JPH0539501Y2 - - Google Patents

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Publication number
JPH0539501Y2
JPH0539501Y2 JP2202587U JP2202587U JPH0539501Y2 JP H0539501 Y2 JPH0539501 Y2 JP H0539501Y2 JP 2202587 U JP2202587 U JP 2202587U JP 2202587 U JP2202587 U JP 2202587U JP H0539501 Y2 JPH0539501 Y2 JP H0539501Y2
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JP
Japan
Prior art keywords
probe
terminal
conductor
grounding conductor
measured
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
JP2202587U
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Japanese (ja)
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JPS63129877U (en
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Filing date
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Priority to JP2202587U priority Critical patent/JPH0539501Y2/ja
Publication of JPS63129877U publication Critical patent/JPS63129877U/ja
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Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Tests Of Electronic Circuits (AREA)
  • Testing Of Individual Semiconductor Devices (AREA)
  • Measuring Leads Or Probes (AREA)
  • Measurement Of Current Or Voltage (AREA)

Description

【考案の詳細な説明】 [産業上の利用分野] 本考案は、パルス信号用プローブに関するもの
である。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a pulse signal probe.

[従来の技術] 第4図は、従来の同軸伝送路を使用したパルス
信号用プローブである。
[Prior Art] FIG. 4 shows a pulse signal probe using a conventional coaxial transmission line.

ECL等のロジツクICからなる被測定物5を測
定する際、このプローブ6を被測定物5に接触さ
せると、被測定物5側のアース端子5bとプロー
ブ6のアース用導体6bとはDC(直流)的に導通
を持つている。
When measuring an object to be measured 5 made of a logic IC such as an ECL, when this probe 6 is brought into contact with the object to be measured 5, the ground terminal 5b on the object to be measured 5 and the grounding conductor 6b of the probe 6 are connected to DC ( It has continuity in terms of direct current (DC).

[考案が解決しようとする問題点] しかし、このような構造では、プローブ6のア
ース用導体6bを被測定物5の電源端子5cに接
続すると、プローブ6に接続したオシロスコープ
(図示略)等のアース端子に電圧がかかつてシヨ
ートし、オシロスコープの内部回路を破壊してし
まうために、電源端子5cを測定用アース端子と
して使用することはできなかつた。
[Problems to be solved by the invention] However, in such a structure, when the grounding conductor 6b of the probe 6 is connected to the power supply terminal 5c of the device under test 5, the oscilloscope (not shown) etc. connected to the probe 6 The power supply terminal 5c could not be used as a measurement ground terminal because the voltage would build up at the ground terminal and cause a shock, destroying the internal circuitry of the oscilloscope.

したがつて通常、信号端子5aとアース端子5
bとを用いようとすれば、これらの間の距離が離
れてしまう場合が多く、特にマイクロ波帯におい
てはリードインダクタンスが増加し測定波形が乱
れやすかつた。
Therefore, normally, the signal terminal 5a and the ground terminal 5
If an attempt is made to use B, the distance between them is often large, and especially in the microwave band, the lead inductance increases and the measured waveform is likely to be disturbed.

本考案は、これらの欠点を取り除くために考え
られたものであり、その目的は、被測定物の信号
端子の近くにある電源端子を測定用アース端子と
して使用することにより、パルス波形が乱れない
状態で被測定物の高周波特性、及び低周波特性が
同時に評価でき、さらにこれを1本のプローブで
容易に行なえるパルス信号用プローブを提供する
ことにある。
The present invention was devised to eliminate these drawbacks, and its purpose is to use the power supply terminal near the signal terminal of the device under test as the measurement ground terminal, so that the pulse waveform is not disturbed. It is an object of the present invention to provide a pulse signal probe capable of simultaneously evaluating high-frequency characteristics and low-frequency characteristics of an object to be measured under the same conditions, and also capable of easily performing this evaluation with a single probe.

[問題点を解決するための手段] 上記問題点を解決するため、本考案によるパル
ス信号用プローブは、信号用導体1aとアース用
導体1bとを有するパルス信号用プローブ1にお
いて、前記アース用導体1bをDC的に切断し、
この切断部1bbをコンデンサ2で高周波的に接
続して交流用アース導体とするとともに、一端が
前記切断部の手前側に電気的に接続され、他端が
被測定物5の終端電圧端子5bにDC的に接続さ
れたDCアーム用導体3を持つことを特徴として
いる。
[Means for Solving the Problems] In order to solve the above problems, a pulse signal probe according to the present invention includes a pulse signal probe 1 having a signal conductor 1a and a grounding conductor 1b. 1b is cut in a DC manner,
This cut section 1bb is connected at high frequency with a capacitor 2 to serve as an AC ground conductor, and one end is electrically connected to the front side of the cut section, and the other end is connected to the terminal voltage terminal 5b of the object to be measured 5. It is characterized by having a DC arm conductor 3 connected in a DC manner.

[作用] 上記構成による作用を説明すると、プローブ1
のアース用導体1bはDC的にカツトされ、コン
デンサ2により高周波的に接続され、信号端子5
aにプローブ1の信号用導体1aを、さらに電源
端子5cにアース用導体1bを接触させれば高周
波特性を測定できる。また、同時に終端電圧端子
(アース端子)5bにプローブ1のDCアース用導
体3を接触させれば低周波特性が測定できる。
[Operation] To explain the operation of the above configuration, probe 1
The grounding conductor 1b is cut in a DC manner, connected in a high frequency manner by a capacitor 2, and connected to a signal terminal 5.
The high frequency characteristics can be measured by bringing the signal conductor 1a of the probe 1 into contact with the probe 1a and by contacting the grounding conductor 1b with the power supply terminal 5c. Furthermore, by simultaneously bringing the DC ground conductor 3 of the probe 1 into contact with the termination voltage terminal (earth terminal) 5b, the low frequency characteristics can be measured.

[実施例] 以下、本考案のパルス信号用プローブの一実施
例を説明する。
[Example] Hereinafter, an example of the pulse signal probe of the present invention will be described.

第1図は、パルス信号用プローブを示す図であ
る。
FIG. 1 is a diagram showing a pulse signal probe.

図において、1はセミリジツトケーブル等によ
り構成される同軸伝送路であり、プローブとして
機能する。このプローブ1は信号用導体1a、ア
ース用導体1bを有する。
In the figure, reference numeral 1 denotes a coaxial transmission line composed of a semi-rigid cable or the like, which functions as a probe. This probe 1 has a signal conductor 1a and a ground conductor 1b.

そして、アース用導体1bは一部が切断されて
おり、この切断部1bbにはコンデンサ2が接続
されている。
A portion of the ground conductor 1b is cut off, and a capacitor 2 is connected to this cut portion 1bb.

したがつて、プローブ1の信号用導体1aは被
測定物5の信号端子5aに接触し、アース用導体
1bは電源端子5cに接触できる。
Therefore, the signal conductor 1a of the probe 1 can contact the signal terminal 5a of the object to be measured 5, and the ground conductor 1b can contact the power supply terminal 5c.

また、コンデンサ2を介さないでアース用導体
1bとアース端子5bとがDC用アース導体3に
より接続される。
Further, the grounding conductor 1b and the grounding terminal 5b are connected by the DC grounding conductor 3 without using the capacitor 2.

第2図aは、プローブ1のみの、同図bは、被
測定物5の動作時の電気的な等価回路であり、同
図cはプローブを使用して被測定物5を測定する
場合の電気的な等価回路である。
Figure 2a shows the electrical equivalent circuit of only the probe 1, Figure 2b shows the electrical equivalent circuit of the device under test 5 when it is in operation, and Figure 2c shows the electrical equivalent circuit when measuring the device 5 using the probe. This is an electrical equivalent circuit.

被測定物としてのECL5は、第2図bに示す
ように、動作時にVcc(コレクタ電圧)が0V、
Vee(エミツタ電圧)が−5.2V、VT(出力Qの終
端電圧)が−2Vであり、出力Qはエミツタフオ
ローであるため、50Ωの抵抗を介して端子VT5
b(−2V)に接続される。
As shown in Figure 2b, the ECL5 as the object to be measured has a Vcc (collector voltage) of 0V,
Vee (emitter voltage) is -5.2V, VT (terminal voltage of output Q) is -2V, and output Q is an emitter follower, so it is connected to terminal VT5 through a 50Ω resistor.
b (-2V).

この場合、VTが−2Vのままであるとシンクロ
スコープ等観測系の外筐(グランド電位)を同電
位、即ち−2Vとしなければならず、シンクロス
コープ内の測定回路の破損等の影響を及ぼし、か
つ外筐が電位を有していて人体に対し危険である
から、測定時にはVTを−2Vから0Vに持ち上げ
て観測系の外筐をGNDとしている。
In this case, if VT remains at -2V, the outer casing (ground potential) of the observation system such as the synchroscope must be at the same potential, that is, -2V, which may damage the measurement circuit inside the synchroscope. , and the outer casing has a potential that is dangerous to the human body, so during measurement, VT is raised from -2V to 0V and the outer casing of the observation system is set to GND.

これにより、Veeは−5.2Vから−3.2Vに、Vcc
は0Vから+2Vに各々シフトされる。
This causes Vee to go from −5.2V to −3.2V and Vcc
are shifted from 0V to +2V, respectively.

これにより、ECL5全体のバイアス電圧がシ
フトされ、出力Qの終端電圧が0V(直流的に0V)
となりシンクロスコープで測定が可能となる。こ
の際、ECL5全体のバイアス電圧がシフトされ
てもこのECL5の機能は変わらない。
As a result, the bias voltage of the entire ECL5 is shifted, and the terminal voltage of output Q is 0V (DC 0V)
This makes it possible to measure with a synchroscope. At this time, even if the bias voltage of the entire ECL 5 is shifted, the function of this ECL 5 does not change.

つまり、第2図cに示すように、電源端子5c
は+2Vの電源であるとともに高周波的なアース
として使用され、電源端子5dは−3.2V(5.2V−
2V=3.2V)の電源となり、信号端子5aの終端
電圧は+2Vシフトし0Vとなりシンクロスコープ
で観測可能な信号となり、端子5bの電源VTは
(直流的に)GNDとなる。
In other words, as shown in FIG. 2c, the power supply terminal 5c
is a +2V power supply and is used as a high frequency ground, and the power supply terminal 5d is -3.2V (5.2V -
2V=3.2V), the terminal voltage of the signal terminal 5a shifts by +2V and becomes 0V, which becomes a signal that can be observed with a synchroscope, and the power supply VT of the terminal 5b becomes GND (in terms of direct current).

この時、観測系のGNDは、ECL5のVTから
取つてもよいし、基準(OV)となるものであれ
ば他から取つてもよい。
At this time, the GND of the observation system may be taken from the VT of ECL5, or may be taken from another source as long as it serves as the reference (OV).

したがつて、プローブ1のアース用導体1bは
DC的にカツトされ、コンデンサ2により高周波
的に接続されているため、信号端子5aにプロー
ブ1の信号用導体1aを、さらに電源端子5cに
アース用導体1bを接触させれば高周波特性を測
定できる。
Therefore, the grounding conductor 1b of the probe 1 is
Since it is cut in a DC manner and connected in a high frequency manner by a capacitor 2, high frequency characteristics can be measured by contacting the signal conductor 1a of the probe 1 to the signal terminal 5a and the grounding conductor 1b to the power supply terminal 5c. .

また、同時にアース端子5bにプローブ1の
DCアース用導体3を接触させれば低周波特性が
測定できる。この時、観測系のGNDは統一され
ている。
At the same time, connect probe 1 to ground terminal 5b.
By bringing the DC grounding conductor 3 into contact, low frequency characteristics can be measured. At this time, the GND of the observation system is unified.

次に第3図は、本考案の他の実施例を示す図で
ある。
Next, FIG. 3 is a diagram showing another embodiment of the present invention.

この図において、前述のDC用アース導体3に
は抵抗7が介挿されている。
In this figure, a resistor 7 is inserted into the DC ground conductor 3 described above.

前述のコンデンサ2とDC用アース導体3が有
するインダクタンスは共振回路を形成し、この共
振周波数が測定帯域内に入る場合は測定に悪影響
を及ぼす場合がある。この影響を軽減するために
DC用アース導体3に直列に抵抗7を介挿すれば、
共振回路のQを下げることができる。
The inductance of the capacitor 2 and the DC ground conductor 3 forms a resonant circuit, and if this resonant frequency falls within the measurement band, it may adversely affect the measurement. To reduce this effect
If a resistor 7 is inserted in series with the DC ground conductor 3,
It is possible to lower the Q of the resonant circuit.

尚、DCアース用導体3自体が抵抗成分を有し
ているものを用いてもよい。
Note that the DC grounding conductor 3 itself may have a resistance component.

尚、上述の実施例では、コンデンサ2の形状を
限定していないが、例えば、アース導体1bに
0.2mm巾で形成した切断部1bbの一部に1mm角の
両面電極(幅が0.4mm)のコンデンサ2をはんだ
付けして良好な特性が得られた。さらに、切断部
1bbの周囲に複数個のコンデンサを設けたり、
切断部1bbの周囲を覆うドーナツ形状のコンデ
ンサであつてもよい。
In the above embodiment, the shape of the capacitor 2 is not limited, but for example, the shape of the capacitor 2 is
A 1 mm square capacitor 2 with double-sided electrodes (width: 0.4 mm) was soldered to a part of the cut portion 1bb formed with a width of 0.2 mm, and good characteristics were obtained. Furthermore, multiple capacitors are provided around the cutting part 1bb,
It may be a donut-shaped capacitor that covers the periphery of the cut portion 1bb.

また、上述の実施例では、プローブ1として同
軸伝送路を用いて説明したが他にトリプレート線
路等マツチング線路であればこれを用いることが
できる。
Further, in the above embodiment, a coaxial transmission line was used as the probe 1, but any other matching line such as a triplate line may be used.

[考案の効果] 以上の説明したように、本考案のパルス信号用
プローブによれば、パルス波形が乱れず測定誤差
を生じない状態で被測定物の高周波特性及び低周
波特性が同時に測定でき、総合的な特性評価がで
きる。
[Effects of the invention] As explained above, according to the pulse signal probe of the invention, the high-frequency characteristics and low-frequency characteristics of the object to be measured can be measured simultaneously without disturbing the pulse waveform and causing measurement errors. Comprehensive characteristic evaluation is possible.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本考案のパルス信号用プローブを示
す図、第2図a,b,cは、同プローブの電気的
な等価回路図であり、第2図cは、基準電源を用
いてプローブのGNDを得ることを示す図、第3
図は、本考案の他の実施例を示す図、第4図は、
従来のプローブを示す図である。 1……同軸伝送路、1a……信号用導体、1b
……アース用導体、2……コンデンサ、3……
DCアース用導体、5……被測定物、5a……信
号端子、5b……アース端子、5c……電源端
子、5a……電源端子、7……抵抗。
FIG. 1 is a diagram showing the pulse signal probe of the present invention, FIG. 2 a, b, and c are electrical equivalent circuit diagrams of the probe, and FIG. Figure 3 shows how to obtain the GND of
The figure shows another embodiment of the present invention, and FIG.
It is a figure showing a conventional probe. 1... Coaxial transmission line, 1a... Signal conductor, 1b
...Grounding conductor, 2...Capacitor, 3...
DC grounding conductor, 5...Object to be measured, 5a...Signal terminal, 5b...Earth terminal, 5c...Power terminal, 5a...Power terminal, 7...Resistor.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 信号用導体1aとアース用導体1bとを有する
パルス信号用プローブ1において、前記アース用
導体1bをDC的に切断し、この切断部1bbをコ
ンデンサ2で高周波的に接続して交流用アース導
体とするとともに、一端が前記切断部の手前側に
電気的に接続され、他端が被測定物5の終端電圧
端子5bにDC的に接続されたDCアース用導体3
を持つことを特徴としたパルス信号用プローブ。
In a pulse signal probe 1 having a signal conductor 1a and a grounding conductor 1b, the grounding conductor 1b is cut in a DC manner, and this cut portion 1bb is connected in a high frequency manner with a capacitor 2 to serve as an AC grounding conductor. At the same time, a DC grounding conductor 3 has one end electrically connected to the front side of the cutting part and the other end DC-connected to the termination voltage terminal 5b of the object to be measured 5.
A pulse signal probe characterized by:
JP2202587U 1987-02-19 1987-02-19 Expired - Lifetime JPH0539501Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2202587U JPH0539501Y2 (en) 1987-02-19 1987-02-19

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2202587U JPH0539501Y2 (en) 1987-02-19 1987-02-19

Publications (2)

Publication Number Publication Date
JPS63129877U JPS63129877U (en) 1988-08-24
JPH0539501Y2 true JPH0539501Y2 (en) 1993-10-06

Family

ID=30819012

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2202587U Expired - Lifetime JPH0539501Y2 (en) 1987-02-19 1987-02-19

Country Status (1)

Country Link
JP (1) JPH0539501Y2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8690762B2 (en) 2008-06-18 2014-04-08 Raytheon Company Transparent endoscope head defining a focal length
US9144664B2 (en) 2009-10-01 2015-09-29 Sarcos Lc Method and apparatus for manipulating movement of a micro-catheter
US9259142B2 (en) 2008-07-30 2016-02-16 Sarcos Lc Method and device for incremental wavelength variation to analyze tissue

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8690762B2 (en) 2008-06-18 2014-04-08 Raytheon Company Transparent endoscope head defining a focal length
US9521946B2 (en) 2008-06-18 2016-12-20 Sarcos Lc Transparent endoscope head defining a focal length
US9259142B2 (en) 2008-07-30 2016-02-16 Sarcos Lc Method and device for incremental wavelength variation to analyze tissue
US9144664B2 (en) 2009-10-01 2015-09-29 Sarcos Lc Method and apparatus for manipulating movement of a micro-catheter

Also Published As

Publication number Publication date
JPS63129877U (en) 1988-08-24

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