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JP3948725B2 - Thermal history estimation sensor - Google Patents
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JP3948725B2 - Thermal history estimation sensor - Google Patents

Thermal history estimation sensor Download PDF

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Publication number
JP3948725B2
JP3948725B2 JP2002360614A JP2002360614A JP3948725B2 JP 3948725 B2 JP3948725 B2 JP 3948725B2 JP 2002360614 A JP2002360614 A JP 2002360614A JP 2002360614 A JP2002360614 A JP 2002360614A JP 3948725 B2 JP3948725 B2 JP 3948725B2
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Japan
Prior art keywords
thermal history
adhesive
temperature
sensor
glass transition
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JP2002360614A
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JP2004191230A (en
Inventor
一司 山下
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Toyo Electric Manufacturing Ltd
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Toyo Electric Manufacturing Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は、熱履歴によって、主に有機材料の劣化により材料や製品の寿命が定まる被検体に設置して、熱履歴、つまり履歴温度およびその履歴時間を容易に推定するためのセンサおよび、熱履歴推定法に関するものである。
【0002】
【従来の技術】
工業で使用される各種材料および、それらを使用して製造された工業製品は、それらの製造中あるいは使用中において、熱ストレスが加わるものが多く、その熱ストレスによって、材料の物性や製品の機能の低下をもたらし、ついには使用に耐えなくなり寿命を迎えることが多い。
一般に、材料の一部または全部に有機物が用いられている製品では、熱ストレスが製品寿命に大きな影響をもたらす要因であることが知られている。
【0003】
この熱ストレスは、製品を構成する有機材料を化学的変化によって劣化させる主な要因であり、その各種物性低下の程度および進行の速さは、温度および時間の関数となる。したがって材料や製品の寿命や劣化の程度を知ろうとする場合、単に温度または時間のみを測定しているだけでは不十分で、曝された温度と曝された時間を同時に把握することが重要であり、使用経過時間後の熱履歴を推定しなくてはならない。
【0004】
従来、温度の測定には各種の方法が知られており、代表的にはサーモラベル等の温度にって変色や融解などの現象を伴う材料(示温材料)がある。また熱電対や放射温度計などを用いて測定することも広く行なわれている。
しかしながら、温度の測定だけでは、材料や製品の寿命や劣化の程度を知るときに重要な、温度に曝された時間の把握ができず、熱履歴の把握は不可能である。
【0005】
一方、温度と時間、つまり熱履歴を測定する手段としては、熱電対や放射温度計を常時モニターし、その温度と時間を記録することによって達成することができるが、常時記録するための装置が別途必要となり、装置が複雑になるばかりか、電源の無いところでは使用できないという問題がある。
【0006】
また材料が熱履歴によって徐々に物理化学的変化を起こすことによってその物性が変化していくことを利用してその物性の変化を測定することにより熱履歴を推定する方法が提案されている。例えば赤外スペクトルで化学構造の変化を捉えてスペクトルから熱履歴の推定を行なう方法(例えば特許文献1参照。)。実働機器から採取した被測定物質を異なる2つの測定方法(例えば、示差走査熱量測定(DSC)と動的粘弾性特性測定(DMA)等)で測定し、そこから熱履歴を推定する方法(例えば特許文献2参照。)、融解熱曲線の低温結晶化特性の変化量を測定する方法(例えば特許文献3参照。)、光の2波長間の反射吸光度差を用いた方法(例えば特許文献4参照。)などが知られている。これらは、ある程度の精度で熱履歴を推定できるが、特別な分析装置などが必要となり、現場で容易に行なえる方法ではない。
本発明の目的は、以上の問題点を考慮し、従来の手段では不可能であった、有機物が使用された材料や製品の熱履歴が容易に推定できる熱履歴推定センサおよびその推定方法を提供するものである。
【0007】
【特許文献1】
特開昭60−42643号公報
【特許文献2】
特開平3−37557号公報
【特許文献3】
特開平9−170989号公報
【特許文献4】
特開2001−22805号公報
【課題を解決するための手段】
【0008】本発明の熱履歴推定の手段としては、2枚の金属板を、金属粉末の球状粒子を含有させた接着剤で加圧して接着したものを熱履歴センサとし、熱環境下に曝されている材料または製品に取り付けまたは組み込み、材料または製品の熱履歴を知りたいときに、そのセンサの電気変数を測定して熱履歴を推定しようとするものである。
【0009】
ここで2枚の金属板を、金属粒子を含有させた接着剤で加圧して接着したものを熱履歴センサとは、温度および時間によって徐々に電気的変数、例えば、抵抗、容量が変化するように製造されたセンサで、あらかじめ温度と時間および電気変化を測定しマスターカーブを作成しておいてそれと比較するといった手段を設けておく。
【0010】
次に上記と同じ方法で作成された新品のセンサを製品にあらかじめ組み込んでおき、その熱履歴が知りたいときに、かかる手段を使って、例えばそのセンサの電気抵抗を測定して、その電気抵抗値とマスターカーブを比較して熱履歴を推定することで目的を達成される。
【0011】
ここでセンサに用いる金属板は、比較的剛性が高く容易に変形しないもので、かつ使用温度領域で融解や著しい劣化(酸化等)等をしないものであれば特に制限はないが、一般的にはAl、Ti、 Fe、Ni、Cu、Zn、Ag、Pt、Au、Mo、Wあるいはそれらの合金などの中から適当な材料が選択される。板の厚さは、作成時に変形が大きくなるような厚さでなければ特に制限はないが、一般的に1mm〜5mm程度が望ましい。
【0012】
この2枚の金属板を張り合せる際には、金属粉末を含有させた接着剤を用いる。金属粉末には各種あるが、ここで用いる金属粒子は大きさ50μm〜2mm程度の比較的粒子径の揃った球状粒子が望ましい。
【0013】
またこの金属粒子の種類は、使用温度で導電性、化学的、物理的特性が安定であるものであれば、特に制限なく用いられ、一般的にAl、Cu、Ag、Ni、Au、Ptあるいはその合金などの粉末粒子が好適である。
【0014】
さらに、接着剤への配合量も、1〜80wt%の広範な範囲で目的とする特性に合わせるように自由に配合可能である。
【0015】
用いる接着剤には特に制限はないが、ある程度の剛性を持ち、用いられる金属板や金属粉末粒子を比較的強固に接着するものが望ましい。中でもエポキシ系、アクリル系、ウレタン系、イミド系などが物性上好適に用いられる。
【0016】
また、用いる接着剤のガラス転移温度は、センサが使用される温度範囲によって適当なものが選択されるが、組み込まれる製品の使用温度を考慮して決定される。
【0017】
また金属粒子含有接着剤を塗布し、金属板で挟み込み、接着剤を硬化させる際には、接着層に含まれる金属粒子が変形する程度に予加圧した状態で硬化させることが必要である。この時の予加圧の程度は、金属粒子の種類、大きさ、含有量などによって適宜選択され、一般には0.1〜10Mpa程度の圧力下で硬化させる。
この時の硬化温度もまた、使用する接着剤で変わるが、一般に室温〜250℃の間が多い。
【0018】
こうして接着硬化したものは、予加圧したまま室温まで冷却し、予加圧を解除した後に、端面を整形し、外部からの汚損や水分などで電気変数値が変化しないようシールや被覆などの適正な端面処理を行ない、熱履歴センサに供する。
【0019】
図1は、本発明による熱履歴推定センサの外観略図であり、その断面構造の拡大略図を図2に示す。
【0020】
このような熱履歴センサは、金属板の種類、接着剤のガラス転移温度、硬化後の弾性率、金属粒子の種類および含有量、製造プロセス中の加圧条件、硬化温度、硬化時間などによって各種の特性を持つものが容易に作成できる。
このようにして得られた熱履歴センサは、前述のようにマスターカーブをあらかじめ作成しておき、熱履歴が推定したい製品の適当な場所にこの熱履歴センサを組み込み、必要が生じた時点でその電気変数を測定し、あらかじめ作成したマスターカーブとの比較により製品の受けた熱履歴を推定する。
【0021】
【作用】
挟まれた金属粒子は加圧によって弾性変形、塑性変形を生じたまま、接着剤が硬化することによって金属板間に拘束される。
従って、接着層内部にはその反発力が内部応力として働くことになるが、接着剤のガラス転移温度よりはるかに低い温度では、接着剤は金属粒子の反発力からくる内部応力によってほとんど変形せず、例えば、電気変数として抵抗の変移を捉えると、初期の電気抵抗からほとんど変化しないが、温度が上昇し、ガラス転移温度近傍になると接着剤の弾性率が低下し、内部応力を緩和する方向に徐々に変形して行く所謂クリープ現象が生じる。この際金属粒子と金属板の接触状態が変化し、接触抵抗に変化を来たし、徐々に電気抵抗が上昇していく。この電気抵抗の上昇度合いは、曝露された温度と時間の関数であり、熱履歴によって定まる。
【発明の実施の形態】
【0022】
以下、本発明の実施例の1形態を述べるが、以下に示す実施形態に限定されるものではない。
長さ50×幅50×厚さ3mmのアルミニウム板2枚を電極として用意し、接着面をアセトンで脱脂し、乾燥させた。一方、エポキシ系接着剤(ガラス転移温度120℃)に直径約0.1mmの球状で粒子径の揃った球状粒子として、銅粒子を約30wt%混入したものを片方のアルミ板に厚さ約0.2mmで塗布し、もう片方のアルミ板と重ね合せ、1MPaの予加圧下で100℃、4時間加熱硬化した。この試験片を、10mm×10mmの大きさに切断し端面を磨いた後、端面の汚損や吸湿で電気変数が変化しないようエポキシ系樹脂で封止し、熱履歴センサとした。電気変数として、抵抗変化、容量変化など交流インピーダンス変化をも含まれることは云うまでもない。
【0023】
このセンサの幾つかを、温度の異なる恒温槽にそれぞれ放置し、電気変数の変化を測定した。ここでは電気変数として抵抗変化をトレースした。時間と共に図3のような曲線が得られ、これをマスターカーブとした。
また、ガラス転移温度の異なるエポキシ系接着剤(160℃、180℃)を用いたほかは、前述の実施形態と変わらぬ方法で同様の熱履歴センサを作成したところ図4、図5のような曲線が得られた。
【0024】
また、熱履歴センサに使用する接着剤のガラス転移温度より高い温度領域ではでは接着剤の弾性率が大きく低下するため、抵抗の変化率が極めて大きく、実用上は製品に許される最高許容温度付近のガラス転移温度を持った接着剤を用いた熱履歴センサを使用することが望ましい。
【0025】
一般的には、本発明の熱履歴センサは、使用接着剤のガラス転移温度より50℃程度低い温度からガラス転移温度付近より10℃程度高い温度までが使用可能温度領域となる。ガラス転移温度の異なる接着剤を用いて作られた幾つかの熱履歴センサを組み込んでおくことによって、熱履歴の推定精度がより向上する。
【0026】
【発明の効果】
以上の説明から明らかなように本発明の熱履歴センサを用いることにより、従来は困難であった熱履歴の推定が、極めて簡便に行なえるようになる。
熱履マスターカーブを取得し、マスターカーブと同一の特性を持つセンサを製品に組み込み、必要なときにセンサの電気変数を測定する手段とマスターカーブとを比較する手段により容易に熱履歴が把握、推定できる。
【図面の簡単な説明】
【図1】本発明による熱履歴センサの外観略図
【図2】本発明による熱履歴センサの断面拡大略図
【図3】ガラス転移温度120℃の接着剤を用いて作成した熱履歴センサの熱履歴と電気抵抗の関係を示すマスターカーブ
【図4】ガラス転移温度160℃の接着剤を用いて作成した熱履歴センサの熱履歴と電気抵抗の関係を示すマスターカーブ
【図5】ガラス転移温度180℃の接着剤を用いて作成した熱履歴センサの熱履歴と電気抵抗の関係を示すマスターカーブ
【符号の説明】
1 金属板
2 接着層
3 金属粒子
[0001]
BACKGROUND OF THE INVENTION
The present invention provides a sensor for easily estimating a thermal history, that is, a history temperature and its history time, installed on a subject whose lifetime is determined mainly by deterioration of organic materials due to deterioration of organic materials. It relates to the history estimation method.
[0002]
[Prior art]
Various materials used in the industry and industrial products manufactured using them are often subjected to thermal stress during their production or use, and the physical properties of the materials and product functions are affected by the thermal stress. In many cases, it will eventually endure its use and end its life.
In general, in a product in which an organic substance is used for a part or all of a material, it is known that thermal stress is a factor that greatly affects the product life.
[0003]
This heat stress is a main factor that causes deterioration of the organic material constituting the product due to chemical change, and the degree of the deterioration of the various physical properties and the speed of progress are functions of temperature and time. Therefore, when trying to know the life and degree of deterioration of materials and products, it is not enough to simply measure temperature or time. It is important to know the temperature and time of exposure at the same time. The heat history after the elapsed time of use must be estimated.
[0004]
Conventionally, various methods are known for measuring temperature. Typically, there are materials (temperature indicating materials) that are accompanied by a phenomenon such as discoloration or melting depending on the temperature of a thermolabel or the like. In addition, measurement using a thermocouple or a radiation thermometer is also widely performed.
However, the temperature measurement alone cannot grasp the time of exposure to temperature, which is important when knowing the life and the degree of deterioration of materials and products, and it is impossible to grasp the heat history.
[0005]
On the other hand, as a means of measuring temperature and time, that is, thermal history, it can be achieved by constantly monitoring a thermocouple or a radiation thermometer and recording the temperature and time. In addition to being complicated, the apparatus is complicated and cannot be used in the absence of a power source.
[0006]
In addition, a method has been proposed in which the thermal history is estimated by measuring the change in physical properties of the material by utilizing the fact that the physical properties of the material gradually change due to the thermal history. For example, a method of estimating a thermal history from a spectrum by capturing a change in chemical structure using an infrared spectrum (see, for example, Patent Document 1). A method of estimating the thermal history from two different measurement methods (for example, differential scanning calorimetry (DSC) and dynamic viscoelasticity measurement (DMA)) for measuring a substance to be measured collected from a working device. Patent Document 2), a method of measuring the amount of change in the low-temperature crystallization characteristics of the heat of fusion curve (see, for example, Patent Document 3), and a method using the difference in reflection absorbance between two wavelengths of light (see, for example, Patent Document 4). .) Etc. are known. Although these methods can estimate the thermal history with a certain degree of accuracy, they require special analyzers and the like, and are not easy methods on site.
In view of the above problems, an object of the present invention is to provide a thermal history estimation sensor that can easily estimate the thermal history of materials and products using organic substances, and an estimation method thereof, which is impossible with conventional means. To do.
[0007]
[Patent Document 1]
JP 60-42643 A [Patent Document 2]
JP-A-3-37557 [Patent Document 3]
Japanese Patent Laid-Open No. 9-170989 [Patent Document 4]
JP 2001-22805 A [Means for Solving the Problems]
As a means for estimating the heat history of the present invention, two metal plates, which are bonded by pressing with an adhesive containing metal powder spherical particles, are used as a heat history sensor and exposed to a thermal environment. When it is desired to know the thermal history of a material or product that is attached to or incorporated in the material or product that is being used, the thermal history is estimated by measuring the electrical variables of the sensor.
[0009]
Here, two metal plates are bonded by pressurizing with an adhesive containing metal particles. A thermal history sensor is such that electrical variables such as resistance and capacitance change gradually with temperature and time. In the sensor manufactured in (1), a means for measuring the temperature, time, and electrical change in advance, creating a master curve and comparing it is prepared.
[0010]
Next, a new sensor prepared in the same manner as described above is incorporated in the product in advance, and when it is desired to know its thermal history, such means are used to measure the electrical resistance of the sensor, for example. The objective is achieved by estimating the thermal history by comparing the value with the master curve.
[0011]
The metal plate used in the sensor is not particularly limited as long as it is relatively rigid and does not easily deform, and does not melt or significantly deteriorate (oxidize, etc.) in the operating temperature range. A suitable material is selected from Al, Ti, Fe, Ni, Cu, Zn, Ag, Pt, Au, Mo, W or alloys thereof. The thickness of the plate is not particularly limited as long as it is not thick enough to cause deformation at the time of production, but generally it is preferably about 1 mm to 5 mm.
[0012]
When the two metal plates are bonded together, an adhesive containing metal powder is used. Although there are various types of metal powder, the metal particles used here are preferably spherical particles having a size of about 50 μm to 2 mm and having a relatively uniform particle diameter.
[0013]
The metal particles can be used without particular limitation as long as the conductivity, chemical and physical properties are stable at the operating temperature, and are generally Al, Cu, Ag, Ni, Au, Pt or Powder particles such as alloys thereof are preferred.
[0014]
Furthermore, the compounding quantity to an adhesive agent can be freely mix | blended so that it may match the target characteristic in the wide range of 1-80 wt%.
[0015]
The adhesive to be used is not particularly limited, but an adhesive having a certain degree of rigidity and relatively strong adhesion to the metal plate or metal powder particles to be used is desirable. Of these, epoxy-based, acrylic-based, urethane-based, imide-based and the like are preferably used in view of physical properties.
[0016]
Further, the glass transition temperature of the adhesive to be used is appropriately selected depending on the temperature range in which the sensor is used, but is determined in consideration of the use temperature of the product to be incorporated.
[0017]
In addition, when the metal particle-containing adhesive is applied, sandwiched between metal plates, and cured, the adhesive needs to be cured in a pre-pressurized state so that the metal particles contained in the adhesive layer are deformed. The degree of pre-pressurization at this time is appropriately selected depending on the type, size, content, and the like of the metal particles, and is generally cured under a pressure of about 0.1 to 10 MPa.
The curing temperature at this time also varies depending on the adhesive to be used, but is generally between room temperature and 250 ° C.
[0018]
After the adhesive is hardened, cool it to room temperature with pre-pressurization, release the pre-pressurization, shape the end face, and seal or cover the electrical variable value so that it does not change due to external contamination or moisture. Appropriate end face processing is performed, and the heat history sensor is provided.
[0019]
FIG. 1 is a schematic external view of a thermal history estimation sensor according to the present invention, and FIG. 2 shows an enlarged schematic view of its cross-sectional structure.
[0020]
Such a heat history sensor can be selected depending on the type of metal plate, the glass transition temperature of the adhesive, the elastic modulus after curing, the type and content of metal particles, the pressing conditions during the manufacturing process, the curing temperature, the curing time, etc. It is easy to create one with the characteristics
The thermal history sensor obtained in this way is prepared in advance as described above, and the thermal history sensor is installed at an appropriate location of the product whose thermal history is to be estimated. Measure electrical variables and estimate the thermal history of the product by comparing it with a master curve created in advance.
[0021]
[Action]
The sandwiched metal particles are constrained between the metal plates as the adhesive is cured while being elastically deformed and plastically deformed by pressurization.
Therefore, the repulsive force acts as an internal stress inside the adhesive layer, but at a temperature much lower than the glass transition temperature of the adhesive, the adhesive is hardly deformed by the internal stress resulting from the repulsive force of the metal particles. For example, when the change in resistance is captured as an electrical variable, the initial electrical resistance hardly changes, but when the temperature rises and near the glass transition temperature, the elastic modulus of the adhesive decreases and the internal stress is relieved. A so-called creep phenomenon that gradually deforms occurs. At this time, the contact state between the metal particles and the metal plate changes, the contact resistance changes, and the electrical resistance gradually increases. This increase in electrical resistance is a function of the exposed temperature and time and is determined by the thermal history.
DETAILED DESCRIPTION OF THE INVENTION
[0022]
Hereinafter, although one form of the Example of this invention is described, it is not limited to embodiment shown below.
Two aluminum plates of length 50 × width 50 × thickness 3 mm were prepared as electrodes, and the adhesive surface was degreased with acetone and dried. On the other hand, about 30mm% of copper particles mixed into an epoxy adhesive (glass transition temperature 120 ° C) as spherical particles with a diameter of about 0.1mm and a uniform particle size are mixed on one aluminum plate with a thickness of about 0.2mm. Then, it was laminated with the other aluminum plate and cured by heating at 100 ° C. for 4 hours under a pre-pressurization of 1 MPa. The test piece was cut to a size of 10 mm × 10 mm and the end face was polished, and then sealed with an epoxy resin so that the electrical variable did not change due to contamination or moisture absorption of the end face, to obtain a thermal history sensor. Needless to say, the electrical variable includes a change in AC impedance such as a resistance change and a capacitance change.
[0023]
Some of these sensors were left in a thermostatic chamber at different temperatures, and changes in electrical variables were measured. Here, the resistance change was traced as an electrical variable. A curve as shown in FIG. 3 was obtained with time, and this was used as a master curve.
Moreover, when the same heat history sensor was created by the same method as the above embodiment except that epoxy adhesives (160 ° C. and 180 ° C.) having different glass transition temperatures were used, as shown in FIG. 4 and FIG. A curve was obtained.
[0024]
Also, in the temperature range higher than the glass transition temperature of the adhesive used for the thermal history sensor, the elastic modulus of the adhesive is greatly reduced, so the rate of change of resistance is extremely large, and practically around the maximum allowable temperature allowed for the product. It is desirable to use a thermal history sensor using an adhesive having a glass transition temperature of
[0025]
Generally, in the thermal history sensor of the present invention, the usable temperature range is from a temperature about 50 ° C. lower than the glass transition temperature of the adhesive used to a temperature about 10 ° C. higher than the vicinity of the glass transition temperature. By incorporating several thermal history sensors made using adhesives having different glass transition temperatures, the estimation accuracy of the thermal history is further improved.
[0026]
【The invention's effect】
As is apparent from the above description, by using the thermal history sensor of the present invention, estimation of thermal history, which has been difficult in the past, can be performed extremely simply.
Obtaining a thermal master curve, incorporating a sensor with the same characteristics as the master curve into the product, and grasping the thermal history easily by means of comparing the master curve with the means to measure the electrical variables of the sensor when necessary, Can be estimated.
[Brief description of the drawings]
FIG. 1 is a schematic external view of a thermal history sensor according to the present invention. FIG. 2 is a schematic enlarged sectional view of a thermal history sensor according to the present invention. FIG. 3 is a thermal history of a thermal history sensor prepared using an adhesive having a glass transition temperature of 120.degree. Master curve showing the relationship between the electrical resistance and the master curve [Fig. 4] Master curve showing the relationship between the thermal history and the electrical resistance of the thermal history sensor made using an adhesive having a glass transition temperature of 160 ° C [Fig. 5] Glass transition temperature of 180 ° C Master curve showing the relationship between thermal history and electrical resistance of thermal history sensors made with adhesives
1 Metal plate
2 Adhesive layer
3 Metal particles

Claims (3)

金属粒子(3)および接着剤の混合物で金属板(1)を貼り合せ、接着層(2)を有するサンドイッチ構造とし、該金属板(1)を貼り合せ硬化させる際に該金属粒子(3)が弾性変形を起こす程度に加圧することを特徴とし、該金属板(1)を電極とした熱履歴推定センサ。When a metal plate (1) is bonded with a mixture of metal particles (3) and an adhesive to form a sandwich structure having an adhesive layer (2), the metal particles (3 ) are bonded and cured when the metal plate (1) is bonded and cured. The thermal history estimation sensor using the metal plate (1) as an electrode. 該接着剤のガラス転移温度が0〜250℃であることを特徴とする請求項1記載の熱履歴推定用センサ。The thermal history estimation sensor according to claim 1, wherein the adhesive has a glass transition temperature of 0 to 250 ° C. 該電極間の電気変化を測定する手段とあらかじめ作成したマスターカーブとを比較する手段を設けたことを特徴とする請求項1〜2記載の熱履歴推定センサ。Thermal history estimating sensor according to claim 1 or 2, wherein in that a means for comparing the master curve prepared in advance with means for measuring the electrical changes between the electrodes.
JP2002360614A 2002-12-12 2002-12-12 Thermal history estimation sensor Expired - Fee Related JP3948725B2 (en)

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