JPH0577246B2 - - Google Patents

Info

Publication number
JPH0577246B2
JPH0577246B2 JP62182282A JP18228287A JPH0577246B2 JP H0577246 B2 JPH0577246 B2 JP H0577246B2 JP 62182282 A JP62182282 A JP 62182282A JP 18228287 A JP18228287 A JP 18228287A JP H0577246 B2 JPH0577246 B2 JP H0577246B2
Authority
JP
Japan
Prior art keywords
temperature
signal
temperature detection
circuit
inverted
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
JP62182282A
Other languages
Japanese (ja)
Other versions
JPS6428516A (en
Inventor
Hisayoshi Masuda
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP62182282A priority Critical patent/JPS6428516A/en
Publication of JPS6428516A publication Critical patent/JPS6428516A/en
Publication of JPH0577246B2 publication Critical patent/JPH0577246B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Indication And Recording Devices For Special Purposes And Tariff Metering Devices (AREA)
  • Measurement Of Current Or Voltage (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

[発明の目的] (産業上の利用分野) 本発明は、工業用計測器等における温度補償回
路に関するものである。 (従来の技術) 種々の工業用計測器等では、一般に計測環境の
温度による影響を補償する温度補償回路が設けら
れている。 第3図は従来の温度補償回路の構成を示してい
る。 温度センサ1により主センサ4(工業用計測
器)の計測環境の温度が検出され、温度信号
PETとして出力されている。また、この温度信
号PETは反転増幅器2で反転され反転信号NET
として出力されている。 温度センサ1の出力端と反転増幅器2の出力端
との間には摺動抵抗61が介挿されており、その
摺動子電圧信号CETが温度補償信号として加重
加算回路5にて主センサ4の計測信号に加重され
る。加重加算回路5のオペアンプ51からは温度
補償後の主センサ計測信号が出力されるようにな
つている。 第4図はこの第3図の回路の温度補償の作用特
性を示している。 上記温度信号PETとその反動信号NETとは温
度に対する変化が逆の信号であり、また、摺動子
電圧信号CETは摺動子の位置により符号及び大
きさが異なる温度補償信号となつている。従つ
て、摺動子の位置を調整することにより温度補償
範囲を温度信号PETと反転信号NETとの間で変
え、主センサ4の温度特性を改善することができ
る。 しかしながら、上記工業用計測器(主センサ
4)は、幅広い温度環境下で使用されるものであ
る。このため主センサが、特に第5図に符号Aで
示すような非直線的な温度特性を持つ場合、温度
補償後の特性Bは、0℃以下の低温領域では比較
的平坦な特性を示すものの、0℃以上の高温領域
では温度の上昇につれて垂下する特性を持ち、良
好な温度補償ができない。 (発明が解決しようとする問題点) 上述のように、従来の温度補償回路は、計測器
の特性を考慮することなく、低温領域、高温領域
によらず一律に温度補償をするようにしていたの
で、精確な温度補償とすることができないという
問題点があつた。 本発明は上記問題点に鑑みてなされたものであ
り、その目的は、高温領域、低温領域に応じて精
確な温度補償を簡易な回路構成によつて行うこと
のできる温度補償回路を提供することにある。 [発明の構成] (問題点を解決するための手段) 上記目的を達成するために、本発明は、種々の
物理量を計測して得られる計測信号に対してその
計測環境の温度に応じた温度補償をする回路であ
つて、前記計測環境の温度を検出する温度検出手
段と、この温度検出手段で得られた温度検出信号
の極性を反転して反転信号として出力する信号反
転手段と、それぞれが所定の抵抗を介して前記温
度検出信号とその反転信号とを接続するととも
に、温度検出信号が反転信号よりも大きい場合と
反転信号が温度検出信号よりも大きい場合とでは
導通状態が相互に反転する2つのスイツチ手段
と、前記所定の抵抗を介して出力される温度補償
信号を前記計測信号に加算する加算手段とを有す
ることを特徴とする。 (作用) 本発明では、計測環境の温度検出信号とその反
転信号が得られ、温度検出信号が反転信号より大
きい場合と小さい場合とで別個独立して温度補償
されている。これにより精確な温度補償が可能と
なる。 (実施例) 第1図は本発明が適用された温度補償回路の一
実施例の構成を示している。 本実施例は、温度センサ1と、この温度センサ
1の温度信号PETの極性を反転した反転信号
NETを得る反転増幅器2と、温度信号PETと反
転信号NETの大小に応じて自動的に温度補償の
レンジ切換が可能なスイツチ回路3とを備えてい
る。 主センサ4は種々の物理量(例えば、物体の
歪、重量等)を計測しており、この計測信号には
加重加算回路5でスイツチ回路3からの温度補償
信号(摺動子電圧信号CET)が加重されて温度
補償されるようになつている。 スイツチ回路3は、2つのPNPトランジスタ
31,32と、2つのNPNトランジスタ33,
34とを備えている。 PNPトランジスタ31と32のベースは抵抗
35を介して接地され、またNPNトランジスタ
のベースには抵抗36を介してバイアス電圧V1
が供給されている。トランジスタ31と34の各
エミツタには温度センサ1の温度信号PETが、
トランジスタ32と33の各エミツタには反転増
幅器2の反転信号NETがそれぞれ供給されてい
る。そして、トランジスタ31と33のコレクタ
間には摺動抵抗37が、またトランジスタ32と
34のコレクタ間には摺動抵抗38がそれぞれ介
挿されている。 これら摺動子抵抗37,38の摺動子電圧信号
C1ET,C2ETは抵抗55,54を介して加重
加算回路5で主センサ4からの計測信号に加算さ
れ、計測信号の温度補償がされる。 すなわち、スイツチ回路3は、温度センサ1の
温度信号PETと反転増幅器2から出力される温
度信号PETの反転信号NETとをそれぞれ摺動抵
抗37,38を介して接続するとともに、トラン
ジスタ31,33から成るスイツチ回路とトラン
ジスタ32,34から成るスイツチ回路とで構成
されている。そして、温度信号PETが反転信号
NETよりも高い場合には、トランジスタ31,
33が導通し摺動抵抗37を介して出力される温
度補償信号が加重加算回路5にて主センサ4の計
測信号に加重されて温度補償がされる。逆に反転
信号NETが温度信号PETよりも高い場合には、
トランジスタ32,34が導通し摺動抵抗38を
介して出力される温度補償信号が加重加算回路5
にて主センサ4の計測信号に加重されて温度補償
がされる。 次にその作用を第2図を参照して説明する。 第2図において、2つのNPNトランジスタ
Qa,Qbの特性を同等とすると、各トランジスタ
Qa,Qbのコレクタ電流Ic(=Ica=Icb)は、 Ic=I0・exp(q・Vbe/k・T) ……(1) となる。ここで、I0は定数、qは電子の電荷の絶
対値、Vbeはベース・エミツタ間電圧、kはボル
ツマン定数、Tは絶対温度である。 2つのトランジスタQa,Qbのコレクタ電流の
比Ica/Icbは次の(2)式のようになる。 Ica/Icb=exp{q(Eb−Ea)/kT} ……(2) 今、温度を25℃とすると、kT/q≒26mVで
あるから、(2)式によりIca/IcbとEb−Eaとの関
係は次表のように求まる。
[Object of the Invention] (Industrial Application Field) The present invention relates to a temperature compensation circuit in an industrial measuring instrument or the like. (Prior Art) Various industrial measuring instruments and the like are generally provided with a temperature compensation circuit that compensates for the influence of the temperature of the measurement environment. FIG. 3 shows the configuration of a conventional temperature compensation circuit. Temperature sensor 1 detects the temperature of the measurement environment of main sensor 4 (industrial measuring instrument), and sends a temperature signal.
It is output as PET. Also, this temperature signal PET is inverted by the inverting amplifier 2 and the inverted signal NET
It is output as . A sliding resistor 61 is inserted between the output end of the temperature sensor 1 and the output end of the inverting amplifier 2, and the slider voltage signal CET is sent to the main sensor 4 by the weighted addition circuit 5 as a temperature compensation signal. The measurement signal is weighted. The operational amplifier 51 of the weighted addition circuit 5 outputs a temperature-compensated main sensor measurement signal. FIG. 4 shows the operational characteristics of the temperature compensation of the circuit of FIG. The temperature signal PET and its reaction signal NET are signals whose changes with respect to temperature are opposite to each other, and the slider voltage signal CET is a temperature compensation signal whose sign and magnitude differ depending on the position of the slider. Therefore, by adjusting the position of the slider, the temperature compensation range can be changed between the temperature signal PET and the inverted signal NET, and the temperature characteristics of the main sensor 4 can be improved. However, the industrial measuring instrument (main sensor 4) is used in a wide range of temperature environments. Therefore, if the main sensor has a nonlinear temperature characteristic, especially as shown by the symbol A in Figure 5, the characteristic B after temperature compensation will be a relatively flat characteristic in the low temperature region below 0°C. , in a high temperature range of 0° C. or higher, it has a characteristic of drooping as the temperature rises, and good temperature compensation cannot be achieved. (Problems to be solved by the invention) As mentioned above, the conventional temperature compensation circuit performs temperature compensation uniformly regardless of the low temperature region or high temperature region, without considering the characteristics of the measuring instrument. Therefore, there was a problem that accurate temperature compensation could not be achieved. The present invention has been made in view of the above problems, and its purpose is to provide a temperature compensation circuit that can perform accurate temperature compensation depending on high temperature and low temperature regions with a simple circuit configuration. It is in. [Structure of the Invention] (Means for Solving the Problems) In order to achieve the above object, the present invention provides temperature control based on the temperature of the measurement environment for measurement signals obtained by measuring various physical quantities. The compensation circuit includes a temperature detection means for detecting the temperature of the measurement environment, and a signal inversion means for inverting the polarity of the temperature detection signal obtained by the temperature detection means and outputting it as an inverted signal. The temperature detection signal and its inverted signal are connected through a predetermined resistor, and the conduction state is mutually inverted when the temperature detection signal is larger than the inverted signal and when the inverted signal is larger than the temperature detection signal. The present invention is characterized in that it includes two switch means and an addition means for adding a temperature compensation signal outputted via the predetermined resistor to the measurement signal. (Function) In the present invention, a temperature detection signal of the measurement environment and its inverted signal are obtained, and temperature compensation is performed separately and independently when the temperature detection signal is larger than the inverted signal and when it is smaller than the inverted signal. This allows accurate temperature compensation. (Embodiment) FIG. 1 shows the configuration of an embodiment of a temperature compensation circuit to which the present invention is applied. This embodiment uses a temperature sensor 1 and an inverted signal obtained by inverting the polarity of the temperature signal PET of this temperature sensor 1.
NET, and a switch circuit 3 that can automatically switch the temperature compensation range according to the magnitude of the temperature signal PET and the inverted signal NET. The main sensor 4 measures various physical quantities (for example, strain and weight of an object), and a weighted addition circuit 5 adds a temperature compensation signal (slider voltage signal CET) to this measurement signal from the switch circuit 3. It is weighted and temperature compensated. The switch circuit 3 includes two PNP transistors 31 and 32, two NPN transistors 33,
It is equipped with 34. The bases of the PNP transistors 31 and 32 are grounded through a resistor 35, and the base of the NPN transistor is connected to a bias voltage V 1 through a resistor 36.
is supplied. The temperature signal PET from the temperature sensor 1 is applied to each emitter of the transistors 31 and 34.
An inverted signal NET from the inverting amplifier 2 is supplied to each emitter of the transistors 32 and 33, respectively. A sliding resistor 37 is inserted between the collectors of the transistors 31 and 33, and a sliding resistor 38 is inserted between the collectors of the transistors 32 and 34, respectively. The slider voltage signals C1ET and C2ET of these slider resistors 37 and 38 are added to the measurement signal from the main sensor 4 via the resistances 55 and 54 in the weighted addition circuit 5, and the measurement signal is subjected to temperature compensation. That is, the switch circuit 3 connects the temperature signal PET of the temperature sensor 1 and the inverted signal NET of the temperature signal PET outputted from the inverting amplifier 2 via sliding resistors 37 and 38, respectively, and and a switch circuit consisting of transistors 32 and 34. Then, the temperature signal PET is an inverted signal
If higher than NET, transistor 31,
33 becomes conductive, and the temperature compensation signal outputted via the sliding resistor 37 is weighted by the measurement signal of the main sensor 4 in the weighting addition circuit 5 to perform temperature compensation. Conversely, if the inverted signal NET is higher than the temperature signal PET,
When the transistors 32 and 34 become conductive, the temperature compensation signal output via the sliding resistor 38 is sent to the weighted addition circuit 5.
The measurement signal from the main sensor 4 is weighted and temperature compensated. Next, its operation will be explained with reference to FIG. In Figure 2, two NPN transistors
If the characteristics of Qa and Qb are the same, each transistor
The collector currents Ic (=Ica=Icb) of Qa and Qb are as follows: Ic=I 0 · exp (q · Vbe / k · T) ... (1). Here, I 0 is a constant, q is the absolute value of the electron charge, Vbe is the base-emitter voltage, k is Boltzmann's constant, and T is the absolute temperature. The ratio Ica/Icb of the collector currents of the two transistors Qa and Qb is expressed by the following equation (2). Ica/Icb=exp{q(Eb-Ea)/kT}...(2) Now, if the temperature is 25℃, kT/q≒26mV, so Ica/Icb and Eb-Ea can be calculated by equation (2). The relationship with is calculated as shown in the table below.

【表】 上表から理解できるようにEa>Ebの場合、Eb
−Eaが負のときにはコレクタ電流Icaはほとんど
流れず、コレクタ電流Icbのみが流れる。逆にEa
<Ebの場合、Eb−Eaが正の値で大きくなるにつ
れてコレクタ電流Icaが増えIcbはほとんど流れな
い。つまり、トランジスタQa,QbはEb−Eaの
値が0より大か、小かによつてON、OFFが入れ
替わる。 従つて、第1図において温度信号PET>反転
信号NETの場合、すなわち温度が0℃以上(以
下、高温領域という)のときには、トランジスタ
31,33は共にオンとなり、摺動抵抗37に電
流が流れる。このときトランジスタ32,34は
オフである。そして、抵抗37の摺動子を調整す
ることによつて所望の摺動子電圧信号C1ETが
得られ、この摺動子電圧信号C1ETが主センサ
4の計測信号に加重されて高温領域での温度補償
がされる。 一方、温度信号PET<反転信号NETの場合、
すなわち温度が0℃以下(以下、低温領域とい
う)のときには、トランジスタ32,34が共に
オンとなり、摺動抵抗38に電流が流れる。この
とき、トランジスタ31,33はオフである。そ
して、抵抗38の摺動子を調整することによつて
所望の摺動子電圧信号C2ETが得られ、この摺
動子電圧信号C2ETが主センサ4の計測信号に
加重されて低温領域での温度補償がされる。 そして、前述した表の説明からも明らかなよう
に、トランジスタ31,33とトランジスタ3
2,34とのオン−オフの切換点は、摺動抵抗3
7と摺動抵抗38との抵抗比で決定されるので、
温度センサ1の出力信号が電源電圧の変動等によ
つて変動しても切換点まで変動することはない。 このように本実施例によれば、高温領域と低温
領域とで別個に独立して温度補償をすることがで
きるので、温度の高低に影響されずに精確に温度
補償をすることができる。しかも、本実施例によ
れば、高価なアンプや比較器等を用いずに簡単な
回路構成で精確な温度補償が可能となる。 [発明の効果] 以上説明したように本発明によれば、高価なア
ンプや比較器等を用いることなく、簡単な回路構
成によつて計測環境の温度検出信号とその反転信
号の大小に応じて個別に正確な温度補償をするこ
とができる。 また、本発明の2つのスイツチ手段は、温度検
出手段の温度検出信号とその反転信号とを所定の
抵抗を介してそれぞれ接続して構成されており、
その切換点がこの抵抗比により決定できるので、
温度検出手段の温度検出信号が電源電圧の変動等
によつて変動しても2つのスイツチ手段間の導通
状態の切換点が変動することはなく、正確な測定
が可能となる。
[Table] As can be understood from the table above, if Ea > Eb, Eb
When −Ea is negative, almost no collector current Ica flows, and only collector current Icb flows. On the other hand, Ea
In the case of <Eb, as Eb-Ea increases with a positive value, collector current Ica increases and Icb hardly flows. In other words, transistors Qa and Qb are switched between ON and OFF depending on whether the value of Eb-Ea is larger or smaller than 0. Therefore, in FIG. 1, when the temperature signal PET>the inverted signal NET, that is, when the temperature is 0° C. or higher (hereinafter referred to as a high temperature region), both transistors 31 and 33 are turned on, and a current flows through the sliding resistor 37. . At this time, transistors 32 and 34 are off. By adjusting the slider of the resistor 37, a desired slider voltage signal C1ET is obtained, and this slider voltage signal C1ET is weighted with the measurement signal of the main sensor 4 to determine the temperature in the high temperature region. Compensation will be provided. On the other hand, if temperature signal PET < inverted signal NET,
That is, when the temperature is below 0° C. (hereinafter referred to as a low temperature region), both transistors 32 and 34 are turned on, and current flows through the sliding resistor 38. At this time, transistors 31 and 33 are off. By adjusting the slider of the resistor 38, a desired slider voltage signal C2ET is obtained, and this slider voltage signal C2ET is weighted with the measurement signal of the main sensor 4 to adjust the temperature in the low temperature region. Compensation will be provided. As is clear from the explanation of the table above, transistors 31 and 33 and transistor 3
The on-off switching point between 2 and 34 is the sliding resistance 3.
7 and the sliding resistance 38, so
Even if the output signal of the temperature sensor 1 fluctuates due to fluctuations in the power supply voltage, etc., it will not fluctuate to the switching point. As described above, according to this embodiment, temperature compensation can be performed separately and independently in the high temperature region and the low temperature region, so that temperature compensation can be performed accurately without being affected by the height of the temperature. Moreover, according to this embodiment, accurate temperature compensation can be performed with a simple circuit configuration without using expensive amplifiers, comparators, etc. [Effects of the Invention] As explained above, according to the present invention, the temperature detection signal of the measurement environment and its inverted signal can be detected using a simple circuit configuration without using expensive amplifiers or comparators. Accurate temperature compensation can be performed individually. Further, the two switch means of the present invention are configured by connecting the temperature detection signal of the temperature detection means and its inverted signal via a predetermined resistor, respectively.
Since the switching point can be determined by this resistance ratio,
Even if the temperature detection signal of the temperature detection means fluctuates due to fluctuations in the power supply voltage or the like, the switching point of the conduction state between the two switch means does not fluctuate, making accurate measurement possible.

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

第1図は本発明が適用された温度補償回路の一
実施例の構成図、第2図は同実施例の動作原理の
説明図、第3図は従来例の構成図、第4図及び第
5図は従来例の作用説明図である。 1……温度センサ、2……反転増幅器、3……
スイツチ回路、31,32……PNPトランジス
タ、33,34……NPNトランジスタ、37,
38……摺動抵抗、4……主センサ、5……加重
加算回路。
Fig. 1 is a block diagram of an embodiment of a temperature compensation circuit to which the present invention is applied, Fig. 2 is an explanatory diagram of the operating principle of the same embodiment, Fig. 3 is a block diagram of a conventional example, and Figs. FIG. 5 is an explanatory diagram of the operation of the conventional example. 1...Temperature sensor, 2...Inverting amplifier, 3...
Switch circuit, 31, 32...PNP transistor, 33, 34...NPN transistor, 37,
38... Sliding resistance, 4... Main sensor, 5... Weighted addition circuit.

Claims (1)

【特許請求の範囲】 1 種々の物理量を計測して得られる計測信号に
対してその計測環境の温度に応じた温度補償をす
る回路であつて、 前記計測環境の温度を検出する温度検出手段
と、 この温度検出手段で得られた温度検出信号の極
性を反転して反転信号として出力する信号反転手
段と、 それぞれが所定の抵抗を介して前記温度検出信
号とその反転信号とを接続するとともに、温度検
出信号が反転信号よりも大きい場合と反転信号が
温度検出信号よりも大きい場合とでは導通状態が
相互に反転する2つのスイツチ手段と、 前記所定の抵抗を介して出力される温度補償信
号を前記計測信号に加算する加算手段と、 を有することを特徴とする温度補償回路。
[Scope of Claims] 1. A circuit that performs temperature compensation on measurement signals obtained by measuring various physical quantities in accordance with the temperature of the measurement environment, the circuit comprising: temperature detection means for detecting the temperature of the measurement environment; , signal inverting means for inverting the polarity of the temperature detection signal obtained by the temperature detection means and outputting it as an inverted signal, each of which connects the temperature detection signal and its inverted signal via a predetermined resistor; two switching means whose conduction states are mutually inverted when the temperature detection signal is larger than the inversion signal and when the inversion signal is larger than the temperature detection signal; and a temperature compensation signal outputted via the predetermined resistor. A temperature compensation circuit comprising: an addition means for adding to the measurement signal.
JP62182282A 1987-07-23 1987-07-23 Temperature compensating circuit Granted JPS6428516A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62182282A JPS6428516A (en) 1987-07-23 1987-07-23 Temperature compensating circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62182282A JPS6428516A (en) 1987-07-23 1987-07-23 Temperature compensating circuit

Publications (2)

Publication Number Publication Date
JPS6428516A JPS6428516A (en) 1989-01-31
JPH0577246B2 true JPH0577246B2 (en) 1993-10-26

Family

ID=16115547

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62182282A Granted JPS6428516A (en) 1987-07-23 1987-07-23 Temperature compensating circuit

Country Status (1)

Country Link
JP (1) JPS6428516A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4905208B2 (en) * 2006-10-25 2012-03-28 株式会社デンソー Overcurrent detection circuit

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57201996A (en) * 1981-06-08 1982-12-10 Anritsu Electric Co Ltd Gain drift correction circuit

Also Published As

Publication number Publication date
JPS6428516A (en) 1989-01-31

Similar Documents

Publication Publication Date Title
US4833406A (en) Temperature compensated Hall-effect sensor apparatus
JPS61176830A (en) Circuit device for temperature compensation of piezoresistance type pressure sensor
JPH0351118B2 (en)
JPH06188657A (en) Circuit for connecting exponential function step to automatic gain control circuit, automatic gain control circuit and temperature compensation circuit
JPH0577246B2 (en)
JPS59122923A (en) Pressure transmitting device
US4804927A (en) Current amplifier circuit
JPH0823482B2 (en) Temperature compensation circuit for semiconductor strain gauge
KR20000046295A (en) Circuit for automatically controlling op amp input-offset-voltage
ATE100585T1 (en) ARRANGEMENT FOR ELECTRONIC CIRCUIT.
JPS62102612A (en) Gain control circuit
JPH089618Y2 (en) Thermistor temperature conversion circuit
JPS6125319A (en) Comparator
JPH087465Y2 (en) Highly stable constant current power supply
SU1401559A1 (en) Broad-band current amplifier
JP3305864B2 (en) Signal conversion circuit
JPS5848597Y2 (en) Reference junction compensation circuit
JPS643371B2 (en)
JPS6213844B2 (en)
JPH06109677A (en) Humidity detection circuit
JPS5826363Y2 (en) Thermocouple room temperature compensation circuit
JPH0546090Y2 (en)
JPH06109678A (en) Humidity detection circuit
JPH0435776Y2 (en)
JPH0233388Y2 (en)

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term
FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20071026

Year of fee payment: 14