JP2826422B2 - Inspection method for multilayer ceramic capacitors - Google Patents
Inspection method for multilayer ceramic capacitorsInfo
- Publication number
- JP2826422B2 JP2826422B2 JP19653392A JP19653392A JP2826422B2 JP 2826422 B2 JP2826422 B2 JP 2826422B2 JP 19653392 A JP19653392 A JP 19653392A JP 19653392 A JP19653392 A JP 19653392A JP 2826422 B2 JP2826422 B2 JP 2826422B2
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- multilayer ceramic
- peak
- change
- mlc
- 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 - Fee Related
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Testing Electric Properties And Detecting Electric Faults (AREA)
Description
【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION
【0001】[0001]
【産業上の利用分野】本発明は、積層セラミックコンデ
ンサの検査方法、より詳しくは積層セラミックコンデン
サにバイアス電圧を印加した状態での等価直列抵抗一周
波数特性を測定することにより内部欠陥の有無を判定す
る検査方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for inspecting a multilayer ceramic capacitor, and more specifically, to determine the presence or absence of an internal defect by measuring the frequency characteristic of equivalent series resistance with a bias voltage applied to the multilayer ceramic capacitor. Inspection method.
【0002】[0002]
【従来技術】積層セラミックコンデンサ(以下MLCと
略記する)の製造工程、特に脱バインダ時におけるトラ
ブルが製品にいろいろな欠陥を発生させ品質に大きく影
響を与えることがある。量産工程では短時間に多くの製
品を処理する必要があるため、デラミネーション(層間
剥離)や微細なクラックなどの内部欠陥が発生する。2. Description of the Related Art A trouble in a manufacturing process of a multilayer ceramic capacitor (hereinafter abbreviated as MLC), particularly, a problem at the time of binder removal may cause various defects in a product and greatly affect the quality. In a mass production process, it is necessary to process many products in a short time, so that internal defects such as delamination (delamination) and minute cracks occur.
【0003】このようなデラミネーションなどの内部欠
陥の発見は、従来MLC製品を切断し、その内部を研磨
して確認する破壊検査法によるのが主体であった。この
破壊検査法の適用は、当然ながら1ロットのうち数個の
サンプルに制限されることになり、個々の製品には適用
できない。Conventionally, the detection of such internal defects such as delamination has been mainly performed by a destructive inspection method in which an MLC product is cut and the inside thereof is polished and confirmed. The application of the destructive inspection method is naturally limited to several samples in one lot, and cannot be applied to individual products.
【0004】一方、非破壊検査法としては(a)超音波
をチップ内に伝播させることにより内部欠陥を検査する
方法、(b)MLCにバイアス電圧を印加し、インピー
ダンス対周波数特性を測定することにより検査する方法
等が知られている。On the other hand, non-destructive inspection methods include (a) a method of inspecting internal defects by propagating ultrasonic waves into a chip, and (b) measuring a impedance-frequency characteristic by applying a bias voltage to MLC. And the like.
【0005】上記インピーダンス対周波数特性を測定す
る方法は米国特許4644259号(特開昭61−10
8956号公報参照)に開示されているが、その要旨は
下記の通りである、MLCにバイアス電圧を印加し、交
流電圧の周波数を変化させてインピーダンス特性の測定
を行うと、該MLCの寸法に応じた特定周波数において
インピーダンスが変化する現象すなわち定在波を生じさ
せる。この現象は交流電圧による圧電現象によりチップ
が振動し、MLC内部全体に伝播するために、振動の1
/2波長の整数倍で共振し、その共振現象により変化が
大きくなり、圧電現象により電荷が変動してインピーダ
ンス変化が発生する。このインピーダンス変化がチップ
内部の状態、つまりデラミネーションなどの欠陥が存在
する個所では共振パターンが妨害されるため、その変化
を基準として用いて内部欠陥を判断し、不良品と良品す
なわち内部欠陥が存在しない製品とを識別することがで
きる。A method for measuring the impedance versus frequency characteristics is disclosed in US Pat. No. 4,644,259 (Japanese Patent Laid-Open No. 61-10 / 1986).
No. 8956), the gist of which is as follows. When a bias voltage is applied to the MLC and the frequency of the AC voltage is changed to measure the impedance characteristics, the dimensions of the MLC are reduced. This causes a phenomenon in which the impedance changes at the corresponding specific frequency, that is, a standing wave. This phenomenon occurs because the chip vibrates due to the piezoelectric phenomenon caused by the AC voltage and propagates throughout the MLC.
Resonance occurs at an integral multiple of a half wavelength, and the change increases due to the resonance phenomenon, and the electric charge fluctuates due to the piezoelectric phenomenon, causing a change in impedance. Since this change in impedance is a condition inside the chip, that is, where a defect such as delamination is present, the resonance pattern is disturbed, the change is used as a reference to determine the internal defect, and a defective product and a good product, that is, an internal defect exists. Products that can not be identified.
【0006】[0006]
【発明が解決しようとする課題】しかしながら、上記超
音波を用いる方法は対象MLCの形状が小さくなった場
合には測定が困難となり、またこの方法ではMLC中の
小さな欠陥を見つけることは難しい。また、インピーダ
ンスを測定して内部欠陥を判断する前記米国特許に示さ
れた技術による方法は、比較的大きい内部欠陥について
検出可能であるが微細な内部欠陥の検出は難しくなる。
なぜなら、欠陥が微細となるのに従って、その欠陥に対
応するインピーダンス変化は高周波数側に移り、後述の
ように高周波数側のインピーダンス変化ほど変化が小さ
く、正常なものとの区別がつかないときがあるからであ
る。However, in the method using ultrasonic waves, measurement becomes difficult when the shape of the target MLC becomes small, and it is difficult to find small defects in the MLC by this method. Further, the method according to the technique disclosed in the above-mentioned U.S. Patent which measures the internal defect by measuring the impedance can detect a relatively large internal defect, but it is difficult to detect a fine internal defect.
Because, as the defect becomes finer, the impedance change corresponding to the defect shifts to the high frequency side, and as described later, the impedance change on the high frequency side has a smaller change and cannot be distinguished from a normal one. Because there is.
【0007】例えば、図6は3.2×1.6mm、1μ
F、F特性のMLCにおいて、バイアス電圧10Vを印
加したのち、周波数を1ないし10MHzの領域に変化
させたときのインピーダンス(Z)の変化および等価直
列抵抗(R)の変化をプロットした曲線を示したもので
あり、図7は周波数2〜4MHzの間を拡大した図であ
るが、図7から判るように、インピーダンス特性変化は
高周波数領域になるほど(ピークの高さの)変化が小さ
くなるという特徴があり、実際の検査工程で問題になる
のは上記微細な欠陥であることから、上記米国特許の技
術による場合は信頼性に欠けるという課題があった。For example, FIG. 6 shows 3.2 × 1.6 mm, 1 μm
In the MLC of F and F characteristics, a curve is plotted showing a change in impedance (Z) and a change in equivalent series resistance (R) when a frequency is changed to a range of 1 to 10 MHz after a bias voltage of 10 V is applied. FIG. 7 is an enlarged view of the frequency range from 2 MHz to 4 MHz. As can be seen from FIG. 7, the impedance characteristic change (peak height) decreases as the frequency becomes higher. There is a characteristic, and the problem in the actual inspection process is the minute defect. Therefore, the technique of the above-mentioned US patent has a problem that the reliability is lacking.
【0008】したがって本発明の目的は、MLCの品
質、特にセラミック材料中に存在するデラミネーション
や微細なクラックによる内部欠陥を非破壊検査するため
の簡便で信頼性の高い方法を提供することにある。Accordingly, an object of the present invention is to provide a simple and highly reliable method for nondestructively inspecting the quality of MLC, especially internal defects due to delamination and fine cracks existing in ceramic materials. .
【0009】[0009]
【課題を解決するための手段】本発明者らは上記目的を
達成すべく研究を進め、以下の(1)〜(4)に述べる
考察に基づいて、MLCの圧電現象による周波数特性変
化をインピーダンスではなく、等価直列抵抗値の変化に
よることとすれば、内部欠陥、特に微細なものまでも容
易に判断できることを見い出し本発明に到達した。Means for Solving the Problems The present inventors have conducted research to achieve the above object, and based on the considerations described in the following (1) to (4), have been able to determine the change in the frequency characteristic due to the piezoelectric phenomenon of the MLC. Instead, the present inventors have found that it is possible to easily determine even an internal defect, particularly a minute one, if it is based on a change in the equivalent series resistance.
【0010】(1)MLCに圧電性がある場合にはバイ
アス電圧を印加することによりコンデンサチップが変位
をおこし、この変位がある周波数になると定在波となっ
て大きな振幅をもち、これがメカニカル共振周波数とな
ってコンデンサの蓄積容量が変化し、このためインピー
ダンス(Z)は図8(a)に示すように共振周波数f。
反共振周波数frを有する特性曲線として得られる。(1) When the MLC has piezoelectricity, the capacitor chip is displaced by applying a bias voltage, and when the displacement reaches a certain frequency, it becomes a standing wave and has a large amplitude, which is a mechanical resonance. As the frequency changes, the storage capacitance of the capacitor changes. Therefore, the impedance (Z) becomes the resonance frequency f as shown in FIG.
It is obtained as a characteristic curve having the anti-resonance frequency fr.
【0011】(2)特に微細な内部欠陥について判断す
るためには基本共振点よりは高次の共振点におけるイン
ピーダンス特性変化を考慮する必要があるが、前記図6
にみられるように、高次の共振点におけるインピーダン
スは高周波数領域になるほど変化が小さくなる傾向があ
る。(2) In order to judge particularly a minute internal defect, it is necessary to consider a change in impedance characteristics at a resonance point higher than the fundamental resonance point.
As can be seen, the impedance at a higher-order resonance point tends to have a smaller change as the frequency becomes higher.
【0012】(3)一方、周波数対等価直列抵抗(ES
R)の特性曲線は図8(b)のような変化を示し(点線
はZ−f特性曲線である)、このf−R特性曲線のピー
クは左右対象であり、ピークの半値幅、すなわちピーク
強度の半分の値における周波数の幅を測定することによ
り数値化が容易である。(3) On the other hand, the frequency versus the equivalent series resistance (ES
The characteristic curve of R) shows a change as shown in FIG. 8B (the dotted line is the Zf characteristic curve), and the peak of this fR characteristic curve is symmetrical with respect to the right and left, and the half width of the peak, that is, the peak It is easy to quantify by measuring the width of the frequency at half the intensity.
【0013】(4)上記内部欠陥の判定に利用できるf
−R曲線中のピークは先ず基本波が現われ、これの高次
の2、3、4、…倍といった周波数にピークが現われ
る。大きな内部欠陥は基本波にその影響が現われるが、
微細な欠陥では基本波には影響が出にくいため、高次の
ピークを見る必要があり、そのため高周波数領域のピー
クの変化を観察することにより微細な欠陥をも判定する
ことができる。(4) f which can be used for determining the internal defect
The peak in the -R curve firstly appears as a fundamental wave, and peaks appear at higher frequencies such as 2, 3, 4,. Large internal defects have their effect on the fundamental wave,
Since a fine defect hardly affects the fundamental wave, it is necessary to look at a higher-order peak. Therefore, a fine defect can be determined by observing a change in a peak in a high-frequency region.
【0014】したがって本発明は、圧電材料よりなる積
層セラミックコンデンサの内部に存在するデラミネーシ
ョンを主とする内部欠陥を検査する方法において、
(イ)検査対象となる上記コンデンサにバイアス電圧を
印加して交流電圧の周波数を変化させ、該コンデンサの
等価直列抵抗を測定して得られる等価直列抵抗対周波数
特性曲線を求め、(ロ)該コンデンサが圧電現象により
機械的に共振する周波数およびこの周波数の整数倍であ
る高次の周波数で現われる該特性曲線のピークにおい
て、ピーク強度の半分の値における周波数の幅でもって
示される半値幅を求め、(ハ)この値が上記検査対象品
と同じ寸法、材料であって、内部欠陥が存在しない積層
セラミックコンデンサから得られた等価直列抵抗対周波
数特性曲線の対応するピークの半値幅と比較して大であ
れば内部欠陥が存在すると判定することからなる積層セ
ラミックコンデンサの検査方法を提供するものである。Accordingly, the present invention provides a method for inspecting an internal defect mainly including delamination present in a multilayer ceramic capacitor made of a piezoelectric material,
(A) A bias voltage is applied to the capacitor to be tested to change the frequency of the AC voltage, and the equivalent series resistance versus frequency characteristic curve obtained by measuring the equivalent series resistance of the capacitor is obtained. At the peak of the characteristic curve that appears at the frequency at which the capacitor mechanically resonates due to the piezoelectric phenomenon and at a higher frequency that is an integral multiple of this frequency, the half-width indicated by the frequency width at half the peak intensity is determined. (C) This value is compared with the half value width of the corresponding peak of the equivalent series resistance vs. frequency characteristic curve obtained from the multilayer ceramic capacitor having the same dimensions and material as the above-mentioned inspection object and having no internal defect. An object of the present invention is to provide a method for inspecting a multilayer ceramic capacitor, which comprises determining that an internal defect is present if it is large.
【0015】[0015]
【作用】ESR−f特性曲線に現われるピークでは半値
幅が容易に求められるため、本発明の方法では、交流電
圧の周波数に対するESRの変化を観察することによ
り、内部欠陥の度合いを定量化することができる。そこ
で得られた被検査MLCの半値幅と良品MLCのそれと
比較することにより、内部欠陥の検出が可能となり、さ
らには高次の周波数に現われるピークの半値幅を求める
ことにより、基本の周波数のピークに影響を及ぼさない
ような微細な内部欠陥をも検出することができる。Since the half width at the peak appearing in the ESR-f characteristic curve can be easily obtained, the method of the present invention quantifies the degree of the internal defect by observing the change of the ESR with respect to the frequency of the AC voltage. Can be. By comparing the obtained half-value width of the MLC to be inspected with that of the non-defective MLC, an internal defect can be detected. Further, the half-value width of a peak appearing in a higher-order frequency can be obtained, thereby obtaining the peak of the basic frequency. It is possible to detect even fine internal defects that do not affect the image quality.
【0016】[0016]
【実施例】図1、図4および図5は、いずれも3.2×
1.6mmで1μF、F特性のMLCにおいて、それぞ
れ小さなデラミネーションが存在する場合、デラミネー
ションが存在しない場合および大きなデラミネーション
が存在する場合のインピーダンス(Z)および等価直列
抵抗(R)対周波数特性曲線を示すグラフ線図、図2お
よび図3はそれぞれ図5および図1に対応するMLCの
断面を示す顕微鏡写真の模式図であって、これらの図を
参照して以下説明する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1, FIG. 4 and FIG.
Impedance (Z) and equivalent series resistance (R) vs. frequency characteristics in the case of small delamination, no delamination, and large delamination in MLC with 1.6 μm and 1 μF and F characteristics 2 and 3 are schematic diagrams of micrographs showing cross sections of the MLC corresponding to FIGS. 5 and 1, respectively, and will be described below with reference to these drawings.
【0017】図1、図4および図5は、いずれもバイア
ス電圧10Vを印加した場合のMLCにおいて、インピ
ーダンスおよび等価直列抵抗の周波数による変化を示し
たものであるが、デラミネーションの存在しない図4に
ついてみると、等価直列抵抗の特性変化の度合いがイン
ピーダンスのそれよりも大きいことがわかる。FIG. 1, FIG. 4 and FIG. 5 show changes in impedance and equivalent series resistance depending on the frequency in the MLC when a bias voltage of 10 V is applied, but FIG. 4 shows no delamination. , It can be seen that the degree of change in the characteristic of the equivalent series resistance is greater than that of the impedance.
【0018】一方、積層セラミックコンデンサ(ML
C)1中に図2にみられるような大きなデラミネーショ
ン2が存在する場合を示す図5の特性曲線においてはイ
ンピーダンス、等価直列抵抗いずれもがその変化度合い
が小さくなってはいるが特性曲線からデラミネーション
による内部欠陥を判断することができる。On the other hand, a multilayer ceramic capacitor (ML)
C) In the characteristic curve of FIG. 5 showing the case where a large delamination 2 as shown in FIG. 2 exists in 1, both the impedance and the equivalent series resistance have a small degree of change. Internal defects due to delamination can be determined.
【0019】しかしながら、MLC1中に図3に見られ
るような小さなデラミネーション2が存在する場合を示
す図1の特性曲線においては、インピーダンス(Z)の
特性曲線ではその特性変化を見ることが難しくなる。し
かし等価直列抵抗の特性変化では例えば矢印Aで示した
個所のピーク部分ではピーク幅が広くなっており、この
ピーク幅を考慮することにより特性変化を容易に判断す
ることができた。However, in the characteristic curve of FIG. 1 showing the case where the small delamination 2 as shown in FIG. 3 exists in the MLC 1, it is difficult to see the characteristic change in the characteristic curve of the impedance (Z). . However, in the change in the characteristic of the equivalent series resistance, for example, the peak portion at the peak indicated by the arrow A has a large peak width, and the characteristic change can be easily determined by considering the peak width.
【0020】上記ピークAについて、デラミネーション
の存在しない図4の場合と比較するため、ピーク強度の
半分の値における周波数の幅、すなわち半値幅を測定し
たところ、デラミネーションの存在しない図4の場合1
82KHzであったのに対し、小さなデラミネーション
が存在する図1のピークAでは438KHzであった。In order to compare the peak A with the case of FIG. 4 where no delamination is present, the width of the frequency at half the peak intensity, that is, the half width was measured. 1
The peak A was 82 KHz, whereas the peak A in FIG. 1 where small delamination was present was 438 KHz.
【0021】したがって、このように内部欠陥のない良
品との半値幅を比較して数値化することにより識別を容
易にすることができる。Therefore, identification can be facilitated by comparing the half-value width of a non-defective product having no internal defect with a numerical value.
【0022】[0022]
【発明の効果】以上説明したように、本発明の方法によ
ればESR−f特性曲線に現われるピークでは半値幅が
容易に求められることから、周波数に対するESRの変
化を観察することによりMLCが機械的に共振する基本
の周波数およびこの周波数の高次の周波数に現れる特性
曲線のピークにおいてその半値幅を数値的に判断できる
ので、大きな内部欠陥のみならず、基本の周波数のピー
クに影響を及ぼさないような微細な内部欠陥をも検出す
ることができる。As described above, according to the method of the present invention, the half width at the peak appearing in the ESR-f characteristic curve can be easily obtained. The half-width at the peak of the characteristic curve appearing at the fundamental frequency that resonates naturally and at the higher-order frequencies of this frequency can be numerically judged, so that not only the large internal defect but also the peak of the fundamental frequency is not affected. Such minute internal defects can be detected.
【図1】小さなデラミネーションが存在するMLCにお
けるインピーダンスおよび等価直列抵抗対周波数特性曲
線を示すグラフ線図である。FIG. 1 is a graph showing impedance and equivalent series resistance versus frequency characteristic curves in an MLC with small delaminations.
【図2】大きなデラミネーションが存在するMLCの縦
断面を示す顕微鏡写真の模式図である。FIG. 2 is a schematic diagram of a micrograph showing a longitudinal section of an MLC in which a large delamination exists.
【図3】小さなデラミネーションが存在するMLCの縦
断面を示す顕微鏡写真の模式図である。FIG. 3 is a schematic diagram of a micrograph showing a longitudinal section of an MLC in which a small delamination exists.
【図4】デラミネーションが存在しないMLCにおける
インピーダンスおよび等価直列抵抗対周波数特性曲線を
示すグラフ線図である。FIG. 4 is a graph showing impedance and equivalent series resistance versus frequency characteristic curves in an MLC without delamination.
【図5】大きなデラミネーションが存在するMLCにお
けるインピーダンスおよび等価直列抵抗対周波数特性曲
線を示すグラフ線図である。FIG. 5 is a graph showing impedance and equivalent series resistance versus frequency characteristic curves in an MLC in which a large delamination exists.
【図6】MLCに置ける周波数変化(1〜10MHz)
に対するインピーダンス(Z)および等価直列抵抗
(R)の変化を示すグラフ線図である。FIG. 6: Frequency change (1 to 10 MHz) in MLC
FIG. 4 is a graph showing changes in impedance (Z) and equivalent series resistance (R) with respect to the threshold voltage.
【図7】図6の周波数2〜4MHzの部分を拡大したグ
ラフ線図である。7 is a graph diagram enlarging a portion of a frequency of 2 to 4 MHz in FIG. 6;
【図8】同図(a)はMLCにおける周波数の変化に対
するインピーダンスの基本的な変化を示した線図、同図
(b)は同じく周波数の変化に対する等価直列抵抗の基
本的な変化を示した線図である。FIG. 8A is a diagram showing a basic change in impedance with respect to a change in frequency in the MLC, and FIG. 8B is a diagram showing a basic change in equivalent series resistance with respect to a change in frequency. FIG.
1 積層セラミックコンデンサ(MLC) 2 デラミネーション 1 Multilayer ceramic capacitor (MLC) 2 Delamination
Claims (1)
による素体の内部に存在する欠陥を検査する方法におい
て、(イ)検査対象となる上記コンデンサに交流バイア
ス電圧を印加してその周波数を変化させ、該コンデンサ
の等価直列抵抗を測定して得られる等価直列抵抗対周波
数特性曲線を求め、(ロ)該コンデンサが圧電現象によ
り機械的に共振する周波数およびこの周波数の整数倍で
ある高次の周波数のいずれかで現れる該特性曲線のピー
クにおいて、ピーク強度の半分の値における周波数の幅
でもって示される半値幅を求め、(ハ)この値を基準の
積層セラミックコンデンサから得られた同様の半値幅と
比較する過程を有する積層セラミックコンデンサの検査
方法。1. A method for inspecting a defect existing inside a body made of a piezoelectric material of a multilayer ceramic capacitor, comprising: (a) applying an AC bias voltage to the capacitor to be inspected to change its frequency; The equivalent series resistance versus frequency characteristic curve obtained by measuring the equivalent series resistance of the capacitor is obtained. (B) The frequency at which the capacitor mechanically resonates due to the piezoelectric phenomenon and the higher order frequency that is an integral multiple of this frequency are calculated. At the peak of the characteristic curve appearing in any of the above cases, a half-width indicated by a frequency width at a half value of the peak intensity is obtained, and (c) this value is determined by the same half-width obtained from the reference multilayer ceramic capacitor. An inspection method of a multilayer ceramic capacitor having a comparing process.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19653392A JP2826422B2 (en) | 1992-06-30 | 1992-06-30 | Inspection method for multilayer ceramic capacitors |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19653392A JP2826422B2 (en) | 1992-06-30 | 1992-06-30 | Inspection method for multilayer ceramic capacitors |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0618462A JPH0618462A (en) | 1994-01-25 |
| JP2826422B2 true JP2826422B2 (en) | 1998-11-18 |
Family
ID=16359325
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19653392A Expired - Fee Related JP2826422B2 (en) | 1992-06-30 | 1992-06-30 | Inspection method for multilayer ceramic capacitors |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2826422B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4845879B2 (en) | 2005-03-18 | 2011-12-28 | 日本碍子株式会社 | Piezoelectric element inspection method, inspection apparatus, and polarization treatment method |
| JP7472380B2 (en) | 2022-09-21 | 2024-04-22 | Yuriホールディングス株式会社 | Capacitor inspection method and inspection device used therein |
-
1992
- 1992-06-30 JP JP19653392A patent/JP2826422B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0618462A (en) | 1994-01-25 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5351543A (en) | Crack detection using resonant ultrasound spectroscopy | |
| US6951133B2 (en) | Electromagnetic acoustic transducer with recessed coils | |
| US5425272A (en) | Relative resonant frequency shifts to detect cracks | |
| US20040134280A1 (en) | Method and device for detecting damage in materials or objects | |
| CN103376266B (en) | A kind of microwave on-line checking elimination method for composite filter | |
| US4644259A (en) | Nondestructive testing of multilayer ceramic capacitors | |
| FR2483073A1 (en) | METHOD AND APPARATUS FOR MEASURING THE THICKNESS OF A VENEER LAYER AND A BASE METAL | |
| JP2826422B2 (en) | Inspection method for multilayer ceramic capacitors | |
| McIntyre et al. | The use of air-coupled ultrasound to test paper | |
| WO2006110089A1 (en) | Method and apparatus for assessing quality of rivets using ultrasound | |
| US6528985B1 (en) | Non-destructive testing of passive components | |
| Johnson et al. | Nonlinear resonant acoustic detection of cracks in multilayer ceramic capacitors | |
| RU2191376C2 (en) | Method measuring sizes of defects in process of ultrasonic inspection of articles | |
| Gaal et al. | Ferroelectret transducers for air-coupled ultrasonic testing of fiber-reinforced polymers | |
| US12117478B2 (en) | Capacitor inspection method and inspection apparatus used for same | |
| JPH07174802A (en) | Method for detecting internal crack in electronic part | |
| Krieger et al. | Defect detection in multilayer ceramic capacitors | |
| SU864117A1 (en) | Ultrasonic method of flaw detection in polycrystalline materials | |
| JPH09218173A (en) | Method for inspecting internal defect of object having electrostrictive phenomenon | |
| Levikari | Detection of cracks: Acoustic experiments on multilayer ceramic capacitors | |
| Buonsanti et al. | Ultrasonic pulse-echoes and eddy current testing for detection, recognition and characterisation of flaws detected in metallic plates | |
| JPH11219871A (en) | Method for detecting defect inside electronic component | |
| Boser et al. | Rapid nondestructive testing of ceramic multilayer capacitors | |
| Basiri et al. | A Successive Wavenumber Filtering Approach for Defect Detection in CFRP Using Wavefield Scanning | |
| Stepinski | Ultrasonic spectroscopy for the inspection of airspace structures |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A01 | Written decision to grant a patent or to grant a registration (utility model) |
Free format text: JAPANESE INTERMEDIATE CODE: A01 Effective date: 19980818 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20080911 Year of fee payment: 10 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20080911 Year of fee payment: 10 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20090911 Year of fee payment: 11 |
|
| LAPS | Cancellation because of no payment of annual fees |