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JP6544402B2 - Method of predicting corrosion of metals by numerical analysis - Google Patents
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JP6544402B2 - Method of predicting corrosion of metals by numerical analysis - Google Patents

Method of predicting corrosion of metals by numerical analysis Download PDF

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JP6544402B2
JP6544402B2 JP2017177826A JP2017177826A JP6544402B2 JP 6544402 B2 JP6544402 B2 JP 6544402B2 JP 2017177826 A JP2017177826 A JP 2017177826A JP 2017177826 A JP2017177826 A JP 2017177826A JP 6544402 B2 JP6544402 B2 JP 6544402B2
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水野 大輔
大輔 水野
祐一 加茂
祐一 加茂
渡辺 裕一
裕一 渡辺
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本発明は、広く産業分野で使用されている金属材料の腐食を数値解析によって予測する方法に関する。本発明は、具体的には、構造物の品質及び性能寿命を予測するために、数値解析(数値シミュレーション)を用いて腐食媒体である電解質溶液中の電位分布や電流密度分布を計算して、金属の耐食性を予測する腐食評価に関連する技術である。   The present invention relates to a method of predicting corrosion of metallic materials widely used in the industrial field by numerical analysis. In the present invention, specifically, in order to predict the quality and performance life of a structure, numerical distribution (numerical simulation) is used to calculate potential distribution and current density distribution in an electrolyte solution which is a corrosive medium, It is a technology related to corrosion evaluation that predicts the corrosion resistance of metals.

従来、金属材料の耐食性評価は、腐食促進試験や大気暴露試験、あるいは電気化学測定によって行われる。例えば鉄鋼材料の耐食性を評価する場合、塩水噴霧試験(SST:Salt Spray Test)や、これに湿潤や乾燥の雰囲気条件を組み合わせる複合サイクル試験(CCT:Combined Cyclic corrosion Test)により、試験片や実部品の腐食を促進して短期間で耐食性の優劣を判断することが行われる。一方、このような腐食促進試験が、実際に鉄鋼材料が使用される環境に比べて厳しい腐食環境であることから、実使用環境における腐食形態や種類の異なる鉄鋼材料の耐食性の序列を再現しない場合がある。そのため、試験片を屋外や屋内に設置して、実使用に近い環境の中で腐食させることで、耐食性を評価する大気暴露試験も広く行われている。しかし、暴露試験は耐食性の優劣を判断するまでに長期間を有するため、耐食性の早期判断が求められる耐食材料の開発には適していない。   Conventionally, the corrosion resistance of a metal material is evaluated by a corrosion promotion test, an air exposure test, or an electrochemical measurement. For example, in the case of evaluating the corrosion resistance of steel materials, test pieces and actual parts are obtained by a salt spray test (SST) or a combined cycle test (CCT: combined cyclic corrosion test) combining the wet and dry atmospheric conditions with this. It is carried out to promote the corrosion of the steel and to judge the superiority or inferiority of the corrosion resistance in a short time. On the other hand, because such a corrosion promotion test is a severe corrosive environment compared to the environment in which steel materials are actually used, it is not possible to reproduce the corrosion resistance hierarchy of steel materials of different corrosion types and types in actual use environments. There is. Therefore, air exposure tests for evaluating corrosion resistance are widely performed by installing test pieces outdoors or indoors and corroding them in an environment close to actual use. However, since the exposure test has a long time to determine the superiority or inferiority of the corrosion resistance, it is not suitable for the development of a corrosion resistant material for which an early judgment of the corrosion resistance is required.

これに対して、近年のコンピュータ技術の発展と計算高速化に伴い、コンピューターシミュレーションにより腐食現象を予測する試みが活発に行われている。数値解析により金属の腐食を予測することができれば、実験では解析困難な腐食原因や腐食機構の解析や、金属の耐食性を短時間で評価することができる可能性がある。   On the other hand, with recent development of computer technology and speeding up of calculation, attempts to predict corrosion phenomena by computer simulation are actively performed. If corrosion of metals can be predicted by numerical analysis, analysis of the causes of corrosion and corrosion mechanisms that are difficult to analyze in experiments may be possible, and the corrosion resistance of metals can be evaluated in a short time.

特許文献1および特許文献2は、腐食媒体内にある金属を電気的に接続された複数の解析セグメントからなる連続体とみなして、当該金属の分極特性を決定する、腐食環境の数値解析方法を開示する。この方法は、モデル中の腐食媒体をラプラス方程式に従うラプラス場とみなして数値解析を行い、対象構造物である金属の電位分布および電流の流出入を計算することで、腐食に対する駆動力や腐食速度を推定する方法である。   Patent document 1 and patent document 2 consider the metal in a corrosion medium as a continuum which consists of a plurality of analysis segments electrically connected, and determine the polarization characteristic of the metal concerned numerically. Disclose. This method considers the corrosion medium in the model as a Laplace field according to the Laplace equation, performs numerical analysis, and calculates the potential distribution of the metal that is the target structure and the inflow and outflow of current to obtain the driving force for corrosion and the corrosion rate. Is a method of estimating

また非特許文献1では、海水ポンプの腐食を境界要素法により解析する技術が報告されている。ここでは、ポンプの材料である鋳鉄(FC200)の分極曲線を境界条件としてラプラス方程式を解くことで、腐食媒体である海水中の電位分布および電流分布を求め、鋳鉄と海水との界面の電位および電流密度から鋳鉄の腐食を予測するモデルを提案している。ここで水溶液中の電気伝導度は実験から求めた値を用いている。   In addition, Non-Patent Document 1 reports a technology for analyzing the corrosion of a seawater pump by the boundary element method. Here, the potential distribution and current distribution in the corrosive medium seawater are determined by solving the Laplace equation with the polarization curve of cast iron (FC200) as the pump material as the boundary condition, and the potential at the interface between cast iron and seawater and We propose a model to predict the corrosion of cast iron from the current density. Here, the electrical conductivity in the aqueous solution uses the value obtained from the experiment.

非特許文献2では、コンクリート中の鉄筋の腐食をシミュレーションしている。コンクリート中の塩化物や酸素などの腐食因子の物質移動を予測し、さらに、Tafel式により腐食電流密度を求めて鉄筋の腐食を予測している。このモデルでは、コンクリートを細孔とみなして溶液と同様に均一な媒体として扱うことで、拡散方程式を用いて物質移動の計算を行っている。   Non-Patent Document 2 simulates the corrosion of reinforcing bars in concrete. The mass transfer of corrosion factors such as chloride and oxygen in concrete is predicted, and furthermore, the corrosion current density is obtained by the Tafel equation to predict the corrosion of reinforcing bars. In this model, mass transfer is calculated using the diffusion equation by treating concrete as pores and treating it as a uniform medium like a solution.

非特許文献3では、亜鉛めっきと下地鋼板の薄水膜下での異種金属接触腐食において、物質移動と化学反応を考慮した数値計算を行い、亜鉛および鋼の腐食を予測している。このモデルでは、亜鉛や鋼の腐食生成物の形成やその分布を微小時間毎に計算しており、境界条件として与えたアノード反応から計算される溶出金属イオンが、物質移動の計算による化学種と反応し、金属酸化物や水酸化物を形成する沈殿反応を、平衡定数を用いる平衡計算により予測しており、これにより種々の腐食生成物の分布と量を予測している。   Non-Patent Document 3 predicts corrosion of zinc and steel by performing numerical calculation in consideration of mass transfer and chemical reaction in galvanizing and dissimilar metal contact corrosion under a thin water film of a base steel sheet. In this model, the formation and distribution of corrosion products of zinc and steel are calculated every minute time, and the eluted metal ions calculated from the anode reaction given as the boundary conditions are the chemical species by mass transfer calculation and The precipitation reactions that react and form metal oxides and hydroxides are predicted by equilibrium calculations using equilibrium constants, which predict the distribution and amount of various corrosion products.

特開2008−249562号公報JP, 2008-249562, A 特開2008−32421号広報Japanese Patent Application Publication No. 2008-32421

エバラ時報 No.223(2009−3)37−45Everla Times No. 223 (2009-3) 37-45 コンクリート工学年次論文集,Vol.24,No.1,(2002)831−836Concrete Engineering Annual Proceedings, Vol. 24, No. 1, (2002) 831-836 材料と環境,Vol.61,(2012),376−383Materials and Environment, Vol. 61, (2012), 376-383.

腐食現象のモデル化や数値解析方法には、様々な手法が考えられる。このうち広く実施されているのが、腐食媒体である電解質溶液を仮定した領域において、腐食速度に相当する電流密度や腐食反応の駆動力となる電位の分布を、物質輸送の理論式やラプラス方程式を解くことにより求める方法である。金属の腐食は、電解質溶液と金属の界面における電流の流出入や電位差によって評価される。このような方程式の解法としては、電解質溶液領域を要素化する連続体モデルとして、差分法や有限要素法などが用いられている。電解質溶液中における金属表面の電位と電流密度との関係である金属の分極特性を境界条件として与え、各要素内の電位および電流の分布、要素内や境界における物質の収支を計算する。   Various methods can be considered for modeling corrosion analysis and numerical analysis methods. Among these, the current density corresponding to the corrosion rate and the distribution of the potential serving as the driving force of the corrosion reaction in the region assuming the electrolyte solution which is a corrosive medium are widely practiced. It is a method to obtain by solving The corrosion of metal is evaluated by the inflow and outflow of the current at the interface between the electrolyte solution and the metal and the potential difference. As a solution method of such an equation, a difference method, a finite element method, or the like is used as a continuum model in which the electrolyte solution region is elementized. The polarization characteristics of the metal, which is the relationship between the electric potential of the metal surface in the electrolyte solution and the current density, are given as boundary conditions, and the distribution of the electric potential and current in each element, and the material balance in the element and at the boundary are calculated.

このような計算を行う上で、電解質溶液中の電気伝導度は、多くの場合一定として計算される。あるいは、電解質溶液全体や各要素に溶解している化学種の濃度から電気伝導度を計算する場合もある。   In making such calculations, the conductivity in the electrolyte solution is often calculated as constant. Alternatively, the conductivity may be calculated from the concentration of chemical species dissolved in the entire electrolyte solution and in each element.

実際の腐食現象では、腐食は単に金属の溶解(イオン化)として進行するばかりでなく、金属の酸化物や水酸化物が生成する、いわゆる「さび」あるいは「腐食生成物」の形成を伴う。以降、溶解した金属の析出物(酸化物、水酸化物等)を腐食生成物と呼ぶ。腐食生成物は金属の腐食速度に大きな影響を及ぼす。例えば、電解質溶液中で活性な亜鉛が、大気環境において優れた耐食性を発揮するのは、亜鉛の腐食生成物が表面を覆うことで金属亜鉛の腐食速度を減少させるためである。   In the actual corrosion phenomenon, the corrosion not only proceeds as dissolution (ionization) of the metal, but also involves the formation of so-called "rust" or "corrosion products", which form oxides and hydroxides of the metal. Hereinafter, precipitates of dissolved metal (oxides, hydroxides, etc.) are referred to as corrosion products. Corrosion products have a significant effect on the corrosion rate of metals. For example, zinc active in an electrolyte solution exerts excellent corrosion resistance in an atmospheric environment because the corrosion products of zinc cover the surface to reduce the corrosion rate of metallic zinc.

特許文献1および特許文献2では、モデル中の腐食媒体をラプラス方程式に従うラプラス場とみなして解析しており、媒質として土壌を例にして電気的物性値を比抵抗5000Ω・cmとして与えている。この発明において媒質が水溶液の場合には、水溶液の電気伝導度が与えられれば、水溶液中における腐食分極特性を評価することができる。しかし、ここで与えられている電気的物性値は、腐食環境のみから与えられる条件であり、腐食に伴う腐食生成物形成の影響は考慮されていない。   In Patent Document 1 and Patent Document 2, the corrosive medium in the model is analyzed as Laplace field according to the Laplace equation, and soil is taken as an example of the medium, and the electrical physical property value is given as a specific resistance of 5000 Ω · cm. In the present invention, when the medium is an aqueous solution, the corrosion polarization characteristics in the aqueous solution can be evaluated if the electric conductivity of the aqueous solution is given. However, the electrical property values given here are conditions given only from the corrosive environment, and the effects of the formation of corrosion products accompanying corrosion are not taken into consideration.

非特許文献1および非特許文献2においても、腐食媒体を海水およびコンクリートとして、それぞれの電気伝導度を与え、ラプラス方程式や物質輸送の式を解いている。しかし、腐食生成物の形成を予測することや、それに伴う腐食媒体や腐食への影響は計算に考慮されていない。   Also in Non-Patent Document 1 and Non-Patent Document 2, the electric conductivity is given to the corrosion medium as seawater and concrete, and the Laplace equation and the equation of mass transport are solved. However, the prediction of the formation of corrosion products and the consequent effects on corrosion media and corrosion are not taken into account in the calculations.

非特許文献3は、水溶液中の亜鉛と鋼の異種金属接触腐食において、物質輸送を考慮して電位分布および電流密度分布を計算している。この文献では、腐食媒体である水溶液中におけるさまざまな種類の化学種の濃度と酸化物や水酸化物の沈殿反応の平衡定数を用いて計算を行うことで、酸化物や水酸化物の生成量と分布を予測している。しかし、腐食生成物形成による金属の水溶液との界面における電気化学特性の変化は考慮されておらず、腐食生成物存在下での金属の腐食速度を正確に見積もることはできなかった。   Non-Patent Document 3 calculates potential distribution and current density distribution in consideration of mass transport in dissimilar metal catalytic corrosion of zinc and steel in an aqueous solution. In this document, the amount of oxides and hydroxides produced is calculated using the concentrations of various types of chemical species in the aqueous solution which is the corrosive medium and the equilibrium constants of the precipitation reactions of oxides and hydroxides. And predict the distribution. However, changes in the electrochemical properties at the interface of the metal with the aqueous solution due to the formation of corrosion products were not considered, and it was not possible to accurately estimate the corrosion rate of the metal in the presence of the corrosion products.

このように従来技術では、金属の腐食生成物が金属表面に堆積することによる腐食速度への影響を数値計算において考慮しておらず、金属の腐食を数値解析によって高精度に予測することができていなかった。   As described above, in the prior art, the influence on the corrosion rate due to the deposition of the metal corrosion products on the metal surface is not considered in the numerical calculation, and the metal corrosion can be predicted with high accuracy by the numerical analysis. It was not.

そこで本発明は、上記課題に鑑み、電解質溶液と接触した金属の腐食を数値解析によってより高精度に予測することが可能な、数値解析による金属の腐食予測方法を提供することを目的とする。   Then, an object of the present invention is to provide a corrosion prediction method of metal by numerical analysis which can predict corrosion of metal in contact with an electrolyte solution with high accuracy by numerical analysis in view of the above-mentioned subject.

上記課題を解決するべく本発明者らは、金属の腐食生成物が金属表面に堆積することによる腐食速度への影響を数値計算において考慮することに着目した。腐食生成物は絶縁性であることから、腐食生成物の形成により金属表面の溶解に必要な過電圧が大きくなることに着目して鋭意検討を重ねた。その結果、金属表面に形成する腐食生成物を考慮して、金属と電解質溶液との界面を流出入する電流密度を補正して境界条件として使用することで、実際に腐食生成物の形成を伴う場合の電位分布や電流密度分布を適切に予測することができるということに想到し、本発明を完成するに至った。   In order to solve the above problems, the present inventors focused attention on the consideration of the influence on the corrosion rate due to the deposition of metal corrosion products on the metal surface in numerical calculation. Since the corrosion product is insulating, the formation of the corrosion product has focused on the fact that the overvoltage necessary for the dissolution of the metal surface is increased. As a result, in consideration of the corrosion products formed on the metal surface, the current density flowing in and out of the interface between the metal and the electrolyte solution is corrected and used as a boundary condition, which actually involves the formation of corrosion products. In light of the fact that the potential distribution and the current density distribution of the case can be properly predicted, the present invention has been completed.

上記知見に基づき完成された本発明の要旨構成は以下のとおりである。
(1)電解質溶液と接触した金属の腐食を数値解析によって予測する方法であって、
電解質溶液中における金属表面の電位Eと電流密度iとの関係である分極曲線を測定する工程と、
前記分極曲線における前記電流密度の値を小さくした補正分極曲線を得る工程と、
前記補正分極曲線を境界条件として、前記金属と前記電解質溶液とが接触した系における所定時刻での前記電解質溶液中の電位分布を数値計算により求める工程と、
を有することを特徴とする数値解析による金属の腐食予測方法。
The essential features of the present invention completed based on the above findings are as follows.
(1) A method of predicting corrosion of a metal in contact with an electrolyte solution by numerical analysis,
Measuring a polarization curve which is the relationship between the potential E of the metal surface in the electrolyte solution and the current density i;
Obtaining a corrected polarization curve in which the value of the current density in the polarization curve is reduced;
Obtaining the potential distribution in the electrolyte solution at a predetermined time in a system in which the metal and the electrolyte solution are in contact, by using the corrected polarization curve as a boundary condition by numerical calculation;
The metal corrosion prediction method by numerical analysis characterized by having.

(2)前記分極曲線を、前記電流密度iを前記電位Eの関数として表わしたi=f(E)としたとき、前記補正分極曲線を、i=α×f(E),0.0010≦α<1.000とする、上記(1)に記載の数値解析による金属の腐食予測方法。   (2) Assuming that the polarization curve is i = f (E) where the current density i is expressed as a function of the potential E, the corrected polarization curve is i = α × f (E), 0.0010 ≦ α < The corrosion prediction method of metal by numerical analysis as described in the above (1), which is 1.000.

(3)前記金属の表面上の単位領域あたりに生成する腐食生成物の生成量pを数値計算により求める工程をさらに有し、
前記分極曲線を、前記電流密度iを前記電位Eの関数として表わしたi=f(E)としたとき、前記補正分極曲線を、i=β×f(E),β=g(p)かつ0.0010≦β<1.000とする、上記(1)に記載の数値解析による金属の腐食予測方法。
(3) The method further includes the step of determining the generation amount p of the corrosion product generated per unit area on the surface of the metal by numerical calculation,
Assuming that the polarization curve is i = f (E) where the current density i is expressed as a function of the potential E, the corrected polarization curve is i = β × f (E), β = g (p) and The corrosion prediction method of metal by numerical analysis as described in the above (1), wherein 0.0010 ≦ β <1.000.

(4)前記所定時刻での前記電解質溶液中の電位分布から、前記所定時刻での前記電解質溶液中の電流密度分布を数値計算により求める工程をさらに有する、上記(1)〜(3)のいずれか一項に記載の数値解析による金属の腐食予測方法。   (4) Any one of the above (1) to (3), further including the step of obtaining the current density distribution in the electrolyte solution at the predetermined time by numerical calculation from the potential distribution in the electrolyte solution at the predetermined time Method of predicting corrosion of metal by numerical analysis as described in paragraph (1).

(5)前記電解質溶液中の電流密度分布のうち、前記電解質溶液中の前記金属との界面近傍における電流密度を用いて、ファラデーの法則により、前記所定時刻での前記金属の腐食量を計算する工程をさらに有する、上記(4)に記載の数値解析による金属の腐食予測方法。   (5) Of the current density distribution in the electrolyte solution, using the current density in the vicinity of the interface with the metal in the electrolyte solution, the amount of corrosion of the metal at the predetermined time is calculated according to Faraday's law. The metal corrosion prediction method by numerical analysis as described in said (4) which further has a process.

(6)前記金属が、亜鉛、鉄、アルミ、銅、及びニッケルから選択される一種以上の金属、又は該金属を主成分とする合金である、上記(1)〜(5)のいずれか一項に記載の数値解析による金属の腐食予測方法。   (6) Any one of the above (1) to (5), wherein the metal is one or more metals selected from zinc, iron, aluminum, copper and nickel, or an alloy containing the metal as a main component Method of predicting corrosion of metal by numerical analysis described in paragraph.

(7)前記腐食の形態が、二種の金属が接触し、金属間の電位差によって一方の金属の腐食が加速される異種金属接触腐食である、上記(1)〜(6)のいずれか一項に記載の数値解析による金属の腐食予測方法。   (7) Any one of the above-mentioned (1) to (6), wherein the form of the corrosion is contact corrosion of dissimilar metals in which two metals are in contact and the corrosion of one metal is accelerated by the potential difference between the metals. Method of predicting corrosion of metal by numerical analysis described in paragraph.

(8)前記二種の金属が、亜鉛又は亜鉛めっきと、鉄又は鋼との組み合わせである、上記(7)に記載の数値解析による金属の腐食予測方法。   (8) The method of predicting metal corrosion by numerical analysis according to (7), wherein the two metals are a combination of zinc or zinc plating and iron or steel.

(9)上記(1)〜(8)のいずれか一項の数値解析による金属の腐食予測方法によって耐食性を予測して、材料を選定することを特徴とする鋼構造物の設計方法。   (9) A method for designing a steel structure, characterized in that corrosion resistance is predicted by the method of predicting corrosion of a metal according to any one of the above (1) to (8), and the material is selected.

(10)上記(1)〜(8)のいずれか一項の数値解析による金属の腐食予測方法によって耐食性を予測して、防錆性能を設計することを特徴とする鉄鋼材料の設計方法。   (10) A method of designing a steel material, wherein corrosion resistance is predicted by the method of predicting corrosion of a metal according to any one of the above-mentioned numerical analysis (1) to (8) to design anticorrosion performance.

(11)コンピュータに、上記(1)〜(8)のいずれか一項の数値解析による金属の腐食予測方法を実行させる腐食予測プログラム。   (11) A corrosion prediction program that causes a computer to execute a method for predicting metal corrosion by numerical analysis according to any one of (1) to (8) above.

本発明の数値解析による金属の腐食予測方法によれば、金属の腐食生成物が金属表面に堆積することによる腐食速度への影響を考慮した数値計算を行うので、電解質溶液と接触した金属の腐食を数値解析によってより高精度に予測することが可能となる。   According to the method of predicting corrosion of metal by numerical analysis of the present invention, since the numerical calculation taking into consideration the influence on the corrosion rate due to the deposition of the corrosion product of the metal on the metal surface is performed, the corrosion of the metal in contact with the electrolyte solution It is possible to predict with higher accuracy by numerical analysis.

本発明の一実施形態による、数値解析による金属の腐食予測方法のフローチャートである。3 is a flowchart of a method of predicting corrosion of a metal by numerical analysis according to an embodiment of the present invention. 2つの金属の異種金属接触腐食の連続体モデルの一例を示す図である。It is a figure which shows an example of the continuum model of the dissimilar metal contact corrosion of two metals. 金属腐食生成物の形成を説明する図である。It is a figure explaining formation of a metal corrosion product. 実施例1で用いた、亜鉛と鉄の異種金属接触腐食のモデル形状を示す図である。It is a figure which shows the model shape of the dissimilar metal contact corrosion of zinc and iron which were used in Example 1. FIG. (a)は、実施例1で行った、亜鉛と鉄の異種金属接触腐食の実験の模式上面図であり、(b)は(a)のA−A’断面図である。(A) is a model top view of the experiment of the dissimilar metal contact corrosion of zinc and iron performed in Example 1, (b) is an A-A 'sectional view of (a). 実施例2で行った、亜鉛と鉄の異種金属接触腐食のモデル形状を示す図である。It is a figure which shows the model shape of the dissimilar metal contact corrosion of zinc and iron which were performed in Example 2. FIG.

本発明は、電解質溶液と接触した金属の腐食を数値解析によって予測する方法である。その一実施形態を、図1〜3を参照して説明する。   The present invention is a method of predicting corrosion of a metal in contact with an electrolyte solution by numerical analysis. One embodiment is described with reference to FIGS.

図1は、本発明の一実施形態による、数値解析による金属の腐食予測方法のフローチャートである。図2は、このような数値解析を適用するための、金属と電解質溶液とが接触した系のモデル図であり、2つの金属A,Bが接触し電気的に短絡した状態の上に電解質溶液が存在する異種金属接触腐食のモデルの一例を示している。   FIG. 1 is a flowchart of a method of predicting corrosion of metal by numerical analysis according to an embodiment of the present invention. FIG. 2 is a model diagram of a system in which a metal and an electrolyte solution are in contact for applying such numerical analysis, and the electrolyte solution is in a state in which two metals A and B are in contact and electrically shorted. Shows an example of a model of heterogeneous metal contact corrosion in which

図2に示すモデルでは、金属と、この金属に接触している電解質溶液の薄膜を、これらの断面において2次元の格子状の領域(以下、「セル」という。)に区切り、境界要素法や有限要素法などを用いて各セル中の電位、電流密度、化学種の濃度などを計算して、腐食量や化合物の沈殿反応を予測する。あるいは、金属及び電解質溶液の薄膜を、3次元の微小な立方体の領域に区画して、これをセルとしてもよい。なお、金属の腐食は、電解質溶液中の電位分布を求めることにより予測できるため、金属はセルに区切らず、電解質溶液のみをセルに区切ることでもよい。以下、計算手順の典型的な例を説明する。   In the model shown in FIG. 2, a thin film of a metal and an electrolyte solution in contact with the metal is divided into two-dimensional lattice-like regions (hereinafter referred to as "cells") in these cross sections, and the boundary element method or The potential, current density, concentration of chemical species, etc. in each cell are calculated using the finite element method etc. to predict the amount of corrosion and the precipitation reaction of the compound. Alternatively, thin films of metal and electrolyte solution may be partitioned into three-dimensional microcube regions, which may be used as cells. Note that since metal corrosion can be predicted by determining the potential distribution in the electrolyte solution, the metal may not be divided into cells, and only the electrolyte solution may be divided into cells. Hereinafter, a typical example of the calculation procedure will be described.

まず、ステップS1において、金属と腐食媒体となる電解質溶液の形状を設定し、電解質溶液中の化学種の初期濃度と物性値を設定する。物性値は、化学種の物質輸送を計算するために用いる拡散係数や、イオンの電荷などである。   First, in step S1, the shapes of the metal and the electrolyte solution to be a corrosive medium are set, and the initial concentrations and physical property values of chemical species in the electrolyte solution are set. Physical property values include the diffusion coefficient used to calculate the transport of chemical species and the charge of ions.

次に、ステップS2において、数値解析に用いる境界条件を設定する。ここで、金属と電解質溶液との界面における境界条件としては、従来、電解質溶液中における金属表面の電流密度iと電位Eの関数i=f(E)で表される分極曲線を設定していた。これに対して、本実施形態では、この分極曲線における電流密度の値を小さくした補正分極曲線を得て、これを境界条件として用いる。詳細については後述する。   Next, in step S2, boundary conditions used for numerical analysis are set. Here, as boundary conditions at the interface between the metal and the electrolyte solution, conventionally, a polarization curve represented by a function i = f (E) of the current density i of the metal surface in the electrolyte solution and the potential E was set. . On the other hand, in the present embodiment, a corrected polarization curve in which the value of the current density in the polarization curve is reduced is obtained and used as a boundary condition. Details will be described later.

次に、ステップS3において、ある時刻tでの電解質溶液中の電位分布を数値計算により求める。数値計算には、(1)式に示すラプラスの式、又は式(2)に示すNernst−Plankの式を解く。

Figure 0006544402
Figure 0006544402
ここで、Фは電位、Cx, Dx, zx, ux, Rx はそれぞれ化学種xの濃度、拡散係数、価数、移動度および反応量を表し、Fはファラデー定数を表す。 Next, in step S3, the potential distribution in the electrolyte solution at a certain time t is determined by numerical calculation. For numerical calculation, the Laplace equation shown in equation (1) or the Nernst-Plank equation shown in equation (2) is solved.
Figure 0006544402
Figure 0006544402
Here, Ф represents the potential, C x , D x , z x , u x , and R x each represent the concentration of the chemical species x, diffusion coefficient, valence, mobility and reaction amount, and F represents the Faraday constant.

このとき、金属と電解質溶液との界面では、上記の補正分極曲線を境界条件として、電解質溶液の気相との界面、及び電解質溶液の端部では、電流の流出入がないという条件を境界条件として、数値計算を行う。   At this time, at the interface between the metal and the electrolyte solution, the above-mentioned corrected polarization curve is taken as the boundary condition, and at the interface between the electrolyte solution and the gas phase, and at the end of the electrolyte solution, no current flows in and out. Perform numerical calculation as.

式(1)を離散化して解くことによって、ある時刻tでの各セルでの電位が算出され、すなわち、ある時刻tでの電解質溶液中の電位分布を得ることができる。なお、金属もセルに区切る場合には、当該計算により金属中の各セルの電位、すなわち金属中の電位分布も得ることができる。   By discretizing equation (1) and solving, the potential in each cell at a certain time t can be calculated, that is, the potential distribution in the electrolyte solution at a certain time t can be obtained. In the case where the metal is divided into cells, the potential of each cell in the metal, that is, the potential distribution in the metal can also be obtained by the calculation.

また、式(2)に示す物質輸送に関するNernst−Plankの式を解くためには、電解質溶液中の各セルにおける各イオン及び分子について、(1)式を成り立たせると同時に、電気的中性条件の式を加えることで連立方程式とする。この連立方程式を解くことにより、ある時刻tでの各セルの電位に加えて、各セルのイオンや分子の濃度も計算結果として導き出される。この結果、ある時刻tでの電解質溶液中の電位分布に加えて、化学種の濃度分布を得ることができる。   In addition, in order to solve the Nernst-Plank equation for mass transport shown in equation (2), it is necessary to satisfy equation (1) for each ion and molecule in each cell in the electrolyte solution, as well as electrically neutral conditions. It becomes a simultaneous equation by adding the equation of. By solving the simultaneous equations, in addition to the potentials of the cells at a certain time t, the concentrations of ions and molecules of the cells are also derived as calculation results. As a result, in addition to the potential distribution in the electrolyte solution at a certain time t, the concentration distribution of chemical species can be obtained.

次に、ステップS4において、ある時刻tでの電解質溶液中の電位分布から、当該時刻tでの電解質溶液中の電流密度分布を数値計算により求める。具体的には、式(3)のオームの法則により、各セルでの電流密度が算出され、すなわち、ある時刻tでの電解質溶液中の電流密度分布を得ることができる。ここでσは電解質溶液の電気伝導度を表す。なお、電気伝導度σは化学種の濃度の関数である。電位分布を式(2)により求める場合には、化学種の濃度分布も得られている。そのため、セルごとの化学種の濃度から求めたセルごとの電気伝導度を、式(3)に適用する。電位分布を式(1)により求める場合には、溶液中の化学種の移動は考慮せず、溶液の濃度から求めた一律な電気伝導度を各セルの電気伝導度として、式(3)に適用する。なお、金属中の電位分布が得られている場合には、式(3)によって金属中の電流密度分布も求めることができる。

Figure 0006544402
Next, in step S4, from the potential distribution in the electrolyte solution at a certain time t, the current density distribution in the electrolyte solution at that time t is determined by numerical calculation. Specifically, the current density in each cell is calculated according to Ohm's law of equation (3), that is, the current density distribution in the electrolyte solution at a certain time t can be obtained. Here, σ represents the electrical conductivity of the electrolyte solution. The electrical conductivity σ is a function of the concentration of chemical species. When the potential distribution is determined by equation (2), the concentration distribution of chemical species is also obtained. Therefore, the electric conductivity for each cell obtained from the concentration of chemical species for each cell is applied to equation (3). When the potential distribution is determined by equation (1), the movement of chemical species in the solution is not taken into consideration, and the uniform electrical conductivity determined from the concentration of the solution is defined as the electrical conductivity of each cell. Apply In the case where the potential distribution in the metal is obtained, the current density distribution in the metal can also be determined by the equation (3).
Figure 0006544402

なお、ここでは典型的な電位及び電流密度の計算方法を示したが、本発明において、電解質溶液をポテンシャル場とみなして電位及び電流密度を計算によって求める方法は、これに限定されるものではない。   Although a typical calculation method of potential and current density is shown here, in the present invention, the method of determining the potential and current density by calculating the electrolyte solution as a potential field is not limited thereto. .

ステップS5では、上記で数値計算を行った時刻tが、予め設定した時刻tsetを超えているか否かを判定する。設定時刻tsetを超えていない場合には、Δtを加えてステップS3に戻り、新たな時刻tでの電解質溶液中の電位分布及び電流密度分布の計算を行う。設定時刻tsetを超えた場合には、ステップS6に進む。 In step S5, it is determined whether the time t at which the numerical calculation has been performed exceeds the preset time t set . If it does not exceed the set time t set , Δt is added and the process returns to step S3 to calculate the potential distribution and current density distribution in the electrolyte solution at a new time t. If it exceeds the set time t set , the process proceeds to step S6.

ステップS6では、電解質溶液中の電流密度分布のうち、電解質溶液中の金属との界面近傍における電流密度を用いて、式(4)に示すファラデーの法則により、設定時刻tsetでの金属の腐食量を計算する。ここでnおよびzは腐食により溶解した金属(化学種)の物質量および価数であり、tは時間である。なお、金属中の電流密度分布が得られている場合には、金属中の電解質溶液との界面近傍における電流密度を用いてもよい。すなわち、金属/電解質溶液境界近傍の金属または電解質溶液の電流密度を用いればよい。ここで、「界面近傍」とは、電解質溶液と金属との境界面を出入りする電流密度と同等と見なせる電流密度が得られる範囲を意味するものとし、具体的には、前記境界面から10mm以内、さらに好適には1mm以内の電解質溶液または金属の領域とする。

Figure 0006544402
In step S6, of the current density distribution in the electrolyte solution, the current density in the vicinity of the interface with the metal in the electrolyte solution is used to corrode the metal at the set time t set according to Faraday's law shown in equation (4). Calculate the quantity. Here, n and z are the amount and the valence of the metal (chemical species) dissolved by corrosion, and t is time. When the current density distribution in the metal is obtained, the current density near the interface with the electrolyte solution in the metal may be used. That is, the current density of the metal or electrolyte solution near the metal / electrolyte solution boundary may be used. Here, “in the vicinity of the interface” means a range in which a current density that can be considered equivalent to the current density flowing in and out of the interface between the electrolyte solution and the metal can be obtained, specifically, within 10 mm from the interface More preferably, it is an area of the electrolyte solution or metal within 1 mm.
Figure 0006544402

なお、実際の計算に際しては、ステップS3及びS4を繰り返したことにより、種々の時刻において、電解質溶液中の金属との界面近傍における電流密度が求まっているので、式(4)を用いて微小時間毎に腐食量を求めて、これを積算することにより、所定時間経過後の腐食量と、金属表面内での腐食量の分布を得ることができる。   In the actual calculation, by repeating steps S3 and S4, the current density in the vicinity of the interface with the metal in the electrolyte solution is obtained at various times, so that the minute time is calculated using equation (4). The amount of corrosion is determined for each time, and this amount is integrated to obtain the amount of corrosion after a predetermined time has elapsed and the distribution of the amount of corrosion within the metal surface.

最後に、ステップS7において、各種計算結果を出力して、本方法を終了とする。   Finally, in step S7, various calculation results are output, and the method ends.

ここで、上記で数値計算によって求めた電位分布、電流密度分布、及び腐食量は、その時刻までに形成した腐食生成物の影響を強く受ける。腐食生成物は、酸化物や水酸化物など絶縁体や半導体の電気的性質を有するものが多く、金属や電解質溶液に比べて電気伝導度が極めて低い。このような物質が電解質溶液中に生成・堆積することで、電解質溶液および金属中の電位分布や電流密度分布が変化する。その結果として、その時間以降の腐食反応や腐食生成物の形成も変化する。   Here, the potential distribution, the current density distribution, and the amount of corrosion obtained by the numerical calculation above are strongly influenced by the corrosion products formed up to that time. Many corrosion products have electrical properties of insulators and semiconductors such as oxides and hydroxides, and they have extremely low electrical conductivity compared to metals and electrolyte solutions. Formation and deposition of such a substance in the electrolyte solution changes the potential distribution and current density distribution in the electrolyte solution and the metal. As a result, the corrosion reaction and formation of corrosion products after that time also change.

そこで本発明では、このような腐食現象に生成した腐食生成物が及ぼす影響を再現した数値解析による金属の腐食予測方法を提供する。   Therefore, the present invention provides a method of predicting metal corrosion by numerical analysis that reproduces the influence of the generated corrosion products on such a corrosion phenomenon.

図3に、金属腐食生成物の形成を説明する図を示す。ここで、金属Aが腐食により金属イオンA+を溶液中に生成する場合、時間経過とともにA+の濃度が高くなり、やがて酸化物あるいは水酸化物の溶解度積との関係から、酸化物AOあるいは水酸化物A(OH)を形成するとする。先に述べたように、腐食生成物の多くは、絶縁体あるいは半導体であり、腐食前の金属に比べると電気化学的に反応不活性である。よって、腐食生成物が堆積していない金属表面と電解質溶液との界面と、腐食生成物が堆積した金属表面と電解質溶液との界面とでは、その腐食反応性が異なる。 FIG. 3 shows a diagram illustrating the formation of metal corrosion products. Here, when metal A generates metal ion A + in the solution by corrosion, the concentration of A + increases with time, and from the relationship with the solubility product of oxide or hydroxide, oxide AO or Suppose that hydroxide A (OH) is formed. As mentioned earlier, many of the corrosion products are insulators or semiconductors, which are electrochemically reactive as compared to the metal before corrosion. Therefore, the corrosion reactivity differs between the interface between the metal surface on which the corrosion product is not deposited and the electrolyte solution and the interface between the metal surface on which the corrosion product is deposited and the electrolyte solution.

そこで、数値計算によって電解質溶液中の電位Φの分布及び電流密度iの分布を計算する際に、境界条件として用いる分極曲線に、腐食生成物の生成を考慮した補正を行う。これにより、実際に観察される腐食現象に近い電位分布や電流密度分布を得ることができる。   Therefore, when calculating the distribution of the potential Φ and the distribution of the current density i in the electrolyte solution by numerical calculation, the polarization curve used as the boundary condition is corrected in consideration of the formation of a corrosion product. This makes it possible to obtain a potential distribution or current density distribution close to the corrosion phenomenon actually observed.

すなわち、ステップS2では、まず、電解質溶液中における金属表面の電流密度iと電位Eとの関係である分極曲線[i=f(E)]を測定する。そして、分極曲線における電流密度の値を小さくした補正分極曲線を作成する。具体的には、補正分極曲線を、i=α×f(E),0.0010≦α<1.000とする。そして、上記分極曲線の代わりに、この補正分極曲線を、金属と電解質溶液との界面における境界条件として用いる。   That is, in step S2, first, a polarization curve [i = f (E)] which is a relationship between the current density i of the metal surface in the electrolyte solution and the potential E is measured. Then, a corrected polarization curve is created in which the value of the current density in the polarization curve is reduced. Specifically, the corrected polarization curve is set to i = α × f (E), 0.0010 ≦ α <1.000. Then, instead of the polarization curve, this corrected polarization curve is used as a boundary condition at the interface between the metal and the electrolyte solution.

ここで、αは腐食生成物の形態や電気的性質に依存する因子である。αを0.0010未満とした場合は、腐食反応の電流密度が小さくなり、腐食生成物による下地金属の腐食抑制効果が大きい想定となる。実際には腐食生成物が物理的に破壊・損傷されるために、腐食速度がそこまで小さく抑制されることはなく、実際の腐食現象と数値計算による乖離が大きくなる。αが1.000の場合は、その溶液中で測定した分極曲線のままに相当し、αが1.000超えでは、腐食生成物の形成が金属の腐食を促進することを意味するが、いずれの場合も腐食生成物堆積による腐食効果が再現されない。この観点からより好適なαの範囲は0.0010以上0.800以下であり、より好適な範囲は0.0100以上0.500以下である。   Here, α is a factor depending on the form and electrical properties of the corrosion product. When α is less than 0.0010, the current density of the corrosion reaction becomes small, and it is assumed that the corrosion inhibition effect of the base metal by the corrosion product is large. In fact, since the corrosion products are physically broken or damaged, the corrosion rate is not suppressed to such a small level, and the difference between the actual corrosion phenomenon and the numerical calculation becomes large. When α is 1.000, it corresponds to the polarization curve measured in the solution, and when α is more than 1.000, it means that the formation of corrosion product promotes the corrosion of metal, but in any case corrosion Corrosion effects due to product deposition are not reproduced. The more preferable range of α from this viewpoint is 0.0010 or more and 0.800 or less, and the more preferable range is 0.0100 or more and 0.500 or less.

分極曲線の測定は、数値解析の対象とする金属と同じ金属を用いて行う必要があり、さらに、数値解析の対象とする電解質溶液の電解質濃度を同じ電解質濃度の電解質溶液中で測定を行うことが好ましい。   It is necessary to measure the polarization curve using the same metal as the target metal of numerical analysis, and further measure the electrolyte concentration of the electrolyte solution to be target of numerical analysis in the electrolyte solution of the same electrolyte concentration. Is preferred.

境界条件として用いる分極特性は、内部分極曲線及び外部分極曲線のいずれでも構わない。内部分極曲線は実験では得られないが、外部分極曲線から外挿して求めることができ、より詳細な電極反応を境界条件として与えられるので好適である。   The polarization characteristic used as the boundary condition may be either an internal polarization curve or an external polarization curve. Although the internal polarization curve can not be obtained by experiment, it can be determined by extrapolating from the external polarization curve, and is more preferable because more detailed electrode reactions can be given as boundary conditions.

生成した腐食生成物の量に応じて金属表面の腐食生成物の被覆率や緻密さは異なるので、金属表面の場所によって、境界条件として用いる補正分極特性を最適化することが好ましい。すなわち、境界条件とする補正分極曲線を、境界となるセルごとに、当該セルにおける腐食物の生成量を考慮して設定することが好ましい。そこで、分極曲線の別の補正方法として、金属の表面上の単位領域あたりに生成する腐食生成物の生成量pを数値計算により求め、補正分極曲線をi=β×f(E),β=g(p)かつ0.0010≦β<1.000とする方法が挙げられる。   Since the coverage and density of the corrosion products on the metal surface vary depending on the amount of corrosion products formed, it is preferable to optimize the correction polarization characteristics used as boundary conditions depending on the location of the metal surface. That is, it is preferable to set the correction polarization curve to be the boundary condition in consideration of the generation amount of the corrosive substance in the cell, which is the boundary. Therefore, as another correction method of the polarization curve, the generation amount p of the corrosion product generated per unit area on the surface of the metal is determined by numerical calculation, and the correction polarization curve is i = β × f (E), β = There is a method of setting g (p) and 0.0010 ≦ β <1.000.

ここで、生成量pは、腐食生成物の体積、重量、物質量、及び厚さ一定とした時の面積率などを用いることができる。また、複数の種類の腐食生成物が同時に生成する場合には、特定の腐食生成物のみの総量を用いても良いし、全ての腐食生成物の総量として計算しても良い。但し、βの範囲は、αと同様の理由で、0.0010≦β<1.000とする。   Here, as the generation amount p, it is possible to use the volume, weight, amount of substance of the corrosion product, and the area ratio when the thickness is constant. When a plurality of types of corrosion products are simultaneously generated, the total amount of only specific corrosion products may be used, or may be calculated as the total amount of all corrosion products. However, the range of β is 0.0010 ≦ β <1.000 for the same reason as α.

例えば、β=1−Vc/V0とすることができる。すなわち、腐食生成物が多く生成しているセルほど、βが小さくなり、分極曲線における電流密度の値を小さくする。
0:電解質溶液中の金属との界面に位置する任意のセルの面積又は体積(単位面積又は単位体積)
c:当該セル中の腐食生成物が占める面積又は体積
For example, β = 1−V c / V 0 can be set. That is, as the cell in which a large amount of corrosion product is generated, β becomes smaller, and the value of the current density in the polarization curve is made smaller.
V 0 : The area or volume (unit area or unit volume) of any cell located at the interface with the metal in the electrolyte solution
V c : Area or volume occupied by corrosion products in the cell

c/V0の計算方法を以下に説明する。まず計算によるセルj内における腐食生成物の生成総量(gまたはmol)とこれらの腐食生成物の密度の関係から体積Vcを計算する。すなわち、例えば質量から計算する場合には、Vc=m/d、により計算する。ここでVcはセルjに占める腐食生成物の体積(cm3)、mは腐食生成物の生成質量(g)、dは腐食生成物の密度(g/cm3)を表す。腐食生成物が多数の成分からなる場合は、全ての成分について計算しても良いが、腐食生成物の主成分となっている酸化物や水酸化物のみについて計算してもよい。この値を元々水溶液のみが占めていた初期のセルjの体積V0で割ることで、Vc/V0を計算する。 The calculation method of V c / V 0 will be described below. First, the volume V c is calculated from the relationship between the calculated total amount (g or mol) of corrosion products in the cell j and the density of these corrosion products. That is, for example, in the case of calculation from mass, it is calculated by V c = m / d. Here, V c represents the volume (cm 3 ) of the corrosion product occupying the cell j, m represents the mass of the corrosion product (g), and d represents the density of the corrosion product (g / cm 3 ). When a corrosion product consists of many components, although it may calculate about all the components, it may calculate about only the oxide and hydroxide which are main components of a corrosion product. By dividing this value by the volume V 0 of the initial cell j originally occupied only by the aqueous solution, V c / V 0 is calculated.

境界条件は、逐次計算の時間インターバルに関わらず一定の条件としてもよい。この場合、ある特定の時間において求めたβを使用する。しかし、形成した腐食生成物の影響は刻々と変化するため、逐次計算の時間インターバル毎に新しい条件を設定することが望ましい。すなわち、逐次計算における時間ステップごとにβが計算できる。そこで、各時間ステップにおける計算は、直前のステップで求められたβを使用して、補正分極曲線を得るものとする。   The boundary condition may be a constant condition regardless of the time interval of sequential calculation. In this case, β determined at a specific time is used. However, since the influence of the formed corrosion product changes constantly, it is desirable to set a new condition for each time interval of sequential calculation. That is, β can be calculated for each time step in sequential calculation. Therefore, the calculation at each time step is to obtain a corrected polarization curve using β obtained in the previous step.

本発明の数値解析による金属の腐食予測方法を適用する金属は、特に限定されないが、亜鉛、鉄、アルミ、銅、及びニッケルから選択される一種以上の金属、又は該金属を主成分とする合金を好適に適用できる。また、本発明の数値解析による金属の腐食予測方法を、図2に示したような異種金属接触腐食に適用すると特に有効である。この場合、金属Aと電解質溶液との界面では、金属Aの補正分極曲線を境界条件とし、金属Bと電解質溶液との界面では、金属Bの補正分極曲線を境界条件とする。異種金属接触腐食の例としては、亜鉛又は亜鉛めっきと、鉄又は鋼との組み合わせが挙げられる。   The metal to which the method for predicting corrosion of a metal according to the numerical analysis of the present invention is applied is not particularly limited, but one or more metals selected from zinc, iron, aluminum, copper and nickel, or an alloy containing the metal as a main component Can be suitably applied. Further, it is particularly effective to apply the method of predicting corrosion of metal by numerical analysis of the present invention to contact corrosion by dissimilar metals as shown in FIG. In this case, the corrected polarization curve of metal A is taken as the boundary condition at the interface between metal A and the electrolyte solution, and the corrected polarization curve of metal B is taken as the boundary condition at the interface between metal B and the electrolyte solution. Examples of dissimilar metal contact corrosion include combinations of zinc or zinc plating with iron or steel.

腐食生成物の金属表面への堆積は、電解質溶液中よりも大気環境で明瞭であり、その影響も大きい。従って、金属の大気腐食を予測するために、金属表面上の電解質溶液の厚さが10mm未満である数値計算に好適である。   The deposition of corrosion products on metal surfaces is clearer in the atmospheric environment than in the electrolyte solution and the effect is also greater. Therefore, in order to predict atmospheric corrosion of metal, it is suitable for numerical calculation in which the thickness of the electrolyte solution on the metal surface is less than 10 mm.

鋼構造物の設計において、上記説明した数値解析による金属の腐食予測方法によって、耐食性を予測して、材料を選定することが好適である。すなわち、ある金属材料に関して、本発明による数値計算で予測される腐食量が、鋼構造物の要求寿命に対して十分小さいとみなせる場合、この金属材料を当該鋼構造物の材料として使用することができる。   In the design of a steel structure, it is preferable to select a material by predicting the corrosion resistance by the method of predicting corrosion of a metal by the above-described numerical analysis. That is, when the amount of corrosion predicted by the numerical calculation according to the present invention can be considered to be sufficiently smaller than the required life of the steel structure with respect to the metal material, using the metal material as the material of the steel structure it can.

また、鉄鋼材料の設計方法において、上記説明した数値解析による金属の腐食予測方法によって耐食性を予測して、防錆性能を設計することが好適である。鋼材の成分や組織を変えることで、分極曲線や電解質中に溶出する成分も変化するため、計算により予測される金属の腐食量も異なる。すなわち、本発明による数値計算で予測される金属の腐食量が、鋼材の要求寿命に対して十分小さくなるように、鋼材の成分や組織を設計することができる。   Further, in the method of designing a steel material, it is preferable to design the anticorrosion performance by predicting the corrosion resistance by the method of predicting corrosion of a metal by the above-described numerical analysis. By changing the composition and structure of the steel material, the polarization curve and the component eluted in the electrolyte also change, so the amount of corrosion of the metal predicted by calculation also differs. That is, the composition and structure of the steel material can be designed such that the corrosion amount of the metal predicted by the numerical calculation according to the present invention becomes sufficiently smaller than the required life of the steel material.

(プログラム)
本発明の目的は、前述した実施形態の各工程を実現するソフトウェアのプログラムコードを記録した記憶媒体を、システムあるいは装置に供給し、そのシステムあるいは装置のコンピュータ(またはCPUやMPU)が記憶媒体に格納されたプログラムコードを読み出し実行することによっても、達成される。この場合、記憶媒体から読み出されたプログラムコード自体が前述した実施形態の機能を実現することになり、そのプログラムおよびプログラムコードを記憶した記憶媒体は、本発明を構成することになる。
(program)
An object of the present invention is to provide a system or apparatus with a storage medium storing a program code of software for realizing each process of the above-described embodiment, and a computer (or CPU or MPU) of the system or apparatus uses the storage medium. It is also achieved by reading and executing the stored program code. In this case, the program code itself read out from the storage medium implements the functions of the above-described embodiments, and the storage medium storing the program and the program code constitutes the present invention.

ここでプログラムコードを記憶する記憶媒体としては、例えば、フレキシブルディスク、ハードディスク、ROM、RAM、磁気テープ、不揮発性のメモリカード、CD−ROM、CD−R、DVD、光ディスク、光磁気ディスク、MOなどが考えられる。また、LAN(ローカル・エリア・ネットワーク)やWAN(ワイド・エリア・ネットワーク)などのコンピュータネットワークを、プログラムコードを供給するために用いることができる。   Here, as a storage medium for storing the program code, for example, a flexible disk, hard disk, ROM, RAM, magnetic tape, non-volatile memory card, CD-ROM, CD-R, DVD, optical disk, magneto-optical disk, MO, etc. Is considered. Also, a computer network such as a LAN (local area network) or a WAN (wide area network) can be used to supply the program code.

(実施例1)
厚さ0.01,0.05または0.1mmの0.6,1.2,または2.0mol/LのNaCl水溶液に表面を覆われた互いに接触した亜鉛と鉄の異種金属接触腐食を数値計算により予測した。図4に本実施例で用いた形状のモデル図を示す。領域ΩはNaCl水溶液の領域であり、化学種の初期濃度としてNa+およびCl-の濃度を0.6,1.2,2.0mol/Lとし、この溶液中において考慮すべき化学種の初期濃度および拡散係数を表1のように設定した。領域Ωでは、式(2)の物質輸送の式が成り立つと仮定し、それぞれの化学種について水溶液中の濃度勾配による拡散、電荷による泳動を考慮した。ここでは対流の影響は考慮していない。
Example 1
Numerical values of dissimilar metal contact corrosion of zinc and iron in contact with each other covered with 0.6, 1.2 or 2.0 mol / L NaCl aqueous solution with a thickness of 0.01, 0.05 or 0.1 mm It predicted by calculation. FIG. 4 shows a model of the shape used in the present embodiment. The region Ω is the region of the aqueous NaCl solution, and the concentration of Na + and Cl is set to 0.6, 1.2, 2.0 mol / L as the initial concentration of the species, and the initial concentration of the species to be considered in this solution Concentrations and diffusion coefficients were set as shown in Table 1. In the region Ω, it was assumed that the mass transport equation of equation (2) holds, and for each chemical species, diffusion due to concentration gradient in aqueous solution and migration due to charge were considered. The influence of convection is not considered here.

Figure 0006544402
Figure 0006544402

式(2)を解くための境界条件として、計算と同じ濃度のNaCl水溶液中で測定した亜鉛のアノード分極曲線をia_zn = f(Ea_zn)、鉄のカソード分極曲線をic_Fe = f(Ec_Fe)とした時、境界1の境界条件をia_zna × f(Ea_zn)、境界2の境界条件をia_Fec × f(Ea_Fe)とした。その他の境界には、電流の流出入がない(∂Ф/∂n=0:ここでnは単位ベクトルを示す)を境界条件として用いた。 As the boundary conditions for solving equation (2), the anodic polarization curve of zinc measured in the same concentration aqueous NaCl solution as i a _ z n = f (E a _ z n ) and the cathodic polarization curve of iron i c When _ Fe = f (E c _ Fe ), the boundary condition of boundary 1 is i a _ zn = α a × f (E a _ z n ), and the boundary condition of boundary 2 is i a _ Fe = α c × It was f (E a _ Fe ). In the other boundaries, no current flow (∂Ф / ∂Ф n = 0: where n represents a unit vector) was used as the boundary condition.

この条件のもと、時間0から時間60minまで逐次計算を行い、電位分布および電流密度分布を計算するとともに、その時間での化学種の濃度および反応生成物の濃度分布を計算した。   Under this condition, the calculation was sequentially performed from time 0 to time 60 min, and the potential distribution and current density distribution were calculated, and the concentration of chemical species and the concentration distribution of reaction products at that time were calculated.

この異種金属接触腐食の計算では、亜鉛がアノード反応により腐食し、鉄はカソード反応としてその表面で酸素の還元反応が生じると仮定した。亜鉛のアノード反応および鉄上の酸素の還元反応は、それぞれ式(5)および(6)で表わされる。
Zn → Zn2+ + 2e- ・・・・(5)
2H2O + O2 + 4e- → 4OH- ・・・・(6)
In this calculation of heterogeneous metal catalytic corrosion, it was assumed that zinc was corroded by an anodic reaction, and iron was a reduction reaction of oxygen at its surface as a cathodic reaction. The anodic reaction of zinc and the reduction reaction of oxygen on iron are represented by formulas (5) and (6) respectively.
Zn → Zn 2+ + 2e - ···· (5)
2H 2 O + O 2 + 4 e → 4 OH ··· (6)

この反応式に基づき、亜鉛と水溶液との界面における電流密度から、ファラデーの法則を用いてZnの溶解量を計算し、これを計算時間に対して積算することで60min後の亜鉛の腐食量を求めた。   Based on this reaction equation, the amount of dissolution of Zn is calculated using Faraday's law from the current density at the interface between zinc and aqueous solution, and this is integrated with respect to the calculation time to calculate the amount of corrosion of zinc after 60 minutes. I asked.

これらの数値計算結果の妥当性を評価するために、数値計算と同じ条件で腐食実験を行った。図5に腐食実験に用いた10mm×10mm×5mmtの亜鉛と鉄(いずれも純度99.999%)を互いに接触させて固定した試験片の模式図を示す。この試験片の表面に数値計算した条件と同じ濃度、同じ厚さのNaCl水溶液を形成させた。金属表面上にいったん形成させた薄い塩水膜を一定の状態に維持するために、試験片をすみやかに室温、相対湿度をRH98%(0.6M相当)、RH93%(1.2M相当)、RH85%(2.0M相当)に設定した恒温恒湿槽に入れて試験片を腐食させた。   In order to evaluate the validity of these numerical calculation results, corrosion experiments were conducted under the same conditions as the numerical calculation. FIG. 5 shows a schematic view of a test piece in which 10 mm × 10 mm × 5 mmt of zinc and iron (both having a purity of 99.999%) used in the corrosion test are brought into contact with each other and fixed. An aqueous solution of NaCl having the same concentration and the same thickness as the conditions calculated numerically was formed on the surface of the test piece. In order to keep the thin salt water film once formed on the metal surface in a fixed state, the test piece is promptly room temperature, relative humidity is RH 98% (equivalent to 0.6 M), RH 93% (equivalent to 1.2 M), RH 85 The test piece was corroded by placing it in a constant temperature and humidity chamber set to% (equivalent to 2.0 M).

恒温恒湿槽に試験片を60分入れたまま腐食させた後、走査型ケルビンプローブを用いて表面の電位分布を測定した。腐食状態を変化させないように、ケルビンプローブによる計測中も恒温恒湿槽内と同じ温度、相対湿度に維持した。測定終了後、すみやかに試験片を蒸留水で洗浄し、乾燥させた後、図5(b)のA−A’断面図に示す試験片中央部を長手方向に切断して、腐食状態を断面から走査型電子顕微鏡(SEM)で観察し、亜鉛の腐食量を厚さから求めた。   After corroding the test piece in a constant temperature and humidity chamber for 60 minutes, the potential distribution on the surface was measured using a scanning Kelvin probe. The same temperature and relative humidity as in the constant temperature and humidity chamber were maintained during measurement with the Kelvin probe so as not to change the corrosion state. After the measurement is completed, the test piece is promptly washed with distilled water and dried, and then the central portion of the test piece shown in the cross-sectional view taken along line AA 'of FIG. From the above, the amount of corrosion of zinc was determined from the thickness by observing with a scanning electron microscope (SEM).

表2に、計算と実験に用いたNaCl水溶液の条件、計算に用いた腐食生成物の影響を考慮するためのパラメーターとしてZn(アノード)側のαaおよび鉄(カソード)側のαc、これらを境界条件として計算した結果と実験による電位および腐食量の測定結果の比較を示す。電位については、試験片長手方向で亜鉛から鉄の表面を1mmおきに全20点測定し、20点全ての計算した電位が実験結果に対して±50mVの範囲となった場合を○、そうでない場合を×とした。腐食量分布は、20点すべての測定点において(計算の腐食量)/(実験の腐食量)=0.5〜1.5である場合に○、この範囲を外れる場合を×として評価した。本発明の範囲であるNo1から7については、異なる溶液濃度、溶液の厚さに対して高い精度で電位および腐食量の分布が予測できた。しかし、比較例に示すように、αa またはαcのいずれかが、0.0010未満、または1.000よりも大きい場合は、電位および腐食量ともに実験を再現できていない。また、腐食生成物の形成による分極特性の変化を考慮していない、αaまたはαcのいずれかが1.00の場合にも、計算結果と実験結果の乖離が大きく、実験結果を再現することができない。 Table 2 shows the conditions of the NaCl aqueous solution used in calculation and experiment, α a on the Zn (anode) side and α c on the iron (cathode) side as parameters for considering the influence of corrosion products used in the calculation, these We show the comparison of the result of calculation with the boundary condition as the boundary condition and the measurement result of potential and corrosion amount by experiment. Regarding potentials, the surface of zinc to iron was measured every 1 mm in the longitudinal direction of the test piece at all 20 points, and the calculated potential at all 20 points was within the range of ± 50 mV with respect to the experimental results ○, not so The case was marked x. The corrosion amount distribution was evaluated as ○ when the calculated corrosion amount / (experimental corrosion amount) = 0.5 to 1.5 at all 20 measurement points, and x when out of this range. With respect to No. 1 to No. 7 which is the scope of the present invention, the distribution of potential and corrosion amount could be predicted with high accuracy for different solution concentrations and solution thicknesses. However, as shown in the comparative example, in the case where either α a or α c is less than 0.0010 or greater than 1.000, neither the potential nor the corrosion amount can reproduce the experiment. In addition, the difference between the calculation result and the experimental result is large even when either α a or α c is 1.00, which does not take into account the change in polarization characteristics due to the formation of corrosion products, and the experimental result is reproduced I can not do it.

Figure 0006544402
Figure 0006544402

(実施例2)
厚さ0.01または0.1mmの1.0または2.0mol/LのNaCl水溶液に表面を覆われた互いに接触した亜鉛と鉄の異種金属接触腐食を数値計算により予測した。図6に本実施例で用いた形状のモデル図を示す。領域ΩはNaCl水溶液の領域であり、化学種の初期濃度としてNa+およびCl-の濃度を1.0または2.0mol/Lとし、この溶液中において考慮すべき化学種の初期濃度および拡散係数を表3のように設定した。本実施例では、亜鉛および鉄と溶液との境界面を計10境界に区切り、境界1から10とした。亜鉛と鉄の界面における境界線が短いのは、この領域で腐食反応が最も大きく、電位や電流密度の変化が大きいためである。領域Ωでは、式(2)の物質輸送の式が成り立つと仮定し、それぞれの化学種について水溶液中の濃度勾配による拡散、電荷による泳動を考慮した。ここでは対流の影響は考慮していない。
(Example 2)
The heterogeneous metal catalytic corrosion of zinc and iron in contact with each other covered with a 1.0 or 2.0 mol / L NaCl aqueous solution with a thickness of 0.01 or 0.1 mm was predicted by numerical calculation. FIG. 6 shows a model of the shape used in this example. The region Ω is the region of the aqueous NaCl solution, and the concentration of Na + and Cl is 1.0 or 2.0 mol / L as the initial concentration of the species, and the initial concentration and diffusion coefficient of the species to be considered in this solution Were set as shown in Table 3. In this example, the interface between zinc and iron and the solution was divided into 10 boundaries in total, and the boundaries 1 to 10 were made. The short boundary at the interface between zinc and iron is because the corrosion reaction is the largest in this region and the change in potential and current density is large. In the region Ω, it was assumed that the mass transport equation of equation (2) holds, and for each chemical species, diffusion due to concentration gradient in aqueous solution and migration due to charge were considered. The influence of convection is not considered here.

Figure 0006544402
Figure 0006544402

式(2)を解くための境界条件として、計算と同じ濃度のNaCl水溶液中で測定した亜鉛のアノード分極曲線をia_zn = f(Ea_zn)、鉄のカソード分極曲線をic_Fe = f(Ec_Fe)とした時、境界1から5の境界条件をia_zn =β× f(Ea_zn)とし、β=1-Vc/V0として境界条件を決定した。ここで、Vcは、Znの腐食生成物の体積を表し、V0は単位体積を表す。一方、本実施例では鉄系の腐食生成物の形成は考慮せず、境界6から10の境界条件を ic_Fe = f(Ec_Fe)とした。厳密には物質の拡散や泳動によってZnの腐食生成物が鉄上にも形成されるが、その影響は無視する前提で計算を行った。ここで、0.0010 ≦ β < 1.000とし、βの計算値が0.0010を下回る場合には、すべてβを0.0010とすることとした。金属と溶液の界面以外の境界には、電流の流出入がない(∂Ф/∂n=0:ここでnは単位ベクトルを示す)を境界条件として用いた。 As the boundary conditions for solving equation (2), the anodic polarization curve of zinc measured in the same concentration aqueous NaCl solution as i a _ z n = f (E a _ z n ) and the cathodic polarization curve of iron i c Assuming that _ Fe = f (E c _ Fe ), the boundary conditions of boundaries 1 to 5 are i a _ zn = β × f (E a _ z n ), and the boundary condition is β = 1 − V c / V 0 It was determined. Here, V c represents the volume of a corrosion product of Zn, and V 0 represents a unit volume. On the other hand, in the present embodiment, the formation of iron-based corrosion products is not taken into consideration, and the boundary conditions of the boundaries 6 to 10 are set to i c — Fe = f (E c — Fe ). Strictly speaking, although Zn corrosion products are also formed on iron due to the diffusion and migration of substances, the calculation was carried out on the assumption that the effects were ignored. Here, 0.00110 ≦ β <1.000, and when the calculated value of β is less than 0.0010, β is set to 0.0010. At the boundaries other than the metal / solution interface, no current flow (∂Ф / の n = 0: where n represents a unit vector) was used as the boundary condition.

Vcは、亜鉛の腐食生成物として考慮したZn(OH)2およびZnCO3の生成量が計算により求まるため、ぞれぞれの密度の値からそれぞれの体積を求め、これら2つの腐食生成物成分の和をVcとした。逐次計算における各時間ステップにおいてVcが求まるため、このVcを用いてβを決定した。このようにして得られた補正した分極曲線を境界条件として、次の時間ステップにおける計算を実施することで逐次計算を行った。 V c can be calculated from the respective density values, since the amounts of Zn (OH) 2 and ZnCO 3 considered as corrosion products of zinc can be determined by calculation, and these two corrosion products can be obtained. the sum of components was V c. Since V c can be determined at each time step in sequential calculation, β is determined using this V c . Calculations were sequentially performed by carrying out the calculation at the next time step with the corrected polarization curve obtained in this way as a boundary condition.

この条件のもと、時間0から時間1440minまで逐次計算を行い、電位分布および電流密度分布を計算するとともに、その時間での化学種の濃度および反応生成物の濃度分布を計算した。水溶液中における化学反応は、亜鉛表面では表4に示す反応を考慮し、鉄表面では表5に示す反応を考慮した。このうち、腐食生成物としてZn(CO3),Zn(OH)2を考慮し、平衡濃度に達した時点で溶液中の余剰濃度分は速やかに沈殿すると仮定して計算した。 Under these conditions, the calculation was sequentially performed from time 0 to time 1440 min, and the potential distribution and current density distribution were calculated, and the concentration of chemical species and the concentration distribution of reaction products at that time were calculated. The chemical reactions in the aqueous solution considered the reactions shown in Table 4 on the zinc surface, and the reactions shown in Table 5 on the iron surface. Among them, Zn (CO 3 ) and Zn (OH) 2 were considered as corrosion products, and it was calculated on the assumption that the excess concentration in the solution would be rapidly precipitated when the equilibrium concentration was reached.

Figure 0006544402
Figure 0006544402

Figure 0006544402
Figure 0006544402

実施例1と同様にして、10,60,1440min後の亜鉛の腐食量を求めた。   In the same manner as in Example 1, the amount of corrosion of zinc after 10, 60, and 1440 min was determined.

これらの数値計算結果の妥当性を評価するために、数値計算と同じ条件で腐食実験を行った。図5に腐食実験に用いた10mm×10mm×5mmtの亜鉛と鉄(いずれも純度99.999%)を互いに接触させて固定した試験片の模式図を示す。この試験片の表面に数値計算した条件と同じ濃度、同じ厚さのNaCl水溶液を形成させた。金属表面上にいったん形成させた薄い塩水膜を一定の状態に維持するために、試験片をすみやかに室温、相対湿度をRH95%(1.0M相当)、RH85%(2.0M相当)に設定した恒温恒湿槽に入れて試験片を腐食させた。   In order to evaluate the validity of these numerical calculation results, corrosion experiments were conducted under the same conditions as the numerical calculation. FIG. 5 shows a schematic view of a test piece in which 10 mm × 10 mm × 5 mmt of zinc and iron (both having a purity of 99.999%) used in the corrosion test are brought into contact with each other and fixed. An aqueous solution of NaCl having the same concentration and the same thickness as the conditions calculated numerically was formed on the surface of the test piece. In order to keep the thin salt water film once formed on the metal surface in a fixed state, the test piece is promptly set to room temperature and relative humidity to RH 95% (equivalent to 1.0 M) and RH 85% (equivalent to 2.0 M) The test piece was corroded by placing it in the constant temperature and humidity chamber.

恒温恒湿槽に試験片を10,60,1440分入れたまま腐食させた後、走査型ケルビンプローブを用いて表面の電位分布を測定した。腐食状態を変化させないように、ケルビンプローブによる計測中も恒温恒湿槽内と同じ温度、相対湿度に維持した。測定終了後、すみやかに試験片を蒸留水で洗浄し、乾燥させた後、図5(b)のA−A’断面図に示す試験片中央部を長手方向に切断して、腐食状態を断面から走査型電子顕微鏡(SEM)で観察し、亜鉛の腐食量を厚さから求めた。   The test piece was corroded in a constant temperature and humidity chamber for 10, 60 and 1440 minutes, and then the potential distribution on the surface was measured using a scanning Kelvin probe. The same temperature and relative humidity as in the constant temperature and humidity chamber were maintained during measurement with the Kelvin probe so as not to change the corrosion state. After the measurement is completed, the test piece is promptly washed with distilled water and dried, and then the central portion of the test piece shown in the cross-sectional view taken along line AA 'of FIG. From the above, the amount of corrosion of zinc was determined from the thickness by observing with a scanning electron microscope (SEM).

表6に、計算と実験に用いたNaCl水溶液の条件と腐食時間、境界条件として用いる分極曲線の補正に用いたβの値を示す。補正方法は、それぞれの溶液での亜鉛の分極曲線をia_zn = f(Ea_zn)とした時、平衡計算から求められる腐食生成物の体積量Vcに対して、β=1-Vc/V0 を用いてia_zn =β× f(Ea_zn)と補正し、電解質溶液と金属の境界1〜5においてβで補正した分極曲線を適用した。なお、βの値は境界1〜5毎に時間ステップ計算毎に更新されるため、表6には、境界3の全ての時間ステップ計算の平均のβ値を記載している。また、β=1.000は分極曲線の補正を行わず、金属の分極曲線をそのまま境界条件として用いたことを意味する。 Table 6 shows the conditions and corrosion time of the NaCl aqueous solution used for calculation and experiment, and the value of β used for correction of the polarization curve used as the boundary condition. The correction method is as follows: when the polarization curve of zinc in each solution is i a _ z n = f (E a _ z n ), β = 1− with respect to the volume amount Vc of corrosion product determined from equilibrium calculation. A polarization curve corrected with β at the boundary 1 to 5 of the electrolyte solution and the metal was applied by using V c / V 0 and correcting it as i a — zn = β × f (E a — zn ). Note that since the value of β is updated for each time step calculation for each of the boundaries 1 to 5, Table 6 describes the average β value of all the time step calculations for the boundary 3. Further, β = 1.000 means that the polarization curve of the metal was used as the boundary condition as it is without correcting the polarization curve.

これらの条件のもと計算した結果と実験による電位および腐食量の測定結果の比較を示す。電位については、試験片長手方向で亜鉛から鉄の表面を1mmおきに全20点測定し、20点全ての計算した電位が実験結果に対して±50mVの範囲となった場合を○、そうでない場合を×とした。本実施例の腐食量分布は、Znの領域だけを対象として、電位と同様に試験片長手方向1mmおきに全10点を測定し、10点すべての測定点において(計算の腐食量)/(実験の腐食量)=0.5〜1.5である場合に○、この範囲を外れる場合を×として評価した。本発明の範囲であるNo1から9については、異なる溶液濃度、溶液の厚さ、腐食時間に対して高い精度で電位および腐食量の分布が予測できた。しかし、比較例に示すように、分極曲線を腐食生成物の生成量に応じて変化させない場合、すなわちβが1.000の場合には、電位および腐食量ともに実験を再現できていない。また、腐食生成物の量が多くなってきた場合、すなわちβが0.0010未満となる場合においても、計算結果と実験結果の乖離が大きく、実験結果を再現することができなかった。   The comparison between the results calculated under these conditions and the measurement results of potential and corrosion amount by experiments is shown. Regarding potentials, the surface of zinc to iron was measured every 1 mm in the longitudinal direction of the test piece at all 20 points, and the calculated potential at all 20 points was within the range of ± 50 mV with respect to the experimental results ○, not so The case was marked x. The corrosion amount distribution of this example measures all ten points at intervals of 1 mm in the longitudinal direction of the test piece in the same manner as the electric potential only for the area of Zn, and the corrosion amount at all ten measurement points The case where the corrosion amount in the experiment) = 0.5 to 1.5 was evaluated as ○, and the case outside this range was evaluated as x. With respect to No. 1 to No. 9 within the scope of the present invention, the distribution of potential and corrosion amount could be predicted with high accuracy with respect to different solution concentrations, solution thicknesses and corrosion times. However, as shown in the comparative example, in the case where the polarization curve is not changed according to the generation amount of the corrosion product, that is, when β is 1.000, both the potential and the amount of corrosion can not be reproduced. In addition, even when the amount of corrosion product increases, that is, when β is less than 0.0010, the difference between the calculation result and the experimental result is large, and the experimental result can not be reproduced.

Figure 0006544402
Figure 0006544402

(実施例3)
実施例1および2と同様に、大気腐食環境下における亜鉛と鉄の異種金属接触腐食を数値計算により予測した。図6に示す形状を本実施例の計算モデルとした。領域Ωは実際の大気環境で付着する海塩を模擬し、海水を模擬した組成の溶液の領域とし、化学種の初期濃度を表7のように設定した。この溶液の組成に含まれる化学種に対して、考慮すべき拡散係数は表8のように設定した。領域Ωでは、式(2)の物質輸送の式が成り立つと仮定し、それぞれの化学種について水溶液中の濃度勾配による拡散、電荷による泳動を考慮した。ここでは対流の影響は考慮していない。
(Example 3)
Similar to Examples 1 and 2, the dissimilar metal catalytic corrosion of zinc and iron in an atmospheric corrosive environment was predicted by numerical calculation. The shape shown in FIG. 6 is used as a calculation model of this example. The region Ω simulates sea salt adhering in an actual atmospheric environment, is a region of a solution having a composition simulating seawater, and the initial concentration of chemical species is set as shown in Table 7. The diffusion coefficients to be considered for the chemical species included in the composition of this solution were set as shown in Table 8. In the region Ω, it was assumed that the mass transport equation of equation (2) holds, and for each chemical species, diffusion due to concentration gradient in aqueous solution and migration due to charge were considered. The influence of convection is not considered here.

Figure 0006544402
Figure 0006544402

Figure 0006544402
Figure 0006544402

式(2)を解くための境界条件として、計算と同様に人工海水(八洲薬品株式会社製、金属腐食試験用溶液)中で測定した亜鉛のアノード分極曲線をia_zn = f(Ea_zn)、鉄のカソード分極曲線をic_Fe = f(Ec_Fe)とした時、境界1から5の境界条件をia_zn =β× f(Ea_zn)とし、β=1-Vc/V0として境界条件を決定した。ここで、Vcは、Znの腐食生成物の体積を表し、V0は単位体積を表す。一方、鉄系の腐食生成物の形成は考慮せず、境界6から10の境界条件をic_Fe = f(Ec_Fe)とした。厳密には物質の拡散や泳動によってZnの腐食生成物が鉄上にも形成されるが、その影響は無視する前提で計算を行った。ここで、0.0010 ≦ β < 1.000とし、βの計算値が0.0010を下回る場合には、すべてβを0.0010とすることとした。金属と溶液の界面以外の境界には、電流の流出入がない(∂Ф/∂n=0:ここでnは単位ベクトルを示す)を境界条件として用いた。 As a boundary condition for solving the equation (2), the anodic polarization curve of zinc measured in artificial seawater (a solution for metal corrosion test, made by Yahata Pharmaceutical Co., Ltd.) is calculated in the same manner as the calculation i a _ z n = f (E a _ zn), when the cathodic polarization curves of iron and i c _ Fe = f (E c _ Fe), from the boundary 1 of 5 boundary conditions i a _ zn = β × f (E a _ zn) The boundary condition is determined as β = 1−V c / V 0 . Here, V c represents the volume of a corrosion product of Zn, and V 0 represents a unit volume. On the other hand, the formation of iron-based corrosion products is not taken into consideration, and the boundary conditions of the boundaries 6 to 10 are set as i c — Fe = f (E c — Fe ). Strictly speaking, although Zn corrosion products are also formed on iron due to the diffusion and migration of substances, the calculation was carried out on the assumption that the effects were ignored. Here, 0.00110 ≦ β <1.000, and when the calculated value of β is less than 0.0010, β is set to 0.0010. At the boundaries other than the metal / solution interface, no current flow (∂Ф / の n = 0: where n represents a unit vector) was used as the boundary condition.

実際の大気腐食環境では、温度や湿度が連続的に変化し、これに伴い金属表面に形成する水溶液膜の濃度や平均厚さは変化する。このため、数値計算においても計算の単位時間毎に、温度と相対湿度の変化に伴う水溶液濃度や厚さを設定し、計算結果を積算することが望ましい。しかし、本実施例では、計算負荷を軽減するため、水溶液濃度は人工海水とほぼ同じ濃度で一定のまま計算を行った。   In an actual atmospheric corrosion environment, the temperature and humidity change continuously, and the concentration and average thickness of the aqueous solution film formed on the metal surface change accordingly. For this reason, also in numerical calculation, it is desirable to set the concentration and thickness of the aqueous solution accompanying changes in temperature and relative humidity for each unit time of calculation, and integrate the calculation results. However, in the present embodiment, in order to reduce the calculation load, the calculation was performed with the aqueous solution concentration kept constant at approximately the same concentration as the artificial seawater.

実施例2と同様に、Vcは、亜鉛の腐食生成物として考慮したZn(OH)2およびZnCO3の生成量が計算により求まるため、それぞれの密度の値からそれぞれの体積を求め、これら2つの腐食生成物成分の和をVcとした。逐次計算における各時間ステップにおいてVcが求まるため、このVcを用いてβを決定した。このようにして得られた補正した分極曲線を境界条件として、次の時間ステップにおける計算を実施することで逐次計算を行った。 As in Example 2, V c can be calculated from the values of the respective densities, since the amounts of Zn (OH) 2 and ZnCO 3 considered as corrosion products of zinc can be determined by calculation. The sum of the two corrosion product components is designated V c . Since V c can be determined at each time step in sequential calculation, β is determined using this V c . Calculations were sequentially performed by carrying out the calculation at the next time step with the corrected polarization curve obtained in this way as a boundary condition.

この条件のもと、表9に示す腐食期間(最大で4週間)まで逐次計算を行い、電位分布および電流密度分布を計算するとともに、その時間での化学種の濃度および反応生成物の濃度分布を計算した。水溶液中における化学反応は、実施例2と同様に、亜鉛表面では表4に示す反応を考慮し、鉄表面では表5に示す反応を考慮した。このうち、腐食生成物としてZn(CO3),Zn(OH)2を考慮し、平衡濃度に達した時点で溶液中の余剰濃度分は速やかに沈殿すると仮定して計算した。 Under this condition, the potential distribution and current density distribution are calculated by sequentially calculating up to the corrosion period shown in Table 9 (up to 4 weeks), and the concentration of chemical species and the concentration distribution of reaction products at that time Was calculated. The chemical reactions in the aqueous solution considered the reactions shown in Table 4 on the zinc surface and the reactions shown in Table 5 on the iron surface, as in Example 2. Among them, Zn (CO 3 ) and Zn (OH) 2 were considered as corrosion products, and it was calculated on the assumption that the excess concentration in the solution would be rapidly precipitated when the equilibrium concentration was reached.

実施例1,2と同様にして、各腐食期間の経過後の亜鉛の腐食量を求めた。   The amount of corrosion of zinc after each corrosion period was determined in the same manner as in Examples 1 and 2.

計算の妥当性を評価するため、実施例2と同様に図5に示す形状の試験片を用いて暴露試験を行った。暴露試験は、神奈川県川崎市川崎区南渡田町で実施し、雨が直接掛からないように、軒下に試験片を設置した。温度と相対湿度を1分毎に記録しながら、4週間試験を実施した。数値計算結果の妥当性は、実施例2と同様にケルビンプローブによる電位の分布および長手方向に切断した試験片を走査型電子顕微鏡(SEM)で観察することにより求めた亜鉛の厚さの分布で調査した。   In order to evaluate the validity of the calculation, an exposure test was conducted using a test piece having the shape shown in FIG. 5 as in Example 2. The exposure test was conducted in Minami-Toda-cho, Kawasaki-ku, Kawasaki-shi, Kanagawa Prefecture, and a test piece was placed under the eaves to prevent direct rain. A four week test was conducted, recording temperature and relative humidity every minute. Similar to Example 2, the validity of the numerical calculation results is the distribution of potential by Kelvin probe and the distribution of thickness of zinc determined by observing a test piece cut in the longitudinal direction with a scanning electron microscope (SEM) investigated.

表9に、各水準における腐食期間と、境界条件として用いる分極曲線の補正に用いたβの値を示す。補正方法は、各水準の人工海水での亜鉛の分極曲線をia_zn = f(Ea_zn)とした時、平衡計算から求められる腐食生成物の体積量Vcに対して、β=1-Vc/V0 を用いてia_zn =β× f(Ea_zn)と補正し、電解質溶液と金属の境界1〜5においてβで補正した分極曲線を適用した。なお、βの値は境界1〜5毎に時間ステップ計算毎に更新されるため、表9には、各境界1〜5について、全ての時間ステップ計算の平均のβ値を記載している。また、β=1.000は分極曲線の補正を行わず、金属の分極曲線をそのまま境界条件として用いたことを意味する。本発明例であるNo1から4については、分極曲線を腐食生成物の形成量に応じたβの値(0.0010〜1.000)を用いて補正した。一方、βは境界1〜5に対して異なる値が与えられるが、比較例では、境界1〜5のうちいずれかのβの値が0.0010〜1.000の範囲外となっている。 Table 9 shows the corrosion period at each level and the value of β used to correct the polarization curve used as the boundary condition. The correction method is β = for the volume amount Vc of the corrosion product determined from the equilibrium calculation, assuming that the polarization curve of zinc in each level of artificial seawater is i a _ z n = f (E a _ z n ). A polarization curve corrected with β at a boundary 1 to 5 of electrolyte solution and metal was applied by correcting 1 a − V c / V 0 with I a — z n = β × f (E a — z n ). Since the value of β is updated for each time step calculation every boundaries 1 to 5, Table 9 describes the average β value of all time step calculations for each boundary 1 to 5. Further, β = 1.000 means that the polarization curve of the metal was used as the boundary condition as it is without correcting the polarization curve. The polarization curves of No. 1 to No. 4, which are inventive examples, were corrected using the value (0.0010 to 1.000) of β according to the formation amount of the corrosion product. On the other hand, although β has different values for boundaries 1 to 5, in the comparative example, the value of any of β among boundaries 1 to 5 is out of the range of 0.0010 to 1.000.

表9に、計算と暴露試験の結果の比較を示す。電位については、試験片長手方向で亜鉛から鉄の表面を1mmおきに全20点測定し、20点全ての計算した電位が実験結果に対して±100mVの範囲となった場合を○、そうでない場合を×とした。腐食量分布は、Znの領域だけを対象として、電位と同様に試験片長手方向1mmおきに全10点を測定し、10点すべての測定点において(計算の腐食量)/(実験の腐食量)=0.25〜2.0である場合に○、この範囲を外れる場合を×として評価した。   Table 9 shows a comparison of the calculated and exposed test results. As for the potential, the surface of zinc to iron was measured at 1 mm intervals in all 20 points in the longitudinal direction of the test piece, and the calculated potential of all 20 points was within the range of ± 100 mV with respect to the experimental result ○, not so The case was marked x. The corrosion amount distribution measures all 10 points at 1 mm intervals in the longitudinal direction of the test piece in the same way as the electric potential only for the area of Zn, and at all 10 measurement points (calculation amount of corrosion) / (experimental corrosion amount O) when it was 0.25-2.0, and the case out of this range was evaluated as x.

7、14、21、28日(4週間)の計算と暴露試験の腐食および電位の分布を比較した結果、本発明では、いずれの腐食期間においても電位分布および腐食の分布ともに精度よく予測することができた。一方、比較例に示すように、分極曲線を腐食生成物の生成量に応じて変化させない場合、あるいは、補正が本発明における範囲から外れた場合、電位および腐食量ともに実験結果との乖離が大きくなることが分かった。腐食生成物の形成を考慮して、補正した分極曲線を境界条件として用いる本発明を適用することで、実際の腐食現象を高い精度で予測することができた。   As a result of comparing the distribution of corrosion and potential in the exposure test with the calculation of 7, 14, 21 and 28 days (4 weeks), the present invention accurately predicts both the potential distribution and the distribution of corrosion in any corrosion period. It was possible. On the other hand, as shown in the comparative example, when the polarization curve is not changed according to the generation amount of the corrosion product, or when the correction is out of the range in the present invention, the potential and the corrosion amount both largely deviate from the experimental results. It turned out that it became. Actual corrosion phenomena can be predicted with high accuracy by applying the present invention using the corrected polarization curve as a boundary condition in consideration of formation of corrosion products.

Figure 0006544402
Figure 0006544402

本発明の数値解析による金属の腐食予測方法によれば、電解質溶液と接触した金属の腐食を数値解析によってより高精度に予測することが可能となる。そのため、金属構造体や製品の設計、材料や構造体の腐食による品質劣化評価、および耐食材料の開発を最適かつ高精度に実施することができ、産業上極めて有益な技術である。   According to the method of predicting corrosion of metal by numerical analysis of the present invention, it is possible to predict corrosion of metal in contact with an electrolyte solution more accurately by numerical analysis. Therefore, the design of metal structures and products, the evaluation of quality deterioration due to the corrosion of materials and structures, and the development of corrosion resistant materials can be carried out optimally and with high precision, which is an industrially extremely useful technology.

Claims (11)

電解質溶液と接触した金属の腐食を数値解析によって予測する方法であって、
電解質溶液中における金属表面の電位Eと電流密度iとの関係である分極曲線を測定する工程と、
前記分極曲線における前記電流密度の値を小さくした補正分極曲線を得る工程と、
前記補正分極曲線を境界条件として、前記金属と前記電解質溶液とが接触した系における所定時刻での前記電解質溶液中の電位分布を数値計算により求める工程と、
を有し、
前記金属の表面上の単位領域あたりに生成する腐食生成物の生成量pを数値計算により求める工程をさらに有し、
前記分極曲線を、前記電流密度iを前記電位Eの関数として表わしたi=f(E)としたとき、前記補正分極曲線を、i=β×f(E),β=g(p)かつ0.0010≦β<1.000とすることを特徴とする数値解析による金属の腐食予測方法。
A method of predicting corrosion of metal in contact with an electrolyte solution by numerical analysis,
Measuring a polarization curve which is the relationship between the potential E of the metal surface in the electrolyte solution and the current density i;
Obtaining a corrected polarization curve in which the value of the current density in the polarization curve is reduced;
Obtaining the potential distribution in the electrolyte solution at a predetermined time in a system in which the metal and the electrolyte solution are in contact, by using the corrected polarization curve as a boundary condition by numerical calculation;
I have a,
The method further includes the step of determining the generation amount p of the corrosion product generated per unit area on the surface of the metal by numerical calculation,
Assuming that the polarization curve is i = f (E) where the current density i is expressed as a function of the potential E, the corrected polarization curve is i = β × f (E), β = g (p) and A method of predicting corrosion of metal by numerical analysis characterized by satisfying 0.0010 ≦ β <1.000 .
前記所定時刻での前記電解質溶液中の電位分布から、前記所定時刻での前記電解質溶液中の電流密度分布を数値計算により求める工程をさらに有する、請求項に記載の数値解析による金属の腐食予測方法。 From the potential distribution of the electrolyte solution at a predetermined time, further comprising corrosion prediction of metal by numerical analysis according to claim 1 the step of obtaining numerically the current density distribution of the electrolyte solution at a predetermined time Method. 前記電解質溶液中の電流密度分布のうち、前記電解質溶液中の前記金属との界面近傍における電流密度を用いて、ファラデーの法則により、前記所定時刻での前記金属の腐食量を計算する工程をさらに有する、請求項に記載の数値解析による金属の腐食予測方法。 In the step of calculating the amount of corrosion of the metal at the predetermined time according to Faraday's law using the current density in the vicinity of the interface with the metal in the electrolyte solution among the current density distribution in the electrolyte solution The corrosion prediction method of metal by numerical analysis according to claim 2 . 電解質溶液と接触した金属の腐食を数値解析によって予測する方法であって、A method of predicting corrosion of metal in contact with an electrolyte solution by numerical analysis,
電解質溶液中における金属表面の電位Eと電流密度iとの関係である分極曲線を測定する工程と、  Measuring a polarization curve which is the relationship between the potential E of the metal surface in the electrolyte solution and the current density i;
前記分極曲線における前記電流密度の値を小さくした補正分極曲線を得る工程と、  Obtaining a corrected polarization curve in which the value of the current density in the polarization curve is reduced;
前記補正分極曲線を境界条件として、前記金属と前記電解質溶液とが接触した系における所定時刻での前記電解質溶液中の電位分布を数値計算により求める工程と、  Obtaining the potential distribution in the electrolyte solution at a predetermined time in a system in which the metal and the electrolyte solution are in contact, by using the corrected polarization curve as a boundary condition by numerical calculation;
を有し、Have
前記所定時刻での前記電解質溶液中の電位分布から、前記所定時刻での前記電解質溶液中の電流密度分布を数値計算により求める工程をさらに有し、  The method further includes the step of obtaining the current density distribution in the electrolyte solution at the predetermined time by numerical calculation from the potential distribution in the electrolyte solution at the predetermined time.
前記電解質溶液中の電流密度分布のうち、前記電解質溶液中の前記金属との界面近傍における電流密度を用いて、ファラデーの法則により、前記所定時刻での前記金属の腐食量を計算する工程をさらに有することを特徴とする数値解析による金属の腐食予測方法。  In the step of calculating the amount of corrosion of the metal at the predetermined time according to Faraday's law using the current density in the vicinity of the interface with the metal in the electrolyte solution among the current density distribution in the electrolyte solution The metal corrosion prediction method by numerical analysis characterized by having.
前記分極曲線を、前記電流密度iを前記電位Eの関数として表わしたi=f(E)としたとき、前記補正分極曲線を、i=α×f(E),0.0010≦α<1.000
とする、請求項に記載の数値解析による金属の腐食予測方法。
Assuming that the polarization curve is i = f (E) where the current density i is expressed as a function of the potential E, the corrected polarization curve is i = α × f (E), 0.0010 ≦ α <1.000.
The corrosion prediction method of metal by numerical analysis according to claim 4 .
前記金属が、亜鉛、鉄、アルミ、銅、及びニッケルから選択される一種以上の金属、又は該金属を主成分とする合金である、請求項1〜5のいずれか一項に記載の数値解析による金属の腐食予測方法。   The numerical analysis according to any one of claims 1 to 5, wherein the metal is one or more metals selected from zinc, iron, aluminum, copper, and nickel, or an alloy containing the metal as a main component. How to predict metal corrosion by 前記腐食の形態が、二種の金属が接触し、金属間の電位差によって一方の金属の腐食が加速される異種金属接触腐食である、請求項1〜6のいずれか一項に記載の数値解析による金属の腐食予測方法。   The numerical analysis according to any one of claims 1 to 6, wherein the form of the corrosion is heterogeneous metal catalytic corrosion in which two metals are in contact and the corrosion of one metal is accelerated by the potential difference between the metals. How to predict metal corrosion by 前記二種の金属が、亜鉛又は亜鉛めっきと、鉄又は鋼との組み合わせである、請求項7に記載の数値解析による金属の腐食予測方法。   The method of predicting corrosion of metal by numerical analysis according to claim 7, wherein the two metals are a combination of zinc or zinc plating and iron or steel. 請求項1〜8のいずれか一項の数値解析による金属の腐食予測方法によって耐食性を予測して、材料を選定することを特徴とする鋼構造物の設計方法。   A method of designing a steel structure, comprising selecting a material by predicting corrosion resistance by the method of predicting corrosion of metal by numerical analysis according to any one of claims 1 to 8. 請求項1〜8のいずれか一項の数値解析による金属の腐食予測方法によって耐食性を予測して、防錆性能を設計することを特徴とする鉄鋼材料の設計方法。   A method of designing a steel material, comprising: predicting corrosion resistance by the method of predicting corrosion of metal by numerical analysis according to any one of claims 1 to 8; and designing anticorrosion performance. コンピュータに、請求項1〜8のいずれか一項の数値解析による金属の腐食予測方法を実行させる腐食予測プログラム。   The corrosion prediction program which makes a computer perform the corrosion prediction method of metal by numerical analysis of any one of Claims 1-8.
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