JPS5937461B2 - Method for measuring rate factors of corrosion reactions - Google Patents
Method for measuring rate factors of corrosion reactionsInfo
- Publication number
- JPS5937461B2 JPS5937461B2 JP128879A JP128879A JPS5937461B2 JP S5937461 B2 JPS5937461 B2 JP S5937461B2 JP 128879 A JP128879 A JP 128879A JP 128879 A JP128879 A JP 128879A JP S5937461 B2 JPS5937461 B2 JP S5937461B2
- Authority
- JP
- Japan
- Prior art keywords
- corrosion
- metal piece
- sample metal
- polarization
- potential
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Landscapes
- Testing Resistance To Weather, Investigating Materials By Mechanical Methods (AREA)
Description
【発明の詳細な説明】
本発明は金属試料片を作用電極とし、その分極特性を得
、さらに解析することにより所定条件下での金属試料片
の関与する速度因子、分極抵技只Pおよびターフエル勾
配等を得ることのできる腐食反応の速度因子の測定方法
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention uses a metal sample piece as a working electrode, obtains its polarization characteristics, and further analyzes the rate factor, polarization resistance, and terf. This invention relates to a method for measuring the rate factor of a corrosion reaction, which allows obtaining gradients and the like.
金属の腐食反応を評価する1つの手段として腐食速度か
ら判定することが知られている。It is known that one way to evaluate the corrosion reaction of metal is to determine it based on the corrosion rate.
そして、腐食速度を測定する方法としては、試料金属片
の分極抵抗馬から求める電気化学的な方法が知られてい
る。ところで、腐食反応の速度因子、分極抵抗馬と、試
料金属片に流れるファラデー電流Iと、分極値ηとの間
にはRp=η/I ・・・・・・・・・(1)の関係の
あることが知られている。As a method for measuring the corrosion rate, an electrochemical method is known in which the corrosion rate is determined from the polarization resistance of a sample metal piece. By the way, there is a relationship between the rate factor of corrosion reaction, polarization resistance, the Faraday current I flowing through the sample metal piece, and the polarization value η as Rp=η/I (1) It is known that there is
一方、理論的には、分極抵抗馬 と腐食電流計corr
との間には次式のような関係がある。βaβc
Rplcorr: ゜゜’゜’゜゜゜゜(2)2.3(
βa+βc)なお(2)式においてβa、βcはターフ
エル勾配である。On the other hand, theoretically, the polarization resistance horse and the corrosion current meter corr
There is a relationship between them as shown in the following equation. βaβc Rplcorr: ゜゜'゜'゜゜゜゜゜(2)2.3(
βa+βc) In equation (2), βa and βc are the Terfel gradients.
他方Icorrと腐食速度Vとの間には次式の関係があ
る。On the other hand, there is a relationship between Icorr and corrosion rate V as shown in the following equation.
V=(M/ZF)・ Icorr・・・・・・・・・(
3)なお(3式においてMは試料金属片の原子量、Zは
溶出金属イオンの原子価数、Fはファラデー定数である
。V=(M/ZF)・Icorr・・・・・・・・・(
3) In the formula (3), M is the atomic weight of the sample metal piece, Z is the valence number of the eluted metal ion, and F is the Faraday constant.
ここで、ターフエル勾配βa、βcは、系に固有な定数
と考えられているが系の種類や測定条件によつて変わつ
てくるため、正確に腐食速度vを把握するには分極抵抗
Rpの他にターフエル勾配^,βcの値が必要である。Here, the terfer gradients βa and βc are considered to be constants specific to the system, but they vary depending on the type of system and measurement conditions. Therefore, in order to accurately grasp the corrosion rate v, polarization resistance Rp The values of the terfel gradient ^ and βc are required.
また、ターフエル勾配^,βcは腐食反応の性質を特徴
づける重要なパラメータである。このような観点から、
分極抵抗式とターフエル勾配βA,βcの値を同時にか
つ正確に求めることは金属材の腐食性の評価あるいは防
食にとつて重要なことである。分極抵抗式を求める手段
としては従来分極抵抗法が知られている。この分極抵抗
法(直線分極法)は、分極抵抗式と与えた電流1が(1
)式の関係で示されることを利用した方法で、定電流1
を流したときの分極値ηを読みとることにより、試料金
属片の分極抵抗Rpを求めるようにしている。しかしこ
の方法ではターフエル勾配βA,βcまで求めることは
できない。また、この方法では腐食速度の遅い系に適用
した場合に、分極値ηが一定値に近づくのに長時間を要
するという不都合さがある。さらに、蒸留水中の如き溶
液抵抗の大きい系の場合には定電流を流すために生ずる
IR−DrOpが求めるべきηに重なつて測定されてし
まうために、そのIR一DrOpを補正しなければなら
ないという不都合さもある。このように、?の値だけが
求まつて、βA.βcの値を評価しえない上記分極抵抗
法(直線分極法)に対し、さらにlηIの値が大きくな
るような大きな電流111を流し次の腐食反応を表わす
式− Cυ五▲ Rvrvを利用し、
βA,βcならびにを求める方法もいくつかある。Furthermore, the terfel gradient ^ and βc are important parameters that characterize the nature of corrosion reactions. From this perspective,
It is important to simultaneously and accurately determine the values of the polarization resistance equation and the terfel gradients βA and βc for evaluating the corrosivity of metal materials or for corrosion prevention. The polarization resistance method is conventionally known as a means for determining the polarization resistance formula. In this polarization resistance method (linear polarization method), the polarization resistance formula and the applied current 1 are (1
) is a method that utilizes the relationship shown in the equation, constant current 1
The polarization resistance Rp of the sample metal piece is determined by reading the polarization value η when flowing the sample metal. However, with this method, it is not possible to obtain the Terfel gradients βA and βc. Furthermore, this method has the disadvantage that when applied to a system with a slow corrosion rate, it takes a long time for the polarization value η to approach a constant value. Furthermore, in the case of a system with high solution resistance, such as in distilled water, the IR-DrOp generated due to the flow of a constant current is measured overlapping the η that should be determined, so the IR-DrOp must be corrected. There is also an inconvenience. in this way,? Only the value of βA. In contrast to the above polarization resistance method (linear polarization method) in which the value of βc cannot be evaluated, by passing a large current 111 that increases the value of lηI and using the formula representing the following corrosion reaction - Cυ5▲ Rvrv,
There are several methods for determining βA, βc, and.
その代表的な方法は10g111とηとの関係を示すと
ころの分極曲線(模式図を第1図に示す)の測定にもと
づくものである。この方法はη〉0のとき(4)式が次
式r―
で示されること、またηく0のときは
式で示されることを利用したものである。A typical method is based on the measurement of a polarization curve (a schematic diagram is shown in FIG. 1) showing the relationship between 10g111 and η. This method utilizes the fact that when η>0, equation (4) is expressed as the following equation r-, and when η<0, it is expressed as the following equation.
すなわち、η−10g111の関係を示す直線の傾きよ
り^,βcを求める。さらにη−10g111の関係を
η→0に内挿することにより、IO。rrを求め、これ
からRpを求めるようにしている。さらに、試料金属片
に3個の異なる大きさの定電流を流したときの分極値を
それぞれ(4)式の関係に代入して得られるところの3
個の方程式を連立させてR,.βA,βcを同時に求め
る方法もある。しかしながら、従来のRp,Ba,βc
を求める方法では、何れも定電流を試験液中に流すこと
になるため、溶液抵抗の大きい系ではIR−DrOpの
補正ないしは補償が問題となるし、また、腐食速度の小
さい系では分極値ηの定常値が得られるのに時間がかか
りすぎる問題がある。That is, ^ and βc are determined from the slope of the straight line representing the relationship η-10g111. Furthermore, by interpolating the relationship η-10g111 to η→0, IO. rr is calculated, and Rp is calculated from this. Furthermore, by substituting the polarization values obtained when three constant currents of different magnitudes are passed through the sample metal piece into the relationship of equation (4), 3 is obtained.
R, . There is also a method of determining βA and βc at the same time. However, conventional Rp, Ba, βc
In all methods of determining , a constant current is passed through the test solution, so in systems with high solution resistance, correction or compensation of IR-DrOp becomes a problem, and in systems with low corrosion rate, the polarization value η There is a problem that it takes too much time to obtain a steady value.
測定時間が長びくことは単に結果が得られるのに時間が
かかるのみならず試料金属片の表面状態を測定中に大き
く変化させてしまう危険が大きいため、測定誤差を生ず
るもとにもなる。そこで本発明者等は先に特願51−5
6076(特公昭56−12812号公報)などとして
、短時間でかつ、溶液抵抗によるIR−DrOpの補正
もしくは補償を必要とせずに試料金属片の腐食反応にお
ける分極抵抗Rp,ターフエル勾配βA.βcなどを容
易に求めることのできる測定方法を出願した。Prolonging the measurement time not only increases the time it takes to obtain results, but also increases the risk of significantly changing the surface condition of the sample metal piece during measurement, which can lead to measurement errors. Therefore, the present inventors first applied for patent application No. 51-5.
6076 (Japanese Patent Publication No. 56-12812), etc., polarization resistance Rp, Terfel gradient βA. We have filed an application for a measurement method that can easily determine βc, etc.
これは腐食系におかれた試料金属片に所定量の電荷を付
与し、この時の試料金属片の電位変化を、分極値η一時
間tの関係として求め、分極値η一時間tの関係から分
極抵抗、ターフエル勾配βA,βcなどの腐食反応にお
ける速度因子を求めるというものであつた。なお上記測
定方法においては、腐食反応の各速度因子(分極抵抗式
、ターフエル勾配βA,βc)測定に必要な付与される
べき電荷量が制限されるため同種又は異種の前記速度因
子を少なくとも2つ以上測定する際には複数回の測定が
必要であつた。In this method, a predetermined amount of charge is applied to a sample metal piece placed in a corrosive system, and the potential change of the sample metal piece at this time is determined as a relationship between polarization value η and time t, and the relationship between polarization value η and time t is The objective was to find rate factors in corrosion reactions such as polarization resistance and terfel gradients βA and βc. In addition, in the above measurement method, since the amount of charge to be applied necessary for measuring each rate factor of corrosion reaction (polarization resistance type, terfel gradient βA, βc) is limited, at least two of the rate factors of the same or different types are used. The above measurements required multiple measurements.
しかしながら上記の如く複数回の測定を行う場合、最初
の測定において腐食電位EcOォを示す試料金属片に所
定量の電荷を与え、電位をステツプさせて、この時の分
極値η一時間tの関係から所要の速度因子を求めた後、
次の測定に移る。However, when performing multiple measurements as described above, a predetermined amount of charge is applied to the sample metal piece exhibiting the corrosion potential EcO in the first measurement, the potential is stepped, and the relationship between the polarization value η and time t is After finding the required speed factor from
Move on to the next measurement.
つまり最初の測定において付与された電荷による分極値
が零(試料金属片の電位が腐食電位EcOrr)まで減
衰した後に、次の測定を行わなければ、腐食状態におけ
る正確な腐食反応の速度因子を求めることができなかつ
た。特に腐食速度の遅い系においては、1つの速度因子
測定後、次の測定までに長時間を要し、また腐食速度の
比較的速い系では、複数個の速度因子の測定中に試料金
属片の腐食状態が変化するため、正確な測定のためには
、可及的に短時間における連続的な測定が望まれていた
。本発明は上記の点に鑑み溶液抵抗によるIR−DrO
pの補正もしくは補償を要せず、容易に試料金属片の複
数個の腐食反応の速度因子を極めて短時間かつ正確に測
定する事のできる測定方法を提供する事を目的とする。
本発明は腐食系におかれた腐食電位E。In other words, if the next measurement is not performed after the polarization value due to the charge applied in the first measurement has decayed to zero (the potential of the sample metal piece is the corrosion potential EcOrr), it is necessary to obtain the accurate rate factor of the corrosion reaction in the corroded state. I couldn't do it. In particular, in systems with slow corrosion rates, it takes a long time to measure one rate factor before the next measurement, and in systems with relatively fast corrosion rates, multiple rate factors are measured during the measurement of the sample metal piece. Since the corrosion state changes, continuous measurement in as short a time as possible is desired for accurate measurement. In view of the above points, the present invention provides IR-DrO using solution resistance.
It is an object of the present invention to provide a measurement method that can easily measure the rate factors of a plurality of corrosion reactions of a sample metal piece in an extremely short time and accurately without requiring correction or compensation of p.
The present invention deals with the corrosion potential E placed in a corrosive system.
Orrを示す試料金属片に所定量の電荷を瞬間的に付与
し、前記試料金属片の電位変化を前記試料金属片に近接
配置した参照電極により分極値η一時間tの関係から前
記試料金属片に関与する腐食反応の速度因子を測定する
方法において、異種叉は同種の前記腐食反応の速度因子
を複数個測定する際に、1つの腐食反応の速度因子の測
定後で、次の腐食反応の速度因子の測定前に前記試料金
属片の電位.を強制的に腐食電位E。Orrに戻す腐食
反応の速度因子の測定方法であり、また前記腐食反応の
速度因子として分極抵抗を求める際には、試料金属片に
おける分極値の絶対値1η1が10mV以下となる如く
電荷を付与し、腐食反応の速度因子としてターフエル勾
配βA.βcを求める際には試料金属片における分極値
の絶対値1η1が60mV以上となる如く電荷を付与す
る事により、さらに正確な測定が可能になるというもの
である。なお本発明方法における腐食反応の速度因子と
しては、例えば分極抵抗式、ターフエル勾配ぬ.βCが
挙げられ、これらの速度因子は以下の如くして求められ
る。A predetermined amount of charge is instantaneously applied to a sample metal piece exhibiting Orr, and a potential change of the sample metal piece is measured by a reference electrode placed close to the sample metal piece from the relationship of polarization value η and time t. In the method for measuring the rate factor of a corrosion reaction involved in a corrosion reaction, when measuring a plurality of rate factors of different or the same type of corrosion reactions, after measuring the rate factor of one corrosion reaction, the rate factor of the next corrosion reaction is measured. The potential of the sample metal piece before measuring the rate factor. Force the corrosion potential E. This is a method for measuring the rate factor of the corrosion reaction that returns to Orr, and when determining the polarization resistance as the rate factor of the corrosion reaction, an electric charge is applied so that the absolute value 1η1 of the polarization value in the sample metal piece is 10 mV or less. , Terfel slope βA. as a rate factor of corrosion reaction. When determining βc, more accurate measurement becomes possible by applying a charge so that the absolute value 1η1 of the polarization value in the sample metal piece is 60 mV or more. In addition, as the rate factor of the corrosion reaction in the method of the present invention, for example, the polarization resistance formula, the terfel gradient, etc. βC is mentioned, and these rate factors are determined as follows.
まず分極抵抗式は、電荷付与による試料金属片における
分極値ηが充分小さい時には、腐食反応によるフアラデ
一電流1、分極抵抗および分極値ηの関係は下式の如く
である故、測定される分極値η一時間t曲線は理論的に
前記腐食反応を表す一般式(4)式より次のように導か
れ、(式中η。First, the polarization resistance equation is based on the following formula: When the polarization value η of the sample metal piece due to charge application is sufficiently small, the relationship between the Farade current 1 due to corrosion reaction, the polarization resistance, and the polarization value η is as shown in the following equation, so the measured polarization The value η-time t curve is theoretically derived from the general formula (4) expressing the corrosion reaction as follows, where η.
は試料金属片に電荷を与えた直後の分極値、COは試料
金属片の電気二重層の微分容量)さらにとして導かれる
。is the polarization value immediately after applying a charge to the sample metal piece, and CO is the differential capacitance of the electric double layer of the sample metal piece).
従つて分極値ηを求め11ηを時間tに対してプロツト
したとき直線が得られればその直線を時間t=oに外挿
することによりη。を求め得る。しかして金属試料片に
電荷を与えた直後の分極値η。Therefore, if a straight line is obtained when the polarization value η is obtained and 11η is plotted against time t, η can be obtained by extrapolating the straight line to time t=o. can be found. Therefore, the polarization value η immediately after applying a charge to the metal sample piece.
と試料金属片に与えた電荷密度の変化量Δqとから次式
によつて微分容量らを求め、さらにこれらのη。The differential capacitance et al. is calculated from the following equation from the amount of change Δq in the charge density given to the sample metal piece, and then these η.
およびC。の値を用いれば上記1nη−t直線の傾きか
ら分極抵抗4を求め得る。特に分極値の絶対値1ηlが
10mV以下の場合上記(7)〜(9)式が成り立ち正
確な分極抵抗を求める事ができる。and C. By using the value of , the polarization resistance 4 can be determined from the slope of the above 1nη-t line. In particular, when the absolute value 1ηl of the polarization value is 10 mV or less, the above equations (7) to (9) hold, and an accurate polarization resistance can be determined.
他方、ターフエル勾配βA,βcを求めるには、次のよ
うにする。On the other hand, the Terfel gradients βA and βc can be obtained as follows.
すなわち、ηが60mV以上のときには(4)式はのよ
うにかける。That is, when η is 60 mV or more, equation (4) is applied as follows.
したがつて、所定量の比較的大きい正の電荷を与えた直
後より、ある程度の時間tが経過してη1になつたとき
の時間をt=oとすれば、ある時間tにおけるηとtと
の関係は理論的に次式の形に導かれる。Therefore, if t=o is the time when η1 is reached after a certain amount of time t has passed immediately after applying a relatively large positive charge of a predetermined amount, then η and t at a certain time t are The relationship is theoretically derived from the following equation.
ここに、Cdは試料金属の電気二重層の微分容量で微少
電位範囲内においては一定と考えてよい。この(12犬
をみれば、測定したη−t曲線より、異なる3個の時間
Tl,t2,t3に対してそれぞれ分極電位η1,η2
,η3を読みとることにより、3個の方程式が得られる
ことが判る。Here, Cd is the differential capacitance of the electric double layer of the sample metal, and can be considered to be constant within a minute potential range. Looking at this (12 dogs), from the measured η-t curve, the polarization potentials η1, η2 for three different times Tl, t2, t3, respectively.
, η3, it can be seen that three equations can be obtained.
(自)弐からα方式を辺々引くと
o方民からCl陳民を辺々引くと
(ロ)式を(15)式で辺々わつて
(ロ)式より、異なる3個の時間Tl.t2,t3に対
応した分極電位η1,η2.η3が判ればβaが求まる
ことがわかる。(au) Subtracting the α method from 2, subtracting Cl Chenmin from o, then subtracting equation (b) from equation (15), and from equation (b), three different times Tl .. Polarization potentials η1, η2 .corresponding to t2, t3. It is understood that βa can be found if η3 is known.
ところで、いま、η1〉η2〉η3でη1=η2+Δη
,η3=η2−Δηになるようなη1,η2,η3を考
え、これらの分極電位に対応するTl,t2,t3をそ
れぞれ得られたη−t曲線よりサンプリングしたとする
。By the way, now η1>η2>η3, η1=η2+Δη
, η3=η2−Δη, and Tl, t2, and t3 corresponding to these polarization potentials are sampled from the obtained η-t curves.
(ただし、Δη〉0である)すなわち1η1−η2(η
2−η3になるようにη1!η29η3を定め、これに
対する時間をそれぞれサンプリングするわけである。こ
のようなη1,η2,η3を用いるとα◆民の左辺はの
形に簡単化される。(However, Δη〉0), that is, 1η1−η2(η
η1 so that it becomes 2-η3! η29η3 are determined, and the times corresponding to these values are sampled. Using such η1, η2, and η3, the left side of α◆min can be simplified into the form.
したがつて
(17)式から、βaは測定したη−t曲線(η》0)
より、ある時間T2におけるη2をまず求め、さらにη
2からΔηだけ大きいη1=η2+Δη,Δηだけ小さ
いη3=η2−Δηに対応する時間、それぞれTl,t
3を読みとれば、それらのTl,t2,t3およびΔη
を用いることにより簡単に計算しうることが判る。Therefore, from equation (17), βa is the measured η-t curve (η》0)
Therefore, first find η2 at a certain time T2, and then η
The times corresponding to η1 = η2 + Δη, which is larger than Δη from 2, and η3 = η2 − Δη, which is smaller by Δη, are Tl and t, respectively.
3, their Tl, t2, t3 and Δη
It can be seen that it can be easily calculated by using .
ところで、上記の解析方法ではIcOrrやCdを含む
項がうまい具合に消去されるので簡単ではあるが、Δη
を大きくとりすぎるとη1とη2、η,とη3との差が
大きくなりすぎてCdの電位変化が生じてくる危険性が
考えられる。By the way, the above analysis method is easy because terms including IcOrr and Cd are eliminated well, but Δη
If .eta.1 and .eta.2, .eta., and .eta.3 are set too large, the difference between .eta.1 and .eta.2 and .eta.
し・たがつて、Δηはたとえば10mV以下にするとか
してCdの電位変化が無視できるように十分小さくする
必要がある。以上は、η〉60mVのときであつたが、
逆にη〈−60mVのときは(4)式はのように書ける
。Therefore, Δη needs to be made sufficiently small, for example, 10 mV or less, so that the change in the potential of Cd can be ignored. The above was when η>60mV,
Conversely, when η<-60mV, equation (4) can be written as follows.
したがつて、一定量の負の電荷を与えた直後より、ある
程度時間が経過してη1になつたときの時間をt=oと
すれば、ある時間tにおけるηとtとの関係は理論的に
次式の形に導かれる。Therefore, if we let t=o be the time when η1 is reached after a certain amount of time has passed immediately after applying a certain amount of negative charge, the relationship between η and t at a certain time t is theoretical. is led to the form of the following equation.
ここで、η1〈η2〈η3、η,=η2−Δη、η3=
η2+Δη、Δη〉Oのように分極値を定め、測定した
η−t曲線より、これらのη1,η2,η3に対応する
時間T,,t2,t3をそれぞれ読み取れば、βaの場
合と同様にβcはつぎの関係1Z1
を用いることにより求めることができる。Here, η1〈η2〈η3, η,=η2−Δη, η3=
If the polarization values are determined as η2+Δη, Δη〉O, and the times T, , t2, and t3 corresponding to these η1, η2, and η3 are read from the measured η-t curve, βc is obtained as in the case of βa. can be determined by using the following relationship 1Z1.
以上の如くして個々の腐食反応の速度因子は測定される
が、複数個の前記速度因子を短時間で連続的かつ正確に
測定する場合には以下の如く行われる。Although the rate factors of individual corrosion reactions are measured as described above, when a plurality of rate factors are to be measured continuously and accurately in a short period of time, it is carried out as follows.
例えば腐食反応の速度因子として分極抵抗式、ターフエ
ル勾配βA,βcを求める場合を、本発明方法を用いた
装置の原理図第1図および試料金属片における電位変化
を示す第2図を用いて説明する。まず分極抵抗を求める
場合、腐食判定セルA中に配設された作用電極としての
試料金属片1に電荷供給機構Bから所定量の電荷を瞬間
的に付与する。For example, the case of determining the polarization resistance equation and the turf gradient βA, βc as rate factors of corrosion reaction will be explained using Fig. 1, which shows the principle of the apparatus using the method of the present invention, and Fig. 2, which shows the potential change in the sample metal piece. do. First, when determining the polarization resistance, a predetermined amount of charge is instantaneously applied from the charge supply mechanism B to the sample metal piece 1 as a working electrode disposed in the corrosion determination cell A.
なおこの時の前記試料金属片1における分極値ηは第2
図領域aに示す如く、数MVステツプした後減衰し、分
極値η一時間t曲線として電位差測定機構Cにより記録
される。さらにこの分極値η一時間t曲線を基に前述の
解析方法により分極抵抗を求める事ができる。なお、次
にターフエル勾配βaを求めるに先立ち、前記分極抵抗
Rpの測定前に電位測定計Dにより求めた腐食電位E。Note that the polarization value η of the sample metal piece 1 at this time is the second
As shown in area a of the figure, the polarization value η decays after several MV steps and is recorded by the potentiometric measurement mechanism C as a polarization value η versus time t curve. Further, based on this polarization value η-time t curve, the polarization resistance can be determined by the above-mentioned analysis method. In addition, prior to determining the Terfel gradient βa, the corrosion potential E was determined using a potential meter D before measuring the polarization resistance Rp.
Orrを基準として、定電圧機構Eにより分極値ηaを
Oとし、試料金属片1の電位を腐食電位E。Orr(分
極値η=0)とする(第2図領域d1)。ターフエル勾
配βaを求める場合、電荷付与による分極値ηのステツ
プ量を第2図領域bに示す如く60mV以上とする以外
は前記分極抵抗R2を求める手段と同様にして分極値η
一時間t曲線を得る。With Orr as a reference, the polarization value ηa is set to O by the constant voltage mechanism E, and the potential of the sample metal piece 1 is set to the corrosion potential E. Orr (polarization value η=0) (region d1 in FIG. 2). When determining the polarization gradient βa, the polarization value η is determined in the same manner as in the method for determining the polarization resistance R2, except that the step amount of the polarization value η due to charge application is set to 60 mV or more as shown in area b of FIG.
Obtain a one-hour t-curve.
そこで前述の解析方法によりターフエル勾配βaを求め
る事ができる。再びターフエル勾配βcを求めるのに先
立ち、前記分極抵抗の測定前に電位測定計Dにより求め
た腐食電位E。Therefore, the terfel gradient βa can be determined by the above-mentioned analysis method. Prior to determining the Terfel gradient βc again, the corrosion potential E was determined using the potentiometer D before measuring the polarization resistance.
Orrを基準として、定電圧機構Eにより分極値ηbを
Oとし、試料金属片1の電位をEcOrrとするO続い
てターフエル勾配βcを求める場合、電荷付与による分
極値ηのステツプ量を第2図領域Cに示す如く−60m
V以下とする以外は前記ターフエル勾配βaを求める方
法と同様にしてターフエル勾配βcを得る事ができる。Orr as a reference, the polarization value ηb is set to O by the constant voltage mechanism E, and the potential of the sample metal piece 1 is set to EcOrr.O Next, when determining the tarfel gradient βc, the step amount of the polarization value η due to charge application is shown in Fig. 2. -60m as shown in area C
The terfel gradient βc can be obtained in the same manner as the method for determining the terfel gradient βa described above, except that it is less than or equal to V.
以上の如く本発明方法を用いた場合、常に試料金属片の
腐食電位EcOrrを基準とした腐食反応の速度因子と
しての分極抵抗、ターフエル勾配βA,βcが得られ、
腐食判定が極めて正確に行える。As described above, when the method of the present invention is used, polarization resistance and terfel gradients βA and βc are always obtained as rate factors of the corrosion reaction based on the corrosion potential EcOrr of the sample metal piece,
Corrosion determination can be performed extremely accurately.
さらに第2図における領域A.b,c,dl,d2は数
10秒程度で行われるため測定が迅速化される事は言う
までもない。Furthermore, area A in FIG. Since b, c, dl, and d2 are carried out in about several tens of seconds, it goes without saying that the measurement is speeded up.
なお上記においては、分極抵抗Rp,ターフエル勾配β
A,βcの順に測定を行つた場合を示したが適宜その順
序を変更しても同様の効果が得られ、さらに同種の前記
速度因子を繰り返し測定する事もできる。Note that in the above, polarization resistance Rp, terfel gradient β
Although the case where the measurements are performed in the order of A and βc is shown, the same effect can be obtained even if the order is changed as appropriate, and it is also possible to repeatedly measure the same type of speed factor.
次に本発明方法を用いた具体的装置例を示す第3図によ
り本発明に係る実施例を説明する。Next, an embodiment according to the present invention will be described with reference to FIG. 3 showing a specific example of an apparatus using the method of the present invention.
第3図において腐食判定セルAは腐食系におかれた試料
金属片1、飽和甘コウ電極など安定な電位を維持する参
照電極3および対極2より構成されている。前記試料金
属片1に所定量の電荷を供給するための電荷供給機構B
は電池5、極性切換えスイツチ6,7および可変抵抗9
などからなる電荷供給源部および電荷を蓄積するコンデ
ンサ16から構成されており、また18,19は、供給
された電荷量を測定するための演算増幅器及び電圧計を
それぞれ示す。In FIG. 3, a corrosion determination cell A is comprised of a sample metal piece 1 placed in a corrosion system, a reference electrode 3 such as a saturated electrode that maintains a stable potential, and a counter electrode 2. A charge supply mechanism B for supplying a predetermined amount of charge to the sample metal piece 1
is battery 5, polarity switch 6, 7 and variable resistor 9
It is composed of a charge supply source section and a capacitor 16 that stores charges, and 18 and 19 indicate an operational amplifier and a voltmeter, respectively, for measuring the amount of supplied charge.
つまり試料金属片1に電荷を付与する以前のコンデンサ
16の電圧V1および前記電荷を供給後の電圧V2を電
位計19で測定し、ΔQ−C1(V1−V2)・・・(
C1 :コンデンサ容量)として試料金属片に付与され
た電荷量ΔQを求める事ができる。なお上記電荷供給機
構Bは、所定量の電荷を瞬間的に供給できる定電圧パル
ス電源等に適宜置き換える事もできる。またFは前記電
荷供給機構Bから供給される所定量の電荷を瞬間的に試
料金属片1に付与するための電荷付与機構を示し、リレ
ー11抵抗12、スイツチ14およびリレー11を作動
させるための電源13から構成されている。That is, the voltage V1 of the capacitor 16 before charging the sample metal piece 1 and the voltage V2 after supplying the charge are measured with the electrometer 19, and ΔQ-C1(V1-V2)...
The amount of charge ΔQ imparted to the sample metal piece can be determined as C1: capacitor capacity). Note that the charge supply mechanism B may be appropriately replaced with a constant voltage pulse power source or the like that can instantaneously supply a predetermined amount of charge. Further, F indicates a charge applying mechanism for instantaneously applying a predetermined amount of charge supplied from the charge supplying mechanism B to the sample metal piece 1, and a charge applying mechanism for activating the relay 11 resistor 12, switch 14 and relay 11. It is composed of a power source 13.
またGは、測定に際し腐食系において高抵抗液を用いた
り、試料金属片1として表面積の大きなものを用いた場
合に有効な遮断機構を示す。Further, G indicates a blocking mechanism that is effective when a high resistance liquid is used in a corrosive system during measurement or when a metal sample 1 with a large surface area is used.
つまり前記の如く腐食系において高抵抗液を用いたり、
表面積の大きな試料金属片を用いた場合、所定量の電荷
が試料金属片に供給される時に試料金属片の電気二重層
への充電に長時間を要するため、充電中に生じるIR−
DrOpにより、正確な分極値を得る事が困難となる可
能性があつた。そこで前記電荷付与機構Fの作動後、所
定時間経過時にタイマー20が動作し、トランジスタ2
1によりFETスイツチ22のソース、ドレイン間が非
導通とし、試料金属片1への電荷供給を停止すると共に
、後述するリレー30を作動せしめ分極値η一時間tの
測定を開始する。つまり所定時間後、電荷供給を停止す
る事により分極値ηへのIR一DrOpの影響を無視す
ることができる。そこで試料金属片1における電位変化
はリレー30を介して電位差測定機構Cにより分極値η
−時間t関係として測定される。In other words, as mentioned above, using a high resistance liquid in a corrosive system,
When using a sample metal piece with a large surface area, it takes a long time to charge the electric double layer of the sample metal piece when a predetermined amount of charge is supplied to the sample metal piece, so the IR-
DrOp could make it difficult to obtain accurate polarization values. Therefore, after the charge applying mechanism F is activated, the timer 20 is activated when a predetermined period of time has elapsed, and the transistor 2 is activated.
1, the source and drain of the FET switch 22 are made non-conductive, stopping the charge supply to the sample metal piece 1, and activating the relay 30, which will be described later, to start measuring the polarization value η and time t. That is, by stopping the charge supply after a predetermined period of time, the influence of IR-DrOp on the polarization value η can be ignored. Therefore, the potential change in the sample metal piece 1 is measured by the potential difference measuring mechanism C via the relay 30, and the polarization value η
- measured as a time t relationship.
なお電位差測定機構Cはインピーダンス変換のための演
算増幅器31、電位差記録回路および解析表示回路33
より構成されている。以上の腐食判定セルA、電荷供給
機構B、電荷付与機構F、電位差測定機構Cおよび必要
であれば遮断機構Gにより個々の腐食反応の速度因子を
求める事が可能となる。Note that the potential difference measuring mechanism C includes an operational amplifier 31 for impedance conversion, a potential difference recording circuit, and an analysis display circuit 33.
It is composed of It becomes possible to determine the rate factor of each corrosion reaction using the above-mentioned corrosion determination cell A, charge supply mechanism B, charge application mechanism F, potential difference measurement mechanism C, and if necessary, cutoff mechanism G.
さらに本発明方法においては、測定開始前にスイツチ3
5、演算増幅器36および電圧計37により構成される
電位測定計Dにより、予め試料金属片1の腐食電位E。Furthermore, in the method of the present invention, switch 3 is
5. The corrosion potential E of the sample metal piece 1 is measured in advance by a potential measuring meter D composed of an operational amplifier 36 and a voltmeter 37.
Orrを測定しておく。そこで前記各速度因子の測定終
了後定電圧機構Eにより強制的に試料金属片の電位を腐
食電位EcOrrとする。なおスイツチング機構Hは前
記定電圧機構Eによる逆バイア・スを印加するためにタ
イマー27およびリレー28により構成されている。Measure Orr in advance. Therefore, after the measurement of each rate factor is completed, the potential of the sample metal piece is forcibly set to the corrosion potential EcOrr by the constant voltage mechanism E. The switching mechanism H includes a timer 27 and a relay 28 in order to apply a reverse bias from the constant voltage mechanism E.
なお上記の如き本発明方法を用いた装置においては以下
の順序で動作する。Note that the apparatus using the method of the present invention as described above operates in the following order.
まず腐食速度の反応因子の測定に先立ち、スィツチ35
により電位測定計Dを腐食判定セルA中の試料金属片1
と接続し、試料金属片1の電位、つまり腐食電位EcO
rrを測定する。First, before measuring the reaction factor of corrosion rate, switch 35
Test the potential measurement meter D with the sample metal piece 1 in the corrosion judgment cell A.
The potential of the sample metal piece 1, that is, the corrosion potential EcO
Measure rr.
そこで定電圧機構E中の可変抵抗40を調整して、常に
参照電極3と試料金属片1との間にEcOrrとなる如
く設定する。次に最初に測定すべき速度因子に対応した
電荷供給機構B中のコンデンサ16−1〜16−5を選
択し、供給する電荷量を設定する。Therefore, the variable resistor 40 in the constant voltage mechanism E is adjusted so that EcOrr is always maintained between the reference electrode 3 and the sample metal piece 1. Next, capacitors 16-1 to 16-5 in charge supply mechanism B corresponding to the speed factor to be measured first are selected, and the amount of charge to be supplied is set.
そこで電荷付与機構F中のスイツチ14を閉じると、電
荷供給機構Bから所定量の電荷がリレー11、FETス
イツチ22およびリレー28を介して試料金属片1に瞬
間的に供給される。所定の微少時間後、タイマー20が
作動し、FETスイツチ22により電荷の供給が停止さ
れ、同時にリレー30により、試料金属片1における電
位変化が分極値η一時間tの関係として測定される。こ
の分極値η一時間tの関係から、所定の解析方法により
最初の速度因子が求められる。続いて、タイマー27に
より試料金属片1と定電圧機構Eは接続され、試料金属
片1の電位は強制的にEcOrrとなり、続いて次の速
度因子の測定が可能となる。後は同様の操査により複数
個の速度因子を正確かつ迅速に測定することができる。
なお2回目以降の測定においては、長時間の放置により
腐食電位EcOrrが大きく変化しない限り、前記電位
測定計D及び定電圧機構Eの調整は不用である。以下上
記第3図に示す本発明方法を用いた装置を用い、市水中
における軟鋼板の腐食状況を測定した。When the switch 14 in the charge applying mechanism F is closed, a predetermined amount of charge is instantaneously supplied from the charge supply mechanism B to the sample metal piece 1 via the relay 11, the FET switch 22, and the relay 28. After a predetermined minute time, the timer 20 is activated, the FET switch 22 stops the supply of electric charge, and at the same time, the relay 30 measures the potential change in the sample metal piece 1 as a relationship between polarization value η and time t. From this relationship between polarization value η and time t, an initial velocity factor is determined by a predetermined analysis method. Subsequently, the timer 27 connects the sample metal piece 1 and the constant voltage mechanism E, the potential of the sample metal piece 1 is forced to EcOrr, and the next rate factor can then be measured. Thereafter, multiple velocity factors can be measured accurately and quickly by similar operations.
In the second and subsequent measurements, it is not necessary to adjust the potential measuring meter D and the constant voltage mechanism E unless the corrosion potential EcOrr changes significantly due to long-term standing. Hereinafter, the corrosion status of a mild steel plate in city water was measured using an apparatus using the method of the present invention shown in FIG. 3 above.
まず試料金属片として表面積5cdの軟鋼板を腐食判定
セルAに設け72時間市水中に浸漬した後の腐食電位E
cOrrを電位測定計Dにより測定したところ−0.6
31Vvs.SCEであつた。First, a mild steel plate with a surface area of 5 cd was placed in corrosion determination cell A as a sample metal piece, and the corrosion potential E after being immersed in city water for 72 hours.
When cOrr was measured using potential meter D, it was -0.6.
31V vs. It was SCE.
続いて定電圧機構Eの可変抵抗40を調整し、定電圧機
構Eと腐食判定セルAとが接続された時、参照電極3を
基準に試料金属片の電位が−0.631Vvs.SCE
となる如し設定した。そこで分極抵抗を求めるために、
電荷供給機構B、電荷付与機構Fおよび遮断機構Gを用
いて、試料金属片1に3μcの電荷を付与し、電位差測
定機構Cにより解析した結果、ら=140ttF/Cd
,R,=2.2mdを得た。Subsequently, the variable resistor 40 of the constant voltage mechanism E is adjusted, and when the constant voltage mechanism E and the corrosion determination cell A are connected, the potential of the sample metal piece is -0.631Vvs. with reference to the reference electrode 3. SCE
I set it up so that Therefore, in order to find the polarization resistance,
A charge of 3 μc was applied to the sample metal piece 1 using the charge supply mechanism B, the charge application mechanism F, and the cutoff mechanism G, and as a result of analysis by the potential difference measurement mechanism C, ra = 140ttF/Cd
, R, = 2.2 md was obtained.
続いて試料金属片1の電位を強制的にEcOrrとした
後、同様の操作により300ttCの電荷を付与した結
果ターフエル勾配βa=62mVとなつた。再び試料金
属片1をE。OO,とした後、−300μCの電荷を付
与し、ターフエル勾配βcを求めた結果66mVとなつ
た。さらに上記測定されたRp,βA.βcを基に腐食
電流を求めるとIcOrr=6.3μA/Cr!lとな
つた。なお測定に要した時間は30秒程度であつた。ま
た上記と同様の測定を従来の浸漬法により求めた結果1
6mddとなり、IcOrrに換算すると6AμA/C
riiとなり、本発明方法によるものとほぼ一致した。
以上の如く本発明方法においては、分極抵抗、ターフエ
ル勾配βA,βcなどの腐食反応の速度因子を連続的に
迅速かつ正確に求める事ができ、特に腐食速度の比較的
遅い系における測定の場合極めて有効なものとなる。Subsequently, the potential of the sample metal piece 1 was forcibly set to EcOrr, and then a charge of 300 ttC was applied by the same operation, resulting in a Terfel gradient βa of 62 mV. E again sample metal piece 1. After setting the voltage to OO, a charge of -300 μC was applied, and the Terfel slope βc was determined to be 66 mV. Furthermore, the above-determined Rp, βA. Calculating the corrosion current based on βc, IcOrr=6.3μA/Cr! It became l. Note that the time required for the measurement was about 30 seconds. In addition, the same measurements as above were obtained using the conventional immersion method.Results 1
6mdd, converted to IcOrr is 6AμA/C
rii, which was almost the same as that obtained by the method of the present invention.
As described above, in the method of the present invention, rate factors of corrosion reactions, such as polarization resistance and terfel gradients βA and βc, can be determined continuously, quickly and accurately, and this is particularly true when measuring systems with relatively slow corrosion rates. It becomes valid.
第1図は本発明方法を用いた装置の原理図、第2図は本
発明方法を用いた場合の試料金属片の電位変化を示す特
性図、第3図は本発明方法を用いた具体的装置例を示す
回路図。
1・・・試料金属片、3・・・参照電極、A・・・腐食
判定セル、B・・・電荷供給機構、C・・・電位差測定
機構、D・・・電位測定計、E・・・定電圧機構。Figure 1 is a principle diagram of an apparatus using the method of the present invention, Figure 2 is a characteristic diagram showing the potential change of a sample metal piece when the method of the present invention is used, and Figure 3 is a diagram of a specific example of the apparatus using the method of the present invention. A circuit diagram showing an example of the device. DESCRIPTION OF SYMBOLS 1... Sample metal piece, 3... Reference electrode, A... Corrosion judgment cell, B... Charge supply mechanism, C... Potential difference measuring mechanism, D... Potential measuring meter, E... - Constant voltage mechanism.
Claims (1)
す試料金属片に所定量の電荷を瞬間的に付与し、前記試
料金属片の電位変化を前記試料金属片に近接配置した参
照電極により分極値η−時間tの関係として開回路状態
で得、この分極値η−時間tの関係から前記試料金属片
に関与する腐食反応の速度因子を測定する手段を少なく
とも2回繰り返して複数の腐食反応の速度因子を連続的
に測定するに当り、1つの腐食反応の速度因子の測定後
で、次の腐食反応の速度因子の測定前に、前記試料金属
片の電位を強制的に腐食電位E_c_o_r_rに戻す
事を特徴とした腐食反応の速度因子の測定方法。 2 特許請求の範囲第1項において、腐食反応の速度因
子として、分極抵抗R_Pを求める際に、試料金属片に
おける分極値の絶対値|η|が10mV以下になる如く
瞬間的に電荷を付与する事を特徴とした腐食反応の速度
因子の測定方法。 3 特許請求の範囲第1項において、腐食反応の速度因
子としてターフエル勾配βa、βcを求める際に、試料
金属片における分極値の絶対値|η|が60mV以上に
なる如く瞬時的に電荷を付与する事を特徴とした腐食反
応の速度因子の測定方法。[Scope of Claims] 1 A predetermined amount of electric charge is instantaneously applied to a sample metal piece exhibiting a corrosion potential E_c_o_r_r placed in a corrosion system, and a potential change of the sample metal piece is measured by a reference placed close to the sample metal piece. A method of obtaining a polarization value η-time t relationship with an electrode in an open circuit state and measuring a rate factor of a corrosion reaction involved in the sample metal piece from this polarization value η-time t relationship is repeated at least twice. In continuously measuring the rate factor of one corrosion reaction, after measuring the rate factor of one corrosion reaction and before measuring the rate factor of the next corrosion reaction, the potential of the sample metal piece is forcibly changed to A method for measuring the rate factor of a corrosion reaction, characterized by returning the potential to E_c_o_r_r. 2 In claim 1, when determining the polarization resistance R_P as a rate factor of the corrosion reaction, an electric charge is instantaneously applied so that the absolute value |η| of the polarization value in the sample metal piece becomes 10 mV or less. A method for measuring the rate factor of corrosion reactions characterized by: 3 In claim 1, when determining the terfel gradients βa and βc as rate factors of corrosion reaction, an electric charge is instantaneously applied so that the absolute value |η| of the polarization value in the sample metal piece becomes 60 mV or more. A method for measuring the rate factor of corrosion reactions.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP128879A JPS5937461B2 (en) | 1979-01-12 | 1979-01-12 | Method for measuring rate factors of corrosion reactions |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP128879A JPS5937461B2 (en) | 1979-01-12 | 1979-01-12 | Method for measuring rate factors of corrosion reactions |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5594142A JPS5594142A (en) | 1980-07-17 |
| JPS5937461B2 true JPS5937461B2 (en) | 1984-09-10 |
Family
ID=11497259
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP128879A Expired JPS5937461B2 (en) | 1979-01-12 | 1979-01-12 | Method for measuring rate factors of corrosion reactions |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5937461B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4593382B2 (en) * | 2004-06-22 | 2010-12-08 | 新日本製鐵株式会社 | Method for measuring corrosion rate of metal and method for preventing metal corrosion by this method |
-
1979
- 1979-01-12 JP JP128879A patent/JPS5937461B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5594142A (en) | 1980-07-17 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US6280603B1 (en) | Electrochemical noise technique for corrosion | |
| US4294667A (en) | Corrosion evaluation testing method of coated metallic material and apparatus employed therefor | |
| US4056445A (en) | Determination of corrosion rates by an electrochemical method | |
| JPS5926660B2 (en) | Measuring method of electroless plating reaction | |
| US3331021A (en) | A. c. corrosion-rate meter and method | |
| US3716460A (en) | Method for determining corrosion rate and meter therefor | |
| US4130464A (en) | Method of evaluating the corrosion rates of metals | |
| GB1580229A (en) | Method and means for determining the immersed surface area of an electrode of an electrochemical bath | |
| US3649499A (en) | Method for establishing the zones occurring in electrophoresis and for their quantitative determination | |
| US3436320A (en) | Method and apparatus for determination of redox current in redox solutions | |
| JPH071289B2 (en) | Method and apparatus for measuring conductivity without influence of polarization | |
| JPS5937461B2 (en) | Method for measuring rate factors of corrosion reactions | |
| JPS5822697B2 (en) | Method for measuring rate factors of corrosion reactions | |
| Loveland et al. | Cathode-Ray Oscilloscopic Investigation of Phenomena at Polarizable Mercury Electrodes. | |
| JPS5926663B2 (en) | Electroless plating reaction measuring device | |
| US4060461A (en) | Method and apparatus for correcting error in corrosion rate measurements | |
| JPS6239703B2 (en) | ||
| JPS5814981B2 (en) | Method for measuring rate factors of corrosion reactions | |
| RU2199734C2 (en) | Technique of electrochemical analysis | |
| JPS58187843A (en) | Apparatus for judging corrosion resistance of coating film | |
| US2842736A (en) | Polarograph | |
| RU18312U1 (en) | DEVICE FOR MEASURING THE VALUE AND DIRECT CURRENT DIRECTIONS IN METAL PIPELINES | |
| JPS6383659A (en) | Monitor for atmospheric corrosion | |
| SU1500911A1 (en) | Method of determining energy of ionization of the surface condition | |
| CA1124325A (en) | Method of evaluating the corrosion rate of metal |