流電圧を印加する
と、電気歪効果(この場合、圧電横効果)に伴な
う機械的変位dS1或はdS2が生じる。
この機械的変位は用途或は搭載される際の機構
にもよるが一般的に変位素子としての機能上でき
るだけ大きい事が望ましく、従つて、例えばPb
(Ni1/3Nb2/3)O3−PbZrO2−PbTiO3系で代表さ
れる様に、比較的圧電定数d31の大きい組成物の
方が有利とされている。
しかしながら、この種の圧電磁器の場合、機械
的変位が大きいとしても電圧−変位ヒステリシス
が大きく、例えば高精度に位置制御する上で、必
ずしも満足できるもとではない。又低ヒシテリシ
スを重視すると材料組成上機械的変位量の低下は
さけられない。
この様な上記圧電磁器材料の欠点を補なう新し
い素材としてペロブスカイト構造を有し、緩和型
強誘電体を主成分とする電歪素子材料が知られて
いる。
この種の材料は、例えば、Pb(Mg1/3Nb2/3)O3
−PbTiO3系組成物から成り室温近傍にキユリー
温度を持ち、通常常誘電相を利用するもので圧電
磁器材料との比較に於いて電界−電気歪ヒステリ
シスが比較的小さい事、分極処理が不要である事
等が主たる特徴の1つとされている。
[発明が解決しようとする課題]
しかしながら、上記電歪素子材料に於いては、
高精度な位置制御が可能である反面、変位素子と
しての機能上、機械的変位が必ずしも十分とは言
えず利用範囲が限定され、又大きな機械的変位を
有する材料はヒツテリシスも大きくなり具合が悪
い。
本発明者等は、かかる上記電歪素子材料の欠点
を解消すべく、種々検討を重ねた結果、機械的変
位が大きく、且つ低ヒステリシスの特徴を有する
Pb(Mg1/3Nb2/3)O3−Pb(Co1/2Nb1/2)O3−
PbTiO3系新組成物を実現している(特願昭61−
13013号)。
そこで、本発明の技術的課題は、更に改良を加
えたもので上記特徴を維持しつつ絶縁耐力が大き
く、従つて、印加する電圧が広範囲に選択できる
ため、機械的変位が広範囲に選択でき、且つ高信
頼性を有し、より幅広い用途に応用でき得る電歪
素子材料の提供をすることにある。
[課題を解決するための手段]
すなわち、本発明の電歪素子素材は、
一般式
Pb[(Mg1/3Nb2/3)A(Co1/2Nb1/2)BTic]O3で示
され
(但しA+B+C=1)0.700≦A≦0.890、
0.010≦B2≦0.150、0.10≦C≦0.15を満足する基
本組成に対し、副成分としてSb2O3、CaOから選
ばれた少くとも1種を0.01〜0.3重量%及びSiO2
を0.005〜0.1重量%添加含有してなることを特徴
とする。
尚、0.700>A、A>0.890、B>0.150、C>
0.15及び副成分Sb2O3、CaOから選ばれた1種が
0.3重量%より多く、又SiO2が0.1重量%より多く
添加含有して成る組成物のものでは機械的変位の
低下、電圧−変位ヒステリシスの増大を招き目的
とする変位素子としては好ましくない。又、B<
0.010、C<0.100の組成物では機械的変位電圧−
変位ヒステリシスの大幅な改善効果が認められ
ず、副成分Sb2O3、CaOから選ばれた少なくとも
1種が0.01重量%未満、SiO2が0.005重量%未満
の組成物のものでは絶縁耐力の大幅な改善か認め
られないため本発明の範囲から除外した。
[実施例]
以下本発明の実施例について、参考例と比較し
ながら詳細に説明する。
出発原料としてPbO、TiO2、MgO、Nb2O5、
Co2O3、Sb2O3、CaCO3、SiO2を選定し、第1表
〜第4表に示す組成になる様に精秤した。
次に、これら原料をボールミルで混合した後、
乾燥し700〜850℃で仮焼成した。次いでボールミ
ルによつて粉砕して得られた粉末に有機バインダ
を適量加えて造粒した後、1ton/cm2の圧力で加圧
成形し1150〜1250℃の温度で数時間焼成した。
(尚、この際必要に応じてホツトプレス処理を施
した。得られた焼結体を所定の形状に切断、研磨
した後電極を付与し所定の測定方法により電歪諸
定数を求めた後実質的な効果を確認するために、
更に研磨、加工を施して長さ35mm、幅10mm、厚さ
0.14mmの矩形状電歪素子を得た。この電歪素子
2,2′を金属製弾性板1に両面からサンドイツ
チして貼り合わせてバイモルフ型変位素子を作製
し第1図に示す様にリード端子を取り出し結線し
た。
この様にして得られた変位素子についてヒステ
リシス、機械的変位を調べた後絶縁耐力を調べる
べく最大印加電圧を測定した。
尚、ヒステリシスは変位素子に100Vの直流電
圧を印加した時の一端固定、他端自由状態での先
端に発生する機械的変位(第2図に於いてdS100
に相当する変位)と、電圧を0に戻した際に生じ
ている残留変位(第2図に於いてdS0に相当する
変位)から次式より算出して求めた。
ヒステリシス=(dS0/dS100)×100[%]
機械的変位は60Vの直流電圧を印加した時の自
由端変位(第2図に於いてdS60)で求めた。
又最大印加電圧は変位素子に直流電圧を20V単
位で増加しながら印加して行き、変位素子が電気
的破壊に至る値、或は変位特性に異常が認められ
た時の値で求めた。尚、最大印加電圧は変位素子
の厚みを1mmにした場合の値に換算して求めた。
第1表〜第4票に結果の一例を示す。
尚、第1表〜第4表に於いて、*印の試料番号
は本発明の電歪素子材料に該当する。
第1表〜第4表からも明らかな様に、本発明の
電歪素子材料から成る試料は参考例と比較して、
機械的変位、ヒステリシス及び最大印加電圧のい
ずれも良好であり、変位素子として好都合な特性
を有している事は明白である。
この様に、本発明によれば、Pb(Mg1/3Nb2/3)
O3−PbTiO3系に、Pb−(Co1/2Nb1/2)O3成分を
固溶せしめたPb[(Mg1/3Nb2/3)A(Co1/2Nb1/2)B
TiOc]O3組成物のA、B、C各成分を適度な範
囲に設定し、且つ好適な副成分を適量添加せしめ
る事により、多きな機械的変位と共に低ヒステリ
シス特性を有し、更に絶縁耐力が大きく、高信頼
性の電歪素子材料を実現したものである。
尚、実施例では示さなかつたが、本実施例の基
本組成に副成分として、Sb2O3、CaOの2種を合
わせて、0.01〜0.3重量%、SiO2を0.005〜0.1重量
%添加した場合においても、本実施例と同様な効
果が得られることは明らかである。
[Industrial Application Field] The present invention relates to an electrostrictive element material whose main component is a relaxation type ferroelectric material, and more specifically, the present invention relates to an electrostrictive element material that has a relaxation type ferroelectric material as its main component, and more specifically, it is capable of generating a large mechanical displacement upon voltage application, has a small voltage-displacement hysteresis, and has high precision. The present invention relates to an electrostrictive element material suitable for voltage-driven displacement elements that require control and have high reliability. [Prior Art] Conventionally, as a new type of drive source to replace the electromagnetic type, for example, a so-called voltage-driven displacement device, which is a functional element that converts electrical energy into mechanical energy by utilizing the electrostriction effect of piezoelectric ceramics, etc. 2. Description of the Related Art Practical use of elements (hereinafter referred to as displacement elements) has been progressing in a wide variety of applications such as minute position control equipment. Furthermore, in recent years, there has been an increasing demand for not only large mechanical displacements but also high-precision control, compactness and weight reduction, and high reliability. For example, as shown in FIG. 3, this type of displacement element is a bimorph structure in which piezoelectric ceramic plates 3 and 3' provided with electrodes are bonded together using an adhesive or the like so as to be sandwiched from both sides by a metal elastic plate 1. The structure is known. When a DC or AC voltage is applied to this displacement element, a mechanical displacement dS 1 or dS 2 occurs due to an electrostrictive effect (in this case, a piezoelectric transverse effect). Although this mechanical displacement depends on the application and the mechanism used when mounting it, it is generally desirable that it be as large as possible in terms of its function as a displacement element.
It is said that a composition having a relatively large piezoelectric constant d 31 is advantageous, as represented by the (Ni 1/3 Nb 2/3 )O 3 -PbZrO 2 -PbTiO 3 system. However, in the case of this type of piezoelectric ceramic, even if the mechanical displacement is large, the voltage-displacement hysteresis is large, and this is not necessarily satisfactory for, for example, highly accurate position control. Furthermore, if low hysteresis is emphasized, a decrease in mechanical displacement cannot be avoided due to the material composition. As a new material that compensates for the drawbacks of the piezoelectric ceramic materials described above, an electrostrictive element material having a perovskite structure and containing a relaxation type ferroelectric material as a main component is known. Materials of this kind are, for example, Pb(Mg 1/3 Nb 2/3 )O 3
- It is made of a PbTiO 3 -based composition, has a Curie temperature near room temperature, and normally uses a paraelectric phase, and has a relatively small electric field-electrostrictive hysteresis compared to piezoelectric ceramic materials, and does not require polarization treatment. Certain things are said to be one of its main characteristics. [Problem to be solved by the invention] However, in the above electrostrictive element material,
Although highly accurate position control is possible, due to its function as a displacement element, the mechanical displacement is not necessarily sufficient and the range of use is limited, and materials with large mechanical displacement also have large hysteresis and are unsuitable. . In order to eliminate the drawbacks of the above-mentioned electrostrictive element material, the present inventors have made various studies and found that it has the characteristics of large mechanical displacement and low hysteresis.
Pb(Mg 1/3 Nb 2/3 )O 3 −Pb(Co 1/2 Nb 1/2 )O 3 −
A new PbTiO 3 -based composition has been realized (patent application 1986-
No. 13013). Therefore, the technical problem of the present invention is to further improve the dielectric strength while maintaining the above-mentioned characteristics, so that the applied voltage can be selected over a wide range, so that the mechanical displacement can be selected over a wide range. Another object of the present invention is to provide an electrostrictive element material that has high reliability and can be applied to a wider range of uses. [Means for Solving the Problems] That is, the electrostrictive element material of the present invention has the general formula Pb[(Mg 1/3 Nb 2/3 ) A (Co 1/2 Nb 1/2 ) B Ti c ]O 3 (however, A+B+C=1) 0.700≦A≦0.890,
With respect to the basic composition satisfying 0.010≦B 2 ≦0.150 and 0.10≦C≦0.15, 0.01 to 0.3% by weight of at least one selected from Sb 2 O 3 and CaO and SiO 2 are added as subcomponents.
It is characterized by containing 0.005 to 0.1% by weight of. In addition, 0.700>A, A>0.890, B>0.150, C>
0.15 and one selected from subcomponents Sb 2 O 3 and CaO.
Compositions containing more than 0.3% by weight or more than 0.1% by weight of SiO 2 result in a decrease in mechanical displacement and an increase in voltage-displacement hysteresis, making them undesirable as intended displacement elements. Also, B<
0.010, for compositions with C<0.100 the mechanical displacement voltage -
No significant improvement effect on displacement hysteresis was observed, and dielectric strength significantly improved in compositions containing less than 0.01% by weight of at least one selected from subcomponents Sb 2 O 3 and CaO and less than 0.005% by weight of SiO 2 . Since no significant improvement was observed, it was excluded from the scope of the present invention. [Example] Examples of the present invention will be described in detail below while comparing with reference examples. PbO, TiO 2 , MgO, Nb 2 O 5 as starting materials,
Co 2 O 3 , Sb 2 O 3 , CaCO 3 and SiO 2 were selected and accurately weighed to give the compositions shown in Tables 1 to 4. Next, after mixing these raw materials in a ball mill,
It was dried and calcined at 700-850°C. Next, an appropriate amount of an organic binder was added to the powder obtained by pulverization using a ball mill, and the mixture was granulated, followed by pressure molding at a pressure of 1 ton/cm 2 and firing at a temperature of 1150 to 1250° C. for several hours.
(In addition, at this time, hot pressing treatment was performed as necessary. After cutting the obtained sintered body into a predetermined shape and polishing it, electrodes were applied and various electrostrictive constants were determined by a predetermined measurement method. In order to confirm the effect,
Further polishing and processing make it 35mm long, 10mm wide, and thick.
A rectangular electrostrictive element of 0.14 mm was obtained. The electrostrictive elements 2, 2' were bonded to the metal elastic plate 1 by sandwiching them from both sides to produce a bimorph type displacement element, and the lead terminals were taken out and wired as shown in FIG. After examining the hysteresis and mechanical displacement of the displacement element thus obtained, the maximum applied voltage was measured to examine the dielectric strength. In addition, hysteresis is the mechanical displacement that occurs at the tip when one end is fixed and the other end is free when a 100V DC voltage is applied to the displacement element (dS 100 in Figure 2).
It was calculated from the following equation from the residual displacement (the displacement corresponding to dS 0 in FIG. 2) that occurs when the voltage is returned to zero. Hysteresis=(dS 0 /dS 100 )×100 [%] The mechanical displacement was determined by the free end displacement (dS 60 in FIG. 2) when a DC voltage of 60 V was applied. Further, the maximum applied voltage was determined by applying a DC voltage to the displacement element in increments of 20 V, and the value at which the displacement element was electrically destroyed or the value at which an abnormality was observed in the displacement characteristics. Note that the maximum applied voltage was calculated by converting it into a value when the thickness of the displacement element was 1 mm. Examples of the results are shown in Tables 1 to 4. In Tables 1 to 4, the sample numbers marked with * correspond to the electrostrictive element materials of the present invention. As is clear from Tables 1 to 4, the sample made of the electrostrictive element material of the present invention has a
It is clear that the mechanical displacement, hysteresis, and maximum applied voltage are all good, and that it has favorable characteristics as a displacement element. Thus, according to the present invention, Pb(Mg 1/3 Nb 2/3 )
Pb [ (Mg 1/3 Nb 2/3 ) A ( Co 1/2 Nb 1/2 ) B
By setting the A, B, and C components of the TiO c ]O 3 composition within appropriate ranges and adding appropriate amounts of suitable subcomponents, it has high mechanical displacement and low hysteresis characteristics, and is also insulating. This material has a high yield strength and is highly reliable. Although not shown in the examples, 0.01 to 0.3% by weight of Sb 2 O 3 and CaO, and 0.005 to 0.1% by weight of SiO 2 were added to the basic composition of this example as subcomponents. It is clear that the same effects as in this embodiment can be obtained also in this case.
【表】【table】
【表】【table】
【表】【table】
【表】【table】
【表】【table】
【表】
[発明の効果]
本発明の電歪素子材料によれば、以下に挙げる
広範囲の用途への適用が期待できる。
(1) 大きな絶縁耐力を有しているので素子の薄型
化、大きな機械的変位の発生が実現でき、小
型、軽量化及び低電圧駆動が可能で、新しい変
位素子分野に適用できる。
(2) 大きな絶縁耐力を有しているので所定の電圧
印加に於いて高信頼性が維持できる。
(3) 電歪素子自体極性を有していないので、バイ
モルフ構成時の取り扱いが容易であり(片側駆
動方式)、且つ印加電圧の大きさを広範囲に選
択でき、広範囲の用途に応じた機械的変位の設
定が可能である。
(4) 長時間の電圧印加に於いても機械的変位の移
動(変位のシフト)が極めて少なく高信頼性を
有しているので、例えば機構上から所定の電圧
で長時間の保持が必要な機器への適用が十分可
能である。
(5) 絶縁耐力が大きいので高電圧印加による大変
位を必要とする応用への適用が可能である。
(6) 変位素子としての用途以外に必要に応じて各
種圧電製品との代替が可能である。
尚本発明の実施例に於いては機械的変位、電圧
−変位ヒステリシス及び絶縁耐力について特にバ
イモルフ型変位素子に関連して説明したが本発明
に係る電歪素子材料を用いて積層構造での場合に
ついても調べその改善効果が確認されており、従
つて例えば積層型変位素子への適用及び積層型変
位素子の小型、軽量化の実現も十分可能である。
以上詳述した様に、本発明の電歪素子材料は広
範囲な用途に利用できる変位素子に好適なもので
あり産業上極めて価値大なるものである。[Table] [Effects of the Invention] The electrostrictive element material of the present invention can be expected to be applied to a wide range of uses listed below. (1) Since it has a large dielectric strength, it is possible to make the element thinner and generate a large mechanical displacement, and it is possible to be smaller, lighter, and driven at a lower voltage, and can be applied to new fields of displacement elements. (2) Since it has a large dielectric strength, high reliability can be maintained when a predetermined voltage is applied. (3) Since the electrostrictive element itself has no polarity, it is easy to handle when configured as a bimorph (one-sided drive system), and the magnitude of the applied voltage can be selected from a wide range, making it suitable for mechanical Displacement can be set. (4) It has high reliability with very little mechanical displacement movement (displacement shift) even when voltage is applied for a long time. It is fully applicable to equipment. (5) Because of its high dielectric strength, it can be applied to applications that require large displacements due to the application of high voltage. (6) In addition to being used as a displacement element, it can be substituted with various piezoelectric products as needed. In the embodiments of the present invention, mechanical displacement, voltage-displacement hysteresis, and dielectric strength were explained in particular in relation to a bimorph type displacement element, but in the case of a laminated structure using the electrostrictive element material according to the present invention. The present invention has also been investigated and its improvement effect has been confirmed. Therefore, it is fully possible to apply the method to, for example, a laminated displacement element, and to make the laminated displacement element smaller and lighter. As described in detail above, the electrostrictive element material of the present invention is suitable for displacement elements that can be used in a wide range of applications, and is extremely valuable industrially.
第1図は本発明の実施例に於いて評価に供した
バイモルフ型変位素子の構成を示した図、第2図
は本発明の実施例に於いて測定基準を示すグラ
フ、第3図は従来のバイモルフ型変位素子の一例
を示す図である。
図中、1……金属製弾性板、2,2′……電歪
素子、3,3′……圧電磁器板。
Fig. 1 is a diagram showing the configuration of a bimorph type displacement element used for evaluation in an embodiment of the present invention, Fig. 2 is a graph showing measurement standards in an embodiment of the present invention, and Fig. 3 is a conventional FIG. 3 is a diagram showing an example of a bimorph type displacement element. In the figure, 1... metal elastic plate, 2, 2'... electrostrictive element, 3, 3'... piezoelectric ceramic plate.
Claims (1)
O3で示され(但しA+B+C=1)0.700≦A≦
0.890、0.010≦B2≦0.150、0.10≦C≦0.15を満足
する基本組成に対し、副成分としてSb2O3、CaO
から選ばれた少くとも1種を0.01〜0.3重量%及
びSiO2を0.005〜0.1重量%添加含有してなること
を特徴とする電歪素子材料。1 General formula Pb [(Mg 1/3 Nb 2/3 ) A (Co 1/2 Nb 1/2 ) B Ti c ]
O 3 (however, A+B+C=1) 0.700≦A≦
For the basic composition satisfying 0.890, 0.010≦B2≦0.150, 0.10≦C≦0.15, Sb 2 O 3 and CaO are added as subcomponents.
An electrostrictive element material characterized in that it contains 0.01 to 0.3% by weight of at least one selected from the following and 0.005 to 0.1% by weight of SiO2 .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1120328A JPH02301171A (en) | 1989-05-16 | 1989-05-16 | Electrostriction element material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1120328A JPH02301171A (en) | 1989-05-16 | 1989-05-16 | Electrostriction element material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02301171A JPH02301171A (en) | 1990-12-13 |
| JPH0582340B2 true JPH0582340B2 (en) | 1993-11-18 |
Family
ID=14783538
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1120328A Granted JPH02301171A (en) | 1989-05-16 | 1989-05-16 | Electrostriction element material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02301171A (en) |
-
1989
- 1989-05-16 JP JP1120328A patent/JPH02301171A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02301171A (en) | 1990-12-13 |
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