JPH09280916A - Ultrasonic flowmeter - Google Patents

Ultrasonic flowmeter

Info

Publication number
JPH09280916A
JPH09280916A JP8089204A JP8920496A JPH09280916A JP H09280916 A JPH09280916 A JP H09280916A JP 8089204 A JP8089204 A JP 8089204A JP 8920496 A JP8920496 A JP 8920496A JP H09280916 A JPH09280916 A JP H09280916A
Authority
JP
Japan
Prior art keywords
flow
flow velocity
ultrasonic
velocity
laminar
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.)
Granted
Application number
JP8089204A
Other languages
Japanese (ja)
Other versions
JP3732570B2 (en
Inventor
Yutaka Tanaka
豊 田中
Toshihiko Miyamoto
俊彦 宮本
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.)
Aichi Tokei Denki Co Ltd
Original Assignee
Aichi Tokei Denki 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 Aichi Tokei Denki Co Ltd filed Critical Aichi Tokei Denki Co Ltd
Priority to JP08920496A priority Critical patent/JP3732570B2/en
Publication of JPH09280916A publication Critical patent/JPH09280916A/en
Application granted granted Critical
Publication of JP3732570B2 publication Critical patent/JP3732570B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To expand rangeability by highly accurate measurement regardless of laminar layer and turbulence. SOLUTION: An ultrasonic pulse is transmitted or received between ultrasonic elements 2 and 3 provided on a wall of a flow pipe 1 to measure a linear average flow velocity Ve on an axis 4. The ultrasonic pulse is transmitted or received between ultrasonic elements 5 and 6 provided within a fluid to measure the maximum flow velocity Va on an axis 7. When the flow velocity ratio Va/Ve is geater than 1.2, a laminar flow is determined and when the ratio is below 1.2, turbulence is determined. A calculation formula for converting the linear average flow velocity Ve to an average flow velocity at the cross section of the flow pipe is altered between the laminar flow and the turbulence. A flow rate is calculated based on the average flow velocity at the cross section of the flow pipe.

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】本発明は超音波流量計の改良
に関する。
The present invention relates to an improvement of an ultrasonic flowmeter.

【0002】[0002]

【従来の技術】従来の超音波流量計では流体の流れ中を
流れと斜め方向に超音波ビームを発射し、超音波ビーム
の軸線上での線平均流速を測定し、それを流管断面での
平均流速に変換し、これに流管断面積を乗算することで
流量の算出を行っている。
2. Description of the Related Art In a conventional ultrasonic flowmeter, an ultrasonic beam is emitted obliquely to a flow of a fluid, and the average line velocity of the ultrasonic beam on the axis is measured. The average flow velocity is calculated and the flow rate is calculated by multiplying this by the flow tube cross-sectional area.

【0003】[0003]

【発明が解決しようとする課題】流管内の流速分布は層
流と乱流では異なるため、正確な流速を求めるには流れ
の状態が層流か乱流かによって計算式を変更する必要が
ある。ところが前記従来の技術では、流管内の流れが層
流か乱流かを判別する手段がないため、流量の計測精度
が向上できないとか、レンジアビリティを拡大できない
という問題点があった。
Since the flow velocity distribution in the flow tube differs between laminar flow and turbulent flow, it is necessary to change the calculation formula depending on whether the flow state is laminar or turbulent in order to obtain an accurate flow velocity. . However, in the above-mentioned conventional technique, there is no means for discriminating whether the flow in the flow tube is a laminar flow or a turbulent flow, and therefore there are problems that the flow rate measurement accuracy cannot be improved and the rangeability cannot be expanded.

【0004】そこで本発明はこれらの問題点を解消でき
る超音波流量計を提供することを目的とする。
Therefore, an object of the present invention is to provide an ultrasonic flowmeter capable of solving these problems.

【0005】[0005]

【課題を解決するための手段】前記目的を達成するため
に、請求項1の発明は、断面が円形の流管内を流れる流
体の流れ中を流れと斜め方向に超音波ビームを発射し、
該超音波ビームの軸線(4)上での線平均流速(Ve)
を測定し、それを流管断面での平均流速に変換した値に
基いて流量を算出する超音波流量計において、流管
(1)の中心軸(X)上を流れと平行な方向に第2の超
音波ビームを発射して最大流速(Va)を測定し、該最
大流速(Va)と前記線平均流速(Ve)との比より流
れが層流であるか乱流であるかを判別して、線平均流速
(Ve)を流管断面での平均流速に変換する計算式を変
更するようにしたことを特徴とする超音波流量計であ
る。
In order to achieve the above-mentioned object, the invention of claim 1 emits an ultrasonic beam obliquely with the flow of a fluid flowing in a flow tube having a circular cross section,
Linear average flow velocity (Ve) on the axis (4) of the ultrasonic beam
In an ultrasonic flowmeter that calculates the flow rate on the basis of the value obtained by measuring the flow rate of the flow tube (1) in the direction parallel to the flow on the central axis (X) of the flow tube (1). The ultrasonic wave beam 2 is emitted to measure the maximum flow velocity (Va), and it is determined whether the flow is laminar flow or turbulent flow based on the ratio between the maximum flow velocity (Va) and the linear average flow velocity (Ve). Then, the calculation formula for converting the linear average flow velocity (Ve) into the average flow velocity in the cross section of the flow tube is changed, which is an ultrasonic flowmeter.

【0006】請求項2の発明は、請求項1の超音波流量
計において、最大流速(Va)と線平均流速(Ve)と
の比(Va/Ve)が一定値を超えるときには流れが層
流であると判別し前記比(Va/Ve)が一定値以下の
ときには流れが乱流であると判別することを特徴とする
ものである。
According to a second aspect of the invention, in the ultrasonic flowmeter according to the first aspect, the flow is laminar when the ratio (Va / Ve) of the maximum flow velocity (Va) to the linear average flow velocity (Ve) exceeds a certain value. And that the flow is turbulent when the ratio (Va / Ve) is equal to or less than a certain value.

【0007】そして、請求項3の発明は、請求項1又は
2の超音波流量計において、流れと斜め方向の超音波ビ
ームによって該ビームの軸線(4)上での線平均流速
(Ve)を測定するために管璧に設けた二つの超音波素
子(2),(3)と、第2の超音波ビームによって最大
流速(Ve)を測定するために流れ中に設けた二つの超
音波素子(5),(6)とを具備したことを特徴とする
ものである。
According to the invention of claim 3, in the ultrasonic flowmeter according to claim 1 or 2, the linear average flow velocity (Ve) on the axis (4) of the beam is determined by the ultrasonic beam in the flow and oblique directions. Two ultrasonic elements (2), (3) provided on the pipe wall for measurement, and two ultrasonic elements provided in the flow for measuring the maximum flow velocity (Ve) by the second ultrasonic beam. It is characterized by comprising (5) and (6).

【0008】[0008]

【発明の実施の形態】図1は本発明の好ましい実施の形
態で、1は断面が円形の流管で、該流管(1)内を図示
左右方向に流体が流れている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows a preferred embodiment of the present invention, in which 1 is a flow tube having a circular cross section, and a fluid flows in the flow tube (1) in the horizontal direction in the drawing.

【0009】2と3は流管1の管壁に設けた超音波素子
で、両素子間で超音波パルスの送受を行うことで超音波
ビームの軸線4上での線平均流速Veを測定するための
素子である。
Reference numerals 2 and 3 are ultrasonic elements provided on the wall of the flow tube 1, and by transmitting and receiving ultrasonic pulses between the elements, the linear average flow velocity Ve of the ultrasonic beam on the axis 4 is measured. It is an element for.

【0010】軸線4上での線平均流速Veは、一方の超
音波素子2から他方の超音波素子3までの超音波の伝搬
時間と、他方の超音波素子3から一方の超音波素子2ま
での超音波の伝搬時間とから、時間逆数差法を用いて音
速と無関係に求める周知の方法で測定する。
The linear average flow velocity Ve on the axis 4 is the propagation time of ultrasonic waves from one ultrasonic element 2 to the other ultrasonic element 3 and the other ultrasonic element 3 to one ultrasonic element 2. It is measured by a well-known method that is obtained independently of the speed of sound using the time reciprocal difference method from the propagation time of the ultrasonic wave.

【0011】5と6は流管1の中心軸X−X上に離れて
配置した超音波素子で、両素子の間で超音波パルスの送
受を行うことで超音波ビームの軸線7上における最大流
速Vaを測定する。
Reference numerals 5 and 6 denote ultrasonic elements arranged apart from each other on the central axis X-X of the flow tube 1, and by transmitting and receiving ultrasonic pulses between the elements, the maximum of the ultrasonic beam on the axis 7 is obtained. The flow velocity Va is measured.

【0012】最大流速Vaは超音波の順方向伝搬時間と
逆方向伝搬時間とから時間逆数差法を用いて音速と無関
係に求める。図2に示すように、流管1の軸線方向の座
標をχ、半径方向の座標をrとすると、円形断面の流管
1内での流速v(r)は、層流の場合(レイノルズ数R
e≦2300)、 v(r)=(R2 /4μ)(−dp/dχ){1−(r/R)2 }…(1) であらわされる。
The maximum flow velocity Va is obtained from the forward propagation time and the backward propagation time of the ultrasonic wave by using the time reciprocal difference method regardless of the speed of sound. As shown in FIG. 2, when the coordinate in the axial direction of the flow tube 1 is χ and the coordinate in the radial direction is r, the flow velocity v (r) in the flow tube 1 having a circular cross section is laminar (Reynolds number). R
e ≦ 2300), v (r) = (R 2 / 4μ) (− dp / dχ) {1- (r / R) 2 } ... (1)

【0013】但し、 R:流管1の半径 μ:流体の粘度 −dp/dχ:管壁による摩擦損失 である。Where R is the radius of the flow tube 1, μ is the viscosity of the fluid, and dp / dχ is the friction loss due to the tube wall.

【0014】上記(1)式より、軸線7上の最大流速V
aは Va=(R2 /4μ)(−dp/dχ)…(2) となる。
From the above equation (1), the maximum flow velocity V on the axis 7
a becomes Va = (R 2 / 4μ) (− dp / dχ) (2).

【0015】また軸線4上の線平均速度Veは Ve=(R2 /6μ)(−dp/dχ)…(3) となる。The linear average velocity Ve on the axis 4 is Ve = (R 2 / 6μ) (− dp / dχ) (3).

【0016】従って、流れが層流の場合の最大流速Va
と線平均流速Veとの比、つまり流速比Kは K=Va/Ve=(R2 /4μ)(−dp/dχ)/ {(R2 /6μ)(−dp/dχ)}=1.5…(4) となり、一定である。
Therefore, the maximum flow velocity Va when the flow is laminar
And the linear average flow velocity Ve, that is, the flow velocity ratio K is K = Va / Ve = (R 2 / 4μ) (− dp / dχ) / {(R 2 / 6μ) (− dp / dχ)} = 1. 5 ... (4), which is constant.

【0017】流れが層流の場合の流速分布を図3(a)
に示す。次に、流れが乱流の場合の流速分布は図3
(b)のようになり、層流とは異なる流速分布になる。
FIG. 3A shows the flow velocity distribution when the flow is laminar.
Shown in Next, Fig. 3 shows the flow velocity distribution when the flow is turbulent.
As shown in (b), the flow velocity distribution is different from the laminar flow.

【0018】乱流の場合の流速分布v(r)は、実験式
である指数法則の式で示すと、次の(5)式となる。 v(r)=Va{1−(r/R)}1/n …(5) 但し、 n=2.1logRe−1.9 である。
The flow velocity distribution v (r) in the case of turbulent flow is expressed by the following equation (5) when expressed by the exponential law equation which is an empirical equation. v (r) = Va {1- (r / R)} 1 / n (5) However, n = 2.1 log Re-1.9.

【0019】(5)式を解いて、超音波ビームの軸線4
上の線平均流速Veを求めると、 Ve={n/(n+1)}Va…(6) となる。従って流速比Kは K=Va/Ve=(n+1)/n…(7) となる。
Solving the equation (5), the axis line 4 of the ultrasonic beam
When the upper linear average flow velocity Ve is calculated, Ve = {n / (n + 1)} Va ... (6) Therefore, the flow velocity ratio K is K = Va / Ve = (n + 1) / n (7)

【0020】ここで、乱流となる最小のレイノルズ数R
e=2300を考えたとき、n=5.16となり、流速
比Kは K≦1.2…(8) となる。
Here, the minimum Reynolds number R that causes turbulence
Considering e = 2300, n = 5.16, and the flow velocity ratio K becomes K ≦ 1.2 (8).

【0021】上述のように、層流と乱流では(4)式と
(8)式に示すように流速比Kの値が明確に違うため、
流速比Kの値によって流れの状態が層流か乱流かを判別
する。
As described above, the values of the flow velocity ratio K are clearly different between the laminar flow and the turbulent flow as shown in the equations (4) and (8).
The value of the flow velocity ratio K determines whether the flow state is laminar or turbulent.

【0022】そして、層流の場合と乱流の場合とで異な
る計算式を用いて、前記線平均流速Veを流管1の断面
での平均流速に変換し、変換した平均流速に基いて流量
を算出する。
The linear average flow velocity Ve is converted into an average flow velocity in the cross section of the flow tube 1 by using different calculation formulas for laminar flow and turbulent flow, and the flow rate is converted based on the converted average flow velocity. To calculate.

【0023】線平均流速Veを、層流や乱流の場合に、
流管断面での平均流速に変換する計算式は周知の式を用
いることができる。そして、こうして求めた流管断面で
の平均流速に流管断面積を乗算して流量を算出するのも
周知の計算を用いる。
The linear mean flow velocity Ve is calculated in the case of laminar flow or turbulent flow.
A well-known formula can be used as a calculation formula for converting into the average flow velocity in the cross section of the flow tube. A well-known calculation is also used to calculate the flow rate by multiplying the average flow velocity in the flow pipe cross section thus obtained by the flow pipe cross sectional area.

【0024】[0024]

【発明の効果】本発明の超音波流量計は上述のように構
成されているので、層流か乱流かで断面平均流速の計算
式を変更できるため、より正確な流量計測が可能とな
り、測定精度が向上する。
Since the ultrasonic flowmeter of the present invention is configured as described above, the calculation formula of the cross-sectional average flow velocity can be changed depending on the laminar flow or the turbulent flow, which enables more accurate flow measurement. Measurement accuracy is improved.

【0025】また層流、乱流にかかわらず高精度の測定
ができるため、広い流量範囲での測定が可能となり、レ
ンジアビリティの拡大に役立つ。
Since highly accurate measurement can be performed regardless of laminar flow or turbulent flow, measurement can be performed in a wide flow rate range, which is useful for expanding rangeability.

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

【図1】本発明の実施の形態を示す縦断面図である。FIG. 1 is a longitudinal sectional view showing an embodiment of the present invention.

【図2】流速分布を説明する図である。FIG. 2 is a diagram illustrating a flow velocity distribution.

【図3】(a)は層流の流速分布、(b)は乱流の流速
分布を示す図である。
FIG. 3A is a diagram showing a laminar flow velocity distribution, and FIG. 3B is a diagram showing a turbulent flow velocity distribution.

【符号の説明】[Explanation of symbols]

1…流管 2,3,5,6…超音波素子 4,7…超音波ビームの軸線 X…流管の中心軸 Va…最大流速 Ve…線平均流速 1 ... Flow tube 2, 3, 5, 6 ... Ultrasonic element 4, 7 ... Axis line of ultrasonic beam X ... Central axis of flow tube Va ... Maximum flow velocity Ve ... Linear average flow velocity

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 断面が円形の流管内を流れる流体の流れ
中を流れと斜め方向に超音波ビームを発射し、該超音波
ビームの軸線(4)上での線平均流速(Ve)を測定
し、それを流管断面での平均流速に変換した値に基いて
流量を算出する超音波流量計において、 流管(1)の中心軸(X)上を流れと平行な方向に第2
の超音波ビームを発射して最大流速(Va)を測定し、 該最大流速(Va)と前記線平均流速(Ve)との比よ
り流れが層流であるか乱流であるかを判別して、線平均
流速(Ve)を流管断面での平均流速に変換する計算式
を変更するようにしたことを特徴とする超音波流量計。
1. A linear average flow velocity (Ve) on an axis (4) of the ultrasonic beam is measured by emitting an ultrasonic beam obliquely to the flow of a fluid flowing in a flow tube having a circular cross section. Then, in the ultrasonic flowmeter that calculates the flow rate based on the value converted into the average flow velocity in the cross section of the flow tube, in the direction parallel to the flow on the central axis (X) of the flow tube (1),
Of the ultrasonic beam to measure the maximum flow velocity (Va), and determine whether the flow is laminar flow or turbulent flow from the ratio of the maximum flow velocity (Va) and the linear average flow velocity (Ve). The ultrasonic flowmeter is characterized in that the calculation formula for converting the linear average flow velocity (Ve) into the average flow velocity in the cross section of the flow tube is changed.
【請求項2】 最大流速(Va)と線平均流速(Ve)
との比(Va/Ve)が一定値を超えるときには流れが
層流であると判別し 前記比(Va/Ve)が一定値以下のときには流れが乱
流であると判別することを特徴とする請求項1記載の超
音波流量計。
2. Maximum flow velocity (Va) and linear average flow velocity (Ve)
When the ratio (Va / Ve) to and exceeds a constant value, the flow is determined to be laminar flow, and when the ratio (Va / Ve) is equal to or less than a constant value, the flow is determined to be turbulent. The ultrasonic flowmeter according to claim 1.
【請求項3】 流れと斜め方向の超音波ビームによって
該ビームの軸線(4)上での線平均流速(Ve)を測定
するために管璧に設けた二つの超音波素子(2),
(3)と、 第2の超音波ビームによって最大流速(Ve)を測定す
るために流れ中に設けた二つの超音波素子(5),
(6)とを具備したことを特徴とする請求項1又は2記
載の超音波流量計。
3. Two ultrasonic elements (2) provided in the pipe wall for measuring the linear mean flow velocity (Ve) on the axis (4) of the beam by the flow and oblique ultrasonic beams,
(3), and two ultrasonic elements (5) provided in the flow for measuring the maximum flow velocity (Ve) by the second ultrasonic beam,
The ultrasonic flowmeter according to claim 1 or 2, further comprising (6).
JP08920496A 1996-04-11 1996-04-11 Ultrasonic flow meter Expired - Fee Related JP3732570B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP08920496A JP3732570B2 (en) 1996-04-11 1996-04-11 Ultrasonic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP08920496A JP3732570B2 (en) 1996-04-11 1996-04-11 Ultrasonic flow meter

Publications (2)

Publication Number Publication Date
JPH09280916A true JPH09280916A (en) 1997-10-31
JP3732570B2 JP3732570B2 (en) 2006-01-05

Family

ID=13964197

Family Applications (1)

Application Number Title Priority Date Filing Date
JP08920496A Expired - Fee Related JP3732570B2 (en) 1996-04-11 1996-04-11 Ultrasonic flow meter

Country Status (1)

Country Link
JP (1) JP3732570B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002267513A (en) * 2001-03-14 2002-09-18 Aichi Tokei Denki Co Ltd Ultrasonic flowmeter
JP2008298560A (en) * 2007-05-31 2008-12-11 Ricoh Elemex Corp Ultrasonic flow meter and flow rate measurement method
JP2009019879A (en) * 2007-07-10 2009-01-29 Ricoh Elemex Corp Ultrasonic flowmeter and flow measuring method
US20130172755A1 (en) * 2011-12-29 2013-07-04 Samsung Medison Co., Ltd. Providing turbulent flow information based on vector doppler in ultrasound system

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002267513A (en) * 2001-03-14 2002-09-18 Aichi Tokei Denki Co Ltd Ultrasonic flowmeter
JP4675490B2 (en) * 2001-03-14 2011-04-20 愛知時計電機株式会社 Ultrasonic flow meter
JP2008298560A (en) * 2007-05-31 2008-12-11 Ricoh Elemex Corp Ultrasonic flow meter and flow rate measurement method
JP2009019879A (en) * 2007-07-10 2009-01-29 Ricoh Elemex Corp Ultrasonic flowmeter and flow measuring method
US20130172755A1 (en) * 2011-12-29 2013-07-04 Samsung Medison Co., Ltd. Providing turbulent flow information based on vector doppler in ultrasound system

Also Published As

Publication number Publication date
JP3732570B2 (en) 2006-01-05

Similar Documents

Publication Publication Date Title
JP2935833B2 (en) Multi-line flow measurement device
US6931945B2 (en) Doppler ultrasonic flowmeter
JP5222858B2 (en) Ultrasonic flow meter system
US10330509B2 (en) Method and arrangement for an ultrasound clamp-on flow measurement and circuit arrangement for control of an ultrasound clamp-on flow measurement
JP2010512510A (en) Ultrasonic flow measurement method and system
EP1726920B1 (en) Method for ultrasonic Doppler fluid flow measurement
JP2002520583A (en) Multi-code flow meter
JPH09280916A (en) Ultrasonic flowmeter
JP2956805B2 (en) Ultrasonic flow meter
JP5641491B2 (en) Ultrasonic flow meter
JP2956804B2 (en) Ultrasonic flow meter
JP4675490B2 (en) Ultrasonic flow meter
JPH10239125A (en) Ultrasonic flowmeter
JP5483192B2 (en) Ultrasonic flow meter
KR100562266B1 (en) Methode of measuring fluid velocity in ultrasonic multi-beam flowmeter by double integral calculus
JP3194270B2 (en) Ultrasonic flow meter
US6923073B2 (en) Ultrasonic flow-measuring method
CN110799808B (en) Apparatus and method for ultrasonic flow measurement
JPS6040916A (en) Correcting method of temperature-change error of ultrasonic wave flow speed and flow rate meter
JPS58811Y2 (en) ultrasonic flow meter
JPH03197822A (en) Ultrasonic flowmeter
JP2006194634A (en) Doppler-type ultrasonic flowmeter, method for adjusting transmission voltage to ultrasonic vibrator in it, and method for monitoring state in fluid inside piping
RU2064164C1 (en) Method of determination of flow rate
SU1476311A1 (en) Ultrasonic flowmeter
JPH05180679A (en) Ultrasonic flow meter

Legal Events

Date Code Title Description
A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20050225

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20050927

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20051013

R150 Certificate of patent or registration of utility model

Free format text: JAPANESE INTERMEDIATE CODE: R150

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20081021

Year of fee payment: 3

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20091021

Year of fee payment: 4

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20091021

Year of fee payment: 4

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20101021

Year of fee payment: 5

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20101021

Year of fee payment: 5

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20111021

Year of fee payment: 6

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20121021

Year of fee payment: 7

LAPS Cancellation because of no payment of annual fees