JPS629176B2 - - Google Patents
Info
- Publication number
- JPS629176B2 JPS629176B2 JP19690881A JP19690881A JPS629176B2 JP S629176 B2 JPS629176 B2 JP S629176B2 JP 19690881 A JP19690881 A JP 19690881A JP 19690881 A JP19690881 A JP 19690881A JP S629176 B2 JPS629176 B2 JP S629176B2
- Authority
- JP
- Japan
- Prior art keywords
- alloy
- metal
- diaphragm
- alb
- young
- 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
Links
- 229910052751 metal Inorganic materials 0.000 claims description 22
- 239000002184 metal Substances 0.000 claims description 22
- 229910000521 B alloy Inorganic materials 0.000 claims description 7
- 229910052796 boron Inorganic materials 0.000 claims description 6
- 239000011159 matrix material Substances 0.000 claims description 5
- 229910045601 alloy Inorganic materials 0.000 description 16
- 239000000956 alloy Substances 0.000 description 16
- 238000000034 method Methods 0.000 description 6
- 239000007769 metal material Substances 0.000 description 5
- 239000000203 mixture Substances 0.000 description 5
- 238000010791 quenching Methods 0.000 description 5
- 239000010936 titanium Substances 0.000 description 5
- 229910000737 Duralumin Inorganic materials 0.000 description 4
- 229910052782 aluminium Inorganic materials 0.000 description 4
- 230000007423 decrease Effects 0.000 description 4
- 238000001816 cooling Methods 0.000 description 3
- 239000013078 crystal Substances 0.000 description 3
- 238000013016 damping Methods 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- 230000006698 induction Effects 0.000 description 3
- 239000007788 liquid Substances 0.000 description 3
- 238000002844 melting Methods 0.000 description 3
- 230000008018 melting Effects 0.000 description 3
- 238000010587 phase diagram Methods 0.000 description 3
- 229910052719 titanium Inorganic materials 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 229910052790 beryllium Inorganic materials 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 239000010453 quartz Substances 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000005507 spraying Methods 0.000 description 2
- 238000007088 Archimedes method Methods 0.000 description 1
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 description 1
- 229910002056 binary alloy Inorganic materials 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 230000008094 contradictory effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 239000008187 granular material Substances 0.000 description 1
- 239000007970 homogeneous dispersion Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 229910001338 liquidmetal Inorganic materials 0.000 description 1
- 229910052749 magnesium Inorganic materials 0.000 description 1
- 239000011777 magnesium Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000155 melt Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000002244 precipitate Substances 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 238000005096 rolling process Methods 0.000 description 1
- 239000007921 spray Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 231100000331 toxic Toxicity 0.000 description 1
- 230000002588 toxic effect Effects 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Landscapes
- Diaphragms For Electromechanical Transducers (AREA)
Description
本発明は、高特性、即ち、小密度ρ、高ヤング
率E、高損失ΔW/Wの金属振動板を提供するも
ので、より具体的には、音響用スピーカーの振動
板、ターンテーブルマツト、ターンテーブル等プ
レーヤー関係の振動板及び低音吸収パネル等に用
いる金属振動板に関する。
従来、音響用振動板として、特に、高特性が要
求されるスピーカー用振動板の金属材料としては
B(ボロン)、Be(ベリリウム)、Ti(チタン)、
ジユラルミン、アルミニウム(Al)等が用いら
れてきたが、それぞれ一長一短があつた。これら
の金属の諸性質を表―1に示す。
The present invention provides a metal diaphragm with high characteristics, that is, a small density ρ, a high Young's modulus E, and a high loss ΔW/W. This invention relates to metal diaphragms used for diaphragms for players such as turntables, bass absorption panels, etc. Traditionally, the metal materials for acoustic diaphragms, particularly for speaker diaphragms that require high characteristics, are B (boron), Be (beryllium), Ti (titanium),
Duralumin, aluminum (Al), etc. have been used, but each has advantages and disadvantages. Table 1 shows the properties of these metals.
【表】【table】
【表】
Mgは、軽く(ρが小さい)、Eも適当にあり、
振動板を伝わる音速v=√は51×102
(m/s)と、悪くはないが、その金属特有の酸
化性が大きいため空気中で、これを薄板化し振動
板として用いることは困難である、Bはρ.E.
√の全ての点から望ましい特性を持つてい
るが、融点Tmが2225℃と非常に高く、又硬いた
めこれを薄板に加工することは困難であり、現在
まで、ステレオのプレーヤーのピツクアツプのカ
ンチレバーパイプにCVD(Chemical Vapour
Deposition)法で、他の金属材のパイプの上にコ
ーテイングするといつた方法でのみ用いられてき
た。優れた特性を持つBeについては、一部スピ
ーカーに実用化されてはいるがBeは人体に対す
る毒性といつた点に問題があり、製造上、使用
上、最適な金属材料とは言い難い。Tiについて
は、√は、ジユラルミン、Al等と同じで
あるが、ρが大きいため、スピーカー用振動板と
してこれを用いた場合、再生能率が低下するとい
う問題があり、聴感覚的には「音が貧しくなる」
という欠点がある。又、値段もアルミ等に較べ高
い。ジユラルミン、Alについては、加工の容易
さや、コスト的には、優れているが、特性特にE
があまり高くなく、よつて、√も(50〜52
×102m/s)の値しか得られないため、周波数
特性が若干悪いという問題がある。
本発明は、かかる上記の金属材料の欠点、問題
点等を解決する金属材料であり、その構成は、
Al―B系において、Bが0.1〜30原子%(at%)
の領域を主成分とする金属振動板である。更に、
このAl―B系合金においてAl母相中にAlB2の結
晶相を微細に均一に分散させたことを特徴とする
金属振動板である。
本発明の効果を、第1図のAl―B二元系合金
状態図(「金属データ・ブツク(丸善)」より抜
粋)を用いて説明する。Al―B系合金は、第1
図の状態図よりわかるように、Bのat%が増加す
るに従つて合金の液相線は高温側に移動し、液相
線より高温側にあつた液体金属は冷却途中でAl
とAlB2の2相分離をして析出する。
本発明においては、AlとBの比を変えて
(B:0〜50at%)異なる組成になるように高周
波誘導加熱により溶解し、溶解した溶湯金属を金
型に鋳込み、母合金とした。この母合金は前述の
ようにAlとAlB2より成り、Alの母晶の中にAlB2
が析出するものである。そして、この母合金につ
いて密度ρ、ヤング率Eを測定した結果、0〜
30at%Bの領域で著しい特性を示すことを見出し
た。この結果を第2図に横軸にBのat%を、縦軸
にはρ及びEを示した。この第2図にも示す様に
ρはBの濃度と共に減少し、さらにEはBが30at
%で、Alの4倍という結果を得た。しかしなが
ら、Bの濃度増と共に母合金全体の靭性、ねばさ
が低下してもろくなり、30at%を越すとBの溶解
も難しくなり、さらに加工が難しく振動板用に薄
体化することが困難となつた。Bがこの様にヤン
グ率Eを上げるのは、組成を変えた母合金のEの
測定から、第3図に示すように0.1at%以上から
であることも見出した。従つて、本発明は、Al
―B系において、Bが0.1〜30at%の領域を主成
分とする金属振動板に適用できる。
更に、本発明のAl―B系合金について、振動
板としての特性向上を図るためその金属組織を観
察し、その母合金の製造法、加工法について検討
した本合金は、Alの母相の中にAlB2の結晶相が
析出するものであるが、この析出相が細かく均質
に分散することが合金の強度、ヤング率のバラツ
キの低減、靭性の向上に効くことを見出した。そ
こで液体超急冷技術を用いて溶湯金属を直接回転
する金属性ローラに吹きつけ、又は一対の金属性
ローラの隙間に吹きつけ圧延することにより金属
薄帯化することを試み、得られた金属薄帯のρ.
Eを測定し、又金属組織の観察、ビツカース硬度
(Hv)の測定を行つた。その結果、超急冷された
金属薄体は冷却速度が〜106℃/secと大きいた
め、AlB2が微細に母相内に一様分布し、ヤング
率のバラツキが減少し、Hvが10〜30%増大する
ことを見出した。本発明のAl―B系合金の超急
冷は、液体超急冷法に限らず他の超急冷法(スパ
ツタ法、蒸着法等)でも、得られた薄体の特性へ
の効果が見られた。従つて、本発明は、Al―B
系(B:0.1〜30at%)合金をAl母相中にAlB2の
結晶相を微細に均一に分散させた金属振動板であ
る。
また、得られた金属の振動減衰能ΔW/W≒
(ao 2−ao 2+1)/ao 2(aoはn番目の振
動の振幅強度)を測定した結果、Al及びジユラ
ルミンのΔW/Wより50%以上高くなつているこ
とを見出した。これは、この合金の高損失、高減
衰能は、その金属組織が母相と第二相との界面で
粘性流動が生じるためであろうと考えられる。
本発明の代表的組成のAl98B2、Al80B20につい
て、その特性値を表―1に示した。融点Tmは、
本合金が、合金系全体で溶ける温度という意味で
( )をつけて示してある。この表よりわかるよ
うに、本発明のAl―B系合金は、ρが小さく、
Eが大きく、結果として√が60〜100×102
(m/s)と、Al,TiとB,Beの中間の値をとる
すぐれた振動板材料であり、かつ高損失、高減衰
能という相反する特性を合わせ持ち、加工性にも
優れ、コスト的にも安く量産できるため極めて振
動板に適した材料である。本発明のAl―B系合
金に機械的加工性等を改善するためCu,Ti,Mg
等他の第三元素を添加しても何ら支障はなく、特
性改善の点でも望ましいものである。
次に本発明の実施例を述べる。
実施例 1
Al96B4の組成比になる様に純度99.99%の粒状
Al221.5gと結晶化粒状(純度99.9%)B3.70gを
アルミナ製のルツボに入れ、減圧後Ar(アルゴ
ン)置換し、Ar圧68cmHg下で高周波(30kHz)
誘導加熱し、Alを約1400℃位まで温度を上げて
溶かし、これにBを溶解させ、Al−Bの均質な
溶湯をつくり、これを鉄製の金型に鋳込んだ。室
温にまで冷却後、大気中に取り出し、この母合金
の特性を測定した。密度はアルキメデス法で測定
しρ=2.7(g/cm3)、ヤング率は短冊状に切り出
した試料を一端を固定したたわみ振動法により測
定し、E=1.1×1012(dyn/cm2)を得た。この値
より√を求めると63×102(m/s)と計
算された。
実施例 2
実施例―1と同様にAl80B20の組成比になる様
に調整した母合金を、高周波誘導加熱により溶解
鋳込みの操作によつて作成した。この母合金を一
端に0.2mm幅、長さ10mmのスリツトを持つ石英ノ
ズルに数g投入し、Ar雰囲気下で1500℃の温度
で溶解した。これを直径300mm、幅30mmの
1600rpmで回転する銅製ローラーの円周にArガ
スを石英ノズルの他端から急激に加え、溶けた金
属を吹きつけることにより、液体超急冷を行な
い、幅10mm、厚さ50umの金属薄帯を得た。この
金属薄帯をエツチングし、顕微鏡観察すると、
Al母相中に数μmの大きさのAlB2結晶相が均一
に分散していた。この金属薄帯のρ、Eを測定
し、ρ=2.66(g/cm3)、E=2.5×1012(dyn/
cm2)の値を得た。この値より√=97×102
(m/s)と計算された。[Table] Mg is light (small ρ) and has a suitable E.
The speed of sound traveling through the diaphragm v=√ is 51×10 2
(m/s), which is not bad, but due to the high oxidizability peculiar to the metal, it is difficult to make it thin and use it as a diaphragm in the air.B is ρ. E.
√ However, it has a very high melting point Tm of 2225℃ and is hard, so it is difficult to process it into a thin plate.Until now, it has been used as a cantilever pipe for pickups in stereo players. CVD (Chemical Vapor)
It has been used only as a coating on pipes made of other metal materials using the Deposition method. Be, which has excellent properties, has been put to practical use in some speakers, but Be has a problem in that it is toxic to the human body, and it is difficult to say that it is an optimal metal material for manufacturing and use. Regarding Ti, √ is the same as duralumin, Al, etc., but since ρ is large, when using it as a speaker diaphragm, there is a problem that the reproduction efficiency decreases, and the auditory sense is become poorer.”
There is a drawback. Also, the price is higher than aluminum etc. Duralumin and Al are superior in terms of ease of processing and cost, but their properties, especially E.
is not very high, and √ is also (50~52
×10 2 m/s), there is a problem that the frequency characteristics are somewhat poor. The present invention is a metal material that solves the drawbacks, problems, etc. of the above-mentioned metal materials, and its structure is as follows:
In Al-B system, B is 0.1 to 30 atomic% (at%)
This is a metal diaphragm whose main component is the area of . Furthermore,
This metal diaphragm is characterized in that, in this Al--B alloy, a crystal phase of AlB 2 is finely and uniformly dispersed in the Al matrix. The effects of the present invention will be explained using the Al--B binary alloy phase diagram shown in FIG. 1 (excerpted from "Metal Data Book (Maruzen)"). Al-B alloy is the first
As can be seen from the phase diagram shown in the figure, as the at% of B increases, the liquidus line of the alloy moves to the high temperature side, and the liquid metal that was on the high temperature side of the liquidus line becomes Al during cooling.
and AlB 2 are separated and precipitated. In the present invention, different ratios of Al and B (B: 0 to 50 at%) are melted by high-frequency induction heating to give different compositions, and the melted molten metal is cast into a mold to obtain a master alloy. As mentioned above, this mother alloy consists of Al and AlB 2 , and AlB 2 is contained in the Al mother crystal.
is precipitated. Then, as a result of measuring the density ρ and Young's modulus E of this master alloy, it was found that the density ρ and the Young's modulus E were 0 to
It has been found that remarkable properties are exhibited in the 30 at% B region. The results are shown in FIG. 2, where the horizontal axis shows at% of B, and the vertical axis shows ρ and E. As shown in Fig. 2, ρ decreases with the concentration of B, and E also decreases with B at 30at.
%, four times that of Al. However, as the concentration of B increases, the toughness and toughness of the entire master alloy decrease, making it brittle.If the concentration exceeds 30 at%, it becomes difficult to dissolve B, and furthermore, it becomes difficult to process and to make it thin for use as a diaphragm. Summer. From measurements of E of master alloys with different compositions, it was found that B increases the Young's modulus E in this way from 0.1 at% or more, as shown in FIG. Therefore, the present invention provides Al
- In the B system, it can be applied to metal diaphragms whose main component is B in the range of 0.1 to 30 at%. Furthermore, in order to improve the properties of the Al-B alloy of the present invention as a diaphragm, the metal structure of the alloy was observed, and the manufacturing and processing methods of the mother alloy were studied. The crystalline phase of AlB 2 precipitates in the alloy, and we have discovered that fine and homogeneous dispersion of this precipitated phase is effective in reducing the strength of the alloy, reducing variations in Young's modulus, and improving toughness. Therefore, an attempt was made to use liquid super-quenching technology to spray molten metal directly onto a rotating metallic roller, or by spraying and rolling it into a gap between a pair of metallic rollers to form a thin metal strip. ρ of the band.
E was measured, the metal structure was observed, and the Vickers hardness (Hv) was measured. As a result, since the ultra-quenched metal thin body has a high cooling rate of ~10 6 °C/sec, AlB 2 is finely distributed uniformly within the matrix, the variation in Young's modulus is reduced, and Hv is 10~10 °C/sec. It was found that the amount increased by 30%. The ultra-quenching of the Al--B alloy of the present invention was not limited to the liquid ultra-quenching method, but also other ultra-quenching methods (sputtering method, vapor deposition method, etc.) were found to have an effect on the properties of the obtained thin body. Therefore, the present invention provides Al-B
This is a metal diaphragm made of a (B: 0.1 to 30 at%) alloy in which AlB 2 crystalline phases are finely and uniformly dispersed in an Al matrix. In addition, the vibration damping capacity ΔW/W≒ of the obtained metal
As a result of measuring (a o 2 - a o 2 +1)/a o 2 (a o is the amplitude intensity of the n-th vibration), it was found that it was more than 50% higher than ΔW/W of Al and duralumin. . This is considered to be due to the high loss and high damping ability of this alloy due to the occurrence of viscous flow at the interface between the parent phase and the second phase in its metallographic structure. Table 1 shows the characteristic values of typical compositions of Al 98 B 2 and Al 80 B 20 of the present invention. The melting point Tm is
The numbers in parentheses indicate the temperature at which the entire alloy system melts. As can be seen from this table, the Al-B alloy of the present invention has a small ρ and
E is large, and as a result, √ is 60 to 100×10 2
(m/s), which is between Al, Ti, and B, Be.It is an excellent diaphragm material that has contradictory properties such as high loss and high damping ability, and has excellent processability and cost. It is an extremely suitable material for diaphragms because it can be mass-produced at low cost. Cu, Ti, and Mg are added to the Al-B alloy of the present invention to improve mechanical workability.
There is no problem in adding other third elements such as, and it is also desirable from the point of view of improving characteristics. Next, examples of the present invention will be described. Example 1 Granules with a purity of 99.99% to have a composition ratio of Al 96 B 4
1.5 g of Al2 and 3.70 g of crystallized granular B (purity 99.9%) are placed in an alumina crucible, the pressure is reduced, the substitution is made with Ar (argon), and high frequency (30 kHz) is applied under an Ar pressure of 68 cmHg.
Al was melted by induction heating to a temperature of about 1400°C, and B was dissolved therein to create a homogeneous Al-B molten metal, which was cast into an iron mold. After cooling to room temperature, it was taken out into the atmosphere and the properties of this master alloy were measured. The density was measured using the Archimedes method, ρ = 2.7 (g/cm 3 ), and the Young's modulus was measured using the flexural vibration method with one end fixed on a sample cut into a strip, E = 1.1×10 12 (dyn/cm 2 ). I got it. From this value, √ was calculated to be 63×10 2 (m/s). Example 2 As in Example-1, a master alloy adjusted to have a composition ratio of Al 80 B 20 was produced by melting and casting using high-frequency induction heating. Several grams of this master alloy was put into a quartz nozzle with a slit of 0.2 mm width and 10 mm length at one end, and melted at a temperature of 1500°C under an Ar atmosphere. This has a diameter of 300mm and a width of 30mm.
By rapidly adding Ar gas from the other end of a quartz nozzle to the circumference of a copper roller rotating at 1600 rpm and spraying the molten metal, liquid ultra-quenching is performed to obtain a metal ribbon with a width of 10 mm and a thickness of 50 um. Ta. When this thin metal strip is etched and observed under a microscope,
AlB 2 crystal phases with a size of several μm were uniformly dispersed in the Al matrix. The ρ and E of this metal ribbon were measured, and ρ=2.66 (g/cm 3 ), E=2.5×10 12 (dyn/
cm 2 ) values were obtained. From this value √=97×10 2
(m/s).
第1図はAl―B系の状態図、第2図はAl―B
系のBの濃度(at%)と密度ρ、ヤング率Eの関
係を示す図、第3図はAl―B系のBの濃度(at
%)とヤング率Eの関係を示す図である。
Figure 1 is a phase diagram of the Al-B system, Figure 2 is Al-B
Figure 3 shows the relationship between the B concentration (at%), density ρ, and Young's modulus E in the Al-B system.
%) and Young's modulus E.
Claims (1)
B合金であつて、Alの母相中にAlB2の結晶相を
微細に均一に分散させたことを特徴とする金属振
動板。1 Al— consisting of 0.1 to 30 atomic% B and the rest Al—
A metal diaphragm made of B alloy, characterized in that a crystalline phase of AlB 2 is finely and uniformly dispersed in a matrix of Al.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56196908A JPS58100653A (en) | 1981-12-09 | 1981-12-09 | Metallic diaphragm |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56196908A JPS58100653A (en) | 1981-12-09 | 1981-12-09 | Metallic diaphragm |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58100653A JPS58100653A (en) | 1983-06-15 |
| JPS629176B2 true JPS629176B2 (en) | 1987-02-26 |
Family
ID=16365645
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56196908A Granted JPS58100653A (en) | 1981-12-09 | 1981-12-09 | Metallic diaphragm |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58100653A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2003041337A (en) * | 2001-07-30 | 2003-02-13 | Nkk Corp | Chloride-containing molten salt contact material and method for producing the same |
| WO2003012155A1 (en) * | 2001-07-30 | 2003-02-13 | Jfe Engineering Corporation | Material being resistant to chloride-containing molten salt corrosion, steel pipe for heat exchanger coated with the same, and method for production thereof |
-
1981
- 1981-12-09 JP JP56196908A patent/JPS58100653A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58100653A (en) | 1983-06-15 |
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