JP6644615B2 - Airtightness evaluation device and airtightness evaluation method - Google Patents

Airtightness evaluation device and airtightness evaluation method Download PDF

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JP6644615B2
JP6644615B2 JP2016069676A JP2016069676A JP6644615B2 JP 6644615 B2 JP6644615 B2 JP 6644615B2 JP 2016069676 A JP2016069676 A JP 2016069676A JP 2016069676 A JP2016069676 A JP 2016069676A JP 6644615 B2 JP6644615 B2 JP 6644615B2
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英二 酒井
英二 酒井
基博 池原
基博 池原
康彦 紺野
康彦 紺野
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本発明は、被測定体の気密の度合いを評価する気密性評価装置、及び気密性評価方法に関する。   The present invention relates to an airtightness evaluation device and an airtightness evaluation method for evaluating the degree of airtightness of an object to be measured.

従来、一般住宅や工場やクリーンルームなど(以下、“被測定体”とする)の気密の度合いを評価するための方法については日本工業規格(JIS A 2201:2003「送風機による住宅等の気密性能試験方法」)に規定されており、その方法を実施するための気密性評価装置については種々のものが提案されている(例えば、特許文献1、2、3参照)。   2. Description of the Related Art Conventionally, Japanese Industrial Standards (JIS A 2201: 2003, “Airtightness test of houses and the like using a blower”) has been described for a method of evaluating the degree of airtightness of a general house, a factory, a clean room, and the like (hereinafter, referred to as “measured object”). Method)), and various airtightness evaluation devices for implementing the method have been proposed (for example, see Patent Documents 1, 2, and 3).

ところで、既に構築されている被測定体の全体の気密性を評価するのではなく、該被測定体の一部の気密性を局所的に評価したいような場合がある。例えば、建物のドアや窓の隙間部の気密性のデータを予め測定しておいて、新たな建物を構築する場合に設計段階で参考にしたいようなケースが挙げられる。   Incidentally, there is a case where it is desired to locally evaluate the airtightness of a part of the object to be measured, instead of evaluating the airtightness of the entire object already constructed. For example, there is a case where airtightness data of gaps between doors and windows of a building is measured in advance, and it is desired to refer to the design stage when constructing a new building.

図4(a)は、そのような気密性評価装置を使って被測定体の局所的な気密性を測定する様子の一例を示す断面図であり、符号D3は被測定体を示し、符号H3は、該被測定体D3の表裏を貫通するように形成されている隙間部(孔部)を示し、符号C3は、該被測定体D3との間に略密閉された空間A3を形成するように該被測定体D3の表面に密着されるチャンバーを示し、符号2Cは、該空間A3内の空気を吸引する吸気手段を示している。このような装置において、該吸気手段2Cを駆動したときの前記空間A3からの風量を測定すれば局所的な気密性を演算により求めることができる。   FIG. 4A is a cross-sectional view showing an example of a state in which the local airtightness of the measured object is measured using such an airtightness evaluation device. Reference numeral D3 indicates the measured object, and reference numeral H3. Denotes a gap (hole) formed so as to penetrate the front and back of the measured object D3, and the symbol C3 defines a substantially sealed space A3 between the measured object D3 and the measured object D3. Shows a chamber which is brought into close contact with the surface of the measured object D3, and reference numeral 2C denotes an intake means for sucking air in the space A3. In such an apparatus, the local airtightness can be obtained by calculation by measuring the air volume from the space A3 when the air intake means 2C is driven.

特開平4−145339号公報JP-A-4-145339 特開2001−91397号公報JP 2001-91397 A 特開2002−228537号公報JP 2002-228537 A

ところで、図4(a)に例示するような被測定体D3の場合、該被測定体D3の裏側(図示の下側)から吸引される空気Mは前記空間A3にそのまま吸引されることとなるので、気密性を正確に評価することが出来るが、図4(b)に例示するような被測定体D4の場合には、隙間部H4は複雑に分岐しているために、該被測定体D4の裏側(図示の下側)から吸引される空気Mだけでなく横からの空気Nも前記空間A3に吸引されることとなり、該横からの空気Nがノイズ成分となってしまい、気密性を正確に評価することができないという問題があった。つまり、図4(a)(b)に例示する方法によれば、気密性の評価は被測定体の隙間部の形状の影響を受けることとなってしまい、気密性を正確に測れたり測れなかったりするという問題があった。   Meanwhile, in the case of the measured object D3 as illustrated in FIG. 4A, the air M sucked from the back side (the lower side in the figure) of the measured object D3 is sucked into the space A3 as it is. Therefore, the airtightness can be accurately evaluated. However, in the case of the measured object D4 as illustrated in FIG. 4B, since the gap H4 is complicatedly branched, the measured object Not only the air M sucked from the back side of D4 (the lower side in the figure) but also the air N from the side is sucked into the space A3, and the air N from the side becomes a noise component, and the airtightness Cannot be evaluated accurately. That is, according to the method illustrated in FIGS. 4A and 4B, the evaluation of the airtightness is affected by the shape of the gap portion of the measured object, and the airtightness cannot be accurately measured or measured. There was a problem that

本発明は、上述の問題を解消することのできる気密性評価装置、及び気密性評価方法を提供することを目的とするものである。   An object of the present invention is to provide an airtightness evaluation device and an airtightness evaluation method that can solve the above-described problems.

本発明の第1の観点は、図1及び図2(a)(b)に例示するものであって、被測定体(D1,D2)の気密の度合いを評価する気密性評価装置(1,11)において、
前記被測定体(D1,D2)の表面(図示上側の面)の一部であって気密の度合いを評価したい部分(E1)に密着させることによって該被測定体(D1,D2)と共に略密閉された第1密閉空間(A1)を形成する略椀状の第1チャンバー(C11,C21)と、
前記被測定体(D1,D2)の表面の一部であって該被測定体(D1,D2)を貫通するように孔部又は隙間部(図1の符号H1、及び図2(a)(b)の符号H2参照)が形成されている部分(E2)に密着させることによって該被測定体(D1,D2)と共に略密閉された第2密閉空間(A2)を形成する略椀状の第2チャンバー(C12,C22)と、
前記第1密閉空間(A1)及び前記第2密閉空間(A2)の空気を吸引するようにそれらの密閉空間(A1,A2)に連結される少なくとも1つの吸気手段(2A,2B)と、
前記第1密閉空間(A1)の気圧である第1気圧(P1)と前記第2密閉空間(A2)の気圧である第2気圧(P2)との差圧であるチャンバー間差圧(ΔPC)を取得するためのチャンバー間差圧取得手段(3)と、
該チャンバー間差圧取得手段(3)で取得したチャンバー間差圧(ΔPC)が略ゼロとなるように、前記吸気手段(2A)によって前記第1密閉空間(A1)から吸引する空気の風量、及び/又は該吸気手段(2B)によって前記第2密閉空間(A2)から吸引する空気の風量を調整する風量調整手段(4)と、
前記被測定体(D1,D2)の裏面側(図示下側であって、符号A3で示す側)の気圧(P3)と前記第1気圧(P1)との差圧である表裏差圧(ΔP)を取得するための表裏差圧取得手段(5)と、
前記吸気手段(2A)によって前記第1密閉空間(A1)から吸引される空気の風量(Q)を計測する風量計測手段(6)と、
前記表裏差圧取得手段(5)によって取得した表裏差圧(ΔP)と前記風量計測手段(6)によって計測した風量(Q)と下式(1)及び下式(2)とからαAの値を演算する演算手段(7)と、
を備え、
該演算手段(7)が演算したαAの値によって気密の度合いを評価するように構成されたことを特徴とする。

Figure 0006644615
Figure 0006644615
A first aspect of the present invention is illustrated in FIGS. 1 and 2A and 2B, and is a hermeticity evaluation device (1, 1) that evaluates the degree of hermeticity of a measured object (D1, D2). 11)
A part of the surface (the upper surface in the figure) of the object to be measured (D1, D2), which is substantially sealed with the object to be measured (D1, D2) by being in close contact with a part (E1) where the degree of airtightness is to be evaluated. A substantially bowl-shaped first chamber (C11, C21) forming a closed first space (A1);
A hole or a gap portion (symbol H1 in FIG. 1 and FIG. 2A) is a part of the surface of the measured object (D1, D2) and penetrates the measured object (D1, D2). b) A substantially bowl-shaped second space (A2) is formed in close contact with the measured object (D1, D2) by closely adhering to the portion (E2) where the H2) is formed. 2 chambers (C12, C22),
At least one intake means (2A, 2B) connected to the first enclosed space (A1) and the second enclosed space (A2) so as to suck air from the first enclosed space (A1) and the second enclosed space (A2);
A pressure difference between chambers (ΔPC) which is a pressure difference between a first pressure (P1) which is a pressure of the first closed space (A1) and a second pressure (P2) which is a pressure of the second closed space (A2). Inter-chamber differential pressure acquisition means (3) for acquiring pressure;
The air volume of air sucked from the first closed space (A1) by the suction means (2A) so that the inter-chamber differential pressure (ΔPC) obtained by the inter-chamber differential pressure obtaining means (3) becomes substantially zero. And / or an air volume adjusting means (4) for adjusting the air volume of air sucked from the second enclosed space (A2) by the air intake means (2B);
A front-back differential pressure (ΔP) which is a differential pressure between the pressure (P3) on the back surface side (the lower side in the figure and indicated by reference numeral A3) of the measured object (D1, D2) and the first pressure (P1). Front and back differential pressure acquisition means (5) for acquiring
An air volume measuring unit (6) for measuring an air volume (Q) of air sucked from the first enclosed space (A1) by the air intake unit (2A);
The value of αA is obtained from the front and back differential pressure (ΔP) obtained by the front and back differential pressure obtaining means (5), the air flow (Q) measured by the air flow measuring means (6), and the following equations (1) and (2). Computing means (7) for computing
With
It is characterized in that the degree of airtightness is evaluated based on the value of αA calculated by the calculating means (7).
Figure 0006644615
Figure 0006644615

本発明の第2の観点は、図1に例示するものであって、前記第2チャンバー(C12)は、前記第1チャンバー(C11)よりも大きくて該第1チャンバー(C11)を囲繞するように配置されてなることを特徴とする。   A second aspect of the present invention is illustrated in FIG. 1, wherein the second chamber (C12) is larger than the first chamber (C11) and surrounds the first chamber (C11). It is characterized by being arranged in.

本発明の第3の観点は、被測定体(D1,D2)の気密の度合いを評価する気密性評価方法において、
前記被測定体(D1,D2)の表面の一部であって気密の度合いを評価したい部分(E1)に略椀状の第1チャンバー(C11,C21)を密着させることによって該被測定体(D1,D2)と共に略密閉された第1密閉空間(A1)を形成する工程と、
前記被測定体(D1,D2)の表面の一部(E2)に略椀状の第2チャンバー(C12,C22)を密着させることによって該被測定体(D1,D2)と共に略密閉された第2密閉空間(A2)を形成する工程と、
前記第1密閉空間(A1)及び前記第2密閉空間(A2)の空気を吸引するように少なくとも1つの吸気手段(2A,2B)をそれらの密閉空間(A1,A2)に連結する工程と、
前記第1密閉空間(A1)の気圧である第1気圧(P1)と前記第2密閉空間(A2)の気圧である第2気圧(P2)との差圧であるチャンバー間差圧(ΔPC)を取得する工程と、
該取得したチャンバー間差圧(ΔPC)が略ゼロとなるように、前記吸気手段(2A)によって前記第1密閉空間(A1)から吸引する空気の風量、及び/又は該吸気手段(2B)によって前記第2密閉空間(A2)から吸引する空気の風量を調整する工程と、
前記被測定体(D1,D2)の裏面側の気圧(P3)と前記第1気圧(P1)との差圧である表裏差圧(ΔP)を取得する工程と、
前記吸気手段(2A,2B)によって前記第1密閉空間(A1)から吸引される空気の風量(Q)を計測する工程と、
前記表裏差圧(ΔP)と前記風量(Q)と下式(1)及び下式(2)とからαAの値を演算する工程と、
を備え、
該演算したαAの値によって気密の度合いを評価することを特徴とする。

Figure 0006644615
Figure 0006644615
According to a third aspect of the present invention, there is provided an airtightness evaluation method for evaluating a degree of airtightness of a measured object (D1, D2),
A substantially bowl-shaped first chamber (C11, C21) is brought into close contact with a part (E1) of the surface of the object to be measured (D1, D2) where the degree of airtightness is to be evaluated. D1, D2) to form a substantially hermetically sealed first enclosed space (A1);
A substantially bowl-shaped second chamber (C12, C22) is brought into close contact with a part (E2) of the surface of the measured object (D1, D2) to form a second chamber substantially sealed with the measured object (D1, D2). (2) forming a closed space (A2);
Connecting at least one intake means (2A, 2B) to the first enclosed space (A1) and the second enclosed space (A2) so as to suck air in the second enclosed space (A2);
A pressure difference between chambers (ΔPC) which is a pressure difference between a first pressure (P1) which is a pressure of the first closed space (A1) and a second pressure (P2) which is a pressure of the second closed space (A2). The step of obtaining
The air volume of the air sucked from the first closed space (A1) by the suction means (2A) and / or the air volume of the air suctioned by the suction means (2B) so that the acquired inter-chamber differential pressure (ΔPC) becomes substantially zero. Adjusting the air volume of the air sucked from the second closed space (A2);
Obtaining a front-back differential pressure (ΔP) that is a differential pressure between a pressure (P3) on the back surface side of the measured object (D1, D2) and the first pressure (P1);
A step of measuring an air volume (Q) of air sucked from the first closed space (A1) by the intake means (2A, 2B);
Calculating a value of αA from the front-back differential pressure (ΔP), the air volume (Q), and the following equations (1) and (2):
With
The degree of airtightness is evaluated by the calculated value of αA.
Figure 0006644615
Figure 0006644615

本発明の第4の観点は、前記第2チャンバー(C12)は、前記第1チャンバー(C11)よりも大きくて該第1チャンバー(C11)を囲繞するように配置することを特徴とする。   A fourth aspect of the present invention is characterized in that the second chamber (C12) is arranged to be larger than the first chamber (C11) and to surround the first chamber (C11).

本発明の第5の観点は、前記第2チャンバー(C12,C22)は、前記被測定体(D1,D2)の表面の一部であって該被測定体(D1,D2)を貫通するように孔部又は隙間部(図1の符号H1、及び図2(a)(b)の符号H2参照)が形成されている部分(E2)に密着させることを特徴とする。   According to a fifth aspect of the present invention, the second chamber (C12, C22) is a part of the surface of the measured object (D1, D2) and penetrates the measured object (D1, D2). And a portion (E2) in which a hole or gap (see reference numeral H1 in FIG. 1 and reference numeral H2 in FIGS. 2A and 2B) is formed.

本発明の第6の観点は、図2(a)(b)に例示するものであって、前記第1チャンバー(C21)は、前記被測定体(D2)の表裏を貫通するように形成されたスリット状の隙間部(H2)の一部(E1)を覆うように配置し、
前記第2チャンバー(C22)は、該第1チャンバー(C21)に隣接させた状態で前記隙間部(H2)の別の部分(E2)を覆うように配置することを特徴とする。
A sixth aspect of the present invention is illustrated in FIGS. 2 (a) and 2 (b), wherein the first chamber (C21) is formed so as to penetrate the front and back of the measured object (D2). Arranged so as to cover a part (E1) of the slit-shaped gap (H2),
The second chamber (C22) is arranged so as to cover another portion (E2) of the gap (H2) while being adjacent to the first chamber (C21).

なお、括弧内の番号などは、図面における対応する要素を示す便宜的なものであり、従って、本記述は図面上の記載に限定拘束されるものではない。   Note that the numbers in parentheses are for convenience showing the corresponding elements in the drawings, and therefore, the description is not limited to the description on the drawings.

上記した第1乃至6の観点によれば、気密性の評価をしたいエリア以外から(被測定体の内部の隙間を通って)該エリアに流入しようとする空気は隙間部を通って前記第2チャンバーの側に吸引されることとなり、前記第1チャンバーの側には吸引されないこととなる。その結果、局所的な気密性を正確に評価することができる。   According to the above-described first to sixth aspects, the air that is going to flow into the area other than the area where the airtightness is to be evaluated (through the gap inside the measured object) passes through the gap and the second air flows through the gap. It will be sucked to the side of the chamber and will not be sucked to the side of the first chamber. As a result, local airtightness can be accurately evaluated.

図1は、本発明に係る気密性評価装置の構成の一例を例示する断面図である。FIG. 1 is a cross-sectional view illustrating an example of the configuration of the airtightness evaluation device according to the present invention. 図2(a)は、本発明に係る気密性評価装置の構成の他の例を例示する平面図であり、同図(b)は、そのK−K断面図である。FIG. 2A is a plan view illustrating another example of the configuration of the airtightness evaluation device according to the present invention, and FIG. 2B is a cross-sectional view taken along the line KK. 図3(a)(b)は、本発明の効果を説明するための断面図である。FIGS. 3A and 3B are cross-sectional views for explaining the effect of the present invention. 図4(a)は、従来の気密性評価装置を使って被測定体の局所的な気密性を測定する様子の一例を示す断面図であり、同図(b)は、その問題点を示すための断面図である。FIG. 4A is a cross-sectional view showing an example of measuring the local airtightness of the measured object using a conventional airtightness evaluation device, and FIG. 4B shows the problem. FIG.

以下、図1乃至図3に沿って、本発明の実施の形態について説明する。   Hereinafter, an embodiment of the present invention will be described with reference to FIGS.

本発明に係る気密性評価装置は、被測定体の気密の度合いを局所的に評価することができるものである。本発明に係る気密性評価装置は、図1及び図2(a)(b)に符号1,11で例示するものであって、略椀状のチャンバーを少なくとも2つ備えている(符号C11,C12、及びC21,C22参照)。これらのチャンバーC11,C12,C21,C22は、開口を有していて、該開口の縁部は前記被測定体(符号D1,D2参照)に密着させることができるような形状になっていて、該開口の縁部を前記被測定体D1,D2に密着させた場合には該被測定体D1,D2と共に略閉塞された密閉空間A1,A2を形成するようになっている。なお、これらのチャンバーC11,C12,C21,C22は、湾曲した面で椀状(カップ状)で形成されている必要は必ずしも無く、少なくとも3つ以上の略平面で略角錐型又は略箱型に形成されていても良い。そして、一方のチャンバー(以下、“第1チャンバー”とする)C11,C21は、前記被測定体D1,D2の表面(図示上側の面)の一部であって気密の度合いを評価したい部分E1に密着させることによって該被測定体D1,D2と共に略密閉された第1密閉空間A1を形成するように構成され、他方のチャンバー(以下、“第2チャンバー”とする)C12,C22は、前記被測定体D1,D2の表面の一部であって該被測定体D1,D2を貫通するように孔部又は隙間部(図1の符号H1、及び図2(a)(b)の符号H2参照)が形成されている部分E2に密着させることによって該被測定体D1,D2と共に略密閉された第2密閉空間A2を形成するように構成されている。   The airtightness evaluation device according to the present invention can locally evaluate the degree of airtightness of an object to be measured. The airtightness evaluation device according to the present invention is exemplified by reference numerals 1 and 11 in FIGS. 1 and 2A and 2B and includes at least two substantially bowl-shaped chambers (reference numerals C11 and C11). C12, and C21 and C22). These chambers C11, C12, C21, and C22 have openings, and the edges of the openings are shaped so that they can be in close contact with the object to be measured (reference numerals D1 and D2). When the edges of the opening are brought into close contact with the measured objects D1 and D2, substantially closed closed spaces A1 and A2 are formed together with the measured objects D1 and D2. Note that these chambers C11, C12, C21, and C22 do not necessarily need to be formed in a bowl shape (cup shape) with a curved surface, and in at least three or more substantially flat surfaces into a substantially pyramid shape or a substantially box shape. It may be formed. One of the chambers (hereinafter, referred to as “first chamber”) C11 and C21 is a part E1 of the surface (upper surface in the drawing) of the measured objects D1 and D2 where the degree of airtightness is to be evaluated. To form a first hermetically sealed space A1 which is substantially sealed together with the measured objects D1 and D2, and the other chambers (hereinafter referred to as "second chambers") C12 and C22 A hole or a gap portion (reference numeral H1 in FIG. 1 and reference numeral H2 in FIGS. 2A and 2B) is a part of the surface of the measured objects D1 and D2 and penetrates the measured objects D1 and D2. (See FIG. 3) is formed so as to form a second hermetically sealed second space A2 together with the measured objects D1 and D2.

そして、本発明に係る気密性評価装置1,11は、
・ 前記第1チャンバーC11,C21と前記被測定体D1,D2とによって形成される第1密閉空間A1の空気、及び
・ 前記第2チャンバーC12,C22と前記被測定体D1,D2とによって形成される第2密閉空間A2の空気、
を吸引する吸気手段(いわゆるブロア)2A,2Bを備えている。なお、図1及び図2(a)(b)に示す例では、2つの吸気手段2A,2Bが配置されていて、前記第1密閉空間A1と前記第2密閉空間A2とを別々の吸気手段によって吸気するように構成されているが、もちろんこれに限られるものではなく、両方の密閉空間A1,A2の空気を1つの吸気手段で吸引するようにしても良い。その場合の吸気量は、該密閉空間A1,A2と該吸気手段との間に介装した絞り弁により調整するようにすると良い。また、3つ以上の吸気手段を備えたものを本発明の範囲から除外するものではない。つまり、本発明においては、前記第1密閉空間A1及び前記第2密閉空間A2の空気を吸引するようにそれらの密閉空間2A,2Bに連結(連通)される少なくとも1つの吸気手段が配置されていれば良い。さらに、図1及び図2(a)(b)に示す例では、各吸気手段2A,2Bは各チャンバーC11,C21,C12,C22に接続されているが、前記密閉空間2A,2Bに連通される構造のものであればもちろんこれに限られるものではなく、
・ 該吸気手段2A,2Bからの吸気通路が前記各チャンバーC11,C21,C12,C22と前記被測定体D1,D2との間に配置されて前記密閉空間A1,A2に開口するようにしても、或いは、
・ 該吸気手段2A,2Bからの吸気通路が前記被測定体D1,D2の内部にも配置されて該被測定体D1,D2の側から前記密閉空間A1,A2に開口するようにしても、
どちらでも良い。
And the airtightness evaluation devices 1 and 11 according to the present invention
Air in the first closed space A1 formed by the first chambers C11 and C21 and the objects D1 and D2; and air formed by the second chambers C12 and C22 and the objects D1 and D2. Air in the second enclosed space A2,
Suction means (so-called blowers) 2A and 2B for sucking air. In the example shown in FIGS. 1 and 2A and 2B, two intake units 2A and 2B are arranged, and the first closed space A1 and the second closed space A2 are separated from each other by separate intake units. However, the present invention is not limited to this, and the air in both the closed spaces A1 and A2 may be sucked by one suction unit. In this case, the amount of intake air is preferably adjusted by a throttle valve interposed between the closed spaces A1, A2 and the intake means. Further, a device provided with three or more intake means is not excluded from the scope of the present invention. That is, in the present invention, at least one intake means connected to (communicated with) the first closed space A1 and the second closed space A2 is provided so as to suck air from the first closed space A1 and the second closed space A2. Just do it. Further, in the examples shown in FIGS. 1 and 2 (a) and 2 (b), each intake means 2A, 2B is connected to each of the chambers C11, C21, C12, C22, but is communicated with the closed spaces 2A, 2B. Of course, it is not limited to this as long as it has a structure
The intake passages from the intake means 2A, 2B may be arranged between the chambers C11, C21, C12, C22 and the objects D1, D2 and open to the closed spaces A1, A2. Or
The intake passages from the intake means 2A, 2B are also arranged inside the measured objects D1, D2, and open from the sides of the measured objects D1, D2 to the closed spaces A1, A2.
both are fine.

一方、本発明に係る気密性評価装置1,11は、前記第1密閉空間A1の気圧(以下、“第1気圧”とする)P1と前記第2密閉空間A2の気圧(以下、“第2気圧”とする)P2との差圧(以下、“チャンバー間差圧”とする)ΔPCを取得するチャンバー間差圧取得手段3を備えている。この場合、市販されているような差圧測定器を該チャンバー間差圧取得手段3に用いて前記チャンバー間差圧ΔPCを直接測定することにより取得しても良いが、該チャンバー間差圧取得手段3を、
・ 前記第1気圧P1を測定する気圧計(不図示)と、
・ 前記第2気圧P2を測定する気圧計(不図示)と、
・ これらの気圧計の測定値に基づいて前記第1気圧と前記第2気圧との差圧を演算するチャンバー間差圧演算手段(不図示)と、
によって構成して前記チャンバー間差圧ΔPCを測定と演算とにより取得するようにしても良い。
On the other hand, the airtightness evaluation devices 1 and 11 according to the present invention are provided with an air pressure (hereinafter referred to as “first air pressure”) P1 of the first enclosed space A1 and an air pressure (hereinafter “second air pressure”) of the second enclosed space A2. An inter-chamber differential pressure acquiring unit 3 for acquiring a differential pressure ΔPC from the pressure P2 (hereinafter referred to as “inter-chamber differential pressure”) P2 is provided. In this case, the pressure difference between the chambers may be obtained by directly measuring the pressure difference ΔPC between the chambers using a commercially available differential pressure measuring device as the means for obtaining the pressure difference between the chambers 3. Means 3
A barometer (not shown) for measuring the first pressure P1;
A barometer (not shown) for measuring the second pressure P2;
An inter-chamber differential pressure calculating means (not shown) for calculating a differential pressure between the first air pressure and the second air pressure based on the measured values of these barometers;
To obtain the inter-chamber differential pressure ΔPC by measurement and calculation.

また、本発明に係る気密性評価装置1,11は、前記被測定体D1,D2の裏面側(符号A3で示す部分であって、図示の下側)であって前記第1チャンバーC11,C21及び前記第2チャンバーC12,C22が密着されていない側の気圧(以下、“裏面側気圧”とする)P3と前記第1気圧P1との差圧(以下、“表裏差圧”とする)ΔPを取得するための表裏差圧取得手段5を備えている。この場合も同様であって、市販されているような差圧測定器を該表裏差圧取得手段5に用いて前記表裏差圧ΔPを直接測定することにより取得しても良いが、該表裏差圧取得手段5を、
・ 前記第1気圧P1を測定する気圧計(不図示)と、
・ 前記裏面側気圧P3を測定する気圧計(不図示)と、
・ これらの気圧計の測定値に基づいて前記第1気圧と前記裏面側気圧との差圧を演算する表裏差圧演算手段(不図示)と、
によって構成して前記表裏差圧ΔPを測定と演算とにより取得するようにしても良い。
In addition, the airtightness evaluation devices 1 and 11 according to the present invention include the first chambers C11 and C21 on the back side of the measured objects D1 and D2 (the portion indicated by reference numeral A3 and the lower side in the drawing). And a pressure difference (hereinafter referred to as “front and back pressure difference”) between the pressure P3 on the side where the second chambers C12 and C22 are not in close contact (hereinafter referred to as “backside pressure”) and the first pressure P1. Is provided. The same applies to this case, and the pressure difference may be obtained by directly measuring the front-back differential pressure ΔP by using a commercially available differential pressure measuring device for the front-back differential pressure obtaining means 5. Pressure acquisition means 5
A barometer (not shown) for measuring the first pressure P1;
A barometer (not shown) for measuring the back side pressure P3;
Front and back pressure difference calculating means (not shown) for calculating a pressure difference between the first pressure and the back pressure based on the measured values of these barometers;
To obtain the front-back differential pressure ΔP by measurement and calculation.

また一方、本発明に係る気密性評価装置1,11は、前記チャンバー間差圧取得手段3が取得するチャンバー間差圧ΔPCが略ゼロとなるように、
(1) 前記第1密閉空間A1から前記吸気手段2Aによって吸引する空気の風量、又は
(2) 前記第2密閉空間A2から前記吸気手段2Bによって吸引する空気の風量、又は、
(3) 上記(1)及び(2)の両方の風量
のいずれかを調整することができる風量調整手段4を備えている。
On the other hand, the airtightness evaluation devices 1 and 11 according to the present invention are arranged so that the inter-chamber differential pressure ΔPC acquired by the inter-chamber differential pressure acquisition means 3 becomes substantially zero.
(1) Air volume of air sucked from the first closed space A1 by the air intake unit 2A, or (2) Air volume of air sucked from the second closed space A2 by the air suction unit 2B, or
(3) An air volume adjusting means 4 capable of adjusting either of the air volumes of (1) and (2) is provided.

また、本発明に係る気密性評価装置1,11は、前記第1密閉空間A1から前記吸気手段2Aによって吸引される空気の風量Qを計測する風量計測手段6を備えている。   Further, the airtightness evaluation devices 1 and 11 according to the present invention include an air volume measuring unit 6 that measures an air volume Q of air sucked from the first closed space A1 by the air intake unit 2A.

さらに、本発明に係る気密性評価装置1,11は、前記表裏差圧取得手段5によって取得した表裏差圧ΔPと前記風量計測手段6によって計測した風量Qと下式(1)及び下式(2)とからαAの値を演算する演算手段7、を備えていて、該演算手段7が演算したαAの値によって気密の度合いを評価するように構成されている。

Figure 0006644615
Figure 0006644615
Further, the airtightness evaluation devices 1 and 11 according to the present invention use the front and back differential pressure ΔP acquired by the front and back differential pressure acquisition unit 5 and the air volume Q measured by the air volume measurement unit 6 with the following equations (1) and ( 2) calculating means for calculating the value of αA from the above, and the degree of airtightness is evaluated based on the value of αA calculated by the calculating means 7.
Figure 0006644615
Figure 0006644615

ここで、前記相当隙間面積αAの具体的演算方法について説明する。   Here, a specific calculation method of the equivalent gap area αA will be described.

前記吸気手段2A,2Bを操作して吸気量を変えつつ、ΔPとQの値を最低3組以上実測(取得)していく。例えば、3つの表裏差圧ΔP,ΔP,ΔPと、3つの風量Q,Q,Qと、を実測によって求めておく。それらの値を上式(1)に代入して例えば最小二乗法を使うことにより、上記aとnの値が求まることとなる。一方、ρは空気密度であって、測定時の気温tと下式(3)とによって求めることができる。例えば、気温が20℃の場合はρの値は約1.2(kg/m)となる。

Figure 0006644615
While changing the amount of intake air by operating the intake means 2A and 2B, at least three sets of values of ΔP and Q are actually measured (acquired). For example, three front-back differential pressures ΔP 1 , ΔP 2 , ΔP 3 and three air volumes Q 1 , Q 2 , Q 3 are obtained by actual measurement. By substituting these values into the above equation (1) and using, for example, the least squares method, the values of the above a and n are obtained. On the other hand, ρ is the air density, which can be obtained from the temperature t at the time of measurement and the following equation (3). For example, when the temperature is 20 ° C., the value of ρ is about 1.2 (kg / m 3 ).
Figure 0006644615

上式(1)と(2)とから、下式(4)を求めることができるが、この式において、aとnとρの値は上述のようにそれぞれ既知であってΔPは9.8(Pa)とすれば良いので、αAの値が求まることとなる。

Figure 0006644615
The following equation (4) can be obtained from the above equations (1) and (2). In this equation, the values of a, n, and ρ are known as described above, and ΔP is 9.8. (Pa), the value of αA is determined.
Figure 0006644615

本発明によれば、気密性の評価をしたいエリア以外から(被測定体D1の内部の隙間を通って)該エリアに流入しようとする空気は隙間部H1を通って前記第2チャンバーC12の側に吸引されることとなり、前記第1チャンバーC11の側には吸引されないこととなる。その結果、局所的な気密性を正確に評価することができる。例えば、図3(a)(b)に例示するような被検体D3,D4の場合、下側からの空気はそのままチャンバー内に吸引されることとなり、気密性を評価したいエリア以外からの空気が第1チャンバーC21に吸引されることはなく、その結果、局所的な気密性を正確に評価することができる。   According to the present invention, the air that is going to flow into the area other than the area where the airtightness is to be evaluated (through the gap inside the measured object D1) passes through the gap H1 on the side of the second chamber C12. And is not sucked into the first chamber C11 side. As a result, local airtightness can be accurately evaluated. For example, in the case of the specimens D3 and D4 as illustrated in FIGS. 3A and 3B, air from the lower side is sucked into the chamber as it is, and air from areas other than the area where the airtightness is to be evaluated is removed. The air is not sucked into the first chamber C21, and as a result, the local airtightness can be accurately evaluated.

ところで、図1に例示する第2チャンバーC12は、前記第1チャンバーC12よりも大きくて該第1チャンバーC11を囲繞するように配置されている(つまり、該第1チャンバーC11及び該第2チャンバーC12が二重になるように配置されている)が、もちろんこれに限られるものではなく、図2(a)(b)に例示するように、第1チャンバーC21と第2チャンバーC22とを隣接するように配置しても良い。また、図1に示す例では、前記第2チャンバーC12の内側に配置されている第1チャンバーC11の個数は1つであるが、もちろんこれに限られるものではなく、2つ以上であっても良い。   Meanwhile, the second chamber C12 illustrated in FIG. 1 is arranged so as to be larger than the first chamber C12 and surround the first chamber C11 (that is, the first chamber C11 and the second chamber C12). Are arranged so as to form a double), but the present invention is not limited to this, and the first chamber C21 and the second chamber C22 are adjacent to each other as illustrated in FIGS. 2A and 2B. It may be arranged as follows. Further, in the example shown in FIG. 1, the number of the first chambers C11 arranged inside the second chamber C12 is one. However, the number of the first chambers C11 is not limited thereto. good.

一方、本発明に係る気密性評価方法は、前記被測定体D1,D2の気密の度合いを評価するためのものであって、
・ 該被測定体D1,D2の表面の一部であって気密の度合いを評価したい部分E1に略椀状の第1チャンバーC11,C21を密着させることによって該被測定体D1,D2と共に略密閉された第1密閉空間A1を形成する工程と、
・ 前記被測定体D1,D2の表面の一部E2に略椀状の第2チャンバーC12,C22を密着させることによって該被測定体D1,D2と共に略密閉された第2密閉空間A2を形成する工程と、
・ 前記第1密閉空間A1及び前記第2密閉空間A2の空気を吸引するように少なくとも1つの吸気手段2A,2Bをそれらの密閉空間A1,A2に連結する工程と、
・ 前記第1密閉空間A1の気圧である第1気圧P1と前記第2密閉空間A2の気圧である第2気圧P2との差圧であるチャンバー間差圧ΔPCを取得する工程と、
・ 該取得したチャンバー間差圧ΔPCが略ゼロとなるように、前記吸気手段2Aによって前記第1密閉空間A1から吸引する空気の風量、及び/又は該吸気手段2Bによって前記第2密閉空間A2から吸引する空気の風量を調整する工程と、
・ 前記被測定体D1,D2の裏面側A3の気圧P3と前記第1気圧P1との差圧である表裏差圧ΔPを取得する工程と、
・ 前記吸気手段2Aによって前記第1密閉空間A1から吸引される空気の風量Qを計測する工程と、
・ 前記表裏差圧ΔPと前記風量Qと下式(1)及び下式(2)とからαAの値を演算する工程と、
を備えていて、該演算したαAの値によって気密の度合いを評価するようになっている。

Figure 0006644615
Figure 0006644615
On the other hand, the airtightness evaluation method according to the present invention is for evaluating the degree of airtightness of the measured objects D1 and D2,
A substantially bowl-shaped first chamber C11, C21 is brought into close contact with a part E1 of the surface of the measured objects D1, D2 where the degree of airtightness is to be evaluated, thereby substantially sealing with the measured objects D1, D2. Forming a closed first closed space A1;
The second chambers C12 and C22, which are substantially bowl-shaped, are brought into close contact with a part E2 of the surface of the measured objects D1 and D2 to form a substantially closed second sealed space A2 together with the measured objects D1 and D2. Process and
Connecting at least one intake means 2A, 2B to the first enclosed space A1 and the second enclosed space A2 so as to suck air in the first enclosed space A1 and the second enclosed space A2;
A step of obtaining an inter-chamber differential pressure ΔPC which is a pressure difference between a first pressure P1 which is the pressure of the first closed space A1 and a second pressure P2 which is a pressure of the second closed space A2;
The amount of air sucked from the first closed space A1 by the suction means 2A and / or the second closed space A2 by the suction means 2B so that the acquired pressure difference ΔPC between the chambers becomes substantially zero. Adjusting the air volume of the air to be sucked;
A step of obtaining a front-back differential pressure ΔP, which is a differential pressure between the pressure P3 of the back surface A3 of the measured objects D1 and D2 and the first pressure P1;
A step of measuring an air volume Q of the air sucked from the first closed space A1 by the suction unit 2A;
A step of calculating a value of αA from the front-back differential pressure ΔP, the air volume Q, and the following equations (1) and (2);
And the degree of airtightness is evaluated based on the calculated value of αA.
Figure 0006644615
Figure 0006644615

本発明によれば、気密性の評価をしたいエリア以外から(被測定体D1の内部の隙間を通って)該エリアに流入しようとする空気は隙間部H1を通って前記第2チャンバーC12の側に吸引されることとなり、前記第1チャンバーC11の側には吸引されないこととなる。その結果、局所的な気密性を正確に評価することができる。   According to the present invention, the air that is going to flow into the area other than the area where the airtightness is to be evaluated (through the gap inside the measured object D1) passes through the gap H1 on the side of the second chamber C12. And is not sucked into the first chamber C11 side. As a result, local airtightness can be accurately evaluated.

この場合、図1に例示するように、前記第2チャンバーC12は、前記第1チャンバーC11よりも大きくて該第1チャンバーC11を囲繞するように配置するようにすると良い。   In this case, as illustrated in FIG. 1, the second chamber C12 is preferably larger than the first chamber C11 so as to surround the first chamber C11.

また、前記第2チャンバーC12,C22は、前記被測定体D1,D2の表面の一部であって該被測定体D1,D2を貫通するように孔部又は隙間部(図1の符号H1、及び図2(a)(b)の符号H2参照)が形成されている部分E2に密着させるようにすると良い。   Further, the second chambers C12 and C22 are holes or gaps (reference numerals H1 and H1 in FIG. 1) that are part of the surfaces of the measurement objects D1 and D2 and penetrate the measurement objects D1 and D2. 2 (a) and 2 (b) (refer to reference numeral H2).

さらに、図2(a)(b)に例示するように、前記第1チャンバーC21は、前記被測定体D2の表裏を貫通するように形成されたスリット状の隙間部H2の一部E1を覆うように配置し、前記第2チャンバーC22は、該第1チャンバーC21に隣接させた状態で前記隙間部H2の別の部分E2を覆うように配置するようにすると良い。このようなスリット状の隙間部H2としては、ドアや窓やガラリの隙間を挙げることができる。   Further, as exemplified in FIGS. 2A and 2B, the first chamber C21 covers a part E1 of a slit-shaped gap H2 formed so as to penetrate the front and back of the measured object D2. It is preferable that the second chamber C22 is arranged so as to cover another portion E2 of the gap H2 in a state of being adjacent to the first chamber C21. Examples of such a slit-shaped gap H2 include a gap between a door, a window, and a rag.

1 気密性評価装置
2A,2B 吸気手段
3 チャンバー間差圧取得手段
4 風量調整手段
5 表裏差圧取得手段
6 風量計測手段
7 演算手段
11 気密性評価装置
A1 第1密閉空間
A2 第2密閉空間
A3 被測定体の裏面側
C11 第1チャンバー
C12 第2チャンバー
C21 第1チャンバー
C22 第2チャンバー
D1 被測定体
D2 被測定体
H1 孔部又は隙間部
H2 スリット状の隙間部
P1 第1気圧
P2 第2気圧
P3 被測定体の裏面側の気圧
ΔP 表裏差圧
ΔPC チャンバー間差圧
DESCRIPTION OF SYMBOLS 1 Airtightness evaluation apparatus 2A, 2B Intake means 3 Inter-chamber differential pressure acquisition means 4 Air volume adjustment means 5 Front and back differential pressure acquisition means 6 Air volume measurement means 7 Calculation means 11 Airtightness evaluation apparatus A1 First enclosed space A2 Second enclosed space A3 Back side C11 of measurement object C1 first chamber C12 second chamber C21 first chamber C22 second chamber D1 measurement object D2 measurement object H1 hole or gap H2 slit-shaped gap P1 first pressure P2 second pressure P3 Air pressure ΔP on the back side of the measured object Differential pressure between front and back ΔPC Differential pressure between chambers

Claims (6)

被測定体の気密の度合いを評価する気密性評価装置において、
前記被測定体の表面の一部であって気密の度合いを評価したい部分に密着させることによって該被測定体と共に略密閉された第1密閉空間を形成する略椀状の第1チャンバーと、
前記被測定体の表面の一部であって該被測定体を貫通するように孔部又は隙間部が形成されている部分に密着させることによって該被測定体と共に略密閉された第2密閉空間を形成する略椀状の第2チャンバーと、
前記第1密閉空間及び前記第2密閉空間の空気を吸引するようにそれらの密閉空間に連結される少なくとも1つの吸気手段と、
前記第1密閉空間の気圧である第1気圧と前記第2密閉空間の気圧である第2気圧との差圧であるチャンバー間差圧を取得するためのチャンバー間差圧取得手段と、
該チャンバー間差圧取得手段で取得したチャンバー間差圧が略ゼロとなるように、前記吸気手段によって前記第1密閉空間から吸引する空気の風量、及び/又は該吸気手段によって前記第2密閉空間から吸引する空気の風量を調整する風量調整手段と、
前記被測定体の裏面側の気圧と前記第1気圧との差圧である表裏差圧を取得するための表裏差圧取得手段と、
前記吸気手段によって前記第1密閉空間から吸引される空気の風量を計測する風量計測手段と、
前記表裏差圧取得手段によって取得した表裏差圧と前記風量計測手段によって計測した風量に基づいて前記被測定体の気密の度合いを演算する演算手段を備えた、
ことを特徴とする気密性評価装置。
In an airtightness evaluation device for evaluating the degree of airtightness of the measured object,
A substantially bowl-shaped first chamber that forms a first sealed space that is substantially sealed together with the measured object by being in close contact with a part of the surface of the measured object and a portion where the degree of airtightness is to be evaluated;
A second closed space substantially sealed with the measured object by being in close contact with a part of the surface of the measured object and having a hole or a gap formed through the measured object; A substantially bowl-shaped second chamber forming
At least one intake means coupled to the first enclosed space and the second enclosed space so as to suck air in the second enclosed space;
An inter-chamber differential pressure acquiring means for acquiring an inter-chamber differential pressure which is a differential pressure between a first atmospheric pressure which is an atmospheric pressure of the first enclosed space and a second atmospheric pressure which is an atmospheric pressure of the second enclosed space,
The air volume of the air sucked from the first closed space by the suction means and / or the second closed space by the suction means so that the inter-chamber differential pressure acquired by the inter-chamber differential pressure acquisition means becomes substantially zero. Air volume adjusting means for adjusting the air volume of air sucked from the
Front and back differential pressure obtaining means for obtaining a front and back differential pressure which is a differential pressure between the pressure on the back side of the measured object and the first air pressure,
Air volume measuring means for measuring an air volume of air sucked from the first closed space by the air intake means;
Comprising arithmetic means for calculating the degree of airtightness of the object to be measured based on the front and back differential pressure acquired by the front and back differential pressure acquisition means and the airflow measured by the airflow measurement means,
An airtightness evaluation device, characterized in that:
前記第2チャンバーは、前記第1チャンバーよりも大きくて該第1チャンバーを囲繞するように配置されてなる、
ことを特徴とする請求項1に記載の気密性評価装置。
The second chamber is larger than the first chamber and is arranged to surround the first chamber.
The airtightness evaluation device according to claim 1, wherein:
被測定体の気密の度合いを評価する気密性評価方法において、
前記被測定体の表面の一部であって気密の度合いを評価したい部分に略椀状の第1チャンバーを密着させることによって該被測定体と共に略密閉された第1密閉空間を形成する工程と、
前記被測定体の表面の一部に略椀状の第2チャンバーを密着させることによって該被測定体と共に略密閉された第2密閉空間を形成する工程と、
前記第1密閉空間及び前記第2密閉空間の空気を吸引するように少なくとも1つの吸気手段をそれらの密閉空間に連結する工程と、
前記第1密閉空間の気圧である第1気圧と前記第2密閉空間の気圧である第2気圧との差圧であるチャンバー間差圧を取得する工程と、
該取得したチャンバー間差圧が略ゼロとなるように、前記吸気手段によって前記第1密閉空間から吸引する空気の風量、及び/又は該吸気手段によって前記第2密閉空間から吸引する空気の風量を調整する工程と、
前記被測定体の裏面側の気圧と前記第1気圧との差圧である表裏差圧を取得する工程と、
前記吸気手段によって前記第1密閉空間から吸引される空気の風量を計測する工程と、
前記表裏差圧と前記風量に基づいて 前記被測定体の気密の度合いを演算評価する、
ことを特徴とする気密性評価方法。
In the airtightness evaluation method for evaluating the degree of airtightness of the measured object,
Forming a substantially closed first sealed space together with the measured object by adhering a substantially bowl-shaped first chamber to a part of the surface of the measured object and a portion where the degree of airtightness is to be evaluated; ,
Forming a substantially closed second sealed space together with the measured object by bringing a substantially bowl-shaped second chamber into close contact with a part of the surface of the measured object;
Coupling at least one intake means to the first enclosed space and the second enclosed space so as to suck air in the second enclosed space;
Obtaining a differential pressure between chambers, which is a differential pressure between a first atmospheric pressure, which is an atmospheric pressure of the first enclosed space, and a second atmospheric pressure, which is an atmospheric pressure of the second enclosed space,
The air volume of the air sucked from the first closed space by the suction unit and / or the air volume of the air sucked from the second closed space by the suction unit so that the acquired pressure difference between the chambers becomes substantially zero. Adjusting,
A step of obtaining a front-back differential pressure that is a differential pressure between a pressure on the back surface side of the measured object and the first pressure;
Measuring the air volume of the air sucked from the first enclosed space by the suction means;
Computing and evaluating the degree of airtightness of the measured object based on the front-back differential pressure and the air volume,
An airtightness evaluation method characterized in that:
前記第2チャンバーは、前記第1チャンバーよりも大きくて該第1チャンバーを囲繞するように配置する、
ことを特徴とする請求項3に記載の気密性評価方法。
The second chamber is arranged to be larger than the first chamber and surround the first chamber.
The airtightness evaluation method according to claim 3, wherein:
前記第2チャンバーは、前記被測定体の表面の一部であって該被測定体を貫通するように孔部又は隙間部が形成されている部分に密着させる、
ことを特徴とする請求項3に記載の気密性評価方法。
The second chamber is in close contact with a part of a surface of the measured object, in which a hole or a gap is formed to penetrate the measured object,
The airtightness evaluation method according to claim 3, wherein:
前記第1チャンバーは、前記被測定体の表裏を貫通するように形成されたスリット状の隙間部の一部を覆うように配置し、
前記第2チャンバーは、該第1チャンバーに隣接させた状態で前記隙間部の別の部分を覆うように配置する、
ことを特徴とする請求項5に記載の気密性評価方法。
The first chamber is disposed so as to cover a part of a slit-shaped gap formed to penetrate the front and back of the measured object,
The second chamber is disposed so as to cover another portion of the gap in a state adjacent to the first chamber.
The airtightness evaluation method according to claim 5, wherein:
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