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JP3344390B2 - Viscosity measurement method for green compacts - Google Patents
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JP3344390B2 - Viscosity measurement method for green compacts - Google Patents

Viscosity measurement method for green compacts

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Publication number
JP3344390B2
JP3344390B2 JP31250799A JP31250799A JP3344390B2 JP 3344390 B2 JP3344390 B2 JP 3344390B2 JP 31250799 A JP31250799 A JP 31250799A JP 31250799 A JP31250799 A JP 31250799A JP 3344390 B2 JP3344390 B2 JP 3344390B2
Authority
JP
Japan
Prior art keywords
sample
viscosity
green compact
temperature
calcined
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
Application number
JP31250799A
Other languages
Japanese (ja)
Other versions
JP2001133378A (en
Inventor
義人 二輪
洋 鷹木
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP31250799A priority Critical patent/JP3344390B2/en
Priority to DE10049022A priority patent/DE10049022B4/en
Priority to US09/679,208 priority patent/US6508106B1/en
Publication of JP2001133378A publication Critical patent/JP2001133378A/en
Priority to US10/191,032 priority patent/US6581439B2/en
Application granted granted Critical
Publication of JP3344390B2 publication Critical patent/JP3344390B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、非晶質ガラス粉末
等をプレス成形してなる圧粉成型体の粘度測定方法に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring the viscosity of a green compact formed by pressing an amorphous glass powder or the like.

【0002】[0002]

【従来の技術】近年、電子業界においては、実装部品や
回路導体の高密度化、信号の高周波化等に対応できるセ
ラミック多層基板や厚膜材料の研究・開発が盛んに行わ
れている。特に、非晶質ガラス粉末や結晶化ガラス粉末
を含んだ混合材料を焼成してなるセラミック多層基板
は、その比誘電率が小さく、また、比抵抗の小さなAg
導体材との同時焼成ができることから、高密度化や高周
波化に十分対応可能である。
2. Description of the Related Art In recent years, in the electronics industry, research and development of ceramic multilayer substrates and thick film materials capable of coping with high density of mounted components and circuit conductors, high frequency of signals, and the like have been actively conducted. In particular, a ceramic multilayer substrate formed by firing a mixed material containing an amorphous glass powder or a crystallized glass powder has a small relative dielectric constant and a small specific resistance.
Since simultaneous firing with a conductor material can be performed, it is possible to sufficiently cope with high density and high frequency.

【0003】こうしたセラミック多層基板において、非
晶質ガラス粉末、結晶化ガラス粉末等の酸化物無機粉末
の物性は、基板特性や厚膜特性に大きく寄与している。
なかでも、非晶質ガラス粉末の粘度特性は、その焼結プ
ロセスやAg導体の拡散挙動等を大きく左右するため、
材料設計やプロセス設計上、極めて重要なパラメータで
ある。
In such a ceramic multilayer substrate, the physical properties of an oxide inorganic powder such as an amorphous glass powder and a crystallized glass powder greatly contribute to substrate characteristics and thick film characteristics.
Above all, the viscosity characteristics of amorphous glass powder greatly affect the sintering process and diffusion behavior of Ag conductor, etc.
This is an extremely important parameter in material design and process design.

【0004】[0004]

【発明が解決しようとする課題】一般に、非晶質ガラス
粉末等の酸化物無機粉末の粘度は、おおよそ1010Pa
・S以上の高粘度領域については繊維延伸粘度計、おお
よそ104Pa・S以下の低粘度領域については回転式
粘度計(球体引き上げ粘度計)によって測定されてい
る。そして、焼結プロセスで特に重要な104〜109
a・Sの中粘度領域については、平行板加圧粘度計によ
る粘度測定が行われている。
Generally, the viscosity of an oxide inorganic powder such as an amorphous glass powder has a viscosity of about 10 10 Pa
A high viscosity region of S or higher is measured by a fiber drawing viscometer, and a low viscosity region of approximately 10 4 Pa · S or lower is measured by a rotary viscometer (spherical viscometer). Then, particularly important 10 4 to 10 9 P in the sintering process
For the medium viscosity region of a · S, the viscosity is measured by a parallel plate pressure viscometer.

【0005】以下、平行板加圧粘度計を用いた粘度ηの
測定方法を説明する。
Hereinafter, a method of measuring the viscosity η using a parallel plate pressure viscometer will be described.

【0006】まず、図22に示すように、支持台3に固
定された石英板2a上に、その高さH及び体積Vが正確
に測定された被測定物(試料)1を配置する。次いで、
これを石英ロッド4に固定された石英板2bで挟み込ん
だ後、石英ロッド4に一定荷重Mを加え、ヒータ5によ
って装置6内を昇温させながら、石英ロッド4に連動し
た差動トランス(図示省略)により、被測定物1の変位
(高さH)を検出する。そして、この変位を経時的に抽
出することによって被測定物1の試料変形速度dh/d
tを算出する。
First, as shown in FIG. 22, an object (sample) 1 whose height H and volume V are accurately measured is placed on a quartz plate 2a fixed to a support table 3. Then
After being sandwiched by a quartz plate 2b fixed to the quartz rod 4, a constant load M is applied to the quartz rod 4 and the temperature inside the device 6 is increased by the heater 5, and the differential transformer (shown in FIG. (Omitted), the displacement (height H) of the DUT 1 is detected. Then, by extracting this displacement with time, the sample deformation speed dh / d of the DUT 1 is obtained.
Calculate t.

【0007】次に、上述の手法で得られた被測定物の体
積V、試料高さH、試料変形速度dh/dtをGENT
式: η=2πMGH5/3V(dh/dt)(2πH3+V) (但し、M:荷重、H:試料高さ、G:重力加速度、
V:試料体積、dh/dt:試料変形速度)にそれぞれ
適用し、被測定物1の粘度ηを算出する(A.N.GENT, BR
ITISH JOURNAL OF APPLIED PHYSICS VOL.11, FEBRUARY
1960参照)。そして、これを各温度について実行して、
温度による粘度ηの変化、すなわち粘度−温度曲線を導
き出す。
Next, the volume V of the measured object, the sample height H, and the sample deformation speed dh / dt obtained by the above-described method are shown in GENT.
Formula: η = 2πMGH 5 / 3V (dh / dt) (2πH 3 + V) (However, M: load, H: sample height, G: gravitational acceleration,
V: sample volume, dh / dt: sample deformation rate) to calculate the viscosity η of the DUT 1 (ANGENT, BR)
ITISH JOURNAL OF APPLIED PHYSICS VOL.11, FEBRUARY
1960). And this is done for each temperature,
A change in viscosity η with temperature, that is, a viscosity-temperature curve is derived.

【0008】ところが、上述した平行板加圧粘度計によ
る粘度測定においては、被測定物1としてバルク試料を
用いることが必要である。つまり、GENT式は被測定
物1が非圧縮性流体と仮定できる場合に成立する粘度換
算式であって、例えば、非晶質ガラス粉末についての粘
度を測定したい場合、非晶質ガラス粉末を溶融、急冷し
てバルク状に成形した試料(バルク試料)を用いる必要
がある。
However, in the above-described viscosity measurement using a parallel plate pressure viscometer, it is necessary to use a bulk sample as the DUT 1. In other words, the GENT formula is a viscosity conversion formula that is established when the DUT 1 can be assumed to be an incompressible fluid. For example, when the viscosity of an amorphous glass powder is to be measured, the amorphous glass powder is melted. It is necessary to use a sample (bulk sample) which is rapidly cooled and formed into a bulk.

【0009】このように、上述した方法では、バルク状
に成形した試料の粘度測定は可能であるが、セラミック
多層基板や厚膜材料の材料設計やプロセス設計に大きな
影響を及ぼす粉末状態の試料については、その粘度を測
定することができない。
As described above, according to the above-described method, the viscosity of a sample formed in a bulk shape can be measured. However, for a sample in a powder state that has a great influence on the material design and process design of a ceramic multilayer substrate or a thick film material. Cannot measure its viscosity.

【0010】本発明は、上述した実情に鑑みてなされた
ものであり、その目的は、無機粉末をプレス成形してな
る圧粉成型体の粘度を高精度に測定する、圧粉成型体の
粘度測定方法を提供することにある。
The present invention has been made in view of the above-mentioned circumstances, and has as its object to measure the viscosity of a compact formed by pressing an inorganic powder with high accuracy. It is to provide a measuring method.

【0011】[0011]

【課題を解決するための手段】すなわち、本発明は、無
機粉末をプレス成形してなる圧粉成型体の粘度ηを、G
ENT式: η=2πMGH5/3V(dh/dt)(2πH3+V) (但し、M:荷重、H:試料高さ、G:重力加速度、
V:試料体積、dh/dt:試料変形速度)にしたがっ
て測定する圧粉成型体の粘度測定方法において、あらか
じめ仮焼した圧粉成型体を前記測定に用いることを特徴
とする、圧粉成型体の粘度測定方法に係るものである。
That is, according to the present invention, the viscosity η of a green compact formed by press-molding an inorganic powder is defined as G
ENT formula: η = 2πMGH 5 / 3V (dh / dt) (2πH 3 + V) (However, M: load, H: sample height, G: gravity acceleration,
(V: sample volume, dh / dt: sample deformation rate) in a method for measuring the viscosity of a green compact, wherein a pre-calcined green compact is used for the measurement. And a method for measuring viscosity.

【0012】本発明の圧粉成型体の粘度測定方法によれ
ば、前記圧粉成型体をあらかじめ仮焼しておくことによ
り、前記無機粉末の粒子同士が十分にネッキングするた
め、その粘性挙動が非圧縮性流体のそれに極めて近くな
り、したがって、各種無機粉末の粉末状態に極めて近い
粘性挙動を示す圧粉成型体について、その粘度を高精度
に測定できる。
According to the method of measuring the viscosity of a green compact of the present invention, the particles of the inorganic powder are sufficiently necked by calcining the green compact in advance, so that the viscous behavior of the powder is reduced. The viscosity can be measured with high accuracy for a compact formed body that is very close to that of an incompressible fluid and that exhibits a viscous behavior very close to the powder state of various inorganic powders.

【0013】[0013]

【発明の実施の形態】本発明の圧粉成型体の粘度測定方
法は、非晶質ガラス粉末等の無機粉末をプレス成形して
なる圧粉成型体の粘度ηを、GENT式: η=2πMGH5/3V(dh/dt)(2πH3+V) (但し、M:荷重、H:試料高さ、G:重力加速度、
V:試料体積、dh/dt:試料変形速度)にしたがっ
て測定するに際し、前記無機粉末の粒子同士が十分にネ
ッキングするような条件であらかじめ仮焼した圧粉成型
体を前記測定に用いるものである。なお、この仮焼は、
圧粉成型体について実施してもよいし、無機粉末につい
て実施してもよい。
BEST MODE FOR CARRYING OUT THE INVENTION The method of measuring the viscosity of a green compact according to the present invention is as follows: The viscosity η of a green compact obtained by press-molding an inorganic powder such as an amorphous glass powder is determined by the GENT formula: η = 2πMGH 5 / 3V (dh / dt) (2πH 3 + V) (however, M: load, H: sample height, G: gravitational acceleration,
(V: sample volume, dh / dt: sample deformation rate), in which a green compact molded in advance and calcined under conditions such that the particles of the inorganic powder are sufficiently necked is used for the measurement. . In addition, this calcining
It may be carried out on a green compact or on an inorganic powder.

【0014】また、本発明の圧粉成型体の粘度測定方法
においては、前記無機粉末を、非晶質ガラス粉末、結晶
化ガラス粉末、及び、ガラスセラミック複合粉末からな
る群より選ばれる1種の酸化物無機粉末とすることが望
ましい。なかでも、前記無機粉末としては、非晶質ガラ
ス粉末を用いることが望ましい。非晶質ガラス粉末は、
仮焼時の加熱・冷却に対して可逆的な性質を示すので、
仮焼温度、仮焼時間、昇温速度等について、比較的広い
条件を適用することができる。
In the method for measuring the viscosity of a green compact according to the present invention, the inorganic powder may be one kind selected from the group consisting of amorphous glass powder, crystallized glass powder, and glass-ceramic composite powder. It is desirable to use an oxide inorganic powder. Above all, it is desirable to use amorphous glass powder as the inorganic powder. Amorphous glass powder is
Since it shows reversible properties to heating and cooling during calcination,
A relatively wide range of conditions can be applied to the calcination temperature, calcination time, heating rate, and the like.

【0015】また、本発明の圧粉成型体の粘度測定方法
においては、前記仮焼を前記無機粉末の軟化温度以下で
実施することが望ましい。すなわち、非晶質ガラス粉
末、結晶化ガラス粉末、ガラスセラミック複合粉末等の
無機粉末を、その軟化温度(軟化点)以下で一定時間仮
焼し、その粒子同士を十分にネッキングさせることによ
って、仮焼後の圧粉成型体の粘性挙動を非圧縮性流体の
それに極めて近づけることができる。
In the method for measuring the viscosity of a green compact according to the present invention, it is preferable that the calcination is performed at a temperature lower than the softening temperature of the inorganic powder. That is, by calcining an inorganic powder such as an amorphous glass powder, a crystallized glass powder, and a glass ceramic composite powder at a temperature lower than its softening temperature (softening point) for a certain period of time and sufficiently necking the particles, thereby temporarily The viscous behavior of the green compact after firing can be made very close to that of the incompressible fluid.

【0016】したがって、仮焼後の圧粉成型体の試料体
積、試料高さについての実測値と、平行板加圧粘度計等
による試料変形速度の実測値(又は計算値)をGENT
式に適用するだけで、圧粉成型体の粘度を高精度に測定
することができる。
Therefore, the measured value (or calculated value) of the sample volume and sample height of the calcined green compact and the measured value (or calculated value) of the sample deformation rate measured by a parallel plate pressure viscometer or the like are used as GENT.
By simply applying the formula, the viscosity of the compact can be measured with high accuracy.

【0017】なお、前記仮焼は、無機粉末の軟化温度を
T(℃)とすると、T−10℃以上、すなわち軟化温度
マイナス10℃以上で実施することが望ましい。つま
り、前記仮焼温度をtとすると、 T−10≦t≦T の関係を満たすような範囲で仮焼すれば、粒子同士を十
分にネッキングさせたうえ、軟化流動による試料変形を
生じること無く、圧粉成型体の粘度を高精度に測定でき
る。
The calcination is preferably carried out at a temperature of T-10 ° C. or higher, that is, a softening temperature minus 10 ° C. or higher, where T (° C.) is the softening temperature of the inorganic powder. In other words, when the calcination temperature is t, if calcination is performed in a range that satisfies the relationship of T−10 ≦ t ≦ T, the particles are sufficiently necked and the sample is not deformed due to the softening flow. The viscosity of the compact can be measured with high accuracy.

【0018】次に、本発明の圧粉成型体の粘度測定方法
を、図1のフローチャートを一例に説明する。
Next, the method for measuring the viscosity of a green compact according to the present invention will be described with reference to the flowchart of FIG. 1 as an example.

【0019】図1に示すように、まず、高温溶融法やゾ
ル−ゲル法等によって、非晶質ガラス粉末を作製する。
次いで、この非晶質ガラス粉末を、有機バインダ(又は
水系バインダ)、溶剤等からなるビヒクル成分と共に混
合、分散する。そして、得られた混合物をプレス成型す
ることよって、非晶質ガラスからなる圧粉成型体を作製
する。
As shown in FIG. 1, first, an amorphous glass powder is prepared by a high-temperature melting method or a sol-gel method.
Next, the amorphous glass powder is mixed and dispersed together with a vehicle component including an organic binder (or an aqueous binder), a solvent, and the like. Then, the obtained mixture is press-molded to produce a green compact formed of amorphous glass.

【0020】次いで、この圧粉成型体を適当な温度で仮
焼し、粉末粒子間を十分にネッキングさせる。ここで、
適当な仮焼温度は、非晶質ガラス粉末の粒子間が十分に
ネッキングするような温度であり、望ましくは、その軟
化温度以下、さらに望ましくは、軟化温度以下かつ軟化
温度マイナス10℃以上である。
Next, the green compact is calcined at an appropriate temperature to sufficiently neck the powder particles. here,
An appropriate calcination temperature is a temperature at which the particles of the amorphous glass powder are sufficiently necked, and is desirably lower than the softening temperature, more desirably lower than the softening temperature and higher than the softening temperature minus 10 ° C. .

【0021】つまり、本発明においては、粉末粒子間を
十分にネッキングさせるような条件で仮焼すればよく、
仮焼時間、昇温速度等は特に限定されない。例えば、非
晶質ガラス粉末からなる圧粉成型体の場合、仮焼温度は
30〜90分程度、昇温速度は1〜10℃/分程度の範
囲を適宜選択できる。
That is, in the present invention, calcining may be performed under conditions such that powder particles are sufficiently necked.
The calcination time, the heating rate, and the like are not particularly limited. For example, in the case of a green compact formed of an amorphous glass powder, the calcining temperature can be appropriately selected in a range of about 30 to 90 minutes, and the heating rate can be appropriately selected in a range of about 1 to 10 ° C./min.

【0022】そして、仮焼後の圧粉成型体について、試
料高さH、試料体積Vをそれぞれ測定し、さらに、図2
2に示した如き平行板加圧粘度計を用い、その温度を徐
々に上昇させることによって、荷重Mを加えたときの圧
粉成型体の試料高さHを経時的に測定し、この測定結果
から試料変形速度dh/dtを算出する。
Then, the sample height H and the sample volume V of the green compact after calcination were measured, and FIG.
By using a parallel plate pressure viscometer as shown in FIG. 2 and gradually increasing the temperature, the sample height H of the green compact when a load M was applied was measured over time. From this, the sample deformation speed dh / dt is calculated.

【0023】その後、得られた試料高さH、試料体積V
及び試料変形速度dh/dtを上述したGENT式に適
用して、圧粉成型体の粘度η(粘度−温度曲線)を導き
出す。
Thereafter, the obtained sample height H and sample volume V
By applying the sample deformation rate dh / dt to the above-mentioned GENT equation, the viscosity η (viscosity-temperature curve) of the green compact is derived.

【0024】このように、平行板加圧粘度計に供する前
に圧粉成型体を仮焼しておくことにより、セラミック多
層基板や厚膜材料等に用いられる非晶質ガラス粉末の粘
度η、さらには粘度−温度曲線を高精度に測定可能とな
る。つまり、非晶質ガラス粉末について、その粉末状態
に極めて近い粘性挙動を示す圧粉成型体の粘性評価を行
うことができるようになる。
As described above, by calcining the green compact before applying it to the parallel plate pressure viscometer, the viscosity η of the amorphous glass powder used for the ceramic multilayer substrate, the thick film material, etc. Further, the viscosity-temperature curve can be measured with high accuracy. That is, it becomes possible to evaluate the viscosity of the green compact which exhibits a viscous behavior very close to the powder state of the amorphous glass powder.

【0025】以上、本発明の圧粉成型体の粘度測定方法
を非晶質ガラス粉末について説明したが、本発明は、こ
の非晶質ガラス粉末からなる圧粉成型体の粘度測定に限
定されるものではない。
Although the method for measuring the viscosity of a green compact according to the present invention has been described above for an amorphous glass powder, the present invention is limited to the measurement of the viscosity of a green compact formed from this amorphous glass powder. Not something.

【0026】例えば、結晶化ガラス粉末やガラスセラミ
ック複合粉末、さらにはその他の無機粉末についても、
同様に適用することにより、その粘度ηを高精度に導き
出し、さらには粘度−温度曲線を高精度に作製すること
ができる。但し、結晶化ガラス粉末やガラスセラミック
複合粉末について本発明を適用する場合、その昇温速度
は例えば1〜5℃/分のようにできるだけ低い方がよ
い。析出する結晶の核を十分に形成できるからである。
For example, crystallized glass powder, glass ceramic composite powder, and other inorganic powders
By similarly applying, the viscosity η can be derived with high accuracy, and further, the viscosity-temperature curve can be prepared with high accuracy. However, when the present invention is applied to crystallized glass powder or glass-ceramic composite powder, the rate of temperature rise is preferably as low as possible, for example, 1 to 5 ° C./min. This is because nuclei of precipitated crystals can be sufficiently formed.

【0027】なお、本発明において、仮焼後の圧粉成型
体は非圧縮性流体に極めて近い粘性挙動を示すが、圧粉
成型体中のバインダの残存状態等によっては、それらの
粘性挙動とはやや異なる挙動を示すことがある。このよ
うな場合、以下に示すように、GENT式を補正してよ
い。
In the present invention, the green compact after calcination exhibits a viscous behavior very close to that of an incompressible fluid. However, depending on the residual state of the binder in the green compact, the viscous behavior of the green compact may be reduced. May exhibit slightly different behavior. In such a case, the GENT equation may be corrected as described below.

【0028】すなわち、上述したように、GENT式
は、被測定物が非圧縮性流体と仮定できる場合に成立す
る粘度換算式である。これに対して、無機粉末とビヒク
ルとをプレス成型によって固めた圧粉成型体は、その焼
成が進むに連れて、バインダの揮発等に伴う体積変化が
生じることがある。
That is, as described above, the GENT equation is a viscosity conversion equation that is satisfied when the object to be measured can be assumed to be an incompressible fluid. On the other hand, in a green compact formed by press-molding an inorganic powder and a vehicle, a volume change accompanying the volatilization of a binder or the like may occur as the firing proceeds.

【0029】この体積変化を補正するには、まず、圧粉
成型体の見かけの体積に圧粉成型体中の無機粉末の充填
率を乗じた体積を、試料体積補正値V’とし、このV’
をGENT式に適用することができる。なお、無機粉末
の充填率は、無機粉末の粉体真比重、調合比、圧粉成型
体の重量から容易に算出できる。
In order to correct this volume change, first, a volume obtained by multiplying the apparent volume of the green compact by the filling rate of the inorganic powder in the green compact is defined as a sample volume correction value V ′. '
Can be applied to the GENT equation. The filling rate of the inorganic powder can be easily calculated from the true specific gravity of the inorganic powder, the mixing ratio, and the weight of the compact.

【0030】例えば、図2のフローチャートに示すよう
に、無機粉末の重量m1、真比重n1、圧粉成型体の試料
重量m、無機粉末の調合量w1、ビヒクル成分の調合量
2を測定し、下式にしたがって、試料体積補正値V’
を算出することができる。 V’=m1/n1、m1=m×{w1/(w1+w
2)}
For example, as shown in the flowchart of FIG. 2, the weight m 1 of the inorganic powder, the true specific gravity n 1 , the sample weight m of the green compact, the amount w 1 of the inorganic powder, and the amount w 2 of the vehicle component Is measured, and the sample volume correction value V ′ is calculated according to the following equation.
Can be calculated. V ′ = m1 / n1, m1 = m × {w1 / (w1 + w
2)}

【0031】また、圧粉成型体の変位について焼結収縮
が支配的な温度領域では、焼結収縮に伴う試料変形速度
を考慮することが望ましい。すなわち、図3に示すよう
に、圧粉成型体の見かけの試料変形速度は、塑性変形に
伴う試料変形速度と焼結収縮に伴う試料変形速度とが含
まれているため、この粘度領域については、それを相殺
した試料変形速度、すなわち試料変形速度補正値(dh
/dt)’をGENT式に適用することが望ましい。
In the temperature region where the sintering shrinkage is dominant in the displacement of the green compact, it is desirable to consider the sample deformation speed accompanying the sintering shrinkage. That is, as shown in FIG. 3, the apparent sample deformation rate of the green compact includes the sample deformation rate due to plastic deformation and the sample deformation rate due to sintering shrinkage. , The sample deformation speed that compensated for it, ie, the sample deformation speed correction value (dh
/ Dt) ′ is desirably applied to the GENT equation.

【0032】ここで、図3に示すように、焼結収縮が支
配的な温度領域Xでは、荷重ゼロでの試料変形速度(d
h/dt)0を焼結収縮に伴う試料変形速度と見なすこ
とができる。したがって、この温度領域Xについての試
料変形速度を導き出すためには、荷重ゼロでの試料変形
速度(dh/dt)0を算出すればよい。
Here, as shown in FIG. 3, in the temperature region X where sintering shrinkage is dominant, the sample deformation rate (d
h / dt) 0 can be regarded as the sample deformation rate accompanying sintering shrinkage. Therefore, in order to derive the sample deformation speed in the temperature region X, the sample deformation speed (dh / dt) 0 at zero load may be calculated.

【0033】この荷重ゼロでの試料変形速度(dh/d
t)0は、図3に示すように、荷重A、荷重B、・・・
のように、荷重を振ったときの試料変形速度(dh/d
t) A、(dh/dt)B・・・を測定し、さらに、それ
ぞれの温度における荷重と試料変形速度の関係が直線近
似できると仮定したうえで荷重ゼロに外挿した値を荷重
ゼロでの試料変形速度(dh/dt)0として算出す
る。
This sample deformation rate at zero load (dh / d
t)0Are loads A, B,... As shown in FIG.
, The sample deformation speed (dh / d
t) A, (Dh / dt)B... and then it
The relationship between the load and the sample deformation rate at each temperature is close to a straight line
The value extrapolated to zero load is assumed to be similar
Sample deformation speed at zero (dh / dt)0Calculated as
You.

【0034】具体的には、図4のフローチャートに示す
ように、圧粉成型体について、温度T1のときの荷重A
での試料変形速度(dh/dt)A、荷重Bでの試料変
形速度(dh/dt)Bを測定する。そして、荷重Aで
の試料変形速度(dh/dt)A、荷重Bでの試料変形
速度(dh/dt)Bを用いて最小二乗法による直線近
似を実行することにより、温度T1のときの荷重ゼロで
の試料変形速度(dh/dt)0を算出する。
[0034] Specifically, as shown in the flowchart of FIG. 4, the green compact, the load A when the temperature T 1 of
Sample deformation rate at (dh / dt) A, to measure the sample deformation rate (dh / dt) B at load B. By executing the linear fit according to the least square method using the sample deformation rate (dh / dt) A at load A, the sample deformation rate (dh / dt) B at load B, when the temperatures T 1 Calculate the sample deformation speed (dh / dt) 0 at zero load.

【0035】同様にして、温度T2、T3・・・のときの
荷重ゼロでの試料変形速度(dh/dt)0を算出し、
図5に示すように、荷重ゼロでの試料変形速度−温度曲
線((dh/dt)0−T曲線)を作製する。なお、荷
重Aでの試料変形速度−温度曲線、荷重Bでの試料変形
速度−温度曲線を作製し、これらの曲線から荷重ゼロで
の試料変形速度−温度曲線((dh/dt)0−T曲
線)を一括に算出することもできる。
Similarly, the sample deformation speed (dh / dt) 0 at zero load at the temperatures T 2 , T 3, ...
As shown in FIG. 5, a sample deformation speed-temperature curve ((dh / dt) 0 -T curve) at zero load is prepared. A sample deformation speed-temperature curve under load A and a sample deformation speed-temperature curve under load B were prepared. From these curves, a sample deformation speed-temperature curve at zero load ((dh / dt) 0 -T Curve) can be calculated at once.

【0036】次いで、図4のフローチャートに示すよう
に、焼結収縮が支配的な温度領域Xに適用する試料変形
速度補正値(dh/dt)’を算出する。この試料変形
速度補正値(dh/dt)’は、見かけの試料変形速度
と焼結収縮に伴う試料変形速度との差を取ることにより
算出できる。
Next, as shown in the flow chart of FIG. 4, a sample deformation speed correction value (dh / dt) ′ to be applied to the temperature region X where sintering shrinkage is dominant is calculated. The sample deformation speed correction value (dh / dt) 'can be calculated by taking the difference between the apparent sample deformation speed and the sample deformation speed accompanying sintering shrinkage.

【0037】具体的には、見かけの試料変形速度である
荷重Aでの試料変形速度(dh/dt)A、又は、荷重
Bでの試料変形速度(dh/dt)Bから、焼結収縮に
伴う試料変形速度である荷重ゼロでの試料変形速度(d
h/dt)0を差し引いた値を試料変形速度補正値(d
h/dt)’とすることができる。この操作を、温度T
1、T2、T3・・・について行い、各温度での試料変形
速度補正値(dh/dt)’を算出する。
Specifically, it is the apparent sample deformation speed.
Sample deformation rate under load A (dh / dt)AOr load
Sample deformation speed at B (dh / dt)BFrom sintering shrinkage
The sample deformation rate at zero load, which is the sample deformation rate (d
h / dt)0Is subtracted from the sample deformation speed correction value (d
h / dt) '. This operation is performed at the temperature T
1, TTwo, TThree…, Deformation of the sample at each temperature
The speed correction value (dh / dt) 'is calculated.

【0038】さらに、図4のフローチャートに示すよう
に、焼結収縮が支配的な温度領域Xと、塑性変形が支配
的な温度領域Yとを分離する。この分離は、図5に示し
た荷重ゼロのときの試料変形速度−温度曲線((dh/
dt)0−T曲線)に基づき実行できる。
Further, as shown in the flowchart of FIG. 4, a temperature region X in which sintering shrinkage is dominant and a temperature region Y in which plastic deformation is dominant are separated. This separation is caused by the sample deformation rate-temperature curve ((dh /
dt) 0 -T curve).

【0039】具体的には、図5に示すように、荷重ゼロ
での試料変形速度−温度曲線((dh/dt)0−T曲
線)における極小値を、その境界温度Tbと見なし、境
界温度Tbよりも低温度側を焼結収縮が支配的な温度領
域X、境界温度Tbよりも高温度側を塑性変形が支配的
な温度領域Yとする。
Specifically, as shown in FIG. 5, the minimum value in the sample deformation speed-temperature curve ((dh / dt) 0 -T curve) at zero load is regarded as its boundary temperature Tb, A temperature region lower than Tb is defined as a temperature region X in which sintering shrinkage is dominant, and a temperature region higher than the boundary temperature Tb is defined as a temperature region Y in which plastic deformation is dominant.

【0040】そして、図6に示すように、圧粉成型体の
変位について、焼結収縮が支配的な温度領域Xでは、G
ENT式について、 試料体積V→試料体積補正値V’ 試料変形速度dh/dt→試料変形速度補正値(dh/
dt)’ の補正を実行し、他方、塑性変形が支配的な温度領域Y
では、GENT式について、 試料体積V→試料体積補正値V’ の補正を実行する。
As shown in FIG. 6, with respect to the displacement of the green compact, in the temperature region X where sintering shrinkage is dominant, G
Regarding the ENT equation, sample volume V → sample volume correction value V ′ sample deformation speed dh / dt → sample deformation speed correction value (dh /
dt) ′, while plastic deformation is dominant in the temperature region Y
Then, correction of the sample volume V → the sample volume correction value V ′ is performed for the GENT equation.

【0041】本発明によれば、こうした一連のGENT
式補正によって、仮焼後の圧粉成型体の粘度をさらに高
精度に測定することができ、非晶質ガラス粉末をはじめ
として、結晶化ガラス粉末、ガラスセラミック複合粉末
等についても、その温度−粘度曲線をより高精度に作製
できるようになる。
According to the present invention, such a series of GENT
By the formula correction, the viscosity of the green compact after calcination can be measured with higher accuracy. The temperature of amorphous glass powder, crystallized glass powder, glass ceramic composite powder, etc. A viscosity curve can be created with higher accuracy.

【0042】すなわち、本発明の圧粉成型体の粘度測定
方法においては、(A)仮焼後の圧粉成型体の試料体積
補正値V’(但し、試料体積補正値V’は、前記圧粉成
型体中の前記無機粉末が占める体積)を求めるステッ
プ、(B)仮焼後の圧粉成型体の試料変形速度補正値
(dh/dt)’(但し、試料変形速度補正値(dh/
dt)’は、見かけの試料変形速度と焼結収縮に伴う試
料変形速度との差)を求めるステップ、(C)仮焼後の
圧粉成型体の変位について、焼結収縮が支配的な温度領
域X、塑性変形が支配的な温度領域Yを分離するステッ
プ、(D)前記焼結収縮が支配的な温度領域Xについて
は、前記GENT式の試料体積Vとして前記試料体積補
正値V’を適用し、かつ、試料変形速度dh/dtとし
て前記試料変形速度補正値(dh/dt)’を適用する
ステップ、(E)前記塑性変形が支配的な温度領域Yに
ついては、前記GENT式の試料体積Vとして前記試料
体積補正値V’を適用するステップ、を有していてもよ
い。
That is, in the method for measuring the viscosity of a green compact according to the present invention, (A) the sample volume correction value V ′ of the green compact after calcination (provided that the sample volume correction value V ′ (B) a sample deformation speed correction value (dh / dt) 'of the green compact after calcination (where the sample deformation speed correction value (dh /
dt) ′ is the step of obtaining the difference between the apparent sample deformation rate and the sample deformation rate due to sintering shrinkage), and (C) the temperature at which sintering shrinkage is dominant for the displacement of the green compact after calcination. (D) For the temperature region X where the sintering shrinkage is dominant, the sample volume correction value V ′ is defined as the sample volume V of the GENT equation. Applying the sample deformation speed correction value (dh / dt) ′ as the sample deformation speed dh / dt, and (E) the GENT-type sample for the temperature region Y where the plastic deformation is dominant. Applying the sample volume correction value V ′ as the volume V.

【0043】また、前記見かけの試料変形速度として、
荷重Aでの試料変形速度(dh/dt)A、荷重Bでの
試料変形速度(dh/dt)Bをそれぞれ求め(但し、
荷重A≠荷重B)、前記荷重Aでの試料変形速度(dh
/dt)A、前記荷重Bでの試料変形速度(dh/d
t)Bの直線近似を行い、荷重ゼロの外挿値を荷重ゼロ
での試料変形速度(dh/dt)0として求め、前記荷
重ゼロでの試料変形速度(dh/dt)0を前記焼結収
縮に伴う試料変形速度と見なし、前記荷重Aでの試料変
形速度(dh/dt)A、又は、前記荷重Bでの試料変
形速度(dh/dt)Bから、前記荷重ゼロでの試料変
形速度(dh/dt)0を差し引いた値を、前記試料変
形速度補正値(dh/dt)’とすることができる。
Further, as the apparent sample deformation speed,
Calculated sample deformation rate of a load A (dh / dt) A, sample deformation rate of a load B a (dh / dt) B respectively (where,
Load A ≠ Load B), Sample deformation speed at the load A (dh
/ Dt) A , the sample deformation rate under the load B (dh / d
t) A linear approximation of B is performed, and an extrapolated value at zero load is determined as a sample deformation speed at zero load (dh / dt) 0 , and the sample deformation speed at zero load (dh / dt) 0 is calculated by the sintering. Considering the sample deformation speed due to shrinkage, from the sample deformation speed (dh / dt) A at the load A or the sample deformation speed (dh / dt) B at the load B, the sample deformation speed at the zero load The value obtained by subtracting (dh / dt) 0 can be used as the sample deformation speed correction value (dh / dt) ′.

【0044】但し、3点以上の異なる荷重(例えば、荷
重A、荷重B及び荷重C:但し、荷重A≠荷重B≠荷重
C)での試料変形速度から、荷重ゼロでの試料変形速度
(dh/dt)0を直線近似によって求めることが望ま
しい。その方が荷重ゼロでの試料変形速度(dh/d
t)0をより正確に抽出できるからである。
However, from the sample deformation rate at three or more different loads (eg, load A, load B and load C: where load A 荷重 load B ≠ load C), the sample deformation rate at zero load (dh) / Dt) It is desirable to obtain 0 by linear approximation. The sample deformation rate at zero load (dh / d
This is because t) 0 can be extracted more accurately.

【0045】この場合、特に、前記荷重Aと前記荷重B
の関係を、荷重A<荷重Bとし、荷重Bでの試料変形速
度(dh/dt)Bと、前記荷重ゼロでの試料変形速度
(dh/dt)0との差を前記試料変形速度補正値(d
h/dt)’とすることが望ましい。試料変形速度補正
値(dh/dt)’を算出する際の見かけの試料変形速
度を荷重小のときの試料変形速度とすると、試料変形速
度補正値を抽出する際のバラツキが大きくなってしまう
傾向がある。
In this case, in particular, the load A and the load B
Is the load A <load B, and the difference between the sample deformation speed (dh / dt) B at load B and the sample deformation speed (dh / dt) 0 at zero load is the sample deformation speed correction value. (D
h / dt) ′. If the apparent sample deformation speed at the time of calculating the sample deformation speed correction value (dh / dt) ′ is the sample deformation speed when the load is small, the variation in extracting the sample deformation speed correction value tends to increase. There is.

【0046】また、本発明においては、前記荷重ゼロで
の試料変形速度(dh/dt)0にしたがって荷重ゼロ
での試料変形速度−温度曲線を作製し、その極小値を境
界温度Tbとして、境界温度Tbよりも低温側を前記焼
結収縮が支配的な温度領域X、境界温度Tbよりも高温
側を前記塑性変形が支配的な温度領域Yとすることがで
きる。
Further, in the present invention, a sample deformation speed at zero load-temperature curve is prepared according to the sample deformation speed at zero load (dh / dt) 0 , and a minimum value thereof is defined as a boundary temperature Tb. The temperature range X where the sintering shrinkage is dominant on the side lower than the temperature Tb can be set as the temperature range Y where the plastic deformation is dominant on the side higher than the boundary temperature Tb.

【0047】但し、境界温度の抽出方法は、上記の方法
に限定されるものではなく、例えば、バルク試料につい
ての試料変形速度−温度曲線を作製し、荷重ゼロでの試
料変形速度−温度曲線が、バルク試料についての試料変
形速度−温度曲線に追随する温度領域を塑性変形が支配
的な温度領域Yと見なすこともできる。
However, the method of extracting the boundary temperature is not limited to the above method. For example, a sample deformation speed-temperature curve for a bulk sample is prepared, and the sample deformation speed-temperature curve at zero load is obtained. The temperature region following the sample deformation speed-temperature curve of the bulk sample can be regarded as a temperature region Y in which plastic deformation is dominant.

【0048】[0048]

【実施例】以下、本発明を具体的な実施例について説明
する。
The present invention will be described below with reference to specific examples.

【0049】まず、高温溶融法によって、試料1、試料
2及び試料3で表される非晶質ガラス粉末を作製した。
試料1、試料2及び試料3の非晶質ガラス粉末の組成
系、熱特性、粉体特性等を下記表1に示す。
First, amorphous glass powders represented by Sample 1, Sample 2 and Sample 3 were produced by a high-temperature melting method.
Table 1 below shows the composition systems, thermal characteristics, powder characteristics, and the like of the amorphous glass powders of Sample 1, Sample 2, and Sample 3.

【0050】[0050]

【表1】 [Table 1]

【0051】次に、試料1、試料2及び試料3の各非晶
質ガラス粉末に水系ビヒクル(酢酸ビニル系)を加え、
ボールミルを用いて混合、分散した。その後、得られた
混合物を金型(φ7mm)を用いてプレス成形し、高さ
8〜8.5mm、直径7〜7.5mmの円柱状圧粉成型
体を作製した。
Next, an aqueous vehicle (vinyl acetate) was added to each of the amorphous glass powders of Samples 1, 2 and 3.
They were mixed and dispersed using a ball mill. Then, the obtained mixture was press-molded using a metal mold (φ7 mm) to produce a columnar compact having a height of 8 to 8.5 mm and a diameter of 7 to 7.5 mm.

【0052】そして、試料1〜3の各非晶質ガラス粉末
からなる圧粉成型体について、電気炉を用いてその圧粉
成型体を軟化点付近で仮焼させ、仮焼後の直径、高さを
マイクロメーターにて測定した。なお、仮焼は、室温か
ら仮焼温度まで3℃/分で昇温させ、仮焼温度で1時間
キープさせてから自然放冷で室温まで降ろすといったプ
ログラムを用いた。
Then, with respect to the green compact formed of each of the amorphous glass powders of Samples 1 to 3, the green compact was calcined in the vicinity of the softening point by using an electric furnace, and the diameter and the high The length was measured with a micrometer. The calcining was performed using a program in which the temperature was raised from room temperature to the calcining temperature at a rate of 3 ° C./min, kept at the calcining temperature for one hour, and allowed to cool to room temperature.

【0053】また、比較のため、表1に示した各組成系
の非晶質ガラス粉末を用いて、バルク試料を作製した。
これらのバルク試料は、各非晶質ガラス粉末を白金るつ
ぼ中に流し込み、それを溶融させ、徐冷温度から室温ま
で徐冷した後、バルクの平行度を出すため、研磨装置に
て研磨を行ったもので、得られた試料は、高さ6mm、
直径7mmの円柱状バルク試料である。
For comparison, a bulk sample was prepared using amorphous glass powder of each composition shown in Table 1.
For these bulk samples, each amorphous glass powder was poured into a platinum crucible, melted and gradually cooled from a slow cooling temperature to room temperature, and then polished with a polishing device to obtain bulk parallelism. The obtained sample was 6 mm high,
It is a cylindrical bulk sample having a diameter of 7 mm.

【0054】次に、試料1、試料2、試料3の圧粉成型
体について、図22に示した構成の平行板加圧粘度計
(オプト企業社製)を用いて試料変位を測定し、上述し
た手順にしたがって、粘度−温度曲線を求めた。なお、
各試料については、荷重138.8gを加え、平行板加
圧粘度計による試料変位測定時の昇温速度は5℃/分と
した。また、同様にしてバルク試料の粘度−温度曲線を
求めた。
Next, with respect to the green compacts of Sample 1, Sample 2, and Sample 3, the sample displacement was measured using a parallel plate pressure viscometer (manufactured by Opto Corporation) having the structure shown in FIG. According to the procedure described above, a viscosity-temperature curve was determined. In addition,
A load of 138.8 g was applied to each sample, and the rate of temperature rise at the time of sample displacement measurement using a parallel plate pressure viscometer was 5 ° C./min. Similarly, a viscosity-temperature curve of the bulk sample was determined.

【0055】また、仮焼温度は、試料1、試料2、試料
3のそれぞれ圧粉成型体及びバルク試料について、 (1)軟化点プラス50℃ (2)軟化点プラス30℃ (3)軟化点プラス20℃ (4)軟化点プラス10℃ (5)軟化点 (6)軟化点マイナス10℃ (7)軟化点マイナス20℃ (8)軟化点マイナス30℃ (9)軟化点マイナス50℃ の9条件で行った。また、モニターとして仮焼しない場
合も測定した。
The calcination temperature was as follows: (1) softening point plus 50 ° C. (2) softening point plus 30 ° C. (3) softening point Plus 20 ° C (4) softening point plus 10 ° C (5) softening point (6) softening point minus 10 ° C (7) softening point minus 20 ° C (8) softening point minus 30 ° C (9) softening point minus 50 ° C 9 Performed under conditions. In addition, the measurement was also performed when not calcined as a monitor.

【0056】その結果、試料1、試料2、試料3のいず
れの圧粉成型体においても、軟化点より高い仮焼温度で
行った場合(1)〜(4)、試料変形が生じることがあ
った。すなわち、非晶質ガラス粉末の軟化点よりも高い
温度で仮焼すると、圧粉成型体中のガラス粉末が軟らか
くなり、それが流動して、圧粉成型体の試料形態が保持
できなくなることがあった。このことから、仮焼温度は
軟化点よりも低い温度であることが望まれる。
As a result, in any of the green compacts of Sample 1, Sample 2, and Sample 3, when the calcination temperature is higher than the softening point (1) to (4), the sample may be deformed. Was. That is, when calcined at a temperature higher than the softening point of the amorphous glass powder, the glass powder in the green compact becomes soft and flows, and the sample form of the green compact cannot be maintained. there were. From this, it is desired that the calcination temperature is lower than the softening point.

【0057】また、試料1の圧粉成型体については、そ
れを軟化点、すなわち450℃で仮焼した場合(5)、
図7に示すように、仮焼したときの粘度−温度曲線
「●」は、バルク法による粘度曲線「□」に近づいてい
ることが分かる。これは軟化点、すなわち450℃で
は、圧粉成型体において、粉末粒子間のネッキングが十
分であるため、その粘性挙動が非圧縮性流体のそれと極
めて近くなっていると思われる。また、それを軟化点マ
イナス10℃(440℃)で仮焼した場合(6)、図8
に示すように、前記と同様に仮焼したときの粘度−温度
曲線「●」は、バルク法による粘度曲線「□」に近づい
ていることが分かる。これは軟化点マイナス10℃、す
なわち440℃でも、圧粉成型体において、粉末粒子間
のネッキングが十分であるため、その粘性挙動が非圧縮
性流体のそれと極めて近くなっていると思われる。な
お、本手法における粘度の目安は同一粘度における温度
で、バルクとの差が2%以内である。
When the green compact of Sample 1 was calcined at its softening point, ie, 450 ° C. (5),
As shown in FIG. 7, it can be seen that the viscosity-temperature curve “•” when calcined approaches the viscosity curve “□” by the bulk method. It seems that at the softening point, that is, at 450 ° C., the necking between the powder particles is sufficient in the green compact, so that its viscous behavior is very close to that of the incompressible fluid. When it was calcined at a softening point minus 10 ° C. (440 ° C.) (6), FIG.
As shown in the figure, it can be seen that the viscosity-temperature curve “●” when calcined in the same manner as above approaches the viscosity curve “□” by the bulk method. It seems that even at the softening point minus 10 ° C., that is, 440 ° C., the necking between the powder particles is sufficient in the green compact, so that its viscous behavior is very close to that of the incompressible fluid. The standard of the viscosity in this method is a temperature at the same viscosity, and the difference from the bulk is within 2%.

【0058】これに対して、試料1の圧粉成型体を軟化
点マイナス20℃(430℃)で仮焼した場合(7)、
軟化点マイナス30℃(420℃)で仮焼した場合
(8)、軟化点マイナス50℃(400℃)で仮焼した
場合(9)、それぞれ図9、図10、図11に示すよう
に、仮焼したときの粘度−温度曲線「●」は、バルク法
による粘度曲線「□」から離れて、仮焼しない場合の粘
度曲線「△」に近づいていることが分かる。これは軟化
点マイナス10℃より低い温度、すなわち440℃より
低温では、圧粉成型体が十分に仮焼されず、粉末粒子間
のネッキングが不完全であったためと思われる。
On the other hand, when the green compact of Sample 1 was calcined at a softening point of minus 20 ° C. (430 ° C.) (7),
When calcined at a softening point of minus 30 ° C. (420 ° C.) (8), and when calcined at a softening point of minus 50 ° C. (400 ° C.) (9), as shown in FIG. 9, FIG. It can be seen that the viscosity-temperature curve “●” when calcined departs from the viscosity curve “□” by the bulk method and approaches the viscosity curve “△” when not calcined. This is presumably because at a temperature lower than the softening point minus 10 ° C., that is, at a temperature lower than 440 ° C., the green compact was not calcined sufficiently and the necking between the powder particles was incomplete.

【0059】また、試料2の圧粉成型体については、そ
れを軟化点、すなわち430℃で仮焼した場合(5)、
図12に示すように、仮焼したときの粘度−温度曲線
「●」は、バルク法による粘度曲線「□」に近づいてい
ることが分かる。これは軟化点、すなわち430℃で
は、圧粉成型体において、粉末粒子間のネッキングが十
分であるため、その粘性挙動が非圧縮性流体のそれと極
めて近くなっていると思われる。また、それを軟化点マ
イナス10℃(420℃)で仮焼した場合(6)、図1
3に示すように、前記と同様に仮焼したときの粘度−温
度曲線「●」は、バルク法による粘度曲線「□」に近づ
いていることが分かる。これは軟化点マイナス10℃、
すなわち420℃でも、圧粉成型体において、粉末粒子
間のネッキングが十分であるため、その粘性挙動が非圧
縮性流体のそれと極めて近くなっていると思われる。な
お、本手法における粘度の目安は同一粘度における温度
で、バルクとの差が2%以内である。
When the green compact of Sample 2 was calcined at the softening point, ie, 430 ° C. (5),
As shown in FIG. 12, it can be seen that the viscosity-temperature curve “●” when calcined approaches the viscosity curve “□” by the bulk method. This seems to indicate that at the softening point, ie, 430 ° C., in the green compact, the necking between the powder particles is sufficient, so that its viscous behavior is very close to that of the incompressible fluid. When calcined at a softening point minus 10 ° C (420 ° C) (6), FIG.
As shown in FIG. 3, it can be seen that the viscosity-temperature curve “•” when calcined in the same manner as described above approaches the viscosity curve “□” by the bulk method. This is the softening point minus 10 ° C,
That is, even at 420 ° C., the necking between the powder particles is sufficient in the green compact, so that its viscous behavior seems to be very close to that of the incompressible fluid. The standard of the viscosity in this method is a temperature at the same viscosity, and the difference from the bulk is within 2%.

【0060】これに対して、試料2の圧粉成型体を軟化
点マイナス20℃(410℃)で仮焼した場合(7)、
軟化点マイナス30℃(400℃)で仮焼した場合
(8)、軟化点マイナス50℃(380℃)で仮焼した
場合(9)、それぞれ図14、図15、図16に示すよ
うに、仮焼したときの粘度−温度曲線「●」は、バルク
法による粘度曲線「□」とは離れて、仮焼しない場合の
粘度曲線「△」に近づいていることが分かる。これは、
上述したのと同様に、軟化点マイナス10℃より低い温
度、すなわち420℃より低温では、圧粉成型体が十分
に仮焼されず、粉末粒子間のネッキングが不完全であっ
たためと思われる。
On the other hand, when the green compact of Sample 2 was calcined at a softening point of minus 20 ° C. (410 ° C.) (7),
When calcined at a softening point minus 30 ° C. (400 ° C.) (8) and when calcined at a softening point minus 50 ° C. (380 ° C.) (9), as shown in FIGS. It can be seen that the viscosity-temperature curve “●” when calcined is different from the viscosity curve “□” according to the bulk method and approaches the viscosity curve “△” when not calcined. this is,
As described above, at a temperature lower than the softening point minus 10 ° C., that is, lower than 420 ° C., it is considered that the green compact was not sufficiently calcined, and necking between powder particles was incomplete.

【0061】一方、試料3の圧粉成型体においては、そ
れを軟化点、すなわち560℃で仮焼した場合(5)、
図17に示すように、仮焼したときの粘度−温度曲線
「●」は、バルク法による粘度曲線「□」に近づいてい
ることが分かる。これは軟化点、すなわち560℃で
は、圧粉成型体において、粉末粒子間のネッキングが十
分であるため、その粘性挙動が非圧縮性流体のそれと極
めて近くなっていると思われる。また、それを軟化点マ
イナス10℃(550℃)で仮焼した場合(6)、図1
8に示すように、前記と同様に仮焼したときの粘度−温
度曲線「●」は、バルク法による粘度曲線「□」に近づ
いていることが分かる。これは軟化点マイナス10℃、
すなわち550℃でも、圧粉成型体において、粉末粒子
間のネッキングが十分であるため、その粘性挙動が非圧
縮性流体のそれと極めて近くなっていると思われる。さ
らに、それを軟化点マイナス20℃(540℃)で仮焼
した場合(7)、軟化点マイナス30℃(530℃)で
仮焼した場合(8)であっても、図19、図20にそれ
ぞれ示すように、前記と同様に仮焼したときの粘度−温
度曲線「●」は、バルク法による粘度曲線「□」に近づ
いていることが分かる。これは軟化点マイナス20℃、
すなわち420℃や軟化点マイナス30℃、すなわち4
10℃でも、圧粉成型体において、粉末粒子間のネッキ
ングが十分であるため、その粘性挙動が非圧縮性流体の
それと極めて近くなっていると思われる。なお、本手法
における粘度の目安は同一粘度における温度で、バルク
との差が2%以内である。
On the other hand, in the green compact of Sample 3, when it was calcined at the softening point, ie, 560 ° C. (5),
As shown in FIG. 17, it can be seen that the viscosity-temperature curve “●” when calcined approaches the viscosity curve “□” by the bulk method. This seems to indicate that at the softening point, ie, 560 ° C., in the green compact, the necking between the powder particles is sufficient, so that its viscous behavior is very close to that of the incompressible fluid. When calcined at a softening point minus 10 ° C (550 ° C) (6), FIG.
As shown in FIG. 8, it can be seen that the viscosity-temperature curve “●” when calcined in the same manner as described above approaches the viscosity curve “□” by the bulk method. This is the softening point minus 10 ° C,
That is, even at 550 ° C., since the necking between the powder particles is sufficient in the green compact, its viscous behavior seems to be very close to that of the incompressible fluid. Further, even when it is calcined at a softening point of minus 20 ° C. (540 ° C.) (7), and when it is calcined at a softening point of minus 30 ° C. (530 ° C.) (8), FIGS. As shown, it can be seen that the viscosity-temperature curve “温度” when calcined in the same manner as described above approaches the viscosity curve “□” by the bulk method. This is the softening point minus 20 ° C,
That is, 420 ° C or softening point minus 30 ° C, that is, 4
Even at 10 ° C, the viscous behavior seems to be very close to that of the incompressible fluid due to sufficient necking between the powder particles in the green compact. The standard of the viscosity in this method is a temperature at the same viscosity, and a difference from the bulk is within 2%.

【0062】ところが、試料3の圧粉成型体を軟化点マ
イナス50℃(510℃)で仮焼した場合(9)、図2
1に示すように、仮焼したときの粘度−温度曲線「●」
は、バルク法による粘度曲線「□」とは離れて、仮焼し
ない場合の粘度曲線「△」に近づいてしまった。これ
は、上述したのと同様に、軟化点マイナス30℃より低
い温度、すなわち530℃より低温では、圧粉成型体が
十分に仮焼されず、粉末粒子間のネッキングが不完全で
あったためと思われる。
However, when the green compact of Sample 3 was calcined at the softening point minus 50 ° C. (510 ° C.) (9), FIG.
As shown in FIG. 1, the viscosity-temperature curve “●” when calcined
Was separated from the viscosity curve “□” obtained by the bulk method, and approached the viscosity curve “△” when not calcined. This is because, as described above, at a temperature lower than the softening point minus 30 ° C., that is, at a temperature lower than 530 ° C., the green compact was not calcined sufficiently, and necking between powder particles was incomplete. Seem.

【0063】以上のことから、仮焼温度としては、非晶
質ガラス粉末の軟化点(軟化温度)以下、さらに、仮焼
条件として一般に適用するためには、軟化点マイナス1
0℃以上、軟化点以下が望ましいことが分かる。
From the above, the calcination temperature is not higher than the softening point (softening temperature) of the amorphous glass powder. Further, in order to generally apply the calcination conditions, the softening point is minus one.
It is understood that the temperature is preferably from 0 ° C. to the softening point.

【0064】すなわち、圧粉成型体をあらかじめ適正な
温度で仮焼することにより、粉末粒子間を十分にネッキ
ングさせ、無機粉末、特に非晶質ガラス粉末をプレス成
型してなる圧粉成型体の粘度について、焼結プロセス等
で極めて重要な104〜109Pa・Sの中粘度領域につ
いて、圧粉成型体の粘性挙動を高精度に評価・測定でき
る。
That is, the powder compact is calcined at an appropriate temperature in advance, whereby the powder particles are sufficiently necked, and the inorganic powder, particularly the amorphous glass powder, is pressed. Regarding the viscosity, the viscosity behavior of the green compact can be evaluated and measured with high accuracy in a medium viscosity region of 10 4 to 10 9 Pa · S, which is extremely important in the sintering process and the like.

【0065】[0065]

【発明の効果】本発明の圧粉成型体の粘度測定方法によ
れば、非晶質ガラス粉末等の無機粉末をプレス成形した
圧粉成型体をあらかじめ仮焼し、その粒子同士を十分に
ネッキングさせておくことによって、その粉末状態に極
めて近い粘性挙動を示す圧粉成型体の粘度を極めて高精
度に測定できる。
According to the method for measuring the viscosity of a green compact of the present invention, a green compact formed by press-molding an inorganic powder such as an amorphous glass powder is calcined in advance, and the particles are sufficiently necked. By doing so, the viscosity of a compact having a viscous behavior very close to the powder state can be measured with extremely high accuracy.

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

【図1】本発明の圧粉成型体の粘度測定方法について、
その一実施形態を示す概略フローチャート図である。
FIG. 1 shows a method for measuring the viscosity of a green compact according to the present invention.
It is a schematic flowchart figure which shows one Embodiment.

【図2】本発明における試料体積補正値の抽出ステップ
を説明するためのフローチャートである。
FIG. 2 is a flowchart illustrating a step of extracting a sample volume correction value according to the present invention.

【図3】本発明における試料変形速度補正を概念的に説
明するための試料変形速度−温度曲線である。
FIG. 3 is a sample deformation speed-temperature curve for conceptually explaining the sample deformation speed correction in the present invention.

【図4】本発明における、試料変形速度補正値の抽出ス
テップ、並びに、焼結収縮が支配的な温度領域と塑性変
形が支配的な温度領域との境界温度の策定ステップを説
明するためのフローチャートである。
FIG. 4 is a flowchart illustrating a step of extracting a sample deformation speed correction value and a step of determining a boundary temperature between a temperature region where sintering shrinkage is dominant and a temperature region where plastic deformation is dominant in the present invention. It is.

【図5】本発明における、焼結収縮が支配的な温度領域
と塑性変形が支配的な温度領域との境界温度策定を説明
するための試料変形速度−温度曲線である。
FIG. 5 is a sample deformation speed-temperature curve for explaining the determination of a boundary temperature between a temperature region where sintering shrinkage is dominant and a temperature region where plastic deformation is dominant in the present invention.

【図6】本発明における、GENT式への試料体積補正
値、試料変形速度補正値の適用方法を説明するためのフ
ローチャートである。
FIG. 6 is a flowchart for explaining a method of applying a sample volume correction value and a sample deformation speed correction value to the GENT equation in the present invention.

【図7】本実施例において、試料1の圧粉成型体をその
軟化温度で仮焼したときの粘度−温度曲線である。
FIG. 7 is a viscosity-temperature curve when the green compact of Sample 1 is calcined at its softening temperature in this example.

【図8】同、試料1の圧粉成型体をその軟化温度マイナ
ス10℃で仮焼したときの粘度−温度曲線である。
FIG. 8 is a viscosity-temperature curve when the green compact of Sample 1 is calcined at a softening temperature minus 10 ° C.

【図9】同、試料1の圧粉成型体をその軟化温度マイナ
ス20℃で仮焼したときの粘度−温度曲線である。
FIG. 9 is a viscosity-temperature curve when the green compact of Sample 1 is calcined at its softening temperature minus 20 ° C.

【図10】同、試料1の圧粉成型体をその軟化温度マイ
ナス30℃で仮焼したときの粘度−温度曲線である。
FIG. 10 is a viscosity-temperature curve when the green compact of Sample 1 is calcined at its softening temperature minus 30 ° C.

【図11】同、試料1の圧粉成型体をその軟化温度マイ
ナス50℃で仮焼したときの粘度−温度曲線である。
FIG. 11 is a viscosity-temperature curve when the green compact of Sample 1 was calcined at a softening temperature minus 50 ° C.

【図12】同、試料2の圧粉成型体をその軟化温度で仮
焼したときの粘度−温度曲線である。
FIG. 12 is a viscosity-temperature curve when the green compact of Sample 2 is calcined at its softening temperature.

【図13】同、試料2の圧粉成型体をその軟化温度マイ
ナス10℃で仮焼したときの粘度−温度曲線である。
FIG. 13 is a viscosity-temperature curve when the green compact of Sample 2 is calcined at a softening temperature minus 10 ° C.

【図14】同、試料2の圧粉成型体をその軟化温度マイ
ナス20℃で仮焼したときの粘度−温度曲線である。
FIG. 14 is a viscosity-temperature curve when the green compact of Sample 2 is calcined at a softening temperature thereof minus 20 ° C.

【図15】同、試料2の圧粉成型体をその軟化温度マイ
ナス30℃で仮焼したときの粘度−温度曲線である。
FIG. 15 shows a viscosity-temperature curve when the green compact of Sample 2 was calcined at a softening temperature thereof minus 30 ° C.

【図16】同、試料2の圧粉成型体をその軟化温度マイ
ナス50℃で仮焼したときの粘度−温度曲線である。
FIG. 16 is a viscosity-temperature curve when the green compact of Sample 2 was calcined at a softening temperature minus 50 ° C.

【図17】同、試料3の圧粉成型体をその軟化温度で仮
焼したときの粘度−温度曲線である。
FIG. 17 shows a viscosity-temperature curve when the green compact of Sample 3 was calcined at the softening temperature.

【図18】同、試料3の圧粉成型体をその軟化温度マイ
ナス10℃で仮焼したときの粘度−温度曲線である。
FIG. 18 shows a viscosity-temperature curve when the green compact of Sample 3 was calcined at a softening temperature of −10 ° C.

【図19】同、試料3の圧粉成型体をその軟化温度マイ
ナス20℃で仮焼したときの粘度−温度曲線である。
FIG. 19 is a viscosity-temperature curve when the green compact of Sample 3 is calcined at a softening temperature of −20 ° C.

【図20】同、試料3の圧粉成型体をその軟化温度マイ
ナス30℃で仮焼したときの粘度−温度曲線である。
FIG. 20 is a viscosity-temperature curve when the green compact of Sample 3 was calcined at a softening temperature thereof minus 30 ° C.

【図21】同、試料3の圧粉成型体をその軟化温度マイ
ナス50℃で仮焼したときの粘度−温度曲線である。
FIG. 21 is a viscosity-temperature curve when the green compact of Sample 3 was calcined at a softening temperature minus 50 ° C.

【図22】平行板加圧粘度計の概略断面図である。FIG. 22 is a schematic sectional view of a parallel plate pressure viscometer.

【符号の説明】[Explanation of symbols]

1…被測定物 2a、2b…石英板 3…支持台 4…石英ロッド 5…ヒータ 6…装置 DESCRIPTION OF SYMBOLS 1 ... Measurement object 2a, 2b ... Quartz plate 3 ... Support base 4 ... Quartz rod 5 ... Heater 6 ... Device

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Claims (5)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 無機粉末をプレス成形してなる圧粉成型
体の粘度ηを、GENT式: η=2πMGH5/3V(dh/dt)(2πH3+V) (但し、M:荷重、H:試料高さ、G:重力加速度、
V:試料体積、dh/dt:試料変形速度)にしたがっ
て測定する圧粉成型体の粘度測定方法において、あらか
じめ仮焼した圧粉成型体を前記測定に用いることを特徴
とする、圧粉成型体の粘度測定方法。
1. The viscosity η of a green compact obtained by press-molding an inorganic powder is determined by the GENT formula: η = 2πMGH 5 / 3V (dh / dt) (2πH 3 + V) (where M: load, H: Sample height, G: gravitational acceleration,
(V: sample volume, dh / dt: sample deformation rate) in a method for measuring the viscosity of a green compact, wherein a pre-calcined green compact is used for the measurement. Viscosity measurement method.
【請求項2】 前記無機粉末を、非晶質ガラス粉末、結
晶化ガラス粉末、及び、ガラスセラミック複合粉末から
なる群より選ばれる1種の酸化物無機粉末とすることを
特徴とする、請求項1に記載の圧粉成型体の粘度測定方
法。
2. The method according to claim 1, wherein the inorganic powder is one kind of oxide inorganic powder selected from the group consisting of amorphous glass powder, crystallized glass powder, and glass-ceramic composite powder. 2. The method for measuring the viscosity of a green compact according to 1.
【請求項3】 前記仮焼を前記無機粉末の軟化温度以下
で実施することを特徴とする、請求項1又は2に記載の
圧粉成型体の粘度測定方法。
3. The method for measuring the viscosity of a green compact according to claim 1, wherein the calcining is performed at a temperature lower than a softening temperature of the inorganic powder.
【請求項4】 前記無機粉末の軟化温度T(℃)とし、
前記仮焼をT−10℃以上で実施することを特徴とす
る、請求項3に記載の圧粉成型体の粘度測定方法。
4. A softening temperature T (° C.) of the inorganic powder,
The method for measuring the viscosity of a green compact according to claim 3, wherein the calcination is performed at a temperature of T-10 ° C or higher.
【請求項5】 前記仮焼後の圧粉成型体の試料高さH、
試料体積Vをそれぞれ測定するステップと、平行板加圧
粘度計によって、荷重Mを加えたときの前記圧粉成型体
の試料変形速度dh/dtを測定するステップと、前記
各ステップによって算出した試料高さH、試料体積V及
び試料変形速度dh/dtを前記GENT式に適用し
て、前記圧粉成型体の粘度ηを算出するステップと、を
有することを特徴とする、請求項1乃至5のいずれかに
記載の圧粉成型体の粘度測定方法。
5. A sample height H of the calcined green compact,
Measuring the sample volume V, measuring the sample deformation speed dh / dt of the green compact when a load M is applied by a parallel plate pressure viscometer, and measuring the sample calculated in each of the steps. Applying the height H, the sample volume V, and the sample deformation rate dh / dt to the GENT equation to calculate the viscosity η of the green compact. The method for measuring the viscosity of a green compact according to any one of the above.
JP31250799A 1999-10-04 1999-11-02 Viscosity measurement method for green compacts Expired - Lifetime JP3344390B2 (en)

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DE10049022A DE10049022B4 (en) 1999-10-04 2000-10-04 Method and device for measuring the viscosity of green compacts and computer-readable recording medium for storing the method for measuring the viscosity of green compacts
US09/679,208 US6508106B1 (en) 1999-10-04 2000-10-04 Method and apparatus for measuring viscosity of green compact, and computer readable recording medium for storing method for measuring viscosity of green compact
US10/191,032 US6581439B2 (en) 1999-10-04 2002-07-02 Method and apparatus for measuring viscosity of green compact sample, and computer readable medium for storing method for measuring viscosity of green compact sample

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Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001108594A (en) 1999-10-04 2001-04-20 Murata Mfg Co Ltd Method and apparatus for measuring viscosity of compact and computer readable storage medium for storing the method

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001108594A (en) 1999-10-04 2001-04-20 Murata Mfg Co Ltd Method and apparatus for measuring viscosity of compact and computer readable storage medium for storing the method

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