JP2659645B2 - Lead terminal flatness measurement method - Google Patents

Lead terminal flatness measurement method

Info

Publication number
JP2659645B2
JP2659645B2 JP3354760A JP35476091A JP2659645B2 JP 2659645 B2 JP2659645 B2 JP 2659645B2 JP 3354760 A JP3354760 A JP 3354760A JP 35476091 A JP35476091 A JP 35476091A JP 2659645 B2 JP2659645 B2 JP 2659645B2
Authority
JP
Japan
Prior art keywords
image
measured
lead terminal
lead
reference plane
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
JP3354760A
Other languages
Japanese (ja)
Other versions
JPH05166907A (en
Inventor
善宣 出口
義博 松井
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP3354760A priority Critical patent/JP2659645B2/en
Publication of JPH05166907A publication Critical patent/JPH05166907A/en
Application granted granted Critical
Publication of JP2659645B2 publication Critical patent/JP2659645B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Investigating Materials By The Use Of Optical Means Adapted For Particular Applications (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)
  • Editing Of Facsimile Originals (AREA)
  • Lead Frames For Integrated Circuits (AREA)
  • Length Measuring Devices By Optical Means (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】この発明は半導体装置に用いられ
るリード端子の平坦度の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 flatness of a lead terminal used in a semiconductor device.

【0002】[0002]

【従来の技術】図5は、測定ステージの基準平面を利用
した従来の半導体装置のリード端子の平坦度(以下、コ
プラナリティとも言う)の測定方法を示す側面図であ
り、図5において、1は被測定半導体装置(以下、被測
定ICと称す)であり、1aはそのモールド部、1bは
リードを示す。2は被測定IC1をその上に搭載して測
定を行うための測定ステージ、3は被測定IC1のリー
ド1bの画像を取り込むカメラ、4aは被測定ICを、
カメラ3と対向する方向から照射する照射光である。ま
た図6は、被測定IC1に照射光4aを当てたときのカ
メラ3が取り込む画像を示す図で、1cはリード1bの
影であり、ここでは4本分のリードの影が示されてい
る。2aは基準平面となる測定ステージ2の影、5は測
定されるコプラナリティ値(平坦度)である。
2. Description of the Related Art FIG. 5 is a side view showing a method for measuring the flatness (hereinafter, also referred to as coplanarity) of a lead terminal of a conventional semiconductor device using a reference plane of a measurement stage. In FIG. A semiconductor device to be measured (hereinafter, referred to as an IC to be measured), 1a is a molded part thereof, and 1b is a lead. Reference numeral 2 denotes a measurement stage for mounting the IC 1 to be measured thereon to perform measurement, 3 denotes a camera for capturing an image of the lead 1b of the IC 1 to be measured, 4a denotes the IC to be measured,
The light is emitted from a direction facing the camera 3. FIG. 6 is a diagram showing an image captured by the camera 3 when the irradiation light 4a is applied to the IC 1 to be measured. In FIG. 6, reference numeral 1c denotes a shadow of the lead 1b. Here, shadows of four leads are shown. . 2a is a shadow of the measurement stage 2 serving as a reference plane, and 5 is a measured coplanarity value (flatness).

【0003】次に測定方法について説明する。測定ステ
ージ2上に被測定IC1を載せ、被測定IC1のリード
端子1bの、カメラ3と対向する方向から照射光4aを
照射する。すると図6のように、被測定IC1のリード
の影1cと測定ステージの基準面の影2aができる。そ
して、同時にこの画像をカメラ3が取り込み、2値処理
を行い、リード1bのコプラナリティ5を算出する。
Next, a measuring method will be described. The IC 1 to be measured is placed on the measurement stage 2, and irradiation light 4 a is emitted from the direction in which the lead terminal 1 b of the IC 1 to be measured faces the camera 3. Then, as shown in FIG. 6, a shadow 1c of the lead of the IC 1 to be measured and a shadow 2a of the reference plane of the measurement stage are formed. At the same time, the image is captured by the camera 3 and subjected to binary processing to calculate a coplanarity value 5 of the lead 1b.

【0004】[0004]

【発明が解決しようとする課題】従来のリード端子平坦
度測定方法は以上のように構成されているので、リード
端子と測定ステージとの空隙が小さく、つまりコプラナ
リティ値が小さければ、照射光の干渉やカメラへの透過
光量の不足により、コプラナリティ値を測定すべき部分
が暗くなり、誤測定を起こすという問題があった。
Since the conventional method for measuring the flatness of a lead terminal is constructed as described above, if the gap between the lead terminal and the measurement stage is small, that is, if the coplanarity value is small, the interference of the illuminating light will not occur. In addition, there is a problem that a portion where the coplanarity value is to be measured becomes dark due to a shortage of the amount of light transmitted to the camera, which causes an erroneous measurement.

【0005】この発明は上記のような問題点を解消する
ためになされたもので、コプラナリティ測定における測
定精度を向上できるリード端子平坦度測定方法を提供す
ることを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and has as its object to provide a lead terminal flatness measurement method capable of improving measurement accuracy in coplanarity measurement.

【0006】[0006]

【課題を解決するための手段】この発明に係るリード端
子平坦度測定方法は、測定ステージの基準平面の画像を
得る第1の工程と、上記測定ステージ上に被測定半導体
装置を搭載して該半導体装置のリード端子のみの画像を
得る第2の工程と、上記第1及び第2の工程で得られた
それぞれの画像を合成し、該合成した画像の上記測定ス
テージの基準平面と上記リード端子間の空隙から上記リ
ード端子の平坦度を測定する第3の工程とを備えたもの
である。
A lead terminal flatness measuring method according to the present invention includes a first step of obtaining an image of a reference plane of a measuring stage, and a method of mounting a semiconductor device to be measured on the measuring stage. A second step of obtaining an image of only the lead terminal of the semiconductor device, and combining the respective images obtained in the first and second steps, a reference plane of the measurement stage of the combined image and the lead terminal And a third step of measuring the flatness of the lead terminal from the gap between them.

【0007】[0007]

【作用】この発明においては、基準平面となる測定ステ
ージの像と、被測定半導体装置のリード端子の像とを別
々に撮像し、これら2つの画像を合成して得られた画像
の、上記測定ステージの基準平面と上記リード端子間の
空隙を測定してリード端子の平坦度を求めるようにした
から、測定ステージの基準平面と上記リード端子間の空
隙が小さくても光の干渉や透過不足によって基準平面と
リード端子との間が暗くなることがない。
According to the present invention, an image of a measurement stage serving as a reference plane and an image of a lead terminal of a semiconductor device to be measured are separately captured, and the above-described measurement of an image obtained by combining these two images is performed. Because the gap between the reference plane of the stage and the lead terminal was measured to determine the flatness of the lead terminal, even if the gap between the reference plane of the measurement stage and the lead terminal was small, light interference and insufficient transmission caused the gap. There is no darkening between the reference plane and the lead terminals.

【0008】[0008]

【実施例】以下、この発明の一実施例によるリード端子
平坦度測定方法を図について説明する。図1において、
図5と同一符号は同一または相当部分を示し、6は被測
定IC1を載せて測定を行うための光透過性を有するガ
ラス製等の測定ステージ、7は基準平面の画像を取り込
むために、測定ステージ6の上方より光を照射するため
の光源である。また図2は第1の測定段階として、基準
平面の影を取り込む際の方法を説明するための図であ
り、図において、7aは光源7から、被測定IC1を搭
載した測定ステージ6に対して垂直に照射される照射光
である。また図3は第2の測定段階として、被測定IC
のリード1bの像を取り込む方法を説明するための図で
ある。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view showing a method for measuring lead terminal flatness according to an embodiment of the present invention. In FIG.
The same reference numerals as those in FIG. 5 denote the same or corresponding parts, 6 denotes a measuring stage made of light-transmitting glass for mounting the IC 1 to be measured, and 7 denotes a measuring stage for capturing an image of a reference plane. A light source for irradiating light from above the stage 6. FIG. 2 is a diagram for explaining a method of capturing a shadow of a reference plane as a first measurement stage. In the drawing, reference numeral 7a denotes a light source 7 from a measurement stage 6 on which the IC 1 to be measured is mounted. This is irradiation light that is irradiated vertically. FIG. 3 shows an IC to be measured as a second measurement stage.
FIG. 4 is a diagram for explaining a method of capturing an image of a lead 1b.

【0009】さらに図4は上記2段階の測定において得
られた被測定IC1の画像を処理してコプラナリティを
算出するための信号処理を説明するための図である。図
において、8は得られた基準平面の画像、9は基準平面
の画像8の白黒を反転させ、基準平面部を黒くした基準
平面の反転画像、10は得られた被測定IC1のリード
1bの画像、11は基準平面の反転画像9と被測定IC
1のリード1bを合成させてコプラナリティ5を得る
ための合成画像である。
FIG. 4 is a diagram for explaining signal processing for calculating the coplanarity by processing the image of the measured IC 1 obtained in the two-stage measurement. In the drawing, reference numeral 8 denotes an obtained image of the reference plane, 9 denotes an inverted image of the reference plane in which the black and white of the image 8 of the reference plane is inverted and the reference plane portion is blackened, and 10 denotes an obtained lead 1b of the IC 1 to be measured. Image 11 is an inverted image 9 of the reference plane and the IC to be measured
9 is a composite image for obtaining a coplanarity value of 5 by synthesizing the lead 1b of No. 1;

【0010】次に測定方法について説明する。まず、図
2のように被測定IC1を測定ステージ6に搭載する前
に測定ステージ6上方より照射光7aを照射し、側方よ
りカメラ3で測定ステージ6の画像を得る(第1の測定
段階)。ここで、周りは暗くしており、また測定ステー
ジ6はガラスでできているため、ここで得られる画像は
図4の基準平面の画像8のように測定ステージ6部は明
るく、その周辺部分は暗くなる。次に、図3に示すよう
に、測定ステージ6上に被測定IC1を載せ、被測定I
C1のリード1bに、カメラ3と対向する方向から照射
光4aを照射する。そして再びカメラ3で、側方より被
測定IC6のリード1bの画像を取る(第2の測定段
階)。このとき図4の被測定IC6のリード1bの画像
10のようにリード1bが存在する部分は照射光が遮ら
れるため暗くなる。
Next, a measuring method will be described. First, as shown in FIG. 2, before mounting the IC 1 to be measured on the measurement stage 6, the irradiation light 7a is irradiated from above the measurement stage 6 and an image of the measurement stage 6 is obtained from the side by the camera 3 (first measurement stage). ). Here, since the periphery is dark and the measurement stage 6 is made of glass, the image obtained here is bright at the measurement stage 6 like the image 8 of the reference plane in FIG. Get dark. Next, as shown in FIG. 3, the IC 1 to be measured is placed on the
The lead 1b of C1 is irradiated with irradiation light 4a from a direction facing the camera 3. Then, an image of the lead 1b of the measured IC 6 is taken from the side again by the camera 3 (second measurement stage). At this time, the portion where the lead 1b exists as shown in the image 10 of the lead 1b of the measured IC 6 in FIG.

【0011】最後に、以上のようにして得られた基準平
面の画像8の明暗を反転させて基準平面の反転画像9と
し、これと第2の測定段階で得られた被測定リードの画
像10とを合成し(図4の11参照)、コプラナリティ
5を求める。
Finally, the brightness of the image 8 of the reference plane obtained as described above is inverted to obtain an inverted image 9 of the reference plane, and the image 10 of the lead to be measured obtained in the second measurement stage. (See 11 in FIG. 4) and coplanarity
Find the value 5.

【0012】このように本実施例によれば、第1の測定
段階として、被測定IC1を搭載する前に、測定ステー
ジ6上方から照射光7aを照射して測定ステージ6の基
準平面の画像をカメラ3で撮影し、これを明暗反転させ
て基準平面の反転画像9とし、第2の測定段階として、
測定ステージ6に被測定IC1を搭載し、側面より照射
光4aを照射してリード1bの画像10を得て、この画
像10と上記基準平面の反転画像9とを合成して得られ
た画像11からコプラナリティ5を求めるようにした
から、測定ステージ6とリード1bとの間隔が小さくて
も光の干渉の発生や、またカメラ3に入射する透過光量
が少なくなってコプラナリティを測定すべき部分が暗く
なることがなく、精度の高い測定を行うことができる。
As described above, according to the present embodiment, as the first measurement step, before mounting the IC 1 to be measured, the irradiation light 7a is irradiated from above the measurement stage 6 and the image of the reference plane of the measurement stage 6 is obtained. The image is taken by the camera 3 and the image is inverted to obtain an inverted image 9 of the reference plane, and as a second measurement step,
The IC 1 to be measured is mounted on the measurement stage 6, and the irradiation light 4a is irradiated from the side to obtain an image 10 of the lead 1b. An image 11 obtained by synthesizing the image 10 and the inverted image 9 of the reference plane is obtained. The coplanarity value 5 is determined from the following equation. Therefore, even when the distance between the measurement stage 6 and the lead 1b is small, interference of light occurs, and the amount of transmitted light incident on the camera 3 is reduced, so that the portion where the coplanarity should be measured is reduced. Highly accurate measurement can be performed without darkening.

【0013】[0013]

【発明の効果】以上のように、この発明に係るリード端
子平坦度測定方法によれば、基準平面となる測定ステー
ジの像と、被測定半導体装置のリード端子の像とを別々
に撮像し、これら2つの画像を合成して得られた画像
の、上記測定ステージの基準平面と上記リード端子間の
空隙を測定してリード端子の平坦度を求めるようにした
ので、光の干渉や透過不足によって基準平面と被測定半
導体装置のリード端子との間が暗くなることがなく、そ
の結果、誤測定を防ぎ、高い精度でもってリード端子の
測定を行うことができるという効果がある。
As described above, according to the lead terminal flatness measuring method of the present invention, an image of a measurement stage serving as a reference plane and an image of a lead terminal of a semiconductor device to be measured are separately imaged. The air gap between the reference plane of the measurement stage and the lead terminal of the image obtained by synthesizing these two images was measured to determine the flatness of the lead terminal. There is no darkening between the reference plane and the lead terminal of the semiconductor device to be measured. As a result, erroneous measurement is prevented, and the lead terminal can be measured with high accuracy.

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

【図1】この発明の一実施例によるリード端子平坦度測
定方法を用いてコプラナリティの測定を行う際の各種機
材の配置を示す図。
FIG. 1 is a diagram showing an arrangement of various equipment when measuring coplanarity using a lead terminal flatness measuring method according to an embodiment of the present invention.

【図2】上記方法により基準平面画像を取り込む際の方
法を示す図。
FIG. 2 is a diagram showing a method for capturing a reference plane image by the above method.

【図3】上記方法により被測定ICのリードの画像を取
り込む際の方法を示す図。
FIG. 3 is a diagram showing a method for capturing an image of a lead of an IC to be measured by the above method.

【図4】上記方法により得られた各画像を処理してコプ
ラナリティを求める方法を説明するための図。
FIG. 4 is a view for explaining a method of processing each image obtained by the above method to obtain coplanarity.

【図5】従来のリード端子平坦度測定方法によりコプラ
ナリティを測定する際の各種機材の配置を示す図。
FIG. 5 is a diagram showing an arrangement of various devices when measuring coplanarity by a conventional lead terminal flatness measuring method.

【図6】従来のリード端子平坦度測定方法により、カメ
ラが取り込む被測定ICのリードの画像を示す図。
FIG. 6 is a diagram showing an image of a lead of an IC to be measured taken by a camera by a conventional lead terminal flatness measuring method.

【符号の説明】[Explanation of symbols]

1 被測定IC 1a モールド部 1b リード部 1c リードの影 3 画像取り込み用カメラ 4 測定ステージ側方よりの照射光源 4a 照射光源4から照射される光 5 コプラナリティ値 6 光透過性測定ステージ 7 測定ステージ上方よりの照射光源 7a 照射光源7よりの照射光 8 基準平面の画像 9 基準平面の画像の反転画像 10 リード1bの画像 11 基準平面の反転画像9とリード1bの画像との合
成画像
REFERENCE SIGNS LIST 1 IC to be measured 1a Mold part 1b Lead part 1c Lead shadow 3 Image capturing camera 4 Irradiation light source from the side of measurement stage 4a Light emitted from irradiation light source 4 5 Coplanarity value 6 Light transmission measurement stage 7 Above measurement stage Irradiation light source 7a Irradiation light from irradiation light source 8 8 Image of reference plane 9 Inversion image of image of reference plane 10 Image of lead 1b 11 Composite image of inverted image 9 of reference plane and image of lead 1b

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 測定ステージ上に被測定半導体装置を搭
載し、所定方向から光を照射して上記被測定半導体装置
のリード端子の影を撮像し、前記リード端子と上記測定
ステージ表面の基準平面との間の空隙から上記リード端
子の平坦度を測定する方法において、 上記測定ステージとして光透過性のものを用い、被測定
半導体装置を搭載する前に光を照射して該ステージ表面
の基準平面の画像を得る第1の工程と、 上記ステージに被測定半導体装置を搭載し、所定方向か
ら光を照射してリード端子のみの画像を得る第2の工程
と、 上記第1の工程で得られた測定ステージの基準平面の画
像と、上記第2の工程で得られたリード端子のみの画像
とを合成し、該画像から得られた上記リード端子と上記
基準平面との間の空隙からリード端子の平坦度を測定す
る第3の工程とを含むことを特徴とするリード端子平坦
度測定方法。
1. A semiconductor device to be measured is mounted on a measurement stage, light is irradiated from a predetermined direction to image a shadow of a lead terminal of the semiconductor device to be measured, and a reference plane between the lead terminal and the surface of the measurement stage is taken. In the method of measuring the flatness of the lead terminal from the gap between the semiconductor device and the semiconductor device to be measured, light is radiated before mounting the semiconductor device to be measured. A second step of mounting the semiconductor device to be measured on the stage, irradiating light from a predetermined direction to obtain an image of only the lead terminals, and a second step of obtaining an image of only the lead terminals. The image of the reference plane of the measurement stage and the image of only the lead terminal obtained in the second step are combined, and the lead terminal is obtained from the gap between the lead terminal and the reference plane obtained from the image. Flatness And a third step of measuring the flatness of the lead terminal.
JP3354760A 1991-12-18 1991-12-18 Lead terminal flatness measurement method Expired - Lifetime JP2659645B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3354760A JP2659645B2 (en) 1991-12-18 1991-12-18 Lead terminal flatness measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3354760A JP2659645B2 (en) 1991-12-18 1991-12-18 Lead terminal flatness measurement method

Publications (2)

Publication Number Publication Date
JPH05166907A JPH05166907A (en) 1993-07-02
JP2659645B2 true JP2659645B2 (en) 1997-09-30

Family

ID=18439722

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3354760A Expired - Lifetime JP2659645B2 (en) 1991-12-18 1991-12-18 Lead terminal flatness measurement method

Country Status (1)

Country Link
JP (1) JP2659645B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR102486819B1 (en) * 2022-06-07 2023-01-10 주식회사 트윔 Product inspection method and appratus using light leaking data

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111537518B (en) * 2020-05-25 2024-05-28 珠海格力智能装备有限公司 Method and device for detecting flaws of capacitor terminal, storage medium and processor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR102486819B1 (en) * 2022-06-07 2023-01-10 주식회사 트윔 Product inspection method and appratus using light leaking data

Also Published As

Publication number Publication date
JPH05166907A (en) 1993-07-02

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