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JP6366172B2 - Flow field measurement method using microbubbles and flow field measurement device for aquarium - Google Patents

Flow field measurement method using microbubbles and flow field measurement device for aquarium Download PDF

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JP6366172B2
JP6366172B2 JP2014107253A JP2014107253A JP6366172B2 JP 6366172 B2 JP6366172 B2 JP 6366172B2 JP 2014107253 A JP2014107253 A JP 2014107253A JP 2014107253 A JP2014107253 A JP 2014107253A JP 6366172 B2 JP6366172 B2 JP 6366172B2
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microbubbles
flow field
bubble
bubble blowing
blowing means
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JP2015222231A (en
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弘樹 大場
弘樹 大場
邦弘 星野
邦弘 星野
勝 辻本
辻本  勝
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National Institute of Maritime Port and Aviation Technology
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Description

本発明は、微小気泡を用いた流場計測方法及び水槽用流場計測装置に関する。   The present invention relates to a flow field measuring method and a water tank flow field measuring apparatus using microbubbles.

船舶の水槽試験では抵抗試験や自航試験により実船の抵抗や推進性能を予測する試験が多く行われているが、近年はより正確な推進性能評価や、船型改良のためにPIV(Particle Image Velocimetry)による流場計測が盛んに行われている。曳航水槽や回流水槽へのPIV適用は既に一般的となり、様々な計測事例が報告されている。船舶の船尾流れ(流場)は複雑な3次元的な流れも多く、この流場を計測するためにカメラを2台以上使用した複眼立体視によるSPIV(Stereo PIV)や3DPTV(3 Dimensional Particle Tracking Velocimetry)を用いた計測が行われ、水槽試験における流場計測手法として利用されている。
PIVやPTVの計測にはトレーサが必要不可欠であり、一般的には銀コート中空ガラスビーズやナイロンパウダー等の水の比重に近い固体粒子を用いることが多い。しかし、供給した固体粒子の回収はほぼ不可能であり、水槽施設の保守及び精度管理の観点から固体粒子の水槽水への散布に問題がある。
一方、固体粒子と異なり水槽中に残留することのない微小気泡をトレーサとして使用した流場計測も行われているが、これらは自由表面を持たない流場を対象としている。
そこで、水槽中に残留することのない微小気泡をトレーサとして使用することで、自由表面を持つ流場の計測が可能な観測、特に船舶試験水槽での平水中及び波浪中における模型船の船尾流れの観測が求められている。
ここで、特許文献1は、可視粒子を用いて機器内部の流場の解析や流速の測定を行うことが可能な可視化用粒子発生装置に関し、可視粒子として気泡を用いている。
また、特許文献2は、気泡を利用して流れを可視化する装置を提案している。
また、特許文献3には、PIV計測やレーザシート光を用いることが記載されている。
また、特許文献4及び特許文献5には、PIVやレーザシート光を用いて複雑な流場における流体の流動を計測することが記載されている。
また、特許文献6には、トレーサとして第1流体をノズル孔から第2流体の流場内に供給し、流場内を横切るようにレーザ光を照射し、流場内を通過したレーザ光を受光し、受光したレーザ光のスキャン強度信号を用いて、第1流体がレーザ光を横切る位置を求めることにより、第2流体の流れを可視化できる装置が開示されている。
There are many tests to predict the resistance and propulsion performance of an actual ship by resistance test and self-propulsion test, but in recent years PIV (Particle Image) has been used for more accurate propulsion performance evaluation and ship shape improvement. Flow field measurement by velocimetry) is actively performed. Application of PIV to towed water tanks and circulating water tanks is already common, and various measurement cases have been reported. The stern flow (flow field) of a ship has many complicated three-dimensional flows. In order to measure this flow field, SPIV (stereo PIV) or 3DPTV (3 Dimensional Particle Tracking) using two or more cameras using two or more cameras. Measurement using Velocity) is performed and used as a flow field measurement method in a water tank test.
A tracer is indispensable for the measurement of PIV and PTV. In general, solid particles close to the specific gravity of water such as silver-coated hollow glass beads and nylon powder are often used. However, it is almost impossible to recover the supplied solid particles, and there is a problem in spraying the solid particles into the aquarium water from the viewpoint of maintenance and accuracy control of the aquarium facility.
On the other hand, unlike solid particles, flow field measurement using microbubbles that do not remain in the water tank as a tracer is also performed, but these are intended for flow fields that do not have a free surface.
Therefore, by using microbubbles that do not remain in the tank as a tracer, it is possible to measure the flow field with a free surface, especially the stern flow of a model ship in plain water and waves in a ship test tank. Observation is required.
Here, Patent Document 1 relates to a visualization particle generator that can analyze a flow field inside a device and measure a flow velocity using visible particles, and uses bubbles as visible particles.
Patent Document 2 proposes an apparatus for visualizing a flow using bubbles.
Patent Document 3 describes using PIV measurement and laser sheet light.
Patent Literature 4 and Patent Literature 5 describe that fluid flow in a complicated flow field is measured using PIV or laser sheet light.
Further, Patent Document 6 supplies a first fluid as a tracer from a nozzle hole into a flow field of a second fluid, irradiates laser light so as to cross the flow field, and receives the laser light that has passed through the flow field, An apparatus is disclosed that can visualize the flow of the second fluid by determining the position at which the first fluid crosses the laser beam using the scan intensity signal of the received laser beam.

特開平6−148216号公報JP-A-6-148216 特開平9−288122号公報JP-A-9-288122 特開2013−29423号公報JP 2013-29423 A 特開2002−22759号公報JP 2002-22759 A 特開2004−20385号公報JP 2004-20385 A 特開2012−103041号公報JP2012-103041A

しかし、特許文献1は、水中を動く対象物の周囲の流場を計測するものではなく、流場そのものを計測するものであり、可視粒子が流場に注入されるときの初速度が流場を乱す問題を解消するため、前段の注入路中に、可視粒子が初速度を持たないように減速され負圧によって流場に注入される可視粒子初速度減速機構を設けたものである。
また、特許文献2は、気泡を鉱物油内に存在させかつ崩壊させ、外部から識別可能な物質として煙状物質等を鉱物油内に析出または発生させることで流れを可視化するものであり、水中を動く対象物の周囲の流場を計測するものではない。
また、特許文献3は、測定対象物内を流れる粒子の流速及び粒径を算出するものである。
また、特許文献4は、外界と環境を異にする閉空間内の流場の流体の流速や流れ方向を計測するものであり、流場内で対象物が動くことに関する記載は無い。
また、特許文献5は、テストセクションのパイプ内の粒子を撮影し、2枚の画像から速度ベクトルを算出し空間の時系列流体速度を計測するものであり、水中を動く対象物の周囲の流場を計測するものではない。
特許文献6は、空気が一定速度で流れる空気の流場を風洞で形成し、この風洞中に物体を置き、トレーサとして二酸化炭素ガスを複数のノズル孔から流体の流場に供給するものであり、対象物である物体は固定されており、対象物が動くときの周囲の流場を計測するものではない。
However, Patent Document 1 does not measure the flow field around an object moving in water, but measures the flow field itself, and the initial velocity when the visible particles are injected into the flow field is the flow field. In order to solve this problem, a visible particle initial velocity reduction mechanism is provided in the preceding injection path so that the visible particles are decelerated so as not to have the initial velocity and injected into the flow field by negative pressure.
Patent Document 2 visualizes a flow by causing bubbles to exist in mineral oil and collapsing, and depositing or generating a smoke-like substance or the like in the mineral oil as a substance identifiable from the outside. It does not measure the flow field around the moving object.
Moreover, patent document 3 calculates the flow velocity and particle size of the particle | grains which flow through the inside of a measuring object.
Patent Document 4 measures the flow velocity and flow direction of a fluid in a closed space that is different from the environment from the outside, and there is no description regarding the movement of an object in the flow field.
Patent Document 5 captures particles in a pipe in a test section, calculates a velocity vector from two images, and measures a time-series fluid velocity in space. It does not measure the field.
In Patent Document 6, an air flow field in which air flows at a constant speed is formed in a wind tunnel, an object is placed in the wind tunnel, and carbon dioxide gas is supplied as a tracer from a plurality of nozzle holes to a fluid flow field. The object that is the object is fixed and does not measure the surrounding flow field when the object moves.

本発明は、例えば、船舶試験水槽での平水中又は波浪中における模型船の船尾流れ等の水中を動く対象物の周囲の流場を、水中に残留することのない微小気泡をトレーサとして使用することで、高い精度で計測が行える微小気泡を用いた流場計測方法及び水槽用流場計測装置を提供することを目的とする。   The present invention uses, as a tracer, microbubbles that do not remain in water, for example, a flow field around an object moving in water, such as a stern flow of a model ship in a flat water or a wave in a ship test tank. Thus, an object of the present invention is to provide a flow field measurement method and a water tank flow field measurement device using microbubbles that can be measured with high accuracy.

請求項1記載の本発明に対応した微小気泡を用いた流場計測方法においては、水中を動く対象物の周囲の流場を計測する流場計測方法であって、対象物の前方に微小気泡を吹き出す気泡吹出手段を設け、気泡吹出手段を対象物と等速で同一方向に動かし、気泡吹出手段から吹き出す微小気泡を、気泡吹出手段に対し相対的に初速度を有して吹き出し、気泡吹出手段から吹き出されて対象物の周囲を流れる微小気泡の動きに基づいて流場を計測し、流場の計測結果を初速度に基づいて補正することを特徴とする。請求項1に記載の本発明によれば、対象物の前方に設けた対象物と等速で同一方向に動く気泡吹出手段から微小気泡を吹き出すため、対象物の周囲のみにタイミングよく微小気泡を供給でき、対象物の周囲の流場が的確に計測できる。また、計測が完了する前に微小気泡が消失してしまうことがないので精度の高い流場の計測結果を得ることができる。また、計測設備中に残留することがない微小気泡をトレーサとして使用するので、固体粒子をトレーサとして使用する場合と比べて計測設備の保守及び精度管理が容易となる。また、微小気泡が初速度を持たないようにする手段が不要となり、また、流場の計測結果を初速度に基づいて補正するので、初速度の影響を取り除いた結果を得ることができる。 The flow field measurement method using microbubbles corresponding to the present invention according to claim 1 is a flow field measurement method for measuring a flow field around an object moving in water, wherein the microbubbles are placed in front of the object. The bubble blowing means is provided to move the bubble blowing means in the same direction as the object at the same speed, and the microbubbles blown from the bubble blowing means are blown out with the initial velocity relative to the bubble blowing means, and the bubble blowing The flow field is measured based on the movement of microbubbles blown out from the means and flowing around the object , and the measurement result of the flow field is corrected based on the initial velocity . According to the first aspect of the present invention, since the microbubbles are blown out from the bubble blowing means that moves in the same direction at the same speed as the target provided in front of the target, the microbubbles are only timely around the target. The flow field around the object can be accurately measured. In addition, since the microbubbles are not lost before the measurement is completed, a highly accurate flow field measurement result can be obtained. In addition, since microbubbles that do not remain in the measurement facility are used as a tracer, the maintenance and accuracy management of the measurement facility is facilitated as compared with the case where solid particles are used as a tracer. Further, a means for preventing the microbubbles from having the initial velocity is not necessary, and the flow field measurement result is corrected based on the initial velocity, so that the result of removing the influence of the initial velocity can be obtained.

請求項記載の本発明は、初速度を水深方向に異ならせ、水深の深いところの初速度を水深の浅いところの初速度よりも遅くしたことを特徴とする。請求項に記載の本発明によれば、気泡吹出手段を簡単な構成で実現できる。 The present invention described in claim 2 is characterized in that the initial velocity is varied in the direction of water depth, and the initial velocity at a deep water depth is made slower than the initial velocity at a shallow water depth. According to the second aspect of the present invention, the bubble blowing means can be realized with a simple configuration.

請求項記載の本発明は、初速度を調整する初速度調整手段により初速度を制御したことを特徴とする。請求項に記載の本発明によれば、微小気泡の初速度を任意に調整することで、計測に最適な状態で微小気泡を供給することができる。 The invention according to claim 3 is characterized in that the initial speed is controlled by the initial speed adjusting means for adjusting the initial speed. According to the third aspect of the present invention, the microbubbles can be supplied in an optimum state for measurement by arbitrarily adjusting the initial velocity of the microbubbles.

請求項記載の本発明は、微小気泡の気泡直径を5μmから100μmの範囲としたことを特徴とする。請求項に記載の本発明によれば、この気泡直径範囲の微小気泡は気泡同士の結合が行われないため上昇速度を抑えることができ、計測が完了する前に対象物の周囲の流場から微小気泡が浮上して消失してしまうことがなく流場の計測が高い精度で行える。 The present invention according to claim 4 is characterized in that the bubble diameter of the microbubbles is in the range of 5 μm to 100 μm. According to the fourth aspect of the present invention, since the microbubbles in the bubble diameter range are not coupled to each other, the rising speed can be suppressed, and the flow field around the object is completed before the measurement is completed. Therefore, it is possible to measure the flow field with high accuracy without causing microbubbles to rise and disappear.

請求項記載の本発明は、水に微小気泡を予め混ぜて気泡吹出手段に供給し、気泡吹出手段から微小気泡を水とともに吹き出すことを特徴とする。請求項に記載の本発明によれば、微小気泡を気泡吹出手段に水とともに連続的に供給することができ、流場への微小気泡拡散が均一化できる。 The present invention according to claim 5 is characterized in that micro bubbles are mixed in advance with water and supplied to the bubble blowing means, and the fine bubbles are blown out together with water from the bubble blowing means. According to the fifth aspect of the present invention, the microbubbles can be continuously supplied to the bubble blowing means together with water, and the microbubble diffusion into the flow field can be made uniform.

請求項記載の本発明は、気泡吹出手段から対象物の幅方向にも微小気泡を吹き出すことを特徴とする。請求項に記載の本発明によれば、微小気泡を幅方向に拡散させ、より流場の計測範囲を広げ、3次元的な流場の計測も可能とすることができる。 The present invention according to claim 6 is characterized in that microbubbles are also blown out from the bubble blowing means in the width direction of the object. According to the sixth aspect of the present invention, it is possible to diffuse the microbubbles in the width direction, further widen the measurement range of the flow field, and to measure the three-dimensional flow field.

請求項記載の本発明は、対象物と等速で同一方向に動くシート光を、シート光照射手段から対象物の近傍に照射して流場を計測することを特徴とする。請求項に記載の本発明によれば、対象物の周囲を動く微小気泡を捉えて流場の計測を良好に行うことができる。 The present invention according to claim 7 is characterized in that the flow field is measured by irradiating the vicinity of the object from the sheet light irradiation means with the sheet light moving in the same direction as the object at the same speed. According to the present invention described in claim 7 , it is possible to satisfactorily measure the flow field by capturing microbubbles moving around the object.

請求項記載の本発明は、シート光を対象物の動く方向と平行に照射したことを特徴とする。請求項に記載の本発明によれば、対象物と同一方向の微小気泡の動きから対象物の前後方向の流場が計測でき、また前後方向に一定の幅をもって流場の計測を行うことができる。 The present invention according to claim 8 is characterized in that the sheet light is irradiated in parallel with the moving direction of the object. According to the present invention described in claim 8 , the flow field in the front-rear direction of the object can be measured from the movement of the microbubbles in the same direction as the object, and the flow field is measured with a certain width in the front-rear direction. Can do.

請求項記載の本発明に対応した微小気泡を用いた水槽用流場計測装置においては、水槽中の対象物を曳引する曳引手段と、対象物の前方に微小気泡を吹き出す気泡吹出手段と、気泡吹出手段に微小気泡を供給する気泡供給手段と、気泡吹出手段から吹き出されて対象物の周囲を流れる微小気泡の動きに基づいて流場を計測する計測手段と、気泡吹出手段から吹き出す微小気泡を、気泡吹出手段に対し相対的に初速度を有して吹き出し、流場の計測結果を初速度に基づいて補正するための初速度調整手段とを備え、気泡吹出手段と計測手段とを曳引手段に取り付けたことを特徴とする。請求項10に記載の本発明によれば、対象物の前方に設けた対象物と等速で同一方向に動く気泡吹出手段から微小気泡を吹き出すため、対象物の周囲のみにタイミングよく微小気泡を供給でき、対象物の周囲の流場が的確に計測できるとともに気泡吹出手段も小規模なもので済む。また、計測が完了する前に微小気泡が消失してしまうことがないので精度の高い流場の計測結果を得ることができる。また、水槽中に残留することがない微小気泡をトレーサとして使用するので、固体粒子をトレーサとして使用する場合と比べて水槽設備の保守及び精度管理が容易となる。また、気泡吹出手段と計測手段は曳引手段に取り付けるので、気泡吹出手段や計測手段を水槽底面等など、曳引手段とは別に設ける必要が無い。また、微小気泡が初速度を持たないようにする手段が不要となり、また、流場の計測結果を初速度に基づいて補正するので、初速度の影響を取り除いた結果を得ることができる。 In the water tank flow field measuring apparatus using microbubbles corresponding to the present invention according to claim 9, a pulling means for pulling the object in the water tank, and a bubble blowing means for blowing out the microbubbles in front of the object A bubble supplying means for supplying microbubbles to the bubble blowing means, a measuring means for measuring the flow field based on the movement of the microbubbles blown from the bubble blowing means and flowing around the object, and blown out from the bubble blowing means The microbubbles are blown out with an initial velocity relative to the bubble blowing means, and the initial velocity adjusting means for correcting the flow field measurement result based on the initial velocity is provided, the bubble blowing means and the measuring means, Is attached to the pulling means. According to the tenth aspect of the present invention, since the microbubbles are blown out from the bubble blowing means that moves in the same direction at the same speed as the target provided in front of the target, the microbubbles are only timely around the target. The flow field around the object can be accurately measured, and the bubble blowing means can be small. In addition, since the microbubbles are not lost before the measurement is completed, a highly accurate flow field measurement result can be obtained. In addition, since microbubbles that do not remain in the water tank are used as the tracer, maintenance and accuracy control of the water tank facilities are facilitated as compared with the case where solid particles are used as the tracer. Further, since the bubble blowing means and the measuring means are attached to the pulling means, it is not necessary to provide the bubble blowing means and the measuring means separately from the pulling means such as the bottom of the water tank. Further, a means for preventing the microbubbles from having the initial velocity is not necessary, and the flow field measurement result is corrected based on the initial velocity, so that the result of removing the influence of the initial velocity can be obtained.

請求項10記載の本発明は、気泡吹出手段を、水深方向に伸びる管状構成とし、水深方向に複数の気泡吹出孔を有したことを特徴とする。請求項10に記載の本発明によれば、水深方向に存在する対象物に対し簡単な構成で多くの微小気泡を吹き出すことができる。 The present invention according to claim 10 is characterized in that the bubble blowing means has a tubular configuration extending in the water depth direction and has a plurality of bubble blowing holes in the water depth direction. According to the tenth aspect of the present invention, a large number of microbubbles can be blown out with a simple configuration with respect to an object existing in the depth direction.

請求項11記載の本発明は、気泡供給手段から供給される微小気泡の量を調整する気泡量調整手段を備えたことを特徴とする。請求項11に記載の本発明によれば、微小気泡の量を任意に調整することで、計測に最適な流場とすることができる。 The present invention described in claim 11 is characterized by comprising a bubble amount adjusting means for adjusting the amount of fine bubbles supplied from the bubble supplying means. According to the eleventh aspect of the present invention, an optimum flow field for measurement can be obtained by arbitrarily adjusting the amount of microbubbles.

請求項12記載の本発明は、微小気泡の気泡直径が5μmから100μmの範囲となるように気泡供給手段を制御したことを特徴とする。請求項12に記載の本発明によれば、この気泡直径範囲の微小気泡は気泡同士の結合が行われないため上昇速度を抑えることができ、計測が完了する前に対象物の周囲の流場から微小気泡が浮上して消失してしまうことがなく流場の計測が高い精度で行える。 The present invention according to claim 12 is characterized in that the bubble supply means is controlled so that the bubble diameter of the microbubbles is in the range of 5 μm to 100 μm. According to the present invention described in claim 12 , the microbubbles in the bubble diameter range can suppress the rising speed because the bubbles are not coupled to each other, and the flow field around the object before the measurement is completed. Therefore, it is possible to measure the flow field with high accuracy without causing microbubbles to rise and disappear.

請求項13記載の本発明は、気泡供給手段が、微小気泡を水に混ぜて供給することを特徴とする。請求項13に記載の本発明によれば、微小気泡を気泡吹出手段に水とともに連続的に供給することができ、流場への微小気泡の拡散が均一化できる。 The present invention as set forth in claim 13 is characterized in that the bubble supply means supplies fine bubbles mixed with water. According to the present invention as set forth in claim 13 , microbubbles can be continuously supplied to the bubble blowing means together with water, and the diffusion of the microbubbles into the flow field can be made uniform.

請求項14記載の本発明は、気泡吹出手段が、対象物の幅方向にも微小気泡を吹き出すことを特徴とする。請求項14に記載の本発明によれば、微小気泡を幅方向に拡散させ、より流場の計測範囲を広げ、3次元的な流場の計測も可能とすることができる。 The present invention according to claim 14 is characterized in that the bubble blowing means blows out micro bubbles in the width direction of the object. According to the present invention of the fourteenth aspect , it is possible to diffuse the microbubbles in the width direction, further widen the flow field measurement range, and to measure the three-dimensional flow field.

請求項15記載の本発明は、シート光を対象物の近傍に照射するシート光照射手段を、曳引手段に取り付けたことを特徴とする。請求項15に記載の本発明によれば、シート光照射手段を対象物と等速で動かし流場の計測を良好に行うことができる。 The present invention according to claim 15 is characterized in that sheet light irradiation means for irradiating the vicinity of the object with sheet light is attached to the pulling means. According to the present invention of the fifteenth aspect , the sheet light irradiating means can be moved at the same speed as the object and the flow field can be measured satisfactorily.

請求項16記載の本発明は、シート光を対象物の動く方向と平行に照射したことを特徴とする。請求項16に記載の本発明によれば、対象物と同一方向の微小気泡の動きから対象物の前後方向の流場が計測でき、また前後方向に一定の幅をもって流場の計測を行うことができる。 The present invention according to claim 16 is characterized in that the sheet light is irradiated in parallel with the moving direction of the object. According to the present invention described in claim 16, it can measure the longitudinal direction of the flow field of the object from the movement of microbubbles of the object in the same direction and by performing the measurement of the flow field with a constant width in the longitudinal direction Can do.

本発明の微小気泡を用いた流場計測方法によれば、対象物の前方に設けた対象物と等速で同一方向に動く気泡吹出手段から微小気泡を吹き出すため、対象物の周囲のみにタイミングよく微小気泡を供給でき、対象物の周囲の流場が的確に計測できる。また、計測が完了する前に微小気泡が消失してしまうことがないので、精度の高い流場の計測結果を得ることができる。また、計測設備中に残留することがない微小気泡をトレーサとして使用するので、固体粒子をトレーサとして使用する場合と比べて計測設備の保守及び精度管理が容易となる。また、微小気泡が初速度を持たないようにする手段が不要となり、また、流場の計測結果を初速度に基づいて補正するので、初速度の影響を取り除いた結果を得ることができる。 According to the flow field measurement method using microbubbles of the present invention, the microbubbles are blown out from the bubble blowing means that moves in the same direction at the same speed as the target provided in front of the target. Microbubbles can be supplied well, and the flow field around the object can be measured accurately. In addition, since the microbubbles are not lost before the measurement is completed, a highly accurate flow field measurement result can be obtained. In addition, since microbubbles that do not remain in the measurement facility are used as a tracer, the maintenance and accuracy management of the measurement facility is facilitated as compared with the case where solid particles are used as a tracer. Further, a means for preventing the microbubbles from having the initial velocity is not necessary, and the flow field measurement result is corrected based on the initial velocity, so that the result of removing the influence of the initial velocity can be obtained.

また、初速度を水深方向に異ならせ、水深の深いところの初速度を水深の浅いところの初速度よりも遅くした場合には、気泡吹出手段を簡単な構成で実現できる。   Further, when the initial velocity is varied in the water depth direction and the initial velocity at a deep water depth is made slower than the initial velocity at a shallow water depth, the bubble blowing means can be realized with a simple configuration.

また、初速度を調整する初速度調整手段により初速度を制御した場合には、微小気泡の初速度を任意に調整することで、計測に最適な状態で微小気泡を供給することができる。   Further, when the initial speed is controlled by the initial speed adjusting means for adjusting the initial speed, the microbubbles can be supplied in an optimum state for measurement by arbitrarily adjusting the initial speed of the microbubbles.

また、微小気泡の気泡直径を5μmから100μmの範囲とした場合には、微小気泡の気泡同士の結合を防いで上昇速度を抑えることができ、計測が完了する前に対象物の周囲の流場から微小気泡が浮上して消失してしまうことがなく流場の計測が高い精度で行える。   In addition, when the bubble diameter of the microbubbles is in the range of 5 μm to 100 μm, the rising speed can be suppressed by preventing the coupling of the microbubbles, and the flow field around the object before the measurement is completed. Therefore, it is possible to measure the flow field with high accuracy without causing microbubbles to rise and disappear.

また、水に微小気泡を予め混ぜて気泡吹出手段に供給し、気泡吹出手段から微小気泡を水とともに吹き出す場合には、微小気泡を気泡吹出手段に水とともに連続的に供給することができ、流場への微小気泡拡散が均一化できる。   In addition, when microbubbles are premixed in water and supplied to the bubble blowing means, and the microbubbles are blown out together with water from the bubble blowing means, the microbubbles can be continuously supplied to the bubble blowing means together with water. Diffusion of microbubbles into the field can be made uniform.

また、気泡吹出手段から対象物の幅方向にも微小気泡を吹き出す場合には、微小気泡を幅方向に拡散させ、より流場の計測範囲を広げ、3次元的な流場の計測も可能とすることができる。   In addition, when blowing out microbubbles from the bubble blowing means in the width direction of the object, it is possible to diffuse the microbubbles in the width direction to further expand the flow field measurement range and to measure three-dimensional flow fields. can do.

また、対象物と等速で同一方向に動くシート光を、シート光照射手段から対象物の近傍に照射して流場を計測する場合には、対象物の周囲を動く微小気泡を捉えて流場の計測を良好に行うことができる。   In addition, when measuring the flow field by irradiating a sheet light moving in the same direction at the same speed as the object from the sheet light irradiating means in the vicinity of the object, the microbubbles moving around the object are captured and flown. The field can be measured well.

また、シート光を対象物の動く方向と平行に照射した場合には、対象物と同一方向の微小気泡の動きから対象物の前後方向の流場が計測でき、また前後方向に一定の幅をもって流場の計測を行うことができる。   In addition, when the sheet light is irradiated in parallel with the moving direction of the object, the flow field in the front-rear direction of the object can be measured from the movement of the microbubbles in the same direction as the object, and with a certain width in the front-rear direction. The flow field can be measured.

また、本発明の微小気泡を用いた水槽用流場計測装置によれば、対象物の前方に設けた対象物と等速で同一方向に動く気泡吹出手段から微小気泡を吹き出すため、対象物の周囲のみにタイミングよく微小気泡を供給でき、対象物の周囲の流場が的確に計測できるとともに気泡吹出手段も小規模なもので済む。また、計測が完了する前に微小気泡が消失してしまうことがないので精度の高い流場の計測結果を得ることができる。また、水槽中に残留することがない微小気泡をトレーサとして使用するので、固体粒子をトレーサとして使用する場合と比べて水槽設備の保守及び精度管理が容易となる。また、気泡吹出手段と計測手段は曳引手段に取り付けるので、気泡吹出手段や計測手段を水槽底面等など、曳引手段とは別に設ける必要が無い。また、微小気泡が初速度を持たないようにする手段が不要となり、また、流場の計測結果を初速度に基づいて補正するので、初速度の影響を取り除いた結果を得ることができる。 Further, according to the flow field measuring apparatus for aquarium using the microbubbles of the present invention, since the microbubbles are blown out from the bubble blowing means moving in the same direction as the target provided in front of the target, Microbubbles can be supplied to only the surroundings in a timely manner, the flow field around the object can be accurately measured, and the bubble blowing means can be small. In addition, since the microbubbles are not lost before the measurement is completed, a highly accurate flow field measurement result can be obtained. In addition, since microbubbles that do not remain in the water tank are used as the tracer, maintenance and accuracy control of the water tank facilities are facilitated as compared with the case where solid particles are used as the tracer. Further, since the bubble blowing means and the measuring means are attached to the pulling means, it is not necessary to provide the bubble blowing means and the measuring means separately from the pulling means such as the bottom of the water tank. Further, a means for preventing the microbubbles from having the initial velocity is not necessary, and the flow field measurement result is corrected based on the initial velocity, so that the result of removing the influence of the initial velocity can be obtained.

また、気泡吹出手段を、水深方向に伸びる管状構成とし、水深方向に複数の気泡吹出孔を有した場合には、水深方向に存在する対象物に対し簡単な構成で多くの微小気泡を吹き出すことができる。   In addition, when the bubble blowing means has a tubular configuration extending in the water depth direction and has a plurality of bubble blowing holes in the water depth direction, a large number of micro bubbles are blown out with a simple configuration with respect to an object existing in the water depth direction. Can do.

また、気泡供給手段から供給される微小気泡の量を調整する気泡量調整手段を備えた場合には、微小気泡の量を任意に調整することで、計測に最適な流場とすることができる。   In addition, when a bubble amount adjusting unit that adjusts the amount of microbubbles supplied from the bubble supply unit is provided, an optimum flow field for measurement can be obtained by arbitrarily adjusting the amount of microbubbles. .

また、微小気泡の気泡直径が5μmから100μmの範囲となるように気泡供給手段を制御した場合には、微小気泡の気泡同士の結合を防いで微小気泡の上昇速度を抑えることができ、計測が完了する前に対象物の周囲の流場から微小気泡が浮上して消失してしまうことがなく流場の計測が高い精度で行える。   In addition, when the bubble supply means is controlled so that the bubble diameter of the microbubbles is in the range of 5 μm to 100 μm, it is possible to prevent the microbubbles from rising and to suppress the rising speed of the microbubbles. The flow field can be measured with high accuracy without causing microbubbles to rise and disappear from the flow field around the object before completion.

また、気泡供給手段が、微小気泡を水に混ぜて供給する場合には、微小気泡を水とともに気泡吹出手段に連続的に供給することができ、流場への微小気泡拡散が均一化できる。   Further, when the bubble supply means supplies the microbubbles mixed with water, the microbubbles can be continuously supplied together with the water to the bubble blowing means, and the microbubble diffusion into the flow field can be made uniform.

また、気泡吹出手段が、対象物の幅方向にも微小気泡を吹き出す場合には、微小気泡を幅方向に拡散させ、より流場の計測範囲を広げ、3次元的な流場の計測も可能とすることができる。   In addition, when the bubble blowing means blows out microbubbles in the width direction of the object, the microbubbles are diffused in the width direction, and the flow field measurement range can be expanded to measure three-dimensional flow fields. It can be.

また、シート光を対象物の近傍に照射するシート光照射手段を、曳引手段に取り付けた場合には、シート光照射手段を対象物と等速で動かし流場の計測を良好に行うことができる。   In addition, when the sheet light irradiating means for irradiating the vicinity of the object with the sheet light is attached to the pulling means, the sheet light irradiating means can be moved at the same speed as the object and the flow field can be measured well. it can.

また、シート光を対象物の動く方向と平行に照射した場合には、対象物と同一方向の微小気泡の動きから対象物の前後方向の流場が計測でき、また前後方向に一定の幅をもって流場の計測を行うことができる。   In addition, when the sheet light is irradiated in parallel with the moving direction of the object, the flow field in the front-rear direction of the object can be measured from the movement of the microbubbles in the same direction as the object, and with a certain width in the front-rear direction. The flow field can be measured.

本発明の一実施形態による微小気泡を用いた水槽用流場計測装置の全体構成を示す構成図The block diagram which shows the whole structure of the flow field measuring apparatus for water tanks using the microbubble by one Embodiment of this invention 同装置の計測手段を示す構成図Configuration diagram showing the measuring means of the device 同装置で生成した気泡直径の分布図Distribution diagram of bubble diameter generated by the same device 同装置の気泡吹出手段を示す構成図Configuration diagram showing bubble blowing means of the apparatus 同装置による一様流中の流場計測の撮影画像を示す図The figure which shows the photographed image of the flow field measurement in the uniform flow with the same device 同装置による一様流中の流場計測の解析結果を示す図The figure which shows the analysis result of the flow field measurement in the uniform flow by the same device 同装置による一様流中の流場計測の主流方向の速度の乱れ度を示す図The figure which shows the turbulence degree of the velocity of the main flow direction of the flow field measurement in the uniform flow by the same device 同装置による一様流中の流場計測のPIVで計測した主流方向の平均速度(E(Vx))とピトー管で計測した主流方向の平均速度(E(Vxp))の相関を示す図The figure which shows the correlation of the average velocity (E (Vx)) of the main flow direction measured with PIV of the flow field measurement in the uniform flow by the same apparatus, and the average velocity (E (Vxp)) of the main flow direction measured with the Pitot tube. 同装置による規則波中の流場計測の撮影画像を示す図The figure which shows the photographed image of the flow field measurement in the regular wave with the same device 同装置による規則波中の流場計測の解析結果を示す図The figure which shows the analysis result of the flow field measurement in the regular wave by the same device 同装置による規則波中の流場計測のz=−0.187mでの主流方向の速度Vxと上下方向の速度Vzを時系列で示す図The figure which shows the velocity Vx of the main flow direction in z = -0.187m of the flow field measurement in the regular wave by the same apparatus, and the speed Vz of an up-down direction in time series. 同装置による規則波中の流場計測のz=−0.224mでの主流方向の速度Vxと上下方向の速度Vzを時系列で示す図The figure which shows the velocity Vx of the main flow direction in z = -0.224m of the flow field measurement in the regular wave by the same apparatus, and the speed Vz of an up-down direction in time series. 同装置による規則波中の流場計測のz=−0.261mでの主流方向の速度Vxと上下方向の速度Vzを時系列で示す図The figure which shows the velocity Vx of the main flow direction in z = -0.261m of the flow field measurement in the regular wave by the same apparatus, and the speed Vz of an up-down direction in time series.

以下に、本発明の実施形態による微小気泡を用いた水槽用流場計測装置について説明する。   Below, the flow field measuring device for water tanks using the microbubble by embodiment of the present invention is explained.

図1は本発明の一実施形態による微小気泡を用いた水槽用流場計測装置の全体構成を示す構成図、図2は同装置の計測手段を示す構成図である。
本実施形態による微小気泡を用いた水槽用流場計測装置は、水槽10中の対象物(模型船)20を曳引する曳引手段30を有し、曳引手段30には、気泡吹出手段40と計測手段50とを取り付けている。
従って、模型船20と気泡吹出手段40と計測手段50とは、曳引手段30によって等速で同一方向に水槽10中で動かされる。
気泡吹出手段40は、水中で模型船20の前方に微小気泡を吹き出す。気泡吹出手段40には、気泡供給手段60から微小気泡を供給する。
計測手段50は、気泡吹出手段40から吹き出されて模型船20の周囲を流れる微小気泡の動きに基づいて流場を計測する。
FIG. 1 is a block diagram showing the overall configuration of a water tank flow field measuring apparatus using microbubbles according to an embodiment of the present invention, and FIG. 2 is a block diagram showing the measuring means of the apparatus.
The water tank flow field measuring device using microbubbles according to the present embodiment has a towing means 30 for towing an object (model ship) 20 in the aquarium 10, and the towing means 30 includes a bubble blowing means. 40 and measuring means 50 are attached.
Accordingly, the model ship 20, the bubble blowing means 40, and the measuring means 50 are moved in the water tank 10 in the same direction at a constant speed by the towing means 30.
The bubble blowing means 40 blows out micro bubbles in front of the model ship 20 in water. Microbubbles are supplied to the bubble blowing means 40 from the bubble supply means 60.
The measuring means 50 measures the flow field based on the movement of the fine bubbles that are blown out from the bubble blowing means 40 and flow around the model ship 20.

気泡吹出手段40は、水槽10内で水深方向に伸びる管状の管部材41で構成され、管部材41には、水深方向に複数の気泡吹出孔42を有している。水深方向に複数の気泡吹出孔42を有することで、水深方向に存在する模型船20の船体に対し簡単な構成で多くの微小気泡を吹き出すことができる。
気泡吹出手段40は、模型船20の幅方向にも微小気泡を吹き出す。複数の管部材41を模型船20の幅方向に配置することで、模型船20の幅方向に微小気泡を吹き出すことができる。幅方向に吹き出すことで、計測を安定的に行うことを実現するとともに、目的によっては3次元的な計測も可能となる。
また、単一の管部材41で、気泡吹出孔42の吹き出し方向をそれぞれ異ならせて幅方向に微小気泡を吹き出してもよい。また、管部材41を平面視した状態で、気泡吹出孔42の吹き出し方向を横方向、前方向等任意の方向に設定することも可能である。
気泡吹出手段40が、模型船20の幅方向にも微小気泡を吹き出すことで、微小気泡を拡散させ、より流場の計測範囲を広げることができる。
気泡吹出手段40から吹き出す、すなわち気泡吹出孔42から吹き出す微小気泡は、気泡吹出手段40に対し相対的に初速度を有して吹き出される。気泡吹出孔42から吹き出す微小気泡は、水深の深いところの初速度が水深の浅いところの初速度よりも遅く、初速度を水深方向に異ならせている。このため、気泡吹出孔42からの吹き出し初速度を揃えるための複雑な機構や構造を必要とすることなく、管部材41を簡単な構成とすることができる。
The bubble blowing means 40 includes a tubular tube member 41 extending in the water depth direction in the water tank 10, and the tube member 41 has a plurality of bubble blowing holes 42 in the water depth direction. By having the plurality of bubble blowing holes 42 in the water depth direction, many micro bubbles can be blown out with a simple configuration with respect to the hull of the model ship 20 existing in the water depth direction.
The bubble blowing means 40 also blows out micro bubbles in the width direction of the model ship 20. By arranging the plurality of pipe members 41 in the width direction of the model ship 20, microbubbles can be blown out in the width direction of the model ship 20. By blowing out in the width direction, it is possible to stably perform measurement and, depending on the purpose, three-dimensional measurement is also possible.
Further, the single tube member 41 may blow out microbubbles in the width direction by changing the blowing direction of the bubble blowing holes 42 respectively. Moreover, it is also possible to set the blowing direction of the bubble blowing holes 42 in an arbitrary direction such as a horizontal direction and a forward direction in a state where the tube member 41 is viewed in plan.
The bubble blowing means 40 blows out microbubbles also in the width direction of the model ship 20, so that the microbubbles can be diffused and the flow field measurement range can be further expanded.
The microbubbles blown out from the bubble blowing means 40, that is, blown out from the bubble blowing holes 42, are blown out with an initial velocity relative to the bubble blowing means 40. The micro bubbles blown out from the bubble blowing holes 42 have an initial velocity at a deep water depth lower than an initial velocity at a shallow water depth, and the initial velocity is varied in the depth direction. For this reason, the pipe member 41 can have a simple configuration without requiring a complicated mechanism or structure for aligning the initial blow-out speed from the bubble blowing hole 42.

本実施形態による微小気泡を用いた水槽用流場計測装置は、初速度を調整する初速度調整手段71と、微小気泡の量を調整する気泡量調整手段72とを備えている。
初速度調整手段71は、気泡吹出孔42から吹き出す微小気泡の初速度を制御する。気泡量調整手段72は、気泡供給手段60から供給される微小気泡の量を調整する。
本実施形態では、気泡供給手段60と気泡吹出手段40とを接続する供給配管81の流路を絞る第1制御弁を初速度調整手段71としている。初速度調整手段71である第1制御弁を絞ることで、初速度を遅くすることができる。
The water tank flow field measuring apparatus using microbubbles according to the present embodiment includes an initial speed adjusting means 71 for adjusting the initial speed and a bubble amount adjusting means 72 for adjusting the amount of microbubbles.
The initial speed adjusting means 71 controls the initial speed of the micro bubbles blown out from the bubble blowing hole 42. The bubble amount adjusting unit 72 adjusts the amount of micro bubbles supplied from the bubble supplying unit 60.
In the present embodiment, the first speed adjustment means 71 is the first control valve that restricts the flow path of the supply pipe 81 that connects the bubble supply means 60 and the bubble blowing means 40. By narrowing the first control valve that is the initial speed adjusting means 71, the initial speed can be slowed down.

また、本実施形態では、管部材41の下端側に設けた第2制御弁を気泡量調整手段72としている。気泡量調整手段72である第2制御弁より下部には気泡逃がし部43を有し、第2制御弁を開くことで気泡逃がし部43からの気泡放出量が増加し、気泡吹出孔42から吹き出す微小気泡の量が減少する。
なお、第1制御弁によっても微小気泡の量を調整でき、第2制御弁によっても初速度を制御できる。また、微小気泡の量は、気泡供給手段60で制御することもできる
In the present embodiment, the second control valve provided on the lower end side of the pipe member 41 is used as the bubble amount adjusting means 72. A bubble escape portion 43 is provided below the second control valve, which is the bubble amount adjusting means 72. By opening the second control valve, the amount of bubble discharge from the bubble escape portion 43 is increased and blown out from the bubble blowing hole 42. The amount of microbubbles is reduced.
Note that the amount of microbubbles can also be adjusted by the first control valve, and the initial speed can be controlled by the second control valve. The amount of microbubbles can also be controlled by the bubble supply means 60.

微小気泡の初速度や量を任意に調整することで、計測に最適な流場とすることができる。
気泡吹出孔42から吹き出す微小気泡は、気泡直径を5μmから100μmの範囲、好ましくは20μmから60μmの範囲、更に好ましくは30μから40μmの範囲とする。このような気泡直径とすることで、微小気泡同士が結合することを抑制し、あるいは防止し、微小気泡の上昇速度を抑えることができ、計測が完了する前に模型船20の周囲の流場から微小気泡が浮上して消失してしまうことがない。
気泡供給手段60は、大気から空気を吸い込み、水槽10から水を吸い込む。吸い込み管82は模型船20の周囲の流場を乱さないように模型船20の後方に距離を置いて設けられており、水槽10から吸い込んだ水を気泡供給手段60に送る。気泡供給手段60では、大気から吸い込んだ空気を微小化し、微小気泡を水に混ぜて供給する。微小気泡を水に混ぜて供給し、気泡吹出手段40から微小気泡を水とともに吹き出すことで、微小気泡を気泡吹出手段40に連続的に供給することができ、流場への微小気泡の拡散を均一化できる。なお、気泡供給手段60では、気泡を水と混ぜて供給し、気泡吹出手段40で気泡を微小化して微小気泡として吹き出すこともできる。また、空気を貯えるタンクを装備して圧力のかかった空気を供給し、気泡吹出手段40で微小気泡として噴出させることも可能である。
By adjusting the initial velocity and amount of microbubbles arbitrarily, it is possible to obtain an optimum flow field for measurement.
The micro bubbles blown out from the bubble blowing holes 42 have a bubble diameter in the range of 5 μm to 100 μm, preferably in the range of 20 μm to 60 μm, more preferably in the range of 30 μm to 40 μm. By setting such a bubble diameter, it is possible to suppress or prevent the bonding of the microbubbles, and to suppress the rising speed of the microbubbles, and the flow field around the model ship 20 before the measurement is completed. Therefore, microbubbles will not rise and disappear.
The bubble supply means 60 sucks air from the atmosphere and sucks water from the water tank 10. The suction pipe 82 is provided at a distance behind the model ship 20 so as not to disturb the flow field around the model ship 20, and sends the water sucked from the water tank 10 to the bubble supply means 60. In the bubble supply means 60, the air sucked from the atmosphere is micronized, and microbubbles are mixed with water and supplied. By supplying microbubbles mixed with water and blowing the microbubbles together with water from the bubble blowing means 40, the microbubbles can be continuously supplied to the bubble blowing means 40, and the microbubbles can be diffused into the flow field. It can be made uniform. In the bubble supply means 60, the bubbles can be mixed with water and supplied, and the bubbles can be made fine by the bubble blowing means 40 and blown out as fine bubbles. It is also possible to equip a tank for storing air, supply air under pressure, and eject the fine bubbles by the bubble blowing means 40.

図2に示すように、計測手段50は、曳引手段30に取り付けられ、シート光を照射するシート光照射手段51と、照射された微小気泡を撮像する撮像手段52とで構成される。シート光照射手段51及び撮像手段52を、曳引手段30に取り付けたことで、模型船20と等速で同一方向に動くシート光を、シート光照射手段51から模型船20の近傍に照射して計測するので、流場の計測を良好に行うことができる。
シート光照射手段51は、シート光を模型船20の近傍に照射する。シート光を模型船20の動く方向と平行に照射することで、模型船20と同一方向に動く微小気泡の動きから模型船20の前後方向の流場が計測でき、また前後方向に一定の幅をもって流場の計測を行うことができる。
本実施形態によるシート光照射手段51は、ミラー53を用いて水中から模型船20の近傍に照射する。シート光照射手段51は、計測手段50の一部として曳引手段30により曳引され模型船20とともに水中を動くので、簡単な手段として実現できる。
なお、光ファイバやシート光照射手段51を防水型として水中から模型船20の近傍を照射しても良い。
As shown in FIG. 2, the measuring unit 50 is attached to the pulling unit 30 and includes a sheet light irradiating unit 51 that irradiates the sheet light and an imaging unit 52 that images the irradiated microbubbles. By attaching the sheet light irradiation means 51 and the imaging means 52 to the towing means 30, the sheet light moving in the same direction as the model ship 20 is irradiated from the sheet light irradiation means 51 to the vicinity of the model ship 20. Therefore, the flow field can be measured satisfactorily.
The sheet light irradiation means 51 irradiates the vicinity of the model ship 20 with sheet light. By irradiating the sheet light in parallel with the moving direction of the model ship 20, the flow field in the front-rear direction of the model ship 20 can be measured from the movement of the microbubbles moving in the same direction as the model ship 20, and a constant width in the front-rear direction. Can be used to measure the flow field.
The sheet light irradiation means 51 according to the present embodiment irradiates the vicinity of the model ship 20 from underwater using the mirror 53. Since the sheet light irradiation means 51 is pulled by the pulling means 30 as part of the measuring means 50 and moves underwater with the model ship 20, it can be realized as a simple means.
In addition, you may irradiate the vicinity of the model ship 20 from underwater by making optical fiber and the sheet light irradiation means 51 into a waterproof type.

本実施形態による微小気泡を用いた流場計測方法は、気泡吹出手段40から吹き出す微小気泡を、気泡吹出手段40に対し相対的に初速度を有して吹き出すとともに、流場の計測結果を初速度に基づいて補正する。流場の計測結果を初速度に基づいて補正することで、初速度の影響を取り除いた結果を得ることができる。
V0を真の速度、VPIVをPIV(Particle Image Velocimetry)で解析される速度、ΔVwを気泡吹出手段40による流速の変化、Vsを初速度、ΔVerrを計測誤差とすると、真の速度V0は次式で表される。
V0=VPIV−ΔVw−Vs−ΔVerr
The flow field measurement method using microbubbles according to the present embodiment blows out microbubbles blown out from the bubble blowing means 40 with an initial velocity relative to the bubble blowing means 40 and the flow field measurement results for the first time. Correct based on speed. By correcting the measurement result of the flow field based on the initial velocity, a result obtained by removing the influence of the initial velocity can be obtained.
When V0 is a true velocity, VPIV is a velocity analyzed by PIV (Particle Image Velocity), ΔVw is a change in flow velocity by the bubble blowing means 40, Vs is an initial velocity, and ΔVerr is a measurement error, the true velocity V0 is expressed by the following equation: It is represented by
V0 = VPIV−ΔVw−Vs−ΔVerr

ΔVwは、ピトー管などの別の計測装置を用い、気泡吹出手段40がない状態と気泡吹出手段40がある状態で比較し、次式により求める。
ΔVw=Vw−Vw0
ここで、Vwは気泡吹出手段40あり、Vw0は気泡吹出手段40なしの状態での速度である。
Vsは、平水中ではピトー管などの別の計測装置を用いて計測し、波浪中では、止まった状態で造波を行い、流速変化の時系列データから平均値を求める。
流場の計測結果を初速度に基づいて補正することにより、微小気泡が初速度を持たないようにする手段が不要となり、水深方向に伸びる管部材41のような簡単な構成で計測が可能となる。
ΔVw is obtained by the following equation using another measuring device such as a Pitot tube, comparing the state without the bubble blowing means 40 and the state with the bubble blowing means 40.
ΔVw = Vw−Vw0
Here, Vw is the speed of the bubble blowing means 40, and Vw0 is the speed without the bubble blowing means 40.
Vs is measured by using another measuring device such as a Pitot tube in plain water, and in waves, wave making is performed in a stopped state, and an average value is obtained from time-series data of flow velocity changes.
By correcting the measurement result of the flow field based on the initial velocity, means for preventing the microbubbles from having the initial velocity becomes unnecessary, and measurement can be performed with a simple configuration such as the tube member 41 extending in the water depth direction. Become.

以下に本発明による微小気泡を用いた流場計測方法の実験結果を示す。
同流場計測方法では、図1及び図2に示す装置を用い、レーザシート光の前方の気泡吹出孔42から微小気泡を吹き出し、その後方にあるレーザシート光により微小気泡を照明し、微小気泡の動きを2台の撮像手段(高速度カメラ)52により連続的にステレオ撮影した。
The experimental results of the flow field measurement method using microbubbles according to the present invention are shown below.
In the same flow field measurement method, the apparatus shown in FIGS. 1 and 2 is used to blow out microbubbles from the bubble blowing holes 42 in front of the laser sheet light, and the microbubbles are illuminated by the laser sheet light behind the microbubbles. The two movements were continuously photographed in stereo by two imaging means (high speed cameras) 52.

本実験では、気泡供給手段(気泡発生装置)60として気液剪断方式とキャビテーション方式を組み合わせたものを用いた。
トレーサとして用いる気泡の基本的な性状を調べるため、気泡発生装置60で生成した気泡直径を計測し、気泡の上昇速度を検討した。気泡直径の計測は、微小気泡を混入した透明な容器にレーザシート光を照射し、マイクロスコープにより計測した。なお、マイクロスコープの解像度は720×480pixであり、撮影範囲は6.5×4.3mm、1pixあたり9.1μmである。
In this experiment, a combination of a gas-liquid shearing method and a cavitation method was used as the bubble supplying means (bubble generating device) 60.
In order to investigate the basic properties of bubbles used as a tracer, the bubble diameter generated by the bubble generator 60 was measured, and the bubble rising speed was examined. The bubble diameter was measured by irradiating a transparent container mixed with microbubbles with laser sheet light and using a microscope. The resolution of the microscope is 720 × 480 pixels, and the imaging range is 6.5 × 4.3 mm, and 9.1 μm per pixel.

撮影画像から気泡のピクセル数を計測し、気泡直径分布を求めた結果を図3に示す。
図3から気泡発生装置60で発生した気泡直径は10〜60μm(平均31μm)の範囲であることがわかる。微小気泡の上昇速度(Vr)は、次式のStokesの法則に従い、気泡直径の2乗に比例する。
Vr=gd/18ν
ここで、gは重力加速度、dは気泡直径、νは水の動粘性係数である。
水の動粘性係数は温度により変化する。実験時の水温(15℃)において平均気泡直径での上昇速度は0.47mm/sと求められる。
FIG. 3 shows the results obtained by measuring the number of pixels of bubbles from the photographed image and obtaining the bubble diameter distribution.
It can be seen from FIG. 3 that the bubble diameter generated by the bubble generator 60 is in the range of 10 to 60 μm (average 31 μm). The rising speed (Vr) of the microbubbles is proportional to the square of the bubble diameter according to the following Stokes' law.
Vr = gd 2 / 18ν
Here, g is the acceleration of gravity, d is the bubble diameter, and ν is the kinematic viscosity coefficient of water.
The kinematic viscosity coefficient of water varies with temperature. The rising speed at the average bubble diameter at the water temperature (15 ° C.) during the experiment is determined to be 0.47 mm / s.

また、今回はこの微小気泡をトレーサとして吹き出す際、図4に示すように、管部材(塩化ビニールパイプ)41に複数の気泡吹出孔42を空けた気泡吹出手段40を使用した。最終的には船尾での流場を計測することを目的としているため、気泡吹出手段40を2本使用し、広い範囲に拡散させるようにしている。そして、整流するためにパイプ41を翼型に成形している。   Further, this time, when blowing out these micro bubbles as a tracer, as shown in FIG. 4, a bubble blowing means 40 having a plurality of bubble blowing holes 42 formed in a pipe member (vinyl chloride pipe) 41 was used. Since the final purpose is to measure the flow field at the stern, two bubble blowing means 40 are used and diffused over a wide range. The pipe 41 is formed into an airfoil for rectification.

気泡発生装置60には、図2に示す計測手段(PIVシステム)50を用いた。
PIVシステム50に使用した高速度カメラ52は、VGAサイズ(640×480pix)の画像を毎秒200フレームで撮影することができ、最低被写体照度は10lux(F値1.4時)である。レンズには焦点距離12mm、F値1.2のものを使用した。高速度カメラ52の撮影範囲は250mm×190mm程度であり、1pixあたりおよそ0.4mmである。
レーザ光学系の光源には、出力4Wのグリーン光(532nm)の連続発振レーザを用いた。レーザ光源を2つのミラー53を介して水中まで導き、レーザ光源をシリンドリカルレンズ54により扇形に拡散させてシート状に成形し、最後にミラー55を介して鉛直上方にレーザシート光を照射する。水槽用流場計測装置は模型船20での計測を考え、船幅方向に移動させるためのトラバース装置90を有する。これにより計測する断面を変更し、三次元的な計測をすることが可能である。
なお、検査領域は、64×64pix、オーバーラップ50%にてFFT相互相関法により解析した。
As the bubble generating device 60, the measuring means (PIV system) 50 shown in FIG. 2 was used.
The high-speed camera 52 used in the PIV system 50 can capture a VGA size (640 × 480 pix) image at 200 frames per second, and the minimum subject illuminance is 10 lux (F value: 1.4). A lens having a focal length of 12 mm and an F value of 1.2 was used. The shooting range of the high-speed camera 52 is about 250 mm × 190 mm, and is about 0.4 mm per pix.
As the light source of the laser optical system, a continuous wave laser of green light (532 nm) with an output of 4 W was used. The laser light source is guided to the water through the two mirrors 53, the laser light source is diffused into a sheet shape by the cylindrical lens 54 and formed into a sheet shape, and finally the laser sheet light is irradiated vertically upward through the mirror 55. The water tank flow field measuring device has a traverse device 90 for moving in the width direction of the ship in consideration of measurement with the model ship 20. As a result, the cross section to be measured can be changed to perform three-dimensional measurement.
The inspection region was analyzed by the FFT cross-correlation method with 64 × 64 pix and 50% overlap.

微小気泡をトレーサとしたPIV計測の精度検証のため、海上技術安全研究所の動揺試験水槽(長さ=50m、幅=8m、深さ=4.5m)で一様流及び規則波の流場計測を行った。一様流の計測時には水槽10のセンターラインに設置した。以下で使用する座標系はx軸を主流方向、y軸を計測画面の遠方から近方、z軸を鉛直上方とする右手系である。
この装置の精度検証のため、本研究では一様流中の流場計測を行った。曳航速度(V)は0.4m/s、0.6m/s、0.8m/sの3種類とし、それぞれ5回ずつ計測を行った。2本の塩化ビニールパイプ41からなる気泡吹出手段40の後方にPIVシステム50の計測断面、ピトー管を設置して同時に計測し、両者の計測値を比較した。
図5及び図6にV=0.4m/sでの撮影画像と解析結果の一例を示す。
In order to verify the accuracy of PIV measurement using microbubbles as a tracer, the flow field of uniform and regular waves in the shaking test water tank (length = 50m, width = 8m, depth = 4.5m) of the National Maritime Research Institute Measurement was performed. It was installed in the center line of the water tank 10 when measuring the uniform flow. The coordinate system used below is a right-handed system in which the x-axis is the mainstream direction, the y-axis is from the far side to the near side of the measurement screen, and the z-axis is vertically upward.
In order to verify the accuracy of this device, we measured the flow field in a uniform flow in this study. The towing speed (V) was set to three types of 0.4 m / s, 0.6 m / s, and 0.8 m / s, and measurement was performed 5 times each. The measurement cross section of the PIV system 50 and the Pitot tube were installed behind the bubble blowing means 40 composed of two vinyl chloride pipes 41 and measured simultaneously, and the measured values were compared.
5 and 6 show an example of a captured image and an analysis result at V = 0.4 m / s.

主流方向の速度の乱れ度(Ivx)を次式で定義する。V=0.4m/sの場合を例として図7に示す。
Ivx=σvx/E(Vx)
ここで、E(Vx)は、PIVシステム50で計測した主流方向の速度の平均値、σvxは、PIVシステム50で計測した主流方向の速度の標準偏差である。
計測範囲の大部分で3%以内の乱れ度であることがわかる。
また、乱れ度の小さい範囲の中心が計測範囲の中心よりずれているのは、左右の高速度カメラ52の角度のズレによって撮影画像の中心が左右で違うためである。計測範囲の外側に向かうにつれて乱れ度が大きくなるのは、レンズの収差によるものと考えられる。
The velocity disturbance (Ivx) in the mainstream direction is defined by the following equation. An example of V = 0.4 m / s is shown in FIG.
Ivx = σvx / E (Vx)
Here, E (Vx) is an average value of the velocity in the mainstream direction measured by the PIV system 50, and σvx is a standard deviation of the velocity in the mainstream direction measured by the PIV system 50.
It can be seen that the degree of disturbance is within 3% in most of the measurement range.
Also, the reason why the center of the range with a small degree of disturbance is shifted from the center of the measurement range is that the center of the captured image differs between the left and right due to the angle shift of the left and right high speed cameras 52. It is considered that the degree of disturbance increases toward the outside of the measurement range due to lens aberration.

PIVシステム50で計測した画像中心部の主流方向の平均速度(E(Vx))とピトー管で計測した主流方向の平均速度(E(Vxp))の相関を図8に示す。
両者の相関係数は0.99以上であり、高い相関を持つことを確認した。
FIG. 8 shows the correlation between the average velocity (E (Vx)) in the mainstream direction measured by the PIV system 50 and the average velocity (E (Vxp)) in the mainstream direction measured by the Pitot tube.
The correlation coefficient of both was 0.99 or more, and it was confirmed that there was a high correlation.

一様流中の流場計測による検証に続いて、規則波中の流場計測を行った。実験状態は波高Hw=0.050m、波周期T=1s、2sとして試験速度V=0m/sの停止状態で行った。
図9にT=2sでの撮影画像の一例を示す。
Following verification by flow field measurement in uniform flow, flow field measurement in regular waves was performed. The experiment was performed in a stopped state where the wave velocity Hw = 0.050 m, the wave period T = 1 s, and 2 s and the test speed V = 0 m / s.
FIG. 9 shows an example of a captured image at T = 2s.

図10にT=2sにおけるPIV解析結果の速度ベクトルを示す。なお、時間t=0〜1.5sまでの速度ベクトルである。波浪中水粒子速度を捉えているため、速度ベクトルの方向が時間的に変化していることがわかる。   FIG. 10 shows the velocity vector of the PIV analysis result at T = 2s. It is a speed vector from time t = 0 to 1.5 s. It can be seen that the direction of the velocity vector changes with time because the water particle velocity in the waves is captured.

図11、図12、図13に、それぞれz=−0.187m、−0.224m、−0.261mでの主流方向の速度Vx、上下方向の速度Vzの時系列データを示す。
図中の実線が微小振幅波理論により求められた計算値であり、点は計測値である。
z=−0.224m、−0.261mではVx、Vz共に理論値と計測値がほぼ一致していることがわかる。なお、z=−0.187mではVzについてはほぼ一致しているが、Vxについては全体的に増速側にシフトしている。これは微小気泡を水槽10中に吹き出すときの速度によるものと考えられる。水深が浅くなるにつれてVxの一致が悪くなるのは水面に近い部分において微小気泡を吹き出す速度が速く、水面から遠くなるにつれて速度が遅くなるためと考えられる。
11, 12, and 13 show time-series data of the velocity Vx in the mainstream direction and the velocity Vz in the vertical direction at z = −0.187 m, −0.224 m, and −0.261 m, respectively.
The solid line in the figure is the calculated value obtained by the micro amplitude wave theory, and the point is the measured value.
It can be seen that at z = −0.224 m and −0.261 m, the theoretical value and the measured value are almost the same for both Vx and Vz. Note that when z = −0.187 m, Vz is almost the same, but Vx is shifted to the speed increasing side as a whole. This is thought to be due to the speed at which the microbubbles are blown into the water tank 10. The reason why the Vx coincides worse as the water depth becomes shallower is that the speed at which the microbubbles are blown out in the portion close to the water surface is high, and the speed decreases as the distance from the water surface increases.

本試験結果より、一様流の計測では、ピトー管の計測値と比較して高い相関関係があることが確認され、規則波中の流場計測では微小振幅波理論により求めた理論値と比較した結果、高い一致性を示した。   From this test result, it was confirmed that the uniform flow measurement had a higher correlation than the measured value of the Pitot tube, and the flow field measurement in the regular wave was compared with the theoretical value obtained by the micro amplitude wave theory. As a result, high consistency was shown.

以上のように本実施形態による微小気泡を用いた流場計測方法においては、対象物(模型船)20の前方に微小気泡を吹き出す気泡吹出手段40を設け、気泡吹出手段40を模型船20と等速で同一方向に動かし、気泡吹出手段40から吹き出されて模型船20の周囲を流れる微小気泡の動きに基づいて流場を計測することで、模型船20の周囲のみにタイミングよく微小気泡を供給でき、対象物の周囲の流場が的確に計測できる。
また、計測が完了する前に微小気泡が浮上して消失してしまうことがない。また、水槽10中に残留することがない微小気泡をトレーサとして使用するので、固体粒子をトレーサとして使用する場合と比べて水槽設備の保守及び精度管理が容易となる。
特に、曳引手段30により曳引されて水中を動く模型船20とともに、同じく曳引手段30に取り付けた気泡吹出手段40と計測手段50が等速で動くため、模型船20の周囲の流場だけに微小気泡を供給し、また模型船20の周囲のみに焦点を当てて計測を行い精度の高い計測結果を得ることができる。
このため、水槽10全体に気泡を連続拡散させたり、模型船20が近づいたら領域ごとに気泡を吹き出す固定的な方式と比較し、気泡吹出手段40を小規模で簡単な構成とすることができる。また、模型船20の周囲の計測をしたい流場だけを対象に微小気泡を供給できるため、微小気泡の量は非常に少なくて済み、更に気泡吹出手段40を小規模で簡単な構成とすることができる。模型船20を直進させるだけでなく、蛇行やジグザグ運転等の平面的な運動を伴う試験を行う場合、気泡吹出手段40が模型船20と同一方向に動くため、この効果は顕著となる。
また、水槽10全体にシート光照射手段や撮像手段を配置したり、シート光照射手段と撮像手段のどちらかを水槽10全体に配置する方式と比較して、シート光照射手段や撮像手段の数を減らし、簡単な設備で実現することができる。また、気泡吹出手段40の場合と同様に、模型船20を直進だけさせるのではなく平面的な運動を伴う試験の場合、計測手段50が模型船20と同一方向に動くため、この効果は顕著となる。
なお、気泡吹出手段40と計測手段50の双方、又は一方、又は構成要素の一部は、曳航手段30以外の等速で動く手段により動かすことも可能である。
As described above, in the flow field measurement method using microbubbles according to the present embodiment, the bubble blowing means 40 for blowing microbubbles is provided in front of the object (model ship) 20, and the bubble blowing means 40 is connected to the model ship 20. By moving in the same direction at a constant speed and measuring the flow field based on the movement of the microbubbles blown out from the bubble blowing means 40 and flowing around the model ship 20, microbubbles can be introduced only around the model ship 20 in a timely manner. The flow field around the object can be accurately measured.
In addition, the microbubbles do not rise and disappear before the measurement is completed. Moreover, since the microbubbles which do not remain in the water tank 10 are used as the tracer, the maintenance and accuracy management of the water tank facilities are facilitated as compared with the case where the solid particles are used as the tracer.
In particular, since the bubble blowing means 40 and the measuring means 50 attached to the towing means 30 move at a constant speed together with the model ship 20 towed by the towing means 30 and move underwater, the flow field around the model ship 20 It is possible to obtain a highly accurate measurement result by supplying the minute bubbles only to the surface of the model ship 20 and focusing on only the periphery of the model ship 20.
For this reason, the bubble blowing means 40 can be made small-scale and simple compared with a fixed method in which bubbles are continuously diffused in the entire water tank 10 or bubbles are blown out for each region when the model ship 20 approaches. . Further, since microbubbles can be supplied only to the flow field around the model ship 20 to be measured, the amount of microbubbles can be very small, and the bubble blowing means 40 should be small and simple. Can do. When the model ship 20 is not only moved straight, but also when a test involving planar motion such as meandering or zigzag operation is performed, the bubble blowing means 40 moves in the same direction as the model ship 20, so this effect becomes remarkable.
In addition, the number of sheet light irradiation means and imaging means is compared with a system in which sheet light irradiation means and imaging means are arranged in the entire water tank 10 or either the sheet light irradiation means or the imaging means is arranged in the entire water tank 10. Can be realized with simple equipment. Further, as in the case of the bubble blowing means 40, in the case of a test involving a planar motion rather than just moving the model ship 20 straight, the measuring means 50 moves in the same direction as the model ship 20, so this effect is remarkable. It becomes.
Note that both or one of the bubble blowing means 40 and the measuring means 50, or a part of the components can be moved by means other than the towing means 30 and moving at a constant speed.

本発明の微小気泡を用いた流場計測方法及び水槽用流場計測装置によれば、例えば、船舶試験水槽での平水中又は波浪中における模型船の船尾流れの観測を高い精度で行える。
なお、上記の実施の形態では対象物を模型船として説明したが、本発明は、浮体や水中航行体の模型などが対象物の場合にも適用することができる。また、水槽は開放型の水槽以外に密閉された水槽にも適用が可能である。
According to the flow field measurement method and the aquarium flow field measurement apparatus using microbubbles according to the present invention, for example, the stern flow of a model ship can be observed with high accuracy in a plain water or a wave in a ship test water tank.
In the above embodiment, the object is described as a model ship. However, the present invention can also be applied to a case where a floating body, a model of an underwater navigation body, or the like is an object. Further, the water tank can be applied to a sealed water tank in addition to the open-type water tank.

10 水槽
20 対象物
30 曳引手段
40 気泡吹出手段
41 管部材
42 気泡吹出孔
43 気泡逃がし部
50 計測手段
51 シート光照射手段
52 撮像手段
53 ミラー
54 シリンドリカルレンズ
55 ミラー
60 気泡供給手段
71 初速度調整手段
72 気泡量調整手段
81 供給配管
82 吸い込み管
90 トラバース装置
DESCRIPTION OF SYMBOLS 10 Water tank 20 Object 30 Pulling means 40 Bubble blowing means 41 Pipe member 42 Bubble blowing hole 43 Bubble escape part 50 Measuring means 51 Sheet light irradiation means 52 Imaging means 53 Mirror 54 Cylindrical lens 55 Mirror 60 Bubble supply means 71 Initial speed adjustment Means 72 Bubble amount adjustment means 81 Supply pipe 82 Suction pipe 90 Traverse device

Claims (16)

水中を動く対象物の周囲の流場を計測する流場計測方法であって、前記対象物の前方に微小気泡を吹き出す気泡吹出手段を設け、前記気泡吹出手段を前記対象物と等速で同一方向に動かし、前記気泡吹出手段から吹き出す前記微小気泡を、前記気泡吹出手段に対し相対的に初速度を有して吹き出し、前記気泡吹出手段から吹き出されて前記対象物の周囲を流れる前記微小気泡の動きに基づいて前記流場を計測し、前記流場の計測結果を前記初速度に基づいて補正することを特徴とする微小気泡を用いた流場計測方法。 A flow field measurement method for measuring a flow field around an object moving in water, wherein a bubble blowing means for blowing out microbubbles is provided in front of the object, and the bubble blowing means is the same as the object at the same speed. The microbubbles that move in the direction and blow out from the bubble blowing means have an initial velocity relative to the bubble blowing means, and are blown out from the bubble blowing means and flow around the object. A flow field measurement method using microbubbles, wherein the flow field is measured based on the movement of the flow field, and the measurement result of the flow field is corrected based on the initial velocity . 前記初速度を水深方向に異ならせ、水深の深いところの前記初速度を水深の浅いところの前記初速度よりも遅くしたことを特徴とする請求項に記載の微小気泡を用いた流場計測方法。 2. The flow field measurement using microbubbles according to claim 1 , wherein the initial velocity is made different in a water depth direction, and the initial velocity at a deep water depth is made slower than the initial velocity at a shallow water depth. Method. 前記初速度を調整する初速度調整手段により前記初速度を制御したことを特徴とする請求項又は請求項に記載の微小気泡を用いた流場計測方法。 The flow field measurement method using microbubbles according to claim 1 or 2 , wherein the initial speed is controlled by an initial speed adjusting means for adjusting the initial speed. 前記微小気泡の気泡直径を5μmから100μmの範囲としたことを特徴とする請求項1から請求項のうちの1項に記載の微小気泡を用いた流場計測方法。 The flow field measurement method using microbubbles according to one of claims 1 to 3 , wherein a bubble diameter of the microbubbles is set in a range of 5 µm to 100 µm. 水に前記微小気泡を予め混ぜて前記気泡吹出手段に供給し、前記気泡吹出手段から前記微小気泡を前記水とともに吹き出すことを特徴とする請求項1から請求項のうちの1項に記載の微小気泡を用いた流場計測方法。 The water microbubbles previously mix was fed to the bubble blowing device, according to one of claims 4 the microbubbles from the bubble blowing means from claim 1, characterized in that blown together with the water Flow field measurement method using microbubbles. 前記気泡吹出手段から前記対象物の幅方向にも前記微小気泡を吹き出すことを特徴とする請求項1から請求項のうちの1項に記載の微小気泡を用いた流場計測方法。 Flow field measurement method using microbubbles according to claims 1 to one of the claims 5, characterized in that blowing the microbubbles in the width direction of the object from said bubble blowing means. 前記対象物と等速で同一方向に動くシート光を、シート光照射手段から前記対象物の近傍に照射して前記流場を計測することを特徴とする請求項1から請求項のうちの1項に記載の微小気泡を用いた流場計測方法。 The light sheet moving in the same direction with the object and the constant velocity, the sheet light irradiation means of claims 1 to 6, characterized in that to measure the flow field by irradiating the vicinity of the object A flow field measurement method using the microbubbles according to item 1. 前記シート光を前記対象物の動く方向と平行に照射したことを特徴とする請求項に記載の微小気泡を用いた流場計測方法。 The flow field measurement method using microbubbles according to claim 7 , wherein the sheet light is irradiated in parallel with a moving direction of the object. 水槽中の対象物を曳引する曳引手段と、前記対象物の前方に微小気泡を吹き出す気泡吹出手段と、前記気泡吹出手段に前記微小気泡を供給する気泡供給手段と、前記気泡吹出手段から吹き出されて前記対象物の周囲を流れる前記微小気泡の動きに基づいて流場を計測する計測手段と、前記気泡吹出手段から吹き出す前記微小気泡を、前記気泡吹出手段に対し相対的に初速度を有して吹き出し、前記流場の計測結果を前記初速度に基づいて補正するための初速度調整手段とを備え、前記気泡吹出手段と前記計測手段とを前記曳引手段に取り付けたことを特徴とする微小気泡を用いた水槽用流場計測装置。 From the pulling means for pulling the object in the water tank, the bubble blowing means for blowing out the fine bubbles in front of the object, the bubble supplying means for supplying the fine bubbles to the bubble blowing means, and the bubble blowing means Measuring means for measuring a flow field based on the movement of the microbubbles that are blown out and flow around the object, and the microbubbles that are blown out from the bubble blowing means have an initial velocity relative to the bubble blowing means. And an initial speed adjusting means for correcting the measurement result of the flow field based on the initial speed , and the bubble blowing means and the measuring means are attached to the pulling means. An aquarium flow field measurement device using microbubbles. 前記気泡吹出手段を、水深方向に伸びる管状構成とし、前記水深方向に複数の気泡吹出孔を有したことを特徴とする請求項に記載の微小気泡を用いた水槽用流場計測装置。 The water tank flow field measuring device using microbubbles according to claim 9 , wherein the bubble blowing means has a tubular configuration extending in a water depth direction and has a plurality of bubble blowing holes in the water depth direction. 前記気泡供給手段から供給される前記微小気泡の量を調整する気泡量調整手段を備えたことを特徴とする請求項又は請求項10に記載の微小気泡を用いた水槽用流場計測装置。 The flow field measuring device for a water tank using microbubbles according to claim 9 or 10 , further comprising a bubble amount adjusting means for adjusting the amount of the microbubbles supplied from the bubble supplying means. 前記微小気泡の気泡直径が5μmから100μmの範囲となるように前記気泡供給手段を制御したことを特徴とする請求項から請求項11のうちの1項に記載の微小気泡を用いた水槽用流場計測装置。 Tanks using microbubbles according to one of claims 11 claim 9, characterized in that the bubble diameter of the microbubbles is controlling the bubble supply means so that the range of 5μm to 100μm Flow field measuring device. 前記気泡供給手段が、前記微小気泡を水に混ぜて供給することを特徴とする請求項から請求項12のうちの1項に記載の微小気泡を用いた水槽用流場計測装置。 The bubble supply means, a water tank for flow field measuring apparatus using microbubbles according to one of claims 12 wherein the microbubbles claim 9, characterized in that the feed mix into water. 前記気泡吹出手段が、前記対象物の幅方向にも前記微小気泡を吹き出すことを特徴とする請求項から請求項13のうちの1項に記載の微小気泡を用いた水槽用流場計測装置。 The said bubble blowing means blows out the said microbubble also in the width direction of the said target object, The flow field measuring apparatus for water tanks using the microbubble of any one of Claim 9 to 13 characterized by the above-mentioned. . シート光を前記対象物の近傍に照射するシート光照射手段を、前記曳引手段に取り付けたことを特徴とする請求項から請求項14のうちの1項に記載の微小気泡を用いた水槽用流場計測装置。 The water tank using microbubbles according to any one of claims 9 to 14 , wherein sheet light irradiation means for irradiating sheet light in the vicinity of the object is attached to the pulling means. Flow field measuring device. 前記シート光を前記対象物の動く方向と平行に照射したことを特徴とする請求項15に記載の微小気泡を用いた水槽用流場計測装置。 The flow field measuring device for aquarium using microbubbles according to claim 15 , wherein the sheet light is irradiated in parallel with the moving direction of the object.
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